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	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23206</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23206"/>
		<updated>2016-04-18T03:58:34Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}&amp;lt;/math&amp;gt;. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
Using derived calculus, the equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{V}&amp;lt;/math&amp;gt; is defined as the voltage across the capacitor. &amp;lt;math&amp;gt;{emf}&amp;lt;/math&amp;gt; is equal to the emf of the DC voltage source. The units of &amp;lt;math&amp;gt;{RC}&amp;lt;/math&amp;gt; are in seconds. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{τ}&amp;lt;/math&amp;gt; is the constant of time in the RC circuit. &lt;br /&gt;
&lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (&amp;lt;math&amp;gt;{I} = {V/R}&amp;lt;/math&amp;gt;). Also the smaller the capacitor (C), the less time it will need to charge. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt; explains both of these. &lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|left|]]&lt;br /&gt;
Kirchoff&#039;s Node Rule is important to RC Circuits because finding the current flow in the different states of an RC Circuit often relies on nodes when the capacitor is in a parallel circuit.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images2.jpeg|100px|right|]]&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At the final state of the circuit after the current has dropped to zero and the capacitor is fully charged, &amp;lt;math&amp;gt;{RI} = {0} &amp;lt;/math&amp;gt;. The new equation for the final state is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-Q/C = 0&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = emf*C&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To find the equation for voltage versus time when charging a capacitor through a resistor, you start with rearranging the energy equation and solving for I: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
You know that &amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}&amp;lt;/math&amp;gt; due to the rate at which charge builds up the positive capactior plate. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If you exponentiate both sides, the following equation is achieved. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{\frac{IR}{emf}} = {e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{emf}{R}e^{\frac{-t}{RC}}={\frac{dQ}{dt}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{dQ} = \int_0^t{\frac{emf}{R}e^{\frac{-t}{RC}}\,\mathrm{d}t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C(emf)(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Since &amp;lt;math&amp;gt;{V} = {Q/C}&amp;lt;/math&amp;gt;, thus &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
This is the formula for the change in voltage of a series RC circuit with respect to time. &lt;br /&gt;
&lt;br /&gt;
The RC time constant formula is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Using a simulation where R and C were equal, the capacitors were charged and then discharged and the two images show the voltage and current of this versus time. &lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the voltage over time. The red line is the voltage and the gray line is the emf. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rcvoltage.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the current over time. The blue line is the current. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rccurrent.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a circuit where time t = RC, the factor &amp;lt;math&amp;gt;{e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt; has fallen from value &amp;lt;math&amp;gt;{e^0} = {1}&amp;lt;/math&amp;gt; to the value: &lt;br /&gt;
&lt;br /&gt;
e^(-t/RC) = e^1 = 1/e = 1/2.718 = 0.37 &lt;br /&gt;
&lt;br /&gt;
Calculate the time constant for the RC circuit with R = 12 ohms and C = 1 farad. &lt;br /&gt;
&lt;br /&gt;
Solution:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; {RC}= {12*1} = {12 seconds}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Using the information from the problem above: &lt;br /&gt;
&lt;br /&gt;
Show that the power dissipated in the bulb at t=RC is only 14% of  the original power? &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
Using &amp;lt;math&amp;gt;{IΔV} = {RI^2}&amp;lt;/math&amp;gt;, reduction in current by factor of 0.37 gives a reduction in power by a factor of (0.37)^2 = 0.1369 &lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
Suppose one wished to capture the picture of a bullet (moving at 0.04 m/s ) that was passing through an orange. The duration of the flash is related to the RC time constant, τ . What size capacitor would one need in the RC circuit to succeed, if the resistance of the flash tube was 10.0 Ω? Assume the oragne is a sphere with a diameter of 0.08 m.&lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
You know the velocity of the bullet and the distance. You can find the time using Physics I principles such as &amp;lt;math&amp;gt;{time} = {\frac{distance}{velocity}} = {\frac{.08}{.04}} = {.0032 seconds} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
the time becomes equal to τ, so: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{C} = {\frac{τ}{v}} = {\frac{0.0032}{10Ω}} = {32μF} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
1. How is this topic connected to something that you are interested in?&lt;br /&gt;
:: I like listening to music and RC currents are used in subwoofers in my car and other audio equipment.&lt;br /&gt;
2. How is it connected to your major?&lt;br /&gt;
:: I&#039;m an ISyE major and RC currents are directly related to every job, but in warehouses where heavy machinery and appliances are involved, RC currents are used in parts either at the warehouse or ones that are being assembled.&lt;br /&gt;
3. Is there an interesting industrial application?&lt;br /&gt;
:: RC circuits are used to hear certain sounds so that in an assembly line something can be sorted or passed through to another area.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The RC circuits have been in use for a long time. Georg Simon Ohm, was someone who spent alot of time researching RC Circuits and Ohm&#039;s Law was founded by him. He did his work from 1830s-1840s and he received recognition, after a long time of being mocked by other scientists. &lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
http://buphy.bu.edu/~duffy/semester2/c11_RC.html&lt;br /&gt;
&lt;br /&gt;
http://ocw.mit.edu/courses/physics/8-022-physics-ii-electricity-and-magnetism-fall-2006/lecture-notes/lecture32.pdf&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.compadre.org/portal/items/detail.cfm?ID=9986&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
https://openstaxcollege.org/textbooks/college-physics&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23192</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23192"/>
		<updated>2016-04-18T03:54:15Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}&amp;lt;/math&amp;gt;. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
Using derived calculus, the equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{V}&amp;lt;/math&amp;gt; is defined as the voltage across the capacitor. &amp;lt;math&amp;gt;{emf}&amp;lt;/math&amp;gt; is equal to the emf of the DC voltage source. The units of &amp;lt;math&amp;gt;{RC}&amp;lt;/math&amp;gt; are in seconds. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{τ}&amp;lt;/math&amp;gt; is the constant of time in the RC circuit. &lt;br /&gt;
&lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (&amp;lt;math&amp;gt;{I} = {V/R}&amp;lt;/math&amp;gt;). Also the smaller the capacitor (C), the less time it will need to charge. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt; explains both of these. &lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|left|]]&lt;br /&gt;
Kirchoff&#039;s Node Rule is important to RC Circuits because finding the current flow in the different states of an RC Circuit often relies on nodes when the capacitor is in a parallel circuit.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images2.jpeg|100px|right|]]&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At the final state of the circuit after the current has dropped to zero and the capacitor is fully charged, &amp;lt;math&amp;gt;{RI} = {0} &amp;lt;/math&amp;gt;. The new equation for the final state is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-Q/C = 0&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = emf*C&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To find the equation for voltage versus time when charging a capacitor through a resistor, you start with rearranging the energy equation and solving for I: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
You know that &amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}&amp;lt;/math&amp;gt; due to the rate at which charge builds up the positive capactior plate. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If you exponentiate both sides, the following equation is achieved. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{\frac{IR}{emf}} = {e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{emf}{R}e^{\frac{-t}{RC}}={\frac{dQ}{dt}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{dQ} = \int_0^t{\frac{emf}{R}e^{\frac{-t}{RC}}\,\mathrm{d}t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C(emf)(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Since &amp;lt;math&amp;gt;{V} = {Q/C}&amp;lt;/math&amp;gt;, thus &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
This is the formula for the change in voltage of a series RC circuit with respect to time. &lt;br /&gt;
&lt;br /&gt;
