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		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2641</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2641"/>
		<updated>2015-11-28T20:14:46Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Connectedness */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields at those two points must be considered. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a potential difference of -0.0115 V.&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The potential calculated for a point charge in a particular region of space is written by V=14xy+6y-4z, what are the electric field components at location &amp;lt;x,y,z&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference &amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; thus Electric field can be calculated as the &amp;lt;math&amp;gt;\frac {-dv}{dx}&amp;lt;/math&amp;gt; So one would take the derivative of the potential difference with respect to each variable giving:&lt;br /&gt;
&lt;br /&gt;
E= &amp;lt;-14y,-14x-6,4&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Connectedness===&lt;br /&gt;
 How is this connected to something you are interested in?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 How is it connected to your major?&lt;br /&gt;
&lt;br /&gt;
I am a Biology major here at Tech. In biochemistry we use the principle of potential energies of half reactions to calculate the standard free energy &amp;lt;math&amp;gt;\vartriangle G &amp;lt;/math&amp;gt; of a reaction in order to understand the reaction&#039;s energetics and determine whether the reaction is favorable or not. This predictive information allows biologists to know what chemical reactions take place in the body and which are able to take place in the body.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2640</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2640"/>
		<updated>2015-11-28T20:13:28Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Connectedness */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields at those two points must be considered. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a potential difference of -0.0115 V.&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The potential calculated for a point charge in a particular region of space is written by V=14xy+6y-4z, what are the electric field components at location &amp;lt;x,y,z&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference &amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; thus Electric field can be calculated as the &amp;lt;math&amp;gt;\frac {-dv}{dx}&amp;lt;/math&amp;gt; So one would take the derivative of the potential difference with respect to each variable giving:&lt;br /&gt;
&lt;br /&gt;
E= &amp;lt;-14y,-14x-6,4&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Connectedness===&lt;br /&gt;
 How is this connected to something you are interested in?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 How is it connected to your major?&lt;br /&gt;
&lt;br /&gt;
I am a Biology major here at Tech. In biochemistry we use the principle of potential energies of half reactions to calculate the &amp;lt;math&amp;gt;\vartriangle G &amp;lt;/math&amp;gt; of a reaction in order to understand the reaction&#039;s energetics and determine whether the reaction is favorable of not. This predictive information allows biologists to know what chemical reactions take place in the body.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2639</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2639"/>
		<updated>2015-11-28T20:12:20Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Connectedness */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields at those two points must be considered. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a potential difference of -0.0115 V.&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The potential calculated for a point charge in a particular region of space is written by V=14xy+6y-4z, what are the electric field components at location &amp;lt;x,y,z&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference &amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; thus Electric field can be calculated as the &amp;lt;math&amp;gt;\frac {-dv}{dx}&amp;lt;/math&amp;gt; So one would take the derivative of the potential difference with respect to each variable giving:&lt;br /&gt;
&lt;br /&gt;
E= &amp;lt;-14y,-14x-6,4&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Connectedness===&lt;br /&gt;
 How is this connected to something you are interested in?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
How is it connected to your major?&lt;br /&gt;
&lt;br /&gt;
I am a Biology major here at Tech. In biochemistry we use the principle of potential energies of half reactions to calculate the &amp;lt;math&amp;gt; vartriangle G &amp;lt;/math&amp;gt; of a reaction in order to understand the reaction&#039;s energetics and determine whether the reaction is favorable of not. This predictive information allows biologists to know what chemical reactions take place in the body.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2638</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2638"/>
		<updated>2015-11-28T20:08:40Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields at those two points must be considered. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a potential difference of -0.0115 V.&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The potential calculated for a point charge in a particular region of space is written by V=14xy+6y-4z, what are the electric field components at location &amp;lt;x,y,z&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference &amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; thus Electric field can be calculated as the &amp;lt;math&amp;gt;\frac {-dv}{dx}&amp;lt;/math&amp;gt; So one would take the derivative of the potential difference with respect to each variable giving:&lt;br /&gt;
&lt;br /&gt;
E= &amp;lt;-14y,-14x-6,4&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Connectedness===&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2354</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2354"/>
