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		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22779</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22779"/>
		<updated>2016-04-18T00:56:09Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* See also */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19 C}*({\tfrac{1}{2e-8 m} - \tfrac{1}{1e-10 m}}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;-14.3 V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
∆K + ∆U = &amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = 0 + (-e)(∆V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = (-1.6e-19 C)(-14.3 V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&#039;&#039;&#039;How is this topic connected to something that you are interested in?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am interested in robotic systems and building circuit boards and electrical systems for manufacturing robots. While studying this section in the book, I was able to connect back many of the concepts and calculations back to robotics and the electrical component of automated systems.&lt;br /&gt;
&lt;br /&gt;
[R] Since high school, I never really understood how to work with the voltmeter and what it measured, and I have always wanted to know, but although this particular wiki page did not go into the details and other branches of electric potential, it led me to find the answers to something I was interested in since high school, the concept of electric potential.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How is it connected to your major?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am a Mechanical Engineering major, so I will be dealing with the electrical components of machines when I work. Therefore, I have to know these certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
[R] As a biochemistry major, electric potential and electric potential difference is not particularly related to my major, but in chemistry classes, we use electrostatic potential maps (electrostatic potential energy maps) that shows the charge distributions throughout a molecule. Although the main use in electric potential is different in physics and biochemistry (where physicists use it identify the effect of the electric field at a location), I still found it interesting as the concept of electric potential (buildup) was being used in quite a different way. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Is there an interesting industrial application?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] Electrical potential is used to find the voltage across a path. This is useful when working with circuit components and attempting to manipulate the power output or current throughout a component.&lt;br /&gt;
&lt;br /&gt;
[R] Electric potential sensors are being used to detect a variety of electrical signals made by the human body, thus contributing to the field of electrophysiology.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential, in a way, started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientists finally began to understand how electric fields were actually affecting the charges and the surrounding environment. Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later, or 261 years ago for us, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature that was viewed quite abstractly.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack. Electricity wasn&#039;t a very well understood phenomenon at that point, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity. Although Franklin is often coined the father of electricity, after he set the foundations of electricity, many other scientists contributed his or her research in the advancement of electricity and eventually led to the discovery of electric potential and potential difference.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Like mentioned multiple times throughout the page, although electric potential is a huge and important topic, it has many branches, which makes the concept of electric potential difficult to stand alone. Even with this page, to support the concept of electric potential, many crucial branches of the topic appeared, like potential difference (which also branched into [[http://www.physicsbook.gatech.edu/Potential_Difference_Path_Independence,_claimed_by_Aditya_Mohile Potential Difference Path Independence]], [[http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field Potential Difference In A Uniform Field]], and [[http://www.physicsbook.gatech.edu/Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field Potential Difference In A Nonuniform Field]]). &lt;br /&gt;
&lt;br /&gt;
===External Links===&lt;br /&gt;
&lt;br /&gt;
[1] https://www.khanacademy.org/test-prep/mcat/physical-processes/electrostatics-1/v/electric-potential-at-a-point-in-space&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=pcWz4tP_zUw&lt;br /&gt;
&lt;br /&gt;
[3] https://www.youtube.com/watch?v=Vpa_uApmNoo&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[1] &amp;quot;Benjamin Franklin and Electricity.&amp;quot; Benjamin Franklin and Electricity. N.p., n.d. Web. 17 Apr. 2016. &amp;lt;http://www.americaslibrary.gov/aa/franklinb/aa_franklinb_electric_1.html&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[2] Bottyan, Thomas. &amp;quot;Electrostatic Potential Maps.&amp;quot; Chemwiki. N.p., 02 Oct. 2013. Web. 17 Apr. 2016. &amp;lt;http://chemwiki.ucdavis.edu/Core/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[3] &amp;quot;Electric Potential Difference.&amp;quot; Electric Potential Difference. The Physics Classroom, n.d. Web. 14 Apr. 2016. &amp;lt;http://www.physicsclassroom.com/class/circuits/Lesson-1/Electric-Potential-Difference&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[4] Harland, C. J., T. D. Clark, and R. J. Prance. &amp;quot;Applications of Electric Potential (Displacement Current) Sensors in Human Body Electrophysiology.&amp;quot; International Society for Industrial Process Tomography, n.d. Web. 16 Apr. 2016. &amp;lt;http://www.isipt.org/world-congress/3/269.html&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[5] Sherwood, Bruce A. &amp;quot;2.1 The Momentum Principle.&amp;quot; Matter &amp;amp; Interactions. By Ruth W. Chabay. 4th ed. Vol. 1. N.p.: John Wiley &amp;amp; Sons, 2015. 45-50. Print. Modern Mechanics.&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22775</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22775"/>
		<updated>2016-04-18T00:51:58Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* See also */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19 C}*({\tfrac{1}{2e-8 m} - \tfrac{1}{1e-10 m}}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;-14.3 V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
∆K + ∆U = &amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = 0 + (-e)(∆V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = (-1.6e-19 C)(-14.3 V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&#039;&#039;&#039;How is this topic connected to something that you are interested in?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am interested in robotic systems and building circuit boards and electrical systems for manufacturing robots. While studying this section in the book, I was able to connect back many of the concepts and calculations back to robotics and the electrical component of automated systems.&lt;br /&gt;
&lt;br /&gt;
[R] Since high school, I never really understood how to work with the voltmeter and what it measured, and I have always wanted to know, but although this particular wiki page did not go into the details and other branches of electric potential, it led me to find the answers to something I was interested in since high school, the concept of electric potential.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How is it connected to your major?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am a Mechanical Engineering major, so I will be dealing with the electrical components of machines when I work. Therefore, I have to know these certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
[R] As a biochemistry major, electric potential and electric potential difference is not particularly related to my major, but in chemistry classes, we use electrostatic potential maps (electrostatic potential energy maps) that shows the charge distributions throughout a molecule. Although the main use in electric potential is different in physics and biochemistry (where physicists use it identify the effect of the electric field at a location), I still found it interesting as the concept of electric potential (buildup) was being used in quite a different way. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Is there an interesting industrial application?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] Electrical potential is used to find the voltage across a path. This is useful when working with circuit components and attempting to manipulate the power output or current throughout a component.&lt;br /&gt;
&lt;br /&gt;