The RC time constant formula is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Using a simulation where R and C were equal, the capacitors were charged and then discharged and the two images show the voltage and current of this versus time. &lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the voltage over time. The red line is the voltage and the gray line is the emf. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rcvoltage.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the current over time. The blue line is the current. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rccurrent.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a circuit where time t = RC, the factor &amp;lt;math&amp;gt;{e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt; has fallen from value &amp;lt;math&amp;gt;{e^0} = {1}&amp;lt;/math&amp;gt; to the value: &lt;br /&gt;
&lt;br /&gt;
e^(-t/RC) = e^1 = 1/e = 1/2.718 = 0.37 &lt;br /&gt;
&lt;br /&gt;
Calculate the time constant for the RC circuit with R = 12 ohms and C = 1 farad. &lt;br /&gt;
&lt;br /&gt;
Solution:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; {RC}= {12*1} = {12 seconds}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Using the information from the problem above: &lt;br /&gt;
&lt;br /&gt;
Show that the power dissipated in the bulb at t=RC is only 14% of  the original power? &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
Using &amp;lt;math&amp;gt;{IΔV} = {RI^2}&amp;lt;/math&amp;gt;, reduction in current by factor of 0.37 gives a reduction in power by a factor of (0.37)^2 = 0.1369 &lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
Suppose one wished to capture the picture of a bullet (moving at 0.04 m/s ) that was passing through an orange. The duration of the flash is related to the RC time constant, τ . What size capacitor would one need in the RC circuit to succeed, if the resistance of the flash tube was 10.0 Ω? Assume the oragne is a sphere with a diameter of 0.08 m.&lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
You know the velocity of the bullet and the distance. You can find the time using Physics I principles such as &amp;lt;math&amp;gt;{time} = {\frac{distance}{velocity}} = {\frac{.08}{.04}} = {.0032 seconds} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
the time becomes equal to τ, so: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{C} = {\frac{τ}{v}} = {\frac{0.0032}{10Ω}} = {32μF} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
1. How is this topic connected to something that you are interested in?&lt;br /&gt;
:: I like listening to music and RC currents are used in subwoofers in my car and other audio equipment.&lt;br /&gt;
2. How is it connected to your major?&lt;br /&gt;
:: I&#039;m an ISyE major and RC currents are directly related to every job, but in warehouses where heavy machinery and appliances are involved, RC currents are used in parts either at the warehouse or ones that are being assembled.&lt;br /&gt;
3. Is there an interesting industrial application?&lt;br /&gt;
:: RC circuits are used to hear certain sounds so that in an assembly line something can be sorted or passed through to another area.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The RC circuits have been in use for a long time. Georg Simon Ohm, was someone who spent alot of time researching RC Circuits and Ohm&#039;s Law was founded by him. He did his work from 1830s-1840s and he received recognition after a long time of being mocked by other scientists. &lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
http://buphy.bu.edu/~duffy/semester2/c11_RC.html&lt;br /&gt;
&lt;br /&gt;
http://ocw.mit.edu/courses/physics/8-022-physics-ii-electricity-and-magnetism-fall-2006/lecture-notes/lecture32.pdf&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.compadre.org/portal/items/detail.cfm?ID=9986&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
https://openstaxcollege.org/textbooks/college-physics&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23191</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23191"/>
		<updated>2016-04-18T03:53:59Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}&amp;lt;/math&amp;gt;. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
Using derived calculus, the equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{V}&amp;lt;/math&amp;gt; is defined as the voltage across the capacitor. &amp;lt;math&amp;gt;{emf}&amp;lt;/math&amp;gt; is equal to the emf of the DC voltage source. The units of &amp;lt;math&amp;gt;{RC}&amp;lt;/math&amp;gt; are in seconds. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{τ}&amp;lt;/math&amp;gt; is the constant of time in the RC circuit. &lt;br /&gt;
&lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (&amp;lt;math&amp;gt;{I} = {V/R}&amp;lt;/math&amp;gt;). Also the smaller the capacitor (C), the less time it will need to charge. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt; explains both of these. &lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|left|]]&lt;br /&gt;
Kirchoff&#039;s Node Rule is important to RC Circuits because finding the current flow in the different states of an RC Circuit often relies on nodes when the capacitor is in a parallel circuit.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images2.jpeg|100px|right|]]&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At the final state of the circuit after the current has dropped to zero and the capacitor is fully charged, &amp;lt;math&amp;gt;{RI} = {0} &amp;lt;/math&amp;gt;. The new equation for the final state is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-Q/C = 0&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = emf*C&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To find the equation for voltage versus time when charging a capacitor through a resistor, you start with rearranging the energy equation and solving for I: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
You know that &amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}&amp;lt;/math&amp;gt; due to the rate at which charge builds up the positive capactior plate. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If you exponentiate both sides, the following equation is achieved. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{\frac{IR}{emf}} = {e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{emf}{R}e^{\frac{-t}{RC}}={\frac{dQ}{dt}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{dQ} = \int_0^t{\frac{emf}{R}e^{\frac{-t}{RC}}\,\mathrm{d}t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C(emf)(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Since &amp;lt;math&amp;gt;{V} = {Q/C}&amp;lt;/math&amp;gt;, thus &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
This is the formula for the change in voltage of a series RC circuit with respect to time. &lt;br /&gt;
&lt;br /&gt;
The RC time constant formula is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===A Computational Model===&lt;br /&gt;
&lt;br /&gt;
Using a simulation where R and C were equal, the capacitors were charged and then discharged and the two images show the voltage and current of this versus time. &lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the voltage over time. The red line is the voltage and the gray line is the emf. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rcvoltage.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the current over time. The blue line is the current. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rccurrent.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
In a circuit where time t = RC, the factor &amp;lt;math&amp;gt;{e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt; has fallen from value &amp;lt;math&amp;gt;{e^0} = {1}&amp;lt;/math&amp;gt; to the value: &lt;br /&gt;
&lt;br /&gt;
e^(-t/RC) = e^1 = 1/e = 1/2.718 = 0.37 &lt;br /&gt;
&lt;br /&gt;
Calculate the time constant for the RC circuit with R = 12 ohms and C = 1 farad. &lt;br /&gt;
&lt;br /&gt;
Solution:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; {RC}= {12*1} = {12 seconds}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
===Middling===&lt;br /&gt;
Using the information from the problem above: &lt;br /&gt;
&lt;br /&gt;
Show that the power dissipated in the bulb at t=RC is only 14% of  the original power? &lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
Using &amp;lt;math&amp;gt;{IΔV} = {RI^2}&amp;lt;/math&amp;gt;, reduction in current by factor of 0.37 gives a reduction in power by a factor of (0.37)^2 = 0.1369 &lt;br /&gt;
&lt;br /&gt;
===Difficult===&lt;br /&gt;
Suppose one wished to capture the picture of a bullet (moving at 0.04 m/s ) that was passing through an orange. The duration of the flash is related to the RC time constant, τ . What size capacitor would one need in the RC circuit to succeed, if the resistance of the flash tube was 10.0 Ω? Assume the oragne is a sphere with a diameter of 0.08 m.&lt;br /&gt;
&lt;br /&gt;
Solution: &lt;br /&gt;
&lt;br /&gt;
You know the velocity of the bullet and the distance. You can find the time using Physics I principles such as &amp;lt;math&amp;gt;{time} = {\frac{distance}{velocity}} = {\frac{.08}{.04}} = {.0032 seconds} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
the time becomes equal to τ, so: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{C} = {\frac{τ}{v}} = {\frac{0.0032}{10Ω}} = {32μF} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Connectedness==&lt;br /&gt;
1. How is this topic connected to something that you are interested in?&lt;br /&gt;
:: I like listening to music and RC currents are used in subwoofers in my car and other audio equipment.&lt;br /&gt;
2. How is it connected to your major?&lt;br /&gt;
:: I&#039;m an ISyE major and RC currents are directly related to every job, but in warehouses where heavy machinery and appliances are involved, RC currents are used in parts either at the warehouse or ones that are being assembled.&lt;br /&gt;