		<updated>2015-11-28T01:42:57Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields at those two points must be considered. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a potential difference of -0.0115 V.&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The potential calculated for a point charge in a particular region of space is written by V=14xy+6y-4z, what are the electric field components at location &amp;lt;x,y,z&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference &amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; thus Electric field can be calculated as the &amp;lt;math&amp;gt;\frac {-dv}{dx}&amp;lt;/math&amp;gt; So one would take the derivative of the potential difference with respect to each variable giving:&lt;br /&gt;
&lt;br /&gt;
E= &amp;lt;-14y,-14x-6,4&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2351</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2351"/>
		<updated>2015-11-28T01:41:10Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a potential difference of -0.0115 V.&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The potential calculated for a point charge in a particular region of space is written by V=14xy+6y-4z, what are the electric field components at location &amp;lt;x,y,z&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference &amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; thus Electric field can be calculated as the &amp;lt;math&amp;gt;\frac {-dv}{dx}&amp;lt;/math&amp;gt; So one would take the derivative of the potential difference with respect to each variable giving:&lt;br /&gt;
&lt;br /&gt;
E= &amp;lt;-14y,-14x-6,4&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2348</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2348"/>
		<updated>2015-11-28T01:37:40Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The potential calculated for a point charge in a particular region of space is written by V=14xy+6y-4z, what are the electric field components at location &amp;lt;x,y,z&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference &amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; thus Electric field can be calculated as the &amp;lt;math&amp;gt;\frac {-dv}{dx}&amp;lt;/math&amp;gt; So one would take the derivative of the potential difference with respect to each variable giving:&lt;br /&gt;
&lt;br /&gt;
E= &amp;lt;-14y,-14x-6,4&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2346</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2346"/>
		<updated>2015-11-28T01:34:25Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The potential calculated for a point charge in a particular region of space is written by V=14xy+6y-4z, what are the electric field components at location &amp;lt;x,y,z&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference &amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; thus Electric field can be calculated as the &amp;lt;math&amp;gt;\frac {-dv}{dx}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2343</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2343"/>
		<updated>2015-11-28T01:29:40Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The potential calculated for a point charge in a particular region of space is written by V=14xy+6y-4z, what are the electric field components at location &amp;lt;x,y,z&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference &amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; thus Electric field can be calculated as &amp;lt;math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2341</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2341"/>
		<updated>2015-11-28T01:27:27Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The potential calculated for a point charge in a particular region of space is written by V=14xy+6y-4z, what are the electric field components at location &amp;lt;x,y,z&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference &amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; thus Electric field can be calculated as &amp;lt;math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2340</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2340"/>
		<updated>2015-11-28T01:25:48Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Difficult */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The potential calculated for a point charge in a particular region of space is written by V=14xy+6y-4z, what are the electric field components at location &amp;lt;x,y,z&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference &amp;lt;math&amp;gt;vartriangleV= -Edl&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2339</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2339"/>
		<updated>2015-11-28T01:22:24Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Working it through&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2338</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2338"/>
		<updated>2015-11-28T01:19:55Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
Working it through&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have:&lt;br /&gt;
&amp;lt;math&amp;gt;((9x10^9)\frac{1.6x10^-19}{9.7x10^-9})-((9x10^9)\frac{1.6x10^-19}{9x10^-9})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which yields a&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2337</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2337"/>
		<updated>2015-11-28T01:18:06Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
Working it through&lt;br /&gt;
&lt;br /&gt;
the final location is: (9.7x10^-9) m&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
the intial location is: (9x10^-9) m &lt;br /&gt;
&lt;br /&gt;
So if we plug these values into the above equation we found by integrating Edr. &lt;br /&gt;
&lt;br /&gt;
We have&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2335</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2335"/>
		<updated>2015-11-28T01:16:15Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;(9x10^-9) m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; (9.7x10^-9) m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2334</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2334"/>
		<updated>2015-11-28T01:15:26Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt;((9x10^9)m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; 4.7x10^-10 m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2333</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2333"/>