[R] Electric potential sensors are being used to detect a variety of electrical signals made by the human body, thus contributing to the field of electrophysiology.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential, in a way, started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientists finally began to understand how electric fields were actually affecting the charges and the surrounding environment. Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later, or 261 years ago for us, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature that was viewed quite abstractly.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack. Electricity wasn&#039;t a very well understood phenomenon at that point, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity. Although Franklin is often coined the father of electricity, after he set the foundations of electricity, many other scientists contributed his or her research in the advancement of electricity and eventually led to the discovery of electric potential and potential difference.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Like mentioned multiple times throughout the page, although electric potential is a huge and important topic, it has many branches, which makes the concept of electric potential difficult to stand alone. Even with this page, to support the concept of electric potential, many crucial branches of the topic appeared, like potential difference (which also branched into [[http://www.physicsbook.gatech.edu/Potential_Difference_Path_Independence,_claimed_by_Aditya_Mohile Potential Difference Path Independence]], [[http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field Potential Difference In A Uniform Field]], and [[http://www.physicsbook.gatech.edu/Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field Potential Difference In A Nonuniform Field]]). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[1] &amp;quot;Benjamin Franklin and Electricity.&amp;quot; Benjamin Franklin and Electricity. N.p., n.d. Web. 17 Apr. 2016. &amp;lt;http://www.americaslibrary.gov/aa/franklinb/aa_franklinb_electric_1.html&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[2] Bottyan, Thomas. &amp;quot;Electrostatic Potential Maps.&amp;quot; Chemwiki. N.p., 02 Oct. 2013. Web. 17 Apr. 2016. &amp;lt;http://chemwiki.ucdavis.edu/Core/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[3] &amp;quot;Electric Potential Difference.&amp;quot; Electric Potential Difference. The Physics Classroom, n.d. Web. 14 Apr. 2016. &amp;lt;http://www.physicsclassroom.com/class/circuits/Lesson-1/Electric-Potential-Difference&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[4] Harland, C. J., T. D. Clark, and R. J. Prance. &amp;quot;Applications of Electric Potential (Displacement Current) Sensors in Human Body Electrophysiology.&amp;quot; International Society for Industrial Process Tomography, n.d. Web. 16 Apr. 2016. &amp;lt;http://www.isipt.org/world-congress/3/269.html&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[5] Sherwood, Bruce A. &amp;quot;2.1 The Momentum Principle.&amp;quot; Matter &amp;amp; Interactions. By Ruth W. Chabay. 4th ed. Vol. 1. N.p.: John Wiley &amp;amp; Sons, 2015. 45-50. Print. Modern Mechanics.&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22761</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22761"/>
		<updated>2016-04-18T00:46:21Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19 C}*({\tfrac{1}{2e-8 m} - \tfrac{1}{1e-10 m}}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;-14.3 V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
∆K + ∆U = &amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = 0 + (-e)(∆V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = (-1.6e-19 C)(-14.3 V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&#039;&#039;&#039;How is this topic connected to something that you are interested in?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am interested in robotic systems and building circuit boards and electrical systems for manufacturing robots. While studying this section in the book, I was able to connect back many of the concepts and calculations back to robotics and the electrical component of automated systems.&lt;br /&gt;
&lt;br /&gt;
[R] Since high school, I never really understood how to work with the voltmeter and what it measured, and I have always wanted to know, but although this particular wiki page did not go into the details and other branches of electric potential, it led me to find the answers to something I was interested in since high school, the concept of electric potential.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How is it connected to your major?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am a Mechanical Engineering major, so I will be dealing with the electrical components of machines when I work. Therefore, I have to know these certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
[R] As a biochemistry major, electric potential and electric potential difference is not particularly related to my major, but in chemistry classes, we use electrostatic potential maps (electrostatic potential energy maps) that shows the charge distributions throughout a molecule. Although the main use in electric potential is different in physics and biochemistry (where physicists use it identify the effect of the electric field at a location), I still found it interesting as the concept of electric potential (buildup) was being used in quite a different way. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Is there an interesting industrial application?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] Electrical potential is used to find the voltage across a path. This is useful when working with circuit components and attempting to manipulate the power output or current throughout a component.&lt;br /&gt;
&lt;br /&gt;
[R] Electric potential sensors are being used to detect a variety of electrical signals made by the human body, thus contributing to the field of electrophysiology.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential, in a way, started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientists finally began to understand how electric fields were actually affecting the charges and the surrounding environment. Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later, or 261 years ago for us, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature that was viewed quite abstractly.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack. Electricity wasn&#039;t a very well understood phenomenon at that point, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity. Although Franklin is often coined the father of electricity, after he set the foundations of electricity, many other scientists contributed his or her research in the advancement of electricity and eventually led to the discovery of electric potential and potential difference.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[1] &amp;quot;Benjamin Franklin and Electricity.&amp;quot; Benjamin Franklin and Electricity. N.p., n.d. Web. 17 Apr. 2016. &amp;lt;http://www.americaslibrary.gov/aa/franklinb/aa_franklinb_electric_1.html&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[2] Bottyan, Thomas. &amp;quot;Electrostatic Potential Maps.&amp;quot; Chemwiki. N.p., 02 Oct. 2013. Web. 17 Apr. 2016. &amp;lt;http://chemwiki.ucdavis.edu/Core/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[3] &amp;quot;Electric Potential Difference.&amp;quot; Electric Potential Difference. The Physics Classroom, n.d. Web. 14 Apr. 2016. &amp;lt;http://www.physicsclassroom.com/class/circuits/Lesson-1/Electric-Potential-Difference&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[4] Harland, C. J., T. D. Clark, and R. J. Prance. &amp;quot;Applications of Electric Potential (Displacement Current) Sensors in Human Body Electrophysiology.&amp;quot; International Society for Industrial Process Tomography, n.d. Web. 16 Apr. 2016. &amp;lt;http://www.isipt.org/world-congress/3/269.html&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[5] Sherwood, Bruce A. &amp;quot;2.1 The Momentum Principle.&amp;quot; Matter &amp;amp; Interactions. By Ruth W. Chabay. 4th ed. Vol. 1. N.p.: John Wiley &amp;amp; Sons, 2015. 45-50. Print. Modern Mechanics.&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22760</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22760"/>
		<updated>2016-04-18T00:45:52Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19 C}*({\tfrac{1}{2e-8 m} - \tfrac{1}{1e-10 m}}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;-14.3 V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
∆K + ∆U = &amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = 0 + (-e)(∆V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = (-1.6e-19 C)(-14.3 V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&#039;&#039;&#039;How is this topic connected to something that you are interested in?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am interested in robotic systems and building circuit boards and electrical systems for manufacturing robots. While studying this section in the book, I was able to connect back many of the concepts and calculations back to robotics and the electrical component of automated systems.&lt;br /&gt;
&lt;br /&gt;
[R] Since high school, I never really understood how to work with the voltmeter and what it measured, and I have always wanted to know, but although this particular wiki page did not go into the details and other branches of electric potential, it led me to find the answers to something I was interested in since high school, the concept of electric potential.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How is it connected to your major?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am a Mechanical Engineering major, so I will be dealing with the electrical components of machines when I work. Therefore, I have to know these certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
[R] As a biochemistry major, electric potential and electric potential difference is not particularly related to my major, but in chemistry classes, we use electrostatic potential maps (electrostatic potential energy maps) that shows the charge distributions throughout a molecule. Although the main use in electric potential is different in physics and biochemistry (where physicists use it identify the effect of the electric field at a location), I still found it interesting as the concept of electric potential (buildup) was being used in quite a different way. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Is there an interesting industrial application?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] Electrical potential is used to find the voltage across a path. This is useful when working with circuit components and attempting to manipulate the power output or current throughout a component.&lt;br /&gt;
&lt;br /&gt;