3. Is there an interesting industrial application?&lt;br /&gt;
:: RC circuits are used to hear certain sounds so that in an assembly line something can be sorted or passed through to another area.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
&lt;br /&gt;
The RC circuits have been in use for a long time. Georg Simon Ohm, was someone who spent alot of time researching RC Circuits and Ohm&#039;s Law was founded by him. He did his work from 1830s-1840s and he received recognition after a long time of being mocked by other scientists. &lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
http://buphy.bu.edu/~duffy/semester2/c11_RC.html&lt;br /&gt;
&lt;br /&gt;
http://ocw.mit.edu/courses/physics/8-022-physics-ii-electricity-and-magnetism-fall-2006/lecture-notes/lecture32.pdf&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.compadre.org/portal/items/detail.cfm?ID=9986&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
https://openstaxcollege.org/textbooks/college-physics&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23109</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23109"/>
		<updated>2016-04-18T03:15:56Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: /* Connectedness */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}&amp;lt;/math&amp;gt;. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
Using derived calculus, the equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{V}&amp;lt;/math&amp;gt; is defined as the voltage across the capacitor. &amp;lt;math&amp;gt;{emf}&amp;lt;/math&amp;gt; is equal to the emf of the DC voltage source. The units of &amp;lt;math&amp;gt;{RC}&amp;lt;/math&amp;gt; are in seconds. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{τ}&amp;lt;/math&amp;gt; is the constant of time in the RC circuit. &lt;br /&gt;
&lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (&amp;lt;math&amp;gt;{I} = {V/R}&amp;lt;/math&amp;gt;). Also the smaller the capacitor (C), the less time it will need to charge. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt; explains both of these. &lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|left|]]&lt;br /&gt;
Kirchoff&#039;s Node Rule is important to RC Circuits because finding the current flow in the different states of an RC Circuit often relies on nodes when the capacitor is in a parallel circuit.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images2.jpeg|100px|right|]]&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At the final state of the circuit after the current has dropped to zero and the capacitor is fully charged, &amp;lt;math&amp;gt;{RI} = {0} &amp;lt;/math&amp;gt;. The new equation for the final state is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-Q/C = 0&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = emf*C&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To find the equation for voltage versus time when charging a capacitor through a resistor, you start with rearranging the energy equation and solving for I: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
You know that &amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}&amp;lt;/math&amp;gt; due to the rate at which charge builds up the positive capactior plate. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If you exponentiate both sides, the following equation is achieved. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{\frac{IR}{emf}} = {e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{emf}{R}e^{\frac{-t}{RC}}={\frac{dQ}{dt}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{dQ} = \int_0^t{\frac{emf}{R}e^{\frac{-t}{RC}}\,\mathrm{d}t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C(emf)(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Since &amp;lt;math&amp;gt;{V} = {Q/C}&amp;lt;/math&amp;gt;, thus &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
This is the formula for the change in voltage of a series RC circuit with respect to time. &lt;br /&gt;
&lt;br /&gt;
The RC time constant formula is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==A Computational Model==&lt;br /&gt;
&lt;br /&gt;
Using a simulation where R and C were equal, the capacitors were charged and then discharged and the two images show the voltage and current of this versus time. &lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the voltage over time. The red line is the voltage and the gray line is the emf. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rcvoltage.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the current over time. The blue line is the current. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rccurrent.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
1. How is this topic connected to something that you are interested in?&lt;br /&gt;
:: I like listening to music and RC currents are used in subwoofers in my car and other audio equipment.&lt;br /&gt;
2. How is it connected to your major?&lt;br /&gt;
:: I&#039;m an ISyE major and RC currents are directly related to every job, but in warehouses wehre heavy machinery and appliances are involved, RC currents are used in parts either at the warehouse or ones that are being assembled.&lt;br /&gt;
3. Is there an interesting industrial application?&lt;br /&gt;
:: RC circuits are used to hear certain sounds so that in an assembly line something can be sorted or passed through to another area.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
http://buphy.bu.edu/~duffy/semester2/c11_RC.html&lt;br /&gt;
&lt;br /&gt;
http://ocw.mit.edu/courses/physics/8-022-physics-ii-electricity-and-magnetism-fall-2006/lecture-notes/lecture32.pdf&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.compadre.org/portal/items/detail.cfm?ID=9986&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
https://openstaxcollege.org/textbooks/college-physics&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23105</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23105"/>
		<updated>2016-04-18T03:15:21Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: /* Connectedness */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}&amp;lt;/math&amp;gt;. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
Using derived calculus, the equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{V}&amp;lt;/math&amp;gt; is defined as the voltage across the capacitor. &amp;lt;math&amp;gt;{emf}&amp;lt;/math&amp;gt; is equal to the emf of the DC voltage source. The units of &amp;lt;math&amp;gt;{RC}&amp;lt;/math&amp;gt; are in seconds. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{τ}&amp;lt;/math&amp;gt; is the constant of time in the RC circuit. &lt;br /&gt;
&lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (&amp;lt;math&amp;gt;{I} = {V/R}&amp;lt;/math&amp;gt;). Also the smaller the capacitor (C), the less time it will need to charge. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt; explains both of these. &lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|left|]]&lt;br /&gt;
Kirchoff&#039;s Node Rule is important to RC Circuits because finding the current flow in the different states of an RC Circuit often relies on nodes when the capacitor is in a parallel circuit.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images2.jpeg|100px|right|]]&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At the final state of the circuit after the current has dropped to zero and the capacitor is fully charged, &amp;lt;math&amp;gt;{RI} = {0} &amp;lt;/math&amp;gt;. The new equation for the final state is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-Q/C = 0&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = emf*C&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To find the equation for voltage versus time when charging a capacitor through a resistor, you start with rearranging the energy equation and solving for I: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
You know that &amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}&amp;lt;/math&amp;gt; due to the rate at which charge builds up the positive capactior plate. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If you exponentiate both sides, the following equation is achieved. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{\frac{IR}{emf}} = {e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{emf}{R}e^{\frac{-t}{RC}}={\frac{dQ}{dt}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{dQ} = \int_0^t{\frac{emf}{R}e^{\frac{-t}{RC}}\,\mathrm{d}t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C(emf)(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Since &amp;lt;math&amp;gt;{V} = {Q/C}&amp;lt;/math&amp;gt;, thus &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
This is the formula for the change in voltage of a series RC circuit with respect to time. &lt;br /&gt;
&lt;br /&gt;
The RC time constant formula is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==A Computational Model==&lt;br /&gt;
&lt;br /&gt;
Using a simulation where R and C were equal, the capacitors were charged and then discharged and the two images show the voltage and current of this versus time. &lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the voltage over time. The red line is the voltage and the gray line is the emf. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rcvoltage.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the current over time. The blue line is the current. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rccurrent.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#1. How is this topic connected to something that you are interested in?&lt;br /&gt;
:: I like listening to music and RC currents are used in subwoofers in my car and other audio equipment.&lt;br /&gt;