		<updated>2015-11-28T01:14:16Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt; 2.3e10^-10 m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; 4.7x10^-10 m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2332</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2332"/>
		<updated>2015-11-28T01:12:59Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Middling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Calculate the change in potential moving from location &amp;lt;math&amp;gt; 2.3x10^-10 m &amp;lt;/math&amp;gt; to location &amp;lt;math&amp;gt; 4.7x10^-10 m &amp;lt;/math&amp;gt; from a proton.&lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2331</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2331"/>
		<updated>2015-11-28T01:10:03Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Simple */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
Refer to the figure above to answer the following question:&lt;br /&gt;
&lt;br /&gt;
If the path is along the line i to f what direction is the electric field of the dipole? &lt;br /&gt;
&lt;br /&gt;
down &lt;br /&gt;
up &lt;br /&gt;
left &lt;br /&gt;
right &lt;br /&gt;
Cannot determine &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Answer: To the left. The electric field would point toward the negative end of the dipole&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the potential difference Vf-Vi &lt;br /&gt;
positive&lt;br /&gt;
negative &lt;br /&gt;
zero&lt;br /&gt;
&lt;br /&gt;
Answer: It is negative because both deltal (displacement) and Electric field are pointing in the same direction which means that their product would have been positive and the negative sign in front of the expression -Edl would make the answer negative. &lt;br /&gt;
&lt;br /&gt;
Shortcut to remember: &lt;br /&gt;
E and dl same direction --&amp;gt; negative potential difference&lt;br /&gt;
E and dl opposite direction--&amp;gt;positive potential difference&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Physicswikiproblem1.jpg&amp;diff=2326</id>
		<title>File:Physicswikiproblem1.jpg</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Physicswikiproblem1.jpg&amp;diff=2326"/>
		<updated>2015-11-28T01:04:58Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: Problem 1 figure&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Problem 1 figure&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2325</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2325"/>
		<updated>2015-11-28T01:04:27Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* Simple */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
[[File:Physicswikiproblem1.jpg]]&lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2314</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2314"/>
		<updated>2015-11-28T00:53:01Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Mathematical Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
This equation can be used to determine the potential difference of a point charge between any two different locations.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2311</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2311"/>
		<updated>2015-11-28T00:50:54Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Mathematical Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;((9x10^9)\frac{Q}{rf})-((9x10^9)\frac{Q}{ri})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2310</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2310"/>
		<updated>2015-11-28T00:49:40Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Mathematical Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)\frac{Q}{r}&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;\((9x10^9)Q/rf)-((9x10^9)Q/ri)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2309</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2309"/>
		<updated>2015-11-28T00:48:38Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Mathematical Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)Q/r&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;\((9x10^9)Q/rf)-((9x10^9)Q/ri)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2307</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2307"/>
		<updated>2015-11-28T00:47:39Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Mathematical Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)\frac{Q}/{r^2}dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)Q/r&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;\((9x10^9)Q/rf)-((9x10^9)Q/ri)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2306</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2306"/>
		<updated>2015-11-28T00:46:13Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location and f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)Q/r^2dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)Q/r&amp;lt;/math&amp;gt; which can also be written &amp;lt;math&amp;gt;\((9x10^9)Q/rf)-((9x10^9)Q/ri)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2305</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2305"/>
		<updated>2015-11-28T00:42:37Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Mathematical Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location an f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula for potential difference to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)Q/r^2dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
If we carry out the integration we find that Vf- Vi = &amp;lt;math&amp;gt;\vartriangle(9x10^9)Q/r&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2300</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2300"/>
		<updated>2015-11-28T00:38:16Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Mathematical Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location an f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)Q/r^2dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2299</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2299"/>
		<updated>2015-11-28T00:37:52Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Mathematical Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location an f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location.&lt;br /&gt;
 &amp;lt;math&amp;gt;\textstyle\int\limits_{i}^{f}(9x10^9)Q/r^2dr&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2298</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2298"/>
		<updated>2015-11-28T00:37:26Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location an f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