[R] Electric potential sensors are being used to detect a variety of electrical signals made by the human body, thus contributing to the field of electrophysiology.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential, in a way, started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientists finally began to understand how electric fields were actually affecting the charges and the surrounding environment. Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later, or 261 years ago for us, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature that was viewed quite abstractly.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack. Electricity wasn&#039;t a very well understood phenomenon at that point, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity. Although Franklin is often coined the father of electricity, after he set the foundations of electricity, many other scientists contributed his or her research in the advancement of electricity and eventually led to the discovery of electric potential and potential difference.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[1] Bottyan, Thomas. &amp;quot;Electrostatic Potential Maps.&amp;quot; Chemwiki. N.p., 02 Oct. 2013. Web. 17 Apr. 2016. &amp;lt;http://chemwiki.ucdavis.edu/Core/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[2] &amp;quot;Electric Potential Difference.&amp;quot; Electric Potential Difference. The Physics Classroom, n.d. Web. 14 Apr. 2016. &amp;lt;http://www.physicsclassroom.com/class/circuits/Lesson-1/Electric-Potential-Difference&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[3] Harland, C. J., T. D. Clark, and R. J. Prance. &amp;quot;Applications of Electric Potential (Displacement Current) Sensors in Human Body Electrophysiology.&amp;quot; International Society for Industrial Process Tomography, n.d. Web. 16 Apr. 2016. &amp;lt;http://www.isipt.org/world-congress/3/269.html&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[4] Sherwood, Bruce A. &amp;quot;2.1 The Momentum Principle.&amp;quot; Matter &amp;amp; Interactions. By Ruth W. Chabay. 4th ed. Vol. 1. N.p.: John Wiley &amp;amp; Sons, 2015. 45-50. Print. Modern Mechanics.&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22752</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22752"/>
		<updated>2016-04-18T00:36:27Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19 C}*({\tfrac{1}{2e-8 m} - \tfrac{1}{1e-10 m}}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;-14.3 V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
∆K + ∆U = &amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = 0 + (-e)(∆V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = (-1.6e-19 C)(-14.3 V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&#039;&#039;&#039;How is this topic connected to something that you are interested in?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am interested in robotic systems and building circuit boards and electrical systems for manufacturing robots. While studying this section in the book, I was able to connect back many of the concepts and calculations back to robotics and the electrical component of automated systems.&lt;br /&gt;
&lt;br /&gt;
[R] Since high school, I never really understood how to work with the voltmeter and what it measured, and I have always wanted to know, but although this particular wiki page did not go into the details and other branches of electric potential, it led me to find the answers to something I was interested in since high school, the concept of electric potential.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How is it connected to your major?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am a Mechanical Engineering major, so I will be dealing with the electrical components of machines when I work. Therefore, I have to know these certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
[R] As a biochemistry major, electric potential and electric potential difference is not particularly related to my major, but in chemistry classes, we use electrostatic potential maps (electrostatic potential energy maps) that shows the charge distributions throughout a molecule. Although the main use in electric potential is different in physics and biochemistry (where physicists use it identify the effect of the electric field at a location), I still found it interesting as the concept of electric potential (buildup) was being used in quite a different way. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Is there an interesting industrial application?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] Electrical potential is used to find the voltage across a path. This is useful when working with circuit components and attempting to manipulate the power output or current throughout a component.&lt;br /&gt;
&lt;br /&gt;
[R] Electric potential sensors are being used to detect a variety of electrical signals made by the human body, thus contributing to the field of electrophysiology.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[1] Bottyan, Thomas. &amp;quot;Electrostatic Potential Maps.&amp;quot; Chemwiki. N.p., 02 Oct. 2013. Web. 17 Apr. 2016. &amp;lt;http://chemwiki.ucdavis.edu/Core/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[2] &amp;quot;Electric Potential Difference.&amp;quot; Electric Potential Difference. The Physics Classroom, n.d. Web. 14 Apr. 2016. &amp;lt;http://www.physicsclassroom.com/class/circuits/Lesson-1/Electric-Potential-Difference&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[3] Harland, C. J., T. D. Clark, and R. J. Prance. &amp;quot;Applications of Electric Potential (Displacement Current) Sensors in Human Body Electrophysiology.&amp;quot; International Society for Industrial Process Tomography, n.d. Web. 16 Apr. 2016. &amp;lt;http://www.isipt.org/world-congress/3/269.html&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[4] Sherwood, Bruce A. &amp;quot;2.1 The Momentum Principle.&amp;quot; Matter &amp;amp; Interactions. By Ruth W. Chabay. 4th ed. Vol. 1. N.p.: John Wiley &amp;amp; Sons, 2015. 45-50. Print. Modern Mechanics.&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22730</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22730"/>
		<updated>2016-04-18T00:28:13Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Connectedness */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19 C}*({\tfrac{1}{2e-8 m} - \tfrac{1}{1e-10 m}}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;-14.3 V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
∆K + ∆U = &amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = 0 + (-e)(∆V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = (-1.6e-19 C)(-14.3 V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&#039;&#039;&#039;How is this topic connected to something that you are interested in?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am interested in robotic systems and building circuit boards and electrical systems for manufacturing robots. While studying this section in the book, I was able to connect back many of the concepts and calculations back to robotics and the electrical component of automated systems.&lt;br /&gt;
&lt;br /&gt;
[R] Since high school, I never really understood how to work with the voltmeter and what it measured, and I have always wanted to know, but although this particular wiki page did not go into the details and other branches of electric potential, it led me to find the answers to something I was interested in since high school, the concept of electric potential.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How is it connected to your major?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] I am a Mechanical Engineering major, so I will be dealing with the electrical components of machines when I work. Therefore, I have to know these certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
[R] As a biochemistry major, electric potential and electric potential difference is not particularly related to my major, but in chemistry classes, we use electrostatic potential maps (electrostatic potential energy maps) that shows the charge distributions throughout a molecule. Although the main use in electric potential is different in physics and biochemistry (where physicists use it identify the effect of the electric field at a location), I still found it interesting as the concept of electric potential (buildup) was being used in quite a different way. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Is there an interesting industrial application?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[A] Electrical potential is used to find the voltage across a path. This is useful when working with circuit components and attempting to manipulate the power output or current throughout a component.&lt;br /&gt;
&lt;br /&gt;
[R] Electric potential sensors are being used to detect a variety of electrical signals made by the human body, thus contributing to the field of electrophysiology.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22729</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22729"/>
		<updated>2016-04-18T00:27:57Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Connectedness */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19 C}*({\tfrac{1}{2e-8 m} - \tfrac{1}{1e-10 m}}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;-14.3 V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
∆K + ∆U = &amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = 0 + (-e)(∆V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = (-1.6e-19 C)(-14.3 V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&#039;&#039;&#039;How is this topic connected to something that you are interested in?&#039;&#039;&#039;&lt;br /&gt;
[A] I am interested in robotic systems and building circuit boards and electrical systems for manufacturing robots. While studying this section in the book, I was able to connect back many of the concepts and calculations back to robotics and the electrical component of automated systems.&lt;br /&gt;
&lt;br /&gt;