#2. How is it connected to your major?&lt;br /&gt;
:: I&#039;m an ISyE major and RC currents are directly related to every job, but in warehouses wehre heavy machinery and appliances are involved, RC currents are used in parts either at the warehouse or ones that are being assembled.&lt;br /&gt;
#3. Is there an interesting industrial application?&lt;br /&gt;
:: RC circuits are used to hear certain sounds so that in an assembly line something can be sorted or passed through to another area.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
http://buphy.bu.edu/~duffy/semester2/c11_RC.html&lt;br /&gt;
&lt;br /&gt;
http://ocw.mit.edu/courses/physics/8-022-physics-ii-electricity-and-magnetism-fall-2006/lecture-notes/lecture32.pdf&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.compadre.org/portal/items/detail.cfm?ID=9986&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
https://openstaxcollege.org/textbooks/college-physics&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23103</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23103"/>
		<updated>2016-04-18T03:14:35Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: /* External links */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}&amp;lt;/math&amp;gt;. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
Using derived calculus, the equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{V}&amp;lt;/math&amp;gt; is defined as the voltage across the capacitor. &amp;lt;math&amp;gt;{emf}&amp;lt;/math&amp;gt; is equal to the emf of the DC voltage source. The units of &amp;lt;math&amp;gt;{RC}&amp;lt;/math&amp;gt; are in seconds. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{τ}&amp;lt;/math&amp;gt; is the constant of time in the RC circuit. &lt;br /&gt;
&lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (&amp;lt;math&amp;gt;{I} = {V/R}&amp;lt;/math&amp;gt;). Also the smaller the capacitor (C), the less time it will need to charge. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt; explains both of these. &lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|left|]]&lt;br /&gt;
Kirchoff&#039;s Node Rule is important to RC Circuits because finding the current flow in the different states of an RC Circuit often relies on nodes when the capacitor is in a parallel circuit.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images2.jpeg|100px|right|]]&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At the final state of the circuit after the current has dropped to zero and the capacitor is fully charged, &amp;lt;math&amp;gt;{RI} = {0} &amp;lt;/math&amp;gt;. The new equation for the final state is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-Q/C = 0&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = emf*C&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To find the equation for voltage versus time when charging a capacitor through a resistor, you start with rearranging the energy equation and solving for I: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
You know that &amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}&amp;lt;/math&amp;gt; due to the rate at which charge builds up the positive capactior plate. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If you exponentiate both sides, the following equation is achieved. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{\frac{IR}{emf}} = {e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{emf}{R}e^{\frac{-t}{RC}}={\frac{dQ}{dt}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{dQ} = \int_0^t{\frac{emf}{R}e^{\frac{-t}{RC}}\,\mathrm{d}t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C(emf)(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Since &amp;lt;math&amp;gt;{V} = {Q/C}&amp;lt;/math&amp;gt;, thus &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
This is the formula for the change in voltage of a series RC circuit with respect to time. &lt;br /&gt;
&lt;br /&gt;
The RC time constant formula is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==A Computational Model==&lt;br /&gt;
&lt;br /&gt;
Using a simulation where R and C were equal, the capacitors were charged and then discharged and the two images show the voltage and current of this versus time. &lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the voltage over time. The red line is the voltage and the gray line is the emf. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rcvoltage.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the current over time. The blue line is the current. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rccurrent.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: I like listening to music and RC currents are used in subwoofers in my car and other audio equipment.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: I&#039;m an ISyE major and RC currents are directly related to every job, but in warehouses wehre heavy machinery and appliances are involved, RC currents are used in parts either at the warehouse or ones that are being assembled.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits are used to hear certain sounds so that in an assembly line something can be sorted or passed through to another area. &lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
http://buphy.bu.edu/~duffy/semester2/c11_RC.html&lt;br /&gt;
&lt;br /&gt;
http://ocw.mit.edu/courses/physics/8-022-physics-ii-electricity-and-magnetism-fall-2006/lecture-notes/lecture32.pdf&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.compadre.org/portal/items/detail.cfm?ID=9986&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
https://openstaxcollege.org/textbooks/college-physics&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23101</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23101"/>
		<updated>2016-04-18T03:13:30Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}&amp;lt;/math&amp;gt;. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
Using derived calculus, the equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{V}&amp;lt;/math&amp;gt; is defined as the voltage across the capacitor. &amp;lt;math&amp;gt;{emf}&amp;lt;/math&amp;gt; is equal to the emf of the DC voltage source. The units of &amp;lt;math&amp;gt;{RC}&amp;lt;/math&amp;gt; are in seconds. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{τ}&amp;lt;/math&amp;gt; is the constant of time in the RC circuit. &lt;br /&gt;
&lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (&amp;lt;math&amp;gt;{I} = {V/R}&amp;lt;/math&amp;gt;). Also the smaller the capacitor (C), the less time it will need to charge. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt; explains both of these. &lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|left|]]&lt;br /&gt;
Kirchoff&#039;s Node Rule is important to RC Circuits because finding the current flow in the different states of an RC Circuit often relies on nodes when the capacitor is in a parallel circuit.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images2.jpeg|100px|right|]]&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At the final state of the circuit after the current has dropped to zero and the capacitor is fully charged, &amp;lt;math&amp;gt;{RI} = {0} &amp;lt;/math&amp;gt;. The new equation for the final state is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-Q/C = 0&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = emf*C&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To find the equation for voltage versus time when charging a capacitor through a resistor, you start with rearranging the energy equation and solving for I: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
You know that &amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}&amp;lt;/math&amp;gt; due to the rate at which charge builds up the positive capactior plate. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If you exponentiate both sides, the following equation is achieved. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{\frac{IR}{emf}} = {e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{emf}{R}e^{\frac{-t}{RC}}={\frac{dQ}{dt}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{dQ} = \int_0^t{\frac{emf}{R}e^{\frac{-t}{RC}}\,\mathrm{d}t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C(emf)(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Since &amp;lt;math&amp;gt;{V} = {Q/C}&amp;lt;/math&amp;gt;, thus &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
This is the formula for the change in voltage of a series RC circuit with respect to time. &lt;br /&gt;
&lt;br /&gt;
The RC time constant formula is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==A Computational Model==&lt;br /&gt;
&lt;br /&gt;
Using a simulation where R and C were equal, the capacitors were charged and then discharged and the two images show the voltage and current of this versus time. &lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the voltage over time. The red line is the voltage and the gray line is the emf. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rcvoltage.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the current over time. The blue line is the current. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rccurrent.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: I like listening to music and RC currents are used in subwoofers in my car and other audio equipment.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: I&#039;m an ISyE major and RC currents are directly related to every job, but in warehouses wehre heavy machinery and appliances are involved, RC currents are used in parts either at the warehouse or ones that are being assembled.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits are used to hear certain sounds so that in an assembly line something can be sorted or passed through to another area. &lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.compadre.org/portal/items/detail.cfm?ID=9986&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