We substitute E for the formula for the electric field of a point charge and dl for r the distance between the point charge and the observation location. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2292</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2292"/>
		<updated>2015-11-28T00:33:07Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Mathematical Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location an f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;In order to apply this general formula to a point charge:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;math&amp;gt;&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2272</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2272"/>
		<updated>2015-11-28T00:20:05Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is being observed (refer to the equation of the electric field made by a point charge). If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location an f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{r}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2267</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2267"/>
		<updated>2015-11-28T00:17:48Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is located. If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-Edl &amp;lt;/math&amp;gt; -- i being the intial location an f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{r}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2265</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2265"/>
		<updated>2015-11-28T00:17:06Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is located. If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be: &lt;br /&gt;
&amp;lt;math&amp;gt; \textstyle\int\limits_{i}^{f}-E,dl &amp;lt;/math&amp;gt; i being the intial location an f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{r}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2256</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2256"/>
		<updated>2015-11-28T00:09:14Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Mathematical Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is located. If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be  i being the intial location an f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{r}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2255</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2255"/>
		<updated>2015-11-28T00:08:44Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is located. If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into account. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be  i being the intial location an f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2253</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2253"/>
		<updated>2015-11-28T00:06:25Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated by point charges because the magnitude is different depending on the location at which the electric field is located. If one is trying to find the electric potential between two different locations due to a point charge the difference in electric fields must be taken into place. Generally, in a non-uniform electric field one can write the change in potential difference between two locations to be  i being the intial location an f being the final location. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2251</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2251"/>
		<updated>2015-11-27T23:58:24Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2111</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2111"/>
		<updated>2015-11-27T21:04:00Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
Non uniform electric fields are generated &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[[Main Idea]]&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2095</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2095"/>
		<updated>2015-11-27T20:49:19Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
This section is about why non uniform fields are hard to calculate &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
[[Main Idea]]&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2089</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2089"/>
		<updated>2015-11-27T20:45:41Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
This section is about why non uniform fields are hard to calculate &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[History]]&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Volt&lt;br /&gt;
&lt;br /&gt;
http://content.time.com/time/specials/2007/article/0,28804,1677329_1677708_1677755,00.html&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2088</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2088"/>
		<updated>2015-11-27T20:44:54Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
This section is about why non uniform fields are hard to calculate &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In 1800, Alessandro Volta (pictured above) found that metals such as zinc and copper could produce currents; thus, he constructed the first battery what is know called a voltic pile. It was constructed from pieces of zinc and copper in salt water which produced an electric current. The SI unit for potential difference is named after Alessandro Volta. &lt;br /&gt;
&lt;br /&gt;
Refer to:&lt;br /&gt;
&lt;br /&gt;
https://en.wikipedia.org/wiki/Alessandro_Volta&lt;br /&gt;
&lt;br /&gt;
To read more about Volta&#039;s early works and life.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2077</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2077"/>
		<updated>2015-11-27T20:31:49Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
This section is about why non uniform fields are hard to calculate &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the magnitude of the arrows decreases as the distance from the point charge increases&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2. Repeat the steps of #1 but replace the positive point charge with a negative point charge. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;You should notice the same trend occur&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
3. Click &amp;quot;Show E-field&amp;quot; on the right menu bar and move the point charge around the plot&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the Electric field gets larger in magnitude as the point charge moves closer to the observation location&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