[R] Since high school, I never really understood how to work with the voltmeter and what it measured, and I have always wanted to know, but although this particular wiki page did not go into the details and other branches of electric potential, it led me to find the answers to something I was interested in since high school, the concept of electric potential.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How is it connected to your major?&#039;&#039;&#039;&lt;br /&gt;
[A] I am a Mechanical Engineering major, so I will be dealing with the electrical components of machines when I work. Therefore, I have to know these certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
[R] As a biochemistry major, electric potential and electric potential difference is not particularly related to my major, but in chemistry classes, we use electrostatic potential maps (electrostatic potential energy maps) that shows the charge distributions throughout a molecule. Although the main use in electric potential is different in physics and biochemistry (where physicists use it identify the effect of the electric field at a location), I still found it interesting as the concept of electric potential (buildup) was being used in quite a different way. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Is there an interesting industrial application?&#039;&#039;&#039;&lt;br /&gt;
[A] Electrical potential is used to find the voltage across a path. This is useful when working with circuit components and attempting to manipulate the power output or current throughout a component.&lt;br /&gt;
&lt;br /&gt;
[R] Electric potential sensors are being used to detect a variety of electrical signals made by the human body, thus contributing to the field of electrophysiology.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22699</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22699"/>
		<updated>2016-04-18T00:10:02Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19 C}*({\tfrac{1}{2e-8 m} - \tfrac{1}{1e-10 m}}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;-14.3 V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
∆K + ∆U = &amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = 0 + (-e)(∆V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = (-1.6e-19 C)(-14.3 V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22691</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22691"/>
		<updated>2016-04-18T00:05:57Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19C}*({\tfrac{1}{2e-8m} - \tfrac{1}{1e-10}}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;{-14.3 V}&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
∆K + ∆U = &amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = 0 + (-e)(∆V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = (-1.6e-19 C)(-14.3 V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22690</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22690"/>
		<updated>2016-04-18T00:05:16Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19C}*({\tfrac{1}{2e-8m} - \tfrac{1}{1e-10}}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = &#039;&#039;&#039;{-14.3 V}&#039;&#039;&#039;&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
∆K + ∆U = &amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = 0 + (-e)(∆V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = (-1.6e-19 C)(-14.3 V)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{W}_{ext}&amp;lt;/math&amp;gt; = &#039;&#039;&#039;2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22687</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22687"/>
		<updated>2016-04-18T00:01:20Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19C}*({\tfrac{1}{2e-8m} - \tfrac{1}{1e-10}}) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22686</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22686"/>
		<updated>2016-04-18T00:00:52Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19C}*{\tfrac{1}{2e-8m} - \tfrac{1}{1e-10}} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22685</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22685"/>
		<updated>2016-04-18T00:00:38Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19C}*{\tfrac{1}{2e-8m} - \tfrac{1}{1e-10}} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22684</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22684"/>
		<updated>2016-04-18T00:00:02Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = \tfrac{1}{4π{ε}_{0}}*{1.6e-19C}*{\tfrac{1}{2e-8m} - \tfrac{1}{1e-10}}&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22681</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22681"/>
		<updated>2016-04-17T23:58:19Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}}*\tfrac{Q}{{x}^{2}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22679</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22679"/>
		<updated>2016-04-17T23:57:37Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_{1e-10}^{2e-8} \tfrac{1}{4π{ε}_{0}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22677</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22677"/>
		<updated>2016-04-17T23:57:09Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_1e-10^2e-8 \tfrac{1}{4π{ε}_{0}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22676</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22676"/>
		<updated>2016-04-17T23:56:52Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &amp;lt;math&amp;gt;\vec{&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_1e-10^2e-8 \tfrac{1}{4π{ε}_{0}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22675</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22675"/>
		<updated>2016-04-17T23:56:27Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = &amp;lt;-(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
Suppose that from x=0 to x=3 the electric field is uniform and given by &amp;lt;math&amp;gt;\vec{&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -\int_1e-10^2e-8 \tfrac{1}{4π{ε}_{0}} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22549</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22549"/>
		<updated>2016-04-17T21:48:58Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = &amp;lt;-(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
(1) &amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22548</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22548"/>
		<updated>2016-04-17T21:48:19Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l} = {&amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = &amp;lt;-(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
(1) &amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22523</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22523"/>
		<updated>2016-04-17T21:32:19Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l} = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = &amp;lt;-(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
(1) &amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22522</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22522"/>
		<updated>2016-04-17T21:31:19Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = &amp;lt;-(500 N/C * 0.6 m + 0*0 + 0*0)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
(1) &amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22520</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22520"/>
		<updated>2016-04-17T21:30:12Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a capacitor, the negative charges are located on the left plate, and the positive charges are located on the right plate. Location A is at the left end of the capacitor, and Location B is at the right end of the capacitor, or in other words, Location A and B are only different in terms of their x component location. The path moves from A to B. What is the direction of the electric field? Is the potential difference positive or negative? [Hint: Draw a picture!]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: The electric field is to the left. The potential difference is increasing, or is positive.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
The electric field always moves away from the positive charge and towards the negative charge, which means the electric field in this example is to the left. Because the direction and the electric field and the direction of the path are opposite, the potential difference is increasing, or is positive. &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -(500 N/C * 0.6 m + 0*0 + 0*0)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -300 V&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -14.3 V ; 2.3e-18 J&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
(1) &amp;lt;math&amp;gt;∆{V} = -\int_C^D {E}_{x} \, dx &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Number_1.jpeg&amp;diff=22504</id>
		<title>File:Number 1.jpeg</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Number_1.jpeg&amp;diff=22504"/>
		<updated>2016-04-17T21:17:57Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22501</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22501"/>
		<updated>2016-04-17T21:16:57Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-), or the potential is decreasing. If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+), or the potential is increasing. If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:ep1.jpg]]&lt;br /&gt;
[[File:ep2.jpg]]&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
           = -(500 N/C * 0.6 m + 0*0 + 0*0)&lt;br /&gt;
&lt;br /&gt;
           = -300 V&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
[[File:Example22.jpg]]&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22490</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22490"/>
		<updated>2016-04-17T21:11:36Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-). If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+). If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Calculate the difference in electric potential between two locations A, which is at &amp;lt;-0.4, 0,0&amp;gt;m, and B, which is at &amp;lt;0.2,0,0&amp;gt;m. The electric field in the location is &amp;lt;500,0,0&amp;gt; N/C.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: -300V&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt; = &amp;lt;0.2,0,0&amp;gt;m - &amp;lt;-0.4,0,0&amp;gt;m = &amp;lt;0.6,0,0&amp;gt;m&lt;br /&gt;