https://openstaxcollege.org/textbooks/college-physics&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23085</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23085"/>
		<updated>2016-04-18T03:09:25Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}&amp;lt;/math&amp;gt;. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
Using derived calculus, the equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{V}&amp;lt;/math&amp;gt; is defined as the voltage across the capacitor. &amp;lt;math&amp;gt;{emf}&amp;lt;/math&amp;gt; is equal to the emf of the DC voltage source. The units of &amp;lt;math&amp;gt;{RC}&amp;lt;/math&amp;gt; are in seconds. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{τ}&amp;lt;/math&amp;gt; is the constant of time in the RC circuit. &lt;br /&gt;
&lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (&amp;lt;math&amp;gt;{I} = {V/R}&amp;lt;/math&amp;gt;). Also the smaller the capacitor (C), the less time it will need to charge. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt; explains both of these. &lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|left|]]&lt;br /&gt;
Kirchoff&#039;s Node Rule is important to RC Circuits because finding the current flow in the different states of an RC Circuit often relies on nodes when the capacitor is in a parallel circuit.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images2.jpeg|100px|right|]]&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At the final state of the circuit after the current has dropped to zero and the capacitor is fully charged, &amp;lt;math&amp;gt;{RI} = {0} &amp;lt;/math&amp;gt;. The new equation for the final state is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-Q/C = 0&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = emf*C&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To find the equation for voltage versus time when charging a capacitor through a resistor, you start with rearranging the energy equation and solving for I: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
You know that &amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}&amp;lt;/math&amp;gt; due to the rate at which charge builds up the positive capactior plate. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If you exponentiate both sides, the following equation is achieved. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{\frac{IR}{emf}} = {e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{emf}{R}e^{\frac{-t}{RC}}={\frac{dQ}{dt}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{dQ} = \int_0^t{\frac{emf}{R}e^{\frac{-t}{RC}}\,\mathrm{d}t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C(emf)(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Since &amp;lt;math&amp;gt;{V} = {Q/C}&amp;lt;/math&amp;gt;, thus &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
This is the formula for the change in voltage of a series RC circuit with respect to time. &lt;br /&gt;
&lt;br /&gt;
The RC time constant formula is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==A Computational Model==&lt;br /&gt;
&lt;br /&gt;
Using a simulation where R and C were equal, the capacitors were charged and then discharged and the two images show the voltage and current of this versus time. &lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the voltage over time. The red line is the voltage and the gray line is the emf. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rcvoltage.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the current over time. The blue line is the current. (May have to click image to see gif)&lt;br /&gt;
&lt;br /&gt;
[[File:rccurrent.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: I like listening to music and RC currents are used in subwoofers in my car and other audio equipment.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: I&#039;m an ISyE major and RC currents are directly related to every job, but in warehouses wehre heavy machinery and appliances are involved, RC currents are used in parts either at the warehouse or ones that are being assembled.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits are used to hear certain sounds so that in an assembly line something can be sorted or passed through to another area. &lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23082</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=23082"/>
		<updated>2016-04-18T03:07:11Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}&amp;lt;/math&amp;gt;. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
Using derived calculus, the equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{V}&amp;lt;/math&amp;gt; is defined as the voltage across the capacitor. &amp;lt;math&amp;gt;{emf}&amp;lt;/math&amp;gt; is equal to the emf of the DC voltage source. The units of &amp;lt;math&amp;gt;{RC}&amp;lt;/math&amp;gt; are in seconds. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{τ}&amp;lt;/math&amp;gt; is the constant of time in the RC circuit. &lt;br /&gt;
&lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (&amp;lt;math&amp;gt;{I} = {V/R}&amp;lt;/math&amp;gt;). Also the smaller the capacitor (C), the less time it will need to charge. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt; explains both of these. &lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|left|]]&lt;br /&gt;
Kirchoff&#039;s Node Rule is important to RC Circuits because finding the current flow in the different states of an RC Circuit often relies on nodes when the capacitor is in a parallel circuit.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images2.jpeg|100px|right|]]&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At the final state of the circuit after the current has dropped to zero and the capacitor is fully charged, &amp;lt;math&amp;gt;{RI} = {0} &amp;lt;/math&amp;gt;. The new equation for the final state is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-Q/C = 0&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = emf*C&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To find the equation for voltage versus time when charging a capacitor through a resistor, you start with rearranging the energy equation and solving for I: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
You know that &amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}&amp;lt;/math&amp;gt; due to the rate at which charge builds up the positive capactior plate. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If you exponentiate both sides, the following equation is achieved. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{\frac{IR}{emf}} = {e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{emf}{R}e^{\frac{-t}{RC}}={\frac{dQ}{dt}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{dQ} = \int_0^t{\frac{emf}{R}e^{\frac{-t}{RC}}\,\mathrm{d}t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C(emf)(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Since &amp;lt;math&amp;gt;{V} = {Q/C}&amp;lt;/math&amp;gt;, thus &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
This is the formula for the change in voltage of a series RC circuit with respect to time. &lt;br /&gt;
&lt;br /&gt;
The RC time constant formula is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==A Computational Model==&lt;br /&gt;
&lt;br /&gt;
Using a simulation where R and C were equal, the capacitors were charged and then discharged and the two images show the voltage and current of this versus time. &lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the voltage over time. The red line is the voltage and the gray line is the emf. &lt;br /&gt;
&lt;br /&gt;
[[File:rcvoltage.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the gif below, the capacitor is charged and then discharged. This shows the current over time. The blue line is the current.&lt;br /&gt;
&lt;br /&gt;
[[File:rccurrent.gif|300px|center|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: I like listening to music and RC currents are used in subwoofers in my car and other audio equipment.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: I&#039;m an ISyE major and RC currents are directly related to every job, but in warehouses wehre heavy machinery and appliances are involved, RC currents are used in parts either at the warehouse or ones that are being assembled.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits are used to hear certain sounds so that in an assembly line something can be sorted or passed through to another area. &lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Rccurrent.gif&amp;diff=23077</id>
		<title>File:Rccurrent.gif</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Rccurrent.gif&amp;diff=23077"/>
		<updated>2016-04-18T03:04:31Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Rcvoltage.gif&amp;diff=23076</id>
		<title>File:Rcvoltage.gif</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Rcvoltage.gif&amp;diff=23076"/>
		<updated>2016-04-18T03:04:07Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22953</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22953"/>
		<updated>2016-04-18T02:06:05Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}&amp;lt;/math&amp;gt;. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
Using derived calculus, the equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{V}&amp;lt;/math&amp;gt; is defined as the voltage across the capacitor. &amp;lt;math&amp;gt;{emf}&amp;lt;/math&amp;gt; is equal to the emf of the DC voltage source. The units of &amp;lt;math&amp;gt;{RC}&amp;lt;/math&amp;gt; are in seconds. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;{τ}&amp;lt;/math&amp;gt; is the constant of time in the RC circuit. &lt;br /&gt;
&lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (&amp;lt;math&amp;gt;{I} = {V/R}&amp;lt;/math&amp;gt;). Also the smaller the capacitor (C), the less time it will need to charge. &amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt; explains both of these. &lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|left|]]&lt;br /&gt;
Kirchoff&#039;s Node Rule is important to RC Circuits because finding the current flow in the different states of an RC Circuit often relies on nodes when the capacitor is in a parallel circuit.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images2.jpeg|100px|right|]]&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At the final state of the circuit after the current has dropped to zero and the capacitor is fully charged, &amp;lt;math&amp;gt;{RI} = {0} &amp;lt;/math&amp;gt;. The new equation for the final state is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-Q/C = 0&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = emf*C&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To find the equation for voltage versus time when charging a capacitor through a resistor, you start with rearranging the energy equation and solving for I: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
You know that &amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}&amp;lt;/math&amp;gt; due to the rate at which charge builds up the positive capactior plate. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{dQ}{dt}}={\frac{emf-Q/C}{R}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If you exponentiate both sides, the following equation is achieved. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{\frac{IR}{emf}} = {e^{\frac{-t}{RC}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{I} = {\frac{emf}{R}e^{\frac{-t}{RC}}={\frac{dQ}{dt}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{dQ} = \int_0^t{\frac{emf}{R}e^{\frac{-t}{RC}}\,\mathrm{d}t}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C(emf)(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Since &amp;lt;math&amp;gt;{V} = {Q/C}&amp;lt;/math&amp;gt;, thus &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
This is the formula for the change in voltage of a series RC circuit with respect to time. &lt;br /&gt;
&lt;br /&gt;
The RC time constant formula is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{τ} = {RC}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22828</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22828"/>
		<updated>2016-04-18T01:20:43Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}&amp;lt;/math&amp;gt;. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
The equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt; V is defined as the voltage across the capacitor. Emf is equal to the emf of the dC voltage source. The units of RC are in seconds. Tau= RC. Tau is the constant of time in the RC circuit. &lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (I=V/R). Also the smaller the capacitor (C), the less time it will need to charge. Tau = RC explains both of these. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22825</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22825"/>
		<updated>2016-04-18T01:19:50Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at &amp;lt;math&amp;gt; {time} = {0}. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to zero as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time &amp;lt;math&amp;gt;{t} = {0}&amp;lt;/math&amp;gt;. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
The equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt; V is defined as the voltage across the capacitor. Emf is equal to the emf of the dC voltage source. The units of RC are in seconds. Tau= RC. Tau is the constant of time in the RC circuit. &lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (I=V/R). Also the smaller the capacitor (C), the less time it will need to charge. Tau = RC explains both of these. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
These three equations are helpful in solving and understanding RC circuit problems&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV}_{round trip} = {0} &amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;{ΔV} = {I}{R} &amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;{Q} = {C}{V} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In a loop of a circuit, the change of potential difference has to be zero. The energy equation for the RC Circuit in the figure at the top of the page is: &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;{V}_{round trip} = emf-RI-Q/C = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22805</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22805"/>
		<updated>2016-04-18T01:06:16Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;/math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at time = 0. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;/math&amp;gt; to 0 as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time t=0. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
The equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt; V is defined as the voltage across the capacitor. Emf is equal to the emf of the dC voltage source. The units of RC are in seconds. Tau= RC. Tau is the constant of time in the RC circuit. &lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (I=V/R). Also the smaller the capacitor (C), the less time it will need to charge. Tau = RC explains both of these. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
ΔV = I * R&lt;br /&gt;
&lt;br /&gt;
Q=CV&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22799</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22799"/>
		<updated>2016-04-18T01:04:45Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as the current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta &amp;lt;math&amp;gt;{V} = {Q}/{C}&amp;lt;math&amp;gt;, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at time = 0. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of &amp;lt;math&amp;gt;{I}_{0} = {emf}/{R}&amp;lt;math&amp;gt; to 0 as the voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time t=0. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
The equation for voltage versus time when the capacitor is charged through resistor R is &amp;lt;math&amp;gt;{V} = {emf(1-e^{\frac{-t}{RC}})}&amp;lt;/math&amp;gt; V is defined as the voltage across the capacitor. Emf is equal to the emf of the dC voltage source. The units of RC are in seconds. Tau= RC. Tau is the constant of time in the RC circuit. &lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (I=V/R). Also the smaller the capacitor (C), the less time it will need to charge. Tau = RC explains both of these. &lt;br /&gt;
&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
ΔV = I * R&lt;br /&gt;
&lt;br /&gt;
Q=CV&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22776</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22776"/>
		<updated>2016-04-18T00:52:44Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit. The capacitor stores electric charge (Q)&lt;br /&gt;
&lt;br /&gt;
RC Circuits use a DC (direct current) voltage source and the capacitor is uncharged at its initial state. In the figure below, you see an RC circuit with a switch. When the switch is closed, the capacitor will begin to charge as current can now flow throughout the circuit. To discharge the capacitor, you simply disconnect the switch. &lt;br /&gt;
&lt;br /&gt;
[[File:Rc_switch.JPG|400px|center|]]&lt;br /&gt;
&lt;br /&gt;
Remember that potential difference across the capacitor is delta V = Q/C, where Q is charge on the plate and C is the capacitance. When the switch is closed, voltage on the capacitor rises rapidly at first, due to the high current at time =0. The voltage opposes the battery, increasing from zero to the max emf when the capacitor is fully charged. The current decreases from its initial value of I0 =emf/R to 0 as voltage on the capacitor reaches the same value as the emf. The current is initially at its max at time t=0. &lt;br /&gt;
&lt;br /&gt;
Kirchhoff’s loop rule explains that the sum of changes in potential around any closed loop must be zero. &lt;br /&gt;
&lt;br /&gt;
The equation for voltage versus time when the capacitor is charged through resistor R is V=emf(1-e) etc. V is defined as the voltage across the capacitor. Emf is equal to the emf of the dC voltage source. The units of RC are in seconds. Tau= RC. Tau is the time constant for the RC circuit. &lt;br /&gt;
The smaller the resistance, the faster a capacitor will be charged. It takes longer to charge than to discharge. This is because a larger current flows through a smaller resistance (I=V/R). Also the smaller the capacitor (C), the less time it will need to charge. Tau = RC explains both of these. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
**&lt;br /&gt;
below shows a capacitor, ( C ) in series with a resistor, ( R ) forming a RC Charging Circuit connected across a DC battery supply ( Vs ) via a mechanical switch. When the switch is closed, the capacitor will gradually charge up through the resistor until the voltage across it reaches the supply voltage of the battery. The manner in which the capacitor charges up is also shown below.&lt;br /&gt;
&lt;br /&gt;
Let us assume left, that the capacitor, C is fully “discharged” and the switch (S) is fully open. These are the initial conditions of the circuit, then t = 0, i = 0 and q = 0. When the switch is closed the time begins at t = 0 and current begins to flow into the capacitor via the resistor.&lt;br /&gt;
&lt;br /&gt;
Since the initial voltage across the capacitor is zero, ( Vc = 0 ) the capacitor appears to be a short circuit to the external circuit and the maximum current flows through the circuit restricted only by the resistor R. &lt;br /&gt;
&lt;br /&gt;