4. Move the point charge closer to the observation location that measures potential difference&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Notice that the closer the point charge is to this location the higher the magnitude of the potential difference&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2074</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2074"/>
		<updated>2015-11-27T20:30:07Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
This section is about why non uniform fields are hard to calculate &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r^2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&lt;br /&gt;
&lt;br /&gt;
Exercises&lt;br /&gt;
1. Put down a positive charge. Put 3 E-Field Sensors down: one close to the charge, the next farther away, the next one even farther stil&lt;br /&gt;
Notice that the magnitude of the arrows decreases as the distance from the point charge increases&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2070</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2070"/>
		<updated>2015-11-27T20:29:13Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
This section is about why non uniform fields are hard to calculate &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&lt;br /&gt;
&lt;br /&gt;
To observe how the electric field of a point charge differs from one location to another because it is proportional to 1/r2. Then play around with measuring the potential difference between two points and see how distance affects the calculation of potential difference. You should observe a 1/r relationship.&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2068</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2068"/>
		<updated>2015-11-27T20:28:54Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
This section is about why non uniform fields are hard to calculate &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
https://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2066</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2066"/>
		<updated>2015-11-27T20:28:35Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* A Computational Model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
This section is about why non uniform fields are hard to calculate &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Refer to this Website:&#039;&#039;&#039;&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2065</id>
		<title>Potential Difference of Point Charge in a Non-Uniform Field</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Potential_Difference_of_Point_Charge_in_a_Non-Uniform_Field&amp;diff=2065"/>
		<updated>2015-11-27T20:26:57Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Claimed by dmengesha3 Dina&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
This section is about why non uniform fields are hard to calculate &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
What are the mathematical equations that allow us to model this topic.  For example &amp;lt;math&amp;gt;{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}&amp;lt;/math&amp;gt; where &#039;&#039;&#039;p&#039;&#039;&#039; is the momentum of the system and &#039;&#039;&#039;F&#039;&#039;&#039; is the net force from the surroundings.&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;
===Middling===&lt;br /&gt;
===Difficult===&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
 &#039;&#039;&#039;Connections in Chemistry&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Electrostatic potential energy maps are made of molecules to portray the charge distribution of a molecule 3 dimensionally. These maps can be used to determine electronegativity, bond characteristics, and also help find the reactive sites of molecules. Reactive sites are defined as a charged region of a molecule that interact with other charged particles. This can become especially important in assessing what types of molecular interactions and reactions will take place between two elements or compounds.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
 &#039;&#039;&#039;Industrial Application&#039;&#039;&#039;&lt;br /&gt;
Coulomb Barrier for Nuclear Fusion: For two particles (ex: 2 protons to fuse), they must be able to get close enough to one another for the nuclear strong force to overcome their electric repulsion. One must understand the potential difference of a point charge and the potential energy that creates a barrier between two point charges which can be calculated using U=ke^2/r where k =9e9 and e=1.6e-19 The r calculated using this formula determines the radius at which the nuclear attractive force becomes dominant.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
[[File:volta.jpg]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Calculating Electric Field of a Point Charge&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Point_Charge&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Difference in Uniform Electric Field&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
http://www.physicsbook.gatech.edu/Potential_Difference_in_a_Uniform_Field&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
&lt;br /&gt;
Chabay, Ruth W., and Bruce A. Sherwood. Matter and Interactions: Electric and Magnetic Interactions. 4th ed. Vol. II. Place of Publication Not Identified: John Wiley, 2015. Print. Chapter 16. Section 16.5&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/potpoi.html&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/mulpoi.html&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
[[Connectedness]]&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/coubar.html#c1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
http://chemwiki.ucdavis.edu/Theoretical_Chemistry/Chemical_Bonding/General_Principles_of_Chemical_Bonding/Electrostatic_Potential_maps&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Volta.jpg&amp;diff=2027</id>
		<title>File:Volta.jpg</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Volta.jpg&amp;diff=2027"/>
		<updated>2015-11-27T20:01:35Z</updated>

		<summary type="html">&lt;p&gt;Dmengesha3: Dmengesha3 uploaded a new version of &amp;amp;quot;File:Volta.jpg&amp;amp;quot;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Dmengesha3</name></author>
	</entry>
</feed>