&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&lt;br /&gt;
           = -(500 N/C * 0.6 m + 0*0 + 0*0)&lt;br /&gt;
           = -300 V&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
[[File:Example22.jpg]]&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22474</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22474"/>
		<updated>2016-04-17T21:03:53Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-). If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+). If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
[[File:DDDDDDD.jpg]]&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
[[File:Example22.jpg]]&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22461</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22461"/>
		<updated>2016-04-17T20:55:35Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-). If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+). If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
[[File:DDDDDDD.jpg]]&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
[[File:Example22.jpg]]&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22459</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22459"/>
		<updated>2016-04-17T20:54:47Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-). If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+). If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE Electric Potential: Visualizing Voltage with 3D animations]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
[[File:DDDDDDD.jpg]]&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
[[File:Example22.jpg]]&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22458</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22458"/>
		<updated>2016-04-17T20:53:53Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: Rmohammed7&#039;&#039;&#039;&lt;br /&gt;
&#039;&#039;&#039;REVISED BY: HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric potential is a rather difficult concept as it is usually accompanied by other topics. For example, electric potential is not the same as electric potential energy as electric potential is defined as the total potential energy per charge and is basically used to describe the electric field&#039;s effect at a certain location. In other words, electric potential is purely dependent on the electric field (whether it is uniform or nonuniform) and the location, whereas the electric potential energy also depends on the amount of charge the object in the system is experiencing. Also, although electric potential is an important topic to learn, most problems encountered will not ask to find just the &amp;quot;electric potential,&amp;quot; instead, questions will most likely ask for the &amp;quot;electric potential difference.&amp;quot; This is because electric potential is measured using different locations, or more specifically pathways between the different locations, so instead of determining the electric potential of location A and the electric potential of final location B, it would make more sense to determine the &amp;quot;difference in electric potential between locations A and B.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Like mentioned in the Main Idea, instead of electric potential, in most cases, electric potential difference is needed to be found. The general equation for the potential difference is &amp;lt;math&amp;gt;∆{{U}_{electric}} = {q} * ∆{V} &amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&amp;lt;math&amp;gt;∆{{U}_{electric}}&amp;lt;/math&amp;gt;&#039;&#039;&#039; is the electric potential energy, which is measured in Joules (J). &#039;&#039;&#039;q&#039;&#039;&#039; is the charge of the particle moving through the path of the electric potential difference, which is measured in coulombs (C). &#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V).&lt;br /&gt;
&lt;br /&gt;
Aside from the general equation, the electric potential difference can also be found in other ways. The potential difference in an &#039;&#039;&#039;uniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -({E}_{x}∆{x} + {E}_{y}∆{y} + {E}_{z}∆{z})&amp;lt;/math&amp;gt;&#039;&#039;&#039;, which can also be written as &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;∆V&#039;&#039;&#039; is the electric potential difference, which is measured in Joules per Coulomb (J/C), or just Volts (V). &#039;&#039;&#039;E&#039;&#039;&#039; is the electric field, which is measured in Newtons per Coulomb (N/C), and it is important to note that the different direction components of the electric field are used in the equation. &#039;&#039;&#039;l&#039;&#039;&#039; (or the &#039;&#039;&#039;x&#039;&#039;&#039;, &#039;&#039;&#039;y&#039;&#039;&#039;, &#039;&#039;&#039;z&#039;&#039;&#039;) is the distance between the two described locations, which is measured in meters, and x, y, and z, are the different components of the difference.&lt;br /&gt;
&lt;br /&gt;
The electric potential difference in a &#039;&#039;&#039;nonuniform field&#039;&#039;&#039; is &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -∑ \vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;. The different parts in this particular equation resembles the equation for the potential difference in an uniform field, except that with the nonuniform field, the potential difference in the different fields are summed up. This situation can be quite easy, but when the system gets difficult, first, choose a path and divide it into smaller pieces of &#039;&#039;&#039;&amp;lt;math&amp;gt;∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039;; second, write an expression for &#039;&#039;&#039;&amp;lt;math&amp;gt;∆{V} = -\vec{E}·∆\vec{l}&amp;lt;/math&amp;gt;&#039;&#039;&#039; of one piece; third, add up the contributions of all the pieces; last, check the result to make sure the magnitude, direction, and units make sense.&lt;br /&gt;
&lt;br /&gt;
Aside from just calculating the value of the electric potential difference, determining the sign is also quite crucial to be successful. If the path being considered is in the same direction as the electric field, then the sign with be negative (-). If the path being considered is in the opposite direction as the electric field, then the sign will be positive (+). If the path being considered is perpendicular to the electric field, then the potential difference will just be zero and have no direction. With these simple tips, the direction of the potential difference can be rechecked with the answer calculated using vectors. &lt;br /&gt;
&lt;br /&gt;
Also, when working with different situations, it is nice to keep in mind that in a conductor, the electric field is zero. Therefore, the potential difference is zero as well. In an insulator, the electric field is &#039;&#039;&#039;&amp;lt;math&amp;gt;{E}_{applied} / K&amp;lt;/math&amp;gt;&#039;&#039;&#039; where &#039;&#039;&#039;K&#039;&#039;&#039; is the dielectric constant. Also, the round trip potential difference is always zero, or in other words, if you start from a certain point and end at the same point, then, the potential difference will be zero. &lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Click on the link to see Electric Potential through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/0a7e486c94 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
Watch this video for a more visual approach! &lt;br /&gt;
&lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
[[File:DDDDDDD.jpg]]&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
[[File:Example22.jpg]]&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22286</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=22286"/>
		<updated>2016-04-17T18:36:47Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;AUTHOR: &lt;br /&gt;
CLAIMED BY HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This page discusses the Electric Potential and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== The Main Idea ==&lt;br /&gt;
&lt;br /&gt;
Electric Potential is the potential energy associated with interacting charged particles that create electric fields and impact each other through these fields. Electric potential is found by travleing across a path through a uniform or nonuniform electric field.&lt;br /&gt;
Potential energy can be thought of as the energy that is stored within a system that will soon be utilized for some other action. It is the opposite of kinetic energy, which is the energy associated with something in motion. For studying electric potential of charged particles, we first need to understand that sigle particles themselves dont really have potential energy. When we analyze a system for electric potential, we need to choose a a system containing one or more objects/particle/etc.. The potential energy will be derived from the interactions between the objects within our system. On the other hand, kineic energy will be related to the work done by the surroundings of the system.This value can be changed if the work done is positive or negative. Therefore, the change in kineic energy of our system must be equal to the work done by the surroundings. Work can be derived by calculating the dot product of the force and displacement. Potential energy is asscociated with the internal work of the system, that is, work that is done by objects counted within the system. Therefore, the potential energy change of a system is equal to the negative interior work. Now, to put all this together, we have the conservation of energy rule. This states that energy cannot be created or destroyed between events of interacting objects. That is why delta K plus delta U must be zero.&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