As the capacitor charges up, the potential difference across its plates slowly increases with the actual time taken for the charge on the capacitor to reach its maximum possible voltage. The maximum voltage the capacitor reaches is equal to the voltage supply of the battery. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
ΔV = I * R&lt;br /&gt;
&lt;br /&gt;
Q=CV&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Rc_switch.JPG&amp;diff=22768</id>
		<title>File:Rc switch.JPG</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Rc_switch.JPG&amp;diff=22768"/>
		<updated>2016-04-18T00:49:53Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: RC diagram created using draw.io&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;RC diagram created using draw.io&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22645</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22645"/>
		<updated>2016-04-17T23:32:52Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel. The figure in the top right of the page shows an RC circuit.&lt;br /&gt;
&lt;br /&gt;
Potential difference across a capacitor is delta V = Q/C. Q is equal to the charge on the plate and C is the capacitnce. &lt;br /&gt;
&lt;br /&gt;
below shows a capacitor, ( C ) in series with a resistor, ( R ) forming a RC Charging Circuit connected across a DC battery supply ( Vs ) via a mechanical switch. When the switch is closed, the capacitor will gradually charge up through the resistor until the voltage across it reaches the supply voltage of the battery. The manner in which the capacitor charges up is also shown below.&lt;br /&gt;
&lt;br /&gt;
Let us assume left, that the capacitor, C is fully “discharged” and the switch (S) is fully open. These are the initial conditions of the circuit, then t = 0, i = 0 and q = 0. When the switch is closed the time begins at t = 0 and current begins to flow into the capacitor via the resistor.&lt;br /&gt;
&lt;br /&gt;
Since the initial voltage across the capacitor is zero, ( Vc = 0 ) the capacitor appears to be a short circuit to the external circuit and the maximum current flows through the circuit restricted only by the resistor R. &lt;br /&gt;
&lt;br /&gt;
As the capacitor charges up, the potential difference across its plates slowly increases with the actual time taken for the charge on the capacitor to reach its maximum possible voltage. The maximum voltage the capacitor reaches is equal to the voltage supply of the battery. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
ΔV = I * R&lt;br /&gt;
&lt;br /&gt;
Q=CV&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22618</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22618"/>
		<updated>2016-04-17T23:20:10Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: /* The Main Idea */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
An RC circuit is a circuit that contains a battery with a known emf, a resistor (R), and a capacitor (C). An RC circuit can be in either series or parallel, but in Physics II, we primarily see it used in series. The figure in the top right of the page shows an RC circuit.  &lt;br /&gt;
&lt;br /&gt;
below shows a capacitor, ( C ) in series with a resistor, ( R ) forming a RC Charging Circuit connected across a DC battery supply ( Vs ) via a mechanical switch. When the switch is closed, the capacitor will gradually charge up through the resistor until the voltage across it reaches the supply voltage of the battery. The manner in which the capacitor charges up is also shown below.&lt;br /&gt;
&lt;br /&gt;
Let us assume left, that the capacitor, C is fully “discharged” and the switch (S) is fully open. These are the initial conditions of the circuit, then t = 0, i = 0 and q = 0. When the switch is closed the time begins at t = 0 and current begins to flow into the capacitor via the resistor.&lt;br /&gt;
&lt;br /&gt;
Since the initial voltage across the capacitor is zero, ( Vc = 0 ) the capacitor appears to be a short circuit to the external circuit and the maximum current flows through the circuit restricted only by the resistor R. &lt;br /&gt;
&lt;br /&gt;
As the capacitor charges up, the potential difference across its plates slowly increases with the actual time taken for the charge on the capacitor to reach its maximum possible voltage. The maximum voltage the capacitor reaches is equal to the voltage supply of the battery. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
ΔV = I * R&lt;br /&gt;
&lt;br /&gt;
Q=CV&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22610</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22610"/>
		<updated>2016-04-17T23:16:56Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|400px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The figure below shows a capacitor, ( C ) in series with a resistor, ( R ) forming a RC Charging Circuit connected across a DC battery supply ( Vs ) via a mechanical switch. When the switch is closed, the capacitor will gradually charge up through the resistor until the voltage across it reaches the supply voltage of the battery. The manner in which the capacitor charges up is also shown below.&lt;br /&gt;
&lt;br /&gt;
Let us assume left, that the capacitor, C is fully “discharged” and the switch (S) is fully open. These are the initial conditions of the circuit, then t = 0, i = 0 and q = 0. When the switch is closed the time begins at t = 0 and current begins to flow into the capacitor via the resistor.&lt;br /&gt;
&lt;br /&gt;
Since the initial voltage across the capacitor is zero, ( Vc = 0 ) the capacitor appears to be a short circuit to the external circuit and the maximum current flows through the circuit restricted only by the resistor R. &lt;br /&gt;
&lt;br /&gt;
As the capacitor charges up, the potential difference across its plates slowly increases with the actual time taken for the charge on the capacitor to reach its maximum possible voltage. The maximum voltage the capacitor reaches is equal to the voltage supply of the battery. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
ΔV = I * R&lt;br /&gt;
&lt;br /&gt;
Q=CV&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22609</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22609"/>
		<updated>2016-04-17T23:16:32Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|300px|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The figure below shows a capacitor, ( C ) in series with a resistor, ( R ) forming a RC Charging Circuit connected across a DC battery supply ( Vs ) via a mechanical switch. When the switch is closed, the capacitor will gradually charge up through the resistor until the voltage across it reaches the supply voltage of the battery. The manner in which the capacitor charges up is also shown below.&lt;br /&gt;
&lt;br /&gt;
Let us assume left, that the capacitor, C is fully “discharged” and the switch (S) is fully open. These are the initial conditions of the circuit, then t = 0, i = 0 and q = 0. When the switch is closed the time begins at t = 0 and current begins to flow into the capacitor via the resistor.&lt;br /&gt;
&lt;br /&gt;
Since the initial voltage across the capacitor is zero, ( Vc = 0 ) the capacitor appears to be a short circuit to the external circuit and the maximum current flows through the circuit restricted only by the resistor R. &lt;br /&gt;
&lt;br /&gt;
As the capacitor charges up, the potential difference across its plates slowly increases with the actual time taken for the charge on the capacitor to reach its maximum possible voltage. The maximum voltage the capacitor reaches is equal to the voltage supply of the battery. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
ΔV = I * R&lt;br /&gt;
&lt;br /&gt;
Q=CV&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22607</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22607"/>
		<updated>2016-04-17T23:15:30Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
[[File:Rc_circuit.JPG|300px|thumb|right|]]&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The figure below shows a capacitor, ( C ) in series with a resistor, ( R ) forming a RC Charging Circuit connected across a DC battery supply ( Vs ) via a mechanical switch. When the switch is closed, the capacitor will gradually charge up through the resistor until the voltage across it reaches the supply voltage of the battery. The manner in which the capacitor charges up is also shown below.&lt;br /&gt;
&lt;br /&gt;
Let us assume left, that the capacitor, C is fully “discharged” and the switch (S) is fully open. These are the initial conditions of the circuit, then t = 0, i = 0 and q = 0. When the switch is closed the time begins at t = 0 and current begins to flow into the capacitor via the resistor.&lt;br /&gt;
&lt;br /&gt;
Since the initial voltage across the capacitor is zero, ( Vc = 0 ) the capacitor appears to be a short circuit to the external circuit and the maximum current flows through the circuit restricted only by the resistor R. &lt;br /&gt;
&lt;br /&gt;
As the capacitor charges up, the potential difference across its plates slowly increases with the actual time taken for the charge on the capacitor to reach its maximum possible voltage. The maximum voltage the capacitor reaches is equal to the voltage supply of the battery. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
ΔV = I * R&lt;br /&gt;
&lt;br /&gt;
Q=CV&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22606</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22606"/>
		<updated>2016-04-17T23:14:38Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The figure below shows a capacitor, ( C ) in series with a resistor, ( R ) forming a RC Charging Circuit connected across a DC battery supply ( Vs ) via a mechanical switch. When the switch is closed, the capacitor will gradually charge up through the resistor until the voltage across it reaches the supply voltage of the battery. The manner in which the capacitor charges up is also shown below.&lt;br /&gt;