When calculating the changes in potential energy of a system, it would be useful to find a quantity that is unique from the charge of out particle. After finding this variable, we can multiply it by the charge to get or delta U. Regardelss of whether our particle is a proton or electron, our change in potential energy formula boils down to &#039;&#039;(some charge)*(-Ex*deltaX)&#039;&#039;. The part that is the same in both cases is the Ex times deltaX. This is called the difference of electric potential between 2 locations. This value is usually notated as DeltaV, with units of volts. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Finding Potential Differences in Uniform Fields.&lt;br /&gt;
DeltaV = -Efield (dot product) deltaL   &lt;br /&gt;
Remember that dot product of 2 vetors = (magnitude of vector1)*(magnitude of vector 2)*cos(angle between them)&lt;br /&gt;
&lt;br /&gt;
How to determine the sign of potential difference:&lt;br /&gt;
If your path that you are considering goes in the same direction as the electric field, the sign will be negative (-)&lt;br /&gt;
If your path goes in the opposite direction of the electric field, the sign will be positive. (+)&lt;br /&gt;
If the path is perpendicular to the electric field, it will be zero.&lt;br /&gt;
&lt;br /&gt;
Finding deltaV in nonuniform Fields:&lt;br /&gt;
DeltaV = -integral from (initial position to final position) of [Efield dot product deltaL]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Some Key Points&#039;&#039;&#039;&lt;br /&gt;
- In a conductor we know that the electric field is zero. Therefore, the potential difference is zero as well(since it is constant everywhere).&lt;br /&gt;
- The potential difference between 2 locations does not depend on the path taken between the locations.&lt;br /&gt;
- Round Trip Potential Difference is always zero, If you start your path from a certain points and end your path at the same point, deltaV will be zero.&lt;br /&gt;
- In an insultor, the electric field is (Eapplied/K)m where K is a dielectric constant.Therefore, DeltaV = (deltaV inside vaccum)/K&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Watch this video for a more visual approach &lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
[[File:DDDDDDD.jpg]]&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
[[File:Example22.jpg]]&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=20628</id>
		<title>Electric Potential</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Electric_Potential&amp;diff=20628"/>
		<updated>2016-03-15T00:08:44Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;CLAIMED BY HAYOUNG KIM (SPRING 2016)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electric Potential is the potential energy associated with interacting charged particles that create electric fields and impact each other through these fields. Electric potential is found by travleing across a path through a uniform or nonuniform electric field.&lt;br /&gt;
&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
== Review of Potential Energy ==&lt;br /&gt;
&lt;br /&gt;
--editing in progress[[User:Rakin Mohammed|rmohammed7]] ([[User talk:Qwu80|talk]]) 17:18, 25 October 2015 (EDT)&lt;br /&gt;
Short Description of Topic&lt;br /&gt;
&lt;br /&gt;
Potential energy can be thought of as the energy that is stored within a system that will soon be utilized for some other action. It is the opposite of kinetic energy, which is the energy associated with something in motion. For studying electric potential of charged particles, we first need to understand that sigle particles themselves dont really have potential energy. When we analyze a system for electric potential, we need to choose a a system containing one or more objects/particle/etc.. The potential energy will be derived from the interactions between the objects within our system. On the other hand, kineic energy will be related to the work done by the surroundings of the system.This value can be changed if the work done is positive or negative. Therefore, the change in kineic energy of our system must be equal to the work done by the surroundings. Work can be derived by calculating the dot product of the force and displacement. Potential energy is asscociated with the internal work of the system, that is, work that is done by objects counted within the system. Therefore, the potential energy change of a system is equal to the negative interior work. Now, to put all this together, we have the conservation of energy rule. This states that energy cannot be created or destroyed between events of interacting objects. That is why delta K plus delta U must be zero.&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
When calculating the changes in potential energy of a system, it would be useful to find a quantity that is unique from the charge of out particle. After finding this variable, we can multiply it by the charge to get or delta U. Regardelss of whether our particle is a proton or electron, our change in potential energy formula boils down to &#039;&#039;(some charge)*(-Ex*deltaX)&#039;&#039;. The part that is the same in both cases is the Ex times deltaX. This is called the difference of electric potential between 2 locations. This value is usually notated as DeltaV, with units of volts. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
Finding Potential Differences in Uniform Fields.&lt;br /&gt;
DeltaV = -Efield (dot product) deltaL   &lt;br /&gt;
Remember that dot product of 2 vetors = (magnitude of vector1)*(magnitude of vector 2)*cos(angle between them)&lt;br /&gt;
&lt;br /&gt;
How to determine the sign of potential difference:&lt;br /&gt;
If your path that you are considering goes in the same direction as the electric field, the sign will be negative (-)&lt;br /&gt;
If your path goes in the opposite direction of the electric field, the sign will be positive. (+)&lt;br /&gt;
If the path is perpendicular to the electric field, it will be zero.&lt;br /&gt;
&lt;br /&gt;
Finding deltaV in nonuniform Fields:&lt;br /&gt;
DeltaV = -integral from (initial position to final position) of [Efield dot product deltaL]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Some Key Points&#039;&#039;&#039;&lt;br /&gt;
- In a conductor we know that the electric field is zero. Therefore, the potential difference is zero as well(since it is constant everywhere).&lt;br /&gt;
- The potential difference between 2 locations does not depend on the path taken between the locations.&lt;br /&gt;
- Round Trip Potential Difference is always zero, If you start your path from a certain points and end your path at the same point, deltaV will be zero.&lt;br /&gt;
- In an insultor, the electric field is (Eapplied/K)m where K is a dielectric constant.Therefore, DeltaV = (deltaV inside vaccum)/K&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
Watch this video for a more visual approach &lt;br /&gt;
[https://www.youtube.com/watch?v=-Rb9guSEeVE]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
[[File:DDDDDDD.jpg]]&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A proton is located at the origin. Location C is 1e-10 m away from the proton, and location D is 2e-8 m from the proton, along a straight line radially outward. First, find the potential difference from C to D. Then find how much work would be required to move an electron from location C to D. &lt;br /&gt;
&lt;br /&gt;
[[File:Example22.jpg]]&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
I am interested in robotic systems and building circuit boards/ electrical systems for manufacturing robots.&lt;br /&gt;
While studying this section in the book, I was able to connect back many of the concepts and calculations back to&lt;br /&gt;
robotics and electrical component of autmated systems.&lt;br /&gt;
&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
I am a Mechanical Engineering major, so I will be dealing with electrical components of machines when I work. Therefore, I have to know these&lt;br /&gt;
certain concepts such as electric potential in order to fully understand how they work and interact.&lt;br /&gt;
&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
Electrical Potential is used to find the voltage across a path. This is useful when working with circuit comppnents and attempting to manupulate the power output or current throught a component.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The idea of electric potential kind of started with Ben Franklin and his experiments in the 1740s. He began to understand the flow of electricity, which eventually paved the path towards explaining electric potential and potential difference. Scientist finally began understading how electric fields were actually affecting the surrounding environment and other charges.&lt;br /&gt;
Benjamin Franklin first shocked himself in 1746, while conducting experiments on electricity with found objects from around his house. Six years later 261 years ago, the founding father flew a kite attached to a key and a silk ribbon in a thunderstorm and effectively trapped lightning in a jar. The experiment is now seen as a watershed moment in mankind&#039;s venture to channel a force of nature so abstract.&lt;br /&gt;
&lt;br /&gt;
By the time Franklin started experimenting with electricity, he&#039;d already found fame and fortune as the author of Poor Richard&#039;s Almanack and was starting to get into science. Electricity wasn&#039;t a very well understood phenomenon at that point, though, so Franklin&#039;s research proved to be fairly foundational. The early experiments, experts believe, were inspired by other scientists&#039; work and the shortcomings therein.&lt;br /&gt;
&lt;br /&gt;
That early brush with the dangers of electricity left an impression on Franklin. He described the sensation as &amp;quot;a universal blow throughout my whole body from head to foot, which seemed within as well as without; after which the first thing I took notice of was a violent quick shaking of my body.&amp;quot; However, it didn&#039;t scare him away. In the handful of years before his famous kite experiment, Franklin contributed everything from designing the first battery designs to establishing some common nomenclature in the study of electricity.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
Here are some cool articles about the topic&lt;br /&gt;
[https://www.insidescience.org/content/soccers-electric-potential/1022]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
This section contains the the references you used while writing this page&lt;br /&gt;
&lt;br /&gt;
[[Category:Which Category did you place this in?]]&lt;br /&gt;
&lt;br /&gt;
Youtube.com&lt;br /&gt;
&lt;br /&gt;
Matter and Interactions: Electric and Magnetic Interactions Volume 2&lt;br /&gt;
&lt;br /&gt;
Modern Physics Wiki&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=11023</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=11023"/>
		<updated>2015-12-03T23:58:07Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Click on the link to see the Momentum Principle through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/8271b15824 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that is used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the Momentum Principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] Harris, William. &amp;quot;How Netwon&#039;s Laws of Motion Works.&amp;quot; HowStuffWorks. HowStuffWorks.com, 29 July 2008. Web. 29 Nov. 2015. &amp;lt;http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion.htm&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[2] Sherwood, Bruce A. &amp;quot;2.1 The Momentum Principle.&amp;quot; Matter &amp;amp; Interactions. By Ruth W. Chabay. 4th ed. Vol. 1. N.p.: John Wiley &amp;amp; Sons, 2015. 45-50. Print. Modern Mechanics.&lt;br /&gt;
&lt;br /&gt;
[3] Fenton, Flavio. &amp;quot;Momentum and Second Newton&#039;s Law.&amp;quot; 26 Aug. 2015. Lecture.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=11011</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=11011"/>
		<updated>2015-12-03T23:48:40Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* See also */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Click on the link to see the Momentum Principle through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/8271b15824 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that is used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the Momentum Principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=11009</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=11009"/>
		<updated>2015-12-03T23:47:27Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Connectedness */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Click on the link to see the Momentum Principle through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/8271b15824 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that is used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=11003</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=11003"/>
		<updated>2015-12-03T23:45:25Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Click on the link to see the Momentum Principle through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/8271b15824 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that would used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=11001</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=11001"/>
		<updated>2015-12-03T23:45:09Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Click on the link to see the Momentum Principle through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/8271b15824 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that would used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10999</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10999"/>
		<updated>2015-12-03T23:44:39Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Click on the link to see the Momentum Principle through VPython!&lt;br /&gt;
&lt;br /&gt;
Make sure to press &amp;quot;Run&amp;quot; to see the principle in action!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/8271b15824 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that would used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10991</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10991"/>
		<updated>2015-12-03T23:43:32Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Click on the link to see the Momentum Principle through VPython!&lt;br /&gt;
&lt;br /&gt;
&amp;lt;iframe src=&amp;quot;https://trinket.io/embed/glowscript/8271b15824?start=result&amp;quot; width=&amp;quot;100%&amp;quot; height=&amp;quot;356&amp;quot; frameborder=&amp;quot;0&amp;quot; marginwidth=&amp;quot;0&amp;quot; marginheight=&amp;quot;0&amp;quot; allowfullscreen&amp;gt;&amp;lt;/iframe&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/embed/glowscript/8271b15824?start=result Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that would used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10988</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10988"/>
		<updated>2015-12-03T23:42:56Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Click on the link to see the Momentum Principle through VPython!&lt;br /&gt;
&lt;br /&gt;
&amp;lt;iframe src=&amp;quot;https://trinket.io/embed/glowscript/8271b15824?start=result&amp;quot; width=&amp;quot;100%&amp;quot; height=&amp;quot;356&amp;quot; frameborder=&amp;quot;0&amp;quot; marginwidth=&amp;quot;0&amp;quot; marginheight=&amp;quot;0&amp;quot; allowfullscreen&amp;gt;&amp;lt;/iframe&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/glowscript/8271b15824 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that would used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10987</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10987"/>
		<updated>2015-12-03T23:41:59Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Click on the link to see the Momentum Principle through VPython!&lt;br /&gt;
&lt;br /&gt;
[https://trinket.io/glowscript/8271b15824 Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that would used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10982</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10982"/>
		<updated>2015-12-03T23:41:10Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Click on the link to see the Momentum Principle through VPython!&lt;br /&gt;
&lt;br /&gt;
[&amp;lt;iframe src=&amp;quot;https://trinket.io/embed/glowscript/8271b15824?start=result&amp;quot; width=&amp;quot;100%&amp;quot; height=&amp;quot;356&amp;quot; frameborder=&amp;quot;0&amp;quot; marginwidth=&amp;quot;0&amp;quot; marginheight=&amp;quot;0&amp;quot; allowfullscreen&amp;gt;&amp;lt;/iframe&amp;gt; Teach hand-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that would used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10969</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=10969"/>
		<updated>2015-12-03T23:36:12Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;iframe src=&amp;quot;https://trinket.io/embed/glowscript/8271b15824?start=result&amp;quot; width=&amp;quot;100%&amp;quot; height=&amp;quot;356&amp;quot; frameborder=&amp;quot;0&amp;quot; marginwidth=&amp;quot;0&amp;quot; marginheight=&amp;quot;0&amp;quot; allowfullscreen&amp;gt;&amp;lt;/iframe&amp;gt; [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that would used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9507</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9507"/>
		<updated>2015-12-03T04:43:34Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Further reading */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that would used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9505</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9505"/>
		<updated>2015-12-03T04:42:48Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Connectedness */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
&lt;br /&gt;
All over the world and at every point in time, interactions are continuously occurring, and I thought it was interesting to see how the Momentum Principle was the most fundamental principle that would used in starting to the analyze the different interactions. Although there is not a direct relationship between the concept of the Momentum Principle and my major in Biochemistry (which would have more connections with the Energy Principle), there are many industrial applications of the Momentum Principle. Again, the Momentum Principle is not directly connected to the applications, but it is used in the process (especially in the beginning) of industrial application. For example, when creating life saving airbags and seat belts for cars, the Momentum Principle is used. The final momentum of a car during an accident would be zero, or would stop, and the initial momentum would be based on the mass and velocity of the car. With the change in momentum fixed, the airbag and seat belt would focus on increasing the time taken for the body&#039;s momentum to reach zero (final momentum), which would consequently reduce the force of the collision and protect the body from getting as injured. With the Momentum Principle being applicable in so many areas of my life, I found the concept even more interesting.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9421</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9421"/>
		<updated>2015-12-03T04:20:36Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * &amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt;) = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9415</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9415"/>
		<updated>2015-12-03T04:19:09Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
In outer space a rock of mass 5kg is acted on by a constant net force &amp;lt;29,-15,40&amp;gt;N during a 4s time interval. At the end of this time interval the rock has a velocity of &amp;lt;114,94,112&amp;gt;m/s. What is the rock&#039;s velocity at the beginning of the time interval?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;90.8,106,80&amp;gt;m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p} = m * \vec{v}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;m\vec{v}_{final} - m\vec{v}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(5kg * &amp;lt;114,94,112&amp;gt;m/s) - (5kg * \vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;29,-15,40&amp;gt;N * 4s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{v}_{initial}&amp;lt;/math&amp;gt; = &amp;lt;90.8,106,80&amp;gt;m/s&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9334</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9334"/>