[[File:Rc_circuit.JPG|300px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
Let us assume left, that the capacitor, C is fully “discharged” and the switch (S) is fully open. These are the initial conditions of the circuit, then t = 0, i = 0 and q = 0. When the switch is closed the time begins at t = 0 and current begins to flow into the capacitor via the resistor.&lt;br /&gt;
&lt;br /&gt;
Since the initial voltage across the capacitor is zero, ( Vc = 0 ) the capacitor appears to be a short circuit to the external circuit and the maximum current flows through the circuit restricted only by the resistor R. &lt;br /&gt;
&lt;br /&gt;
As the capacitor charges up, the potential difference across its plates slowly increases with the actual time taken for the charge on the capacitor to reach its maximum possible voltage. The maximum voltage the capacitor reaches is equal to the voltage supply of the battery. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
ΔV = I * R&lt;br /&gt;
&lt;br /&gt;
Q=CV&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22605</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22605"/>
		<updated>2016-04-17T23:12:58Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The figure below shows a capacitor, ( C ) in series with a resistor, ( R ) forming a RC Charging Circuit connected across a DC battery supply ( Vs ) via a mechanical switch. When the switch is closed, the capacitor will gradually charge up through the resistor until the voltage across it reaches the supply voltage of the battery. The manner in which the capacitor charges up is also shown below.&lt;br /&gt;
[[File:rc circuit.jpg|300px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
Let us assume left, that the capacitor, C is fully “discharged” and the switch (S) is fully open. These are the initial conditions of the circuit, then t = 0, i = 0 and q = 0. When the switch is closed the time begins at t = 0 and current begins to flow into the capacitor via the resistor.&lt;br /&gt;
&lt;br /&gt;
Since the initial voltage across the capacitor is zero, ( Vc = 0 ) the capacitor appears to be a short circuit to the external circuit and the maximum current flows through the circuit restricted only by the resistor R. &lt;br /&gt;
&lt;br /&gt;
As the capacitor charges up, the potential difference across its plates slowly increases with the actual time taken for the charge on the capacitor to reach its maximum possible voltage. The maximum voltage the capacitor reaches is equal to the voltage supply of the battery. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
ΔV = I * R&lt;br /&gt;
&lt;br /&gt;
Q=CV&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=File:Rc_circuit.JPG&amp;diff=22603</id>
		<title>File:Rc circuit.JPG</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=File:Rc_circuit.JPG&amp;diff=22603"/>
		<updated>2016-04-17T23:10:58Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: RC circuit made using draw.io&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;RC circuit made using draw.io&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=Main_Page&amp;diff=22463</id>
		<title>Main Page</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=Main_Page&amp;diff=22463"/>
		<updated>2016-04-17T20:55:47Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: /* Electric field and potential in circuits with capacitors */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;__NOTOC__&lt;br /&gt;
Welcome to the Georgia Tech Wiki for Introductory Physics.  This resource was created so that students can contribute and curate content to help those with limited or no access to a textbook.  When reading this website, please correct any errors you may come across. If you read something that isn&#039;t clear, please consider revising it for future students!&lt;br /&gt;
&lt;br /&gt;
Looking to make a contribution?&lt;br /&gt;
#Pick one of the topics from intro physics listed below&lt;br /&gt;
#Add content to that topic or improve the quality of what is already there.&lt;br /&gt;
#Need to make a new topic? Edit this page and add it to the list under the appropriate category.  Then copy and paste the default [[Template]] into your new page and start editing.&lt;br /&gt;
&lt;br /&gt;
Please remember that this is not a textbook and you are not limited to expressing your ideas with only text and equations.  Whenever possible embed: pictures, videos, diagrams, simulations, computational models (e.g. Glowscript), and whatever content you think makes learning physics easier for other students.&lt;br /&gt;
&lt;br /&gt;
== Source Material ==&lt;br /&gt;
All of the content added to this resource must be in the public domain or similar free resource.  If you are unsure about a source, contact the original author for permission. That said, there is a surprisingly large amount of introductory physics content scattered across the web.  Here is an incomplete list of intro physics resources (please update as needed).&lt;br /&gt;
* A physics resource written by experts for an expert audience [https://en.wikipedia.org/wiki/Portal:Physics Physics Portal]&lt;br /&gt;
* A wiki written for students by a physics expert [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes MSU Physics Wiki]&lt;br /&gt;
* A wiki book on modern physics [https://en.wikibooks.org/wiki/Modern_Physics Modern Physics Wiki]&lt;br /&gt;
* The MIT open courseware for intro physics [http://ocw.mit.edu/resources/res-8-002-a-wikitextbook-for-introductory-mechanics-fall-2009/index.htm MITOCW Wiki]&lt;br /&gt;
* An online concept map of intro physics [http://hyperphysics.phy-astr.gsu.edu/hbase/hph.html HyperPhysics]&lt;br /&gt;
* Interactive physics simulations [https://phet.colorado.edu/en/simulations/category/physics PhET]&lt;br /&gt;
* OpenStax algebra based intro physics textbook [https://openstaxcollege.org/textbooks/college-physics College Physics]&lt;br /&gt;
* The Open Source Physics project is a collection of online physics resources [http://www.opensourcephysics.org/ OSP]&lt;br /&gt;
* A resource guide compiled by the [http://www.aapt.org/ AAPT] for educators [http://www.compadre.org/ ComPADRE]&lt;br /&gt;
&lt;br /&gt;
== Organizing Categories ==&lt;br /&gt;
These are the broad, overarching categories, that we cover in three semester of introductory physics.  You can add subcategories as needed but a single topic should direct readers to a page in one of these categories.&lt;br /&gt;
&lt;br /&gt;
== Resources ==&lt;br /&gt;
* Commonly used wiki commands [https://en.wikipedia.org/wiki/Help:Cheatsheet Wiki Cheatsheet]&lt;br /&gt;
* A guide to representing equations in math mode [https://en.wikipedia.org/wiki/Help:Displaying_a_formula Wiki Math Mode]&lt;br /&gt;
* A page to keep track of all the physics [[Constants]]&lt;br /&gt;
* A page for review of [[Vectors]] and vector operations&lt;br /&gt;
* A listing of [[Notable Scientist]] with links to their individual pages &lt;br /&gt;
&lt;br /&gt;
&amp;lt;div style=&amp;quot;float:left; width:30%; padding:1%;&amp;quot;&amp;gt;&lt;br /&gt;
==Physics 1==&lt;br /&gt;
===Week 1===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Help with VPython=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[VPython]]&lt;br /&gt;
*[[VPython basics]]&lt;br /&gt;
*[[VPython Common Errors and Troubleshooting]]&lt;br /&gt;
*[[VPython Functions]]&lt;br /&gt;
*[[VPython Lists]]&lt;br /&gt;
*[[VPython Loops]]&lt;br /&gt;
*[[VPython Multithreading]]&lt;br /&gt;
*[[VPython Animation]]&lt;br /&gt;
*[[VPython Objects]]&lt;br /&gt;
*[[VPython 3D Objects]]&lt;br /&gt;
*[[VPython Reference]]&lt;br /&gt;
*[[VPython MapReduceFilter]]&lt;br /&gt;
*[[VPython GUIs]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Vectors and Units=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Vectors]]&lt;br /&gt;
*[[SI units]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=====Interactions=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
*[[Types of Interactions and How to Detect Them]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=====Velocity and Momentum=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Newton’s First Law of Motion]]&lt;br /&gt;
*[[Velocity]]&lt;br /&gt;
*[[Mass]]&lt;br /&gt;
*[[Speed and Velocity]]&lt;br /&gt;
*[[Relative Velocity]]&lt;br /&gt;
*[[Derivation of Average Velocity]]&lt;br /&gt;
*[[2-Dimensional Motion]]&lt;br /&gt;
*[[3-Dimensional Position and Motion]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:vpython_resources Software for Projects]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 2===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Momentum and the Momentum Principle=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Momentum Principle]]&lt;br /&gt;
*[[Inertia]]&lt;br /&gt;
*[[Net Force]]&lt;br /&gt;
*[[Derivation of the Momentum Principle]]&lt;br /&gt;
*[[Impulse Momentum]]&lt;br /&gt;
*[[Acceleration]]&lt;br /&gt;
*[[Momentum with respect to external Forces]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Iterative Prediction with a Constant Force=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Newton’s Second Law of Motion]]&lt;br /&gt;
*[[Iterative Prediction]]&lt;br /&gt;
*[[Kinematics]]&lt;br /&gt;
*[[Newton’s Laws and Linear Momentum]]&lt;br /&gt;
*[[Projectile Motion]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:scalars_and_vectors Scalars and Vectors]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:displacement_and_velocity Displacement and Velocity]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:modeling_with_vpython Modeling Motion with VPython]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:relative_motion Relative Motion]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:graphing_motion