		<updated>2015-12-03T04:06:16Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* A Mathematical Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum (measured in kg*m/s) is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;t&#039;&#039;&#039; is the time (measured in seconds, or s). Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
&lt;br /&gt;
Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
&lt;br /&gt;
A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Books, Articles or other print media on this topic&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
&lt;br /&gt;
[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
&lt;br /&gt;
[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
&lt;br /&gt;
[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9331</id>
		<title>Momentum Principle</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Momentum_Principle&amp;diff=9331"/>
		<updated>2015-12-03T04:05:21Z</updated>

		<summary type="html">&lt;p&gt;Hyk96610: /* Examples */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page discusses the Momentum Principle and examples of how it is used.&lt;br /&gt;
&lt;br /&gt;
Claimed by hyk96610&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is the first fundamental principle of mechanics where it describes the relationship between the change in momentum of a system and the total amount of interaction (or total amount of force) with the surroundings. In terms of the system and surroundings, both can be set in any way necessary, where the system may just include a person or the entire Earth. The Momentum Principle can be used in nearly all situations, and it is always advised to start a problem by first writing out the Momentum Principle and then branching out (by rearranging or substituting values) in order to solve a problem.&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
The Momentum Principle is defined as &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system}=  \vec{F}_{net}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system. In the equation, momentum is expressed as the &amp;quot;change in momentum&amp;quot; (&amp;lt;math&amp;gt;∆\vec{p} = \vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt;), which includes both the magnitude and direction of the momentum.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings. Force (measured in Newtons, or N) includes the interactions between system and the surroundings, like the gravitational force exerted by the Earth on us or the force that a compressed spring exerts on a mass. In the Momentum Principle, the force includes both the magnitude and direction. Also, it is important to note that the Momentum Principle calls for the &#039;&#039;net&#039;&#039; force, which is the sum of all the different forces from the surroundings, like adding both the force of gravity and the force of the spring together to calculate the net force. Because of this, it is even more crucial to pay attention to the direction of the forces as a positive or negative sign error could cause an error in the calculated net force. &lt;br /&gt;
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&#039;&#039;&#039;t&#039;&#039;&#039; is the time. Specifically, the Momentum Principle calls for the &amp;quot;change in time&amp;quot; (&amp;lt;math&amp;gt;∆\vec{t} = \vec{t}_{final} - \vec{t}_{initial}&amp;lt;/math&amp;gt;), or in other words, the duration of the interaction is needed.&lt;br /&gt;
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===A Computational Model===&lt;br /&gt;
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How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]&lt;br /&gt;
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==Examples==&lt;br /&gt;
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Be sure to show all steps in your solution and include diagrams whenever possible&lt;br /&gt;
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===Simple===&lt;br /&gt;
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Two external forces &amp;lt;40,-70,0&amp;gt;N and &amp;lt;20,10,0&amp;gt;N, act on a system. What is the net force acting on the system?&lt;br /&gt;
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&#039;&#039;&#039;Answer: &amp;lt;60,-60,0&amp;gt;N&#039;&#039;&#039;&lt;br /&gt;
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&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
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&amp;lt;math&amp;gt;\vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F}_{net}&amp;lt;/math&amp;gt; = &amp;lt;40,-70,0)N + &amp;lt;20,10,0&amp;gt;N = &amp;lt;60,-60,0&amp;gt;N&lt;br /&gt;
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===Middling===&lt;br /&gt;
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A hockey puck is sliding along the ice with nearly constant momentum &amp;lt;10,0,5&amp;gt;kg*m/s when it is suddenly struck by a hockey stick with a force &amp;lt;0,0,2000&amp;gt;N that lasts for only 3 milliseconds (3e-3s). What is the new (vector) momentum of the puck?&lt;br /&gt;
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&#039;&#039;&#039;Answer: &amp;lt;10,0,11&amp;gt;kg*m/s&#039;&#039;&#039;&lt;br /&gt;
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&#039;&#039;&#039;Explanation:&#039;&#039;&#039;&lt;br /&gt;
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&amp;lt;math&amp;gt;∆\vec{p} = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
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&amp;lt;math&amp;gt;\vec{p}_{final} - \vec{p}_{initial}&amp;lt;/math&amp;gt; = \vec{F}_{net} * {∆t}&amp;lt;/math&amp;gt;&lt;br /&gt;
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&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; - &amp;lt;10,0,5&amp;gt;kg*m/s = &amp;lt;0,0,2000&amp;gt;N * (3e-3)s&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{p}_{final}&amp;lt;/math&amp;gt; = &amp;lt;10,0,11&amp;gt;kg*m/s&lt;br /&gt;
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===Difficult===&lt;br /&gt;
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==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
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==History==&lt;br /&gt;
&lt;br /&gt;
Although the Momentum Principle is credited as Newton’s second law of motion, it is difficult to just credit Isaac Newton (1643AD – 1727AD) for the development of the principle. As the Momentum Principle is the quantitative and more in-depth representation of Newton’s first law of motion (“An object tends to be at rest or moves in a straight line and a constant speed except to the extent that it interact with other objects”), the development of the first law also serves an important role in the history of the Momentum Principle. Aristotle (384BC – 322BC) initially proposed that objects had the natural tendency to be at rest and that a push (or a force) was absolutely needed to keep the object moving. His proposal was challenged by Galileo (1564AD – 1642AD), who introduced the idea that objects had the natural tendency to travel in a straight line at constant speed unless something (or a force) was interacting with something. Likewise, Descartes (1596AD – 1650AD) also contributed as he proposed three laws of nature in his “Principle of Philosophy,” which actually outlined the later published Newton’s first law of motion. After studying Descartes, Newton adopted Descartes’ principles as his first law of motion, and alongside the famous story of Newton sitting under an apple, Newton was able to create the Momentum Principle, or his second law of motion.&lt;br /&gt;
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== See also ==&lt;br /&gt;
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As the Momentum Principle is the first of three fundamental principles of mechanics, the next possible topics to examine would be the other fundamental principles, the [http://www.physicsbook.gatech.edu/The_Energy_Principle Energy Principle] and the [http://www.physicsbook.gatech.edu/The_Angular_Momentum_Principle Angular Momentum Principle]. Also, although the momentum principle is an extremely important concept that usually signals the start of a momentum related problem, the principle branches out into other momentum topics like [http://www.physicsbook.gatech.edu/Impulse_Momentum Impulse] and [http://www.physicsbook.gatech.edu/Iterative_Prediction Iterative Prediction], which are used to solve other types of problems.&lt;br /&gt;
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===Further reading===&lt;br /&gt;
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Books, Articles or other print media on this topic&lt;br /&gt;
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===External links===&lt;br /&gt;
[1] https://www.khanacademy.org/science/physics/linear-momentum/momentum-tutorial/v/introduction-to-momentum&lt;br /&gt;
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[2] https://www.youtube.com/watch?v=ZvPrn3aBQG8&lt;br /&gt;
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==References==&lt;br /&gt;
[1] http://science.howstuffworks.com/innovation/scientific-experiments/newton-law-of-motion2.htm&lt;br /&gt;
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[2] Matters &amp;amp; Interactions: Modern Mechanics 4th Ed. Vol. 1 (Chabay &amp;amp; Sherwood)&lt;br /&gt;
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[3] Dr. Flavio Fenton&#039;s Lecture Notes on the Momentum Principle (8/26/15)&lt;br /&gt;
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[[Category:Momentum]]&lt;/div&gt;</summary>
		<author><name>Hyk96610</name></author>
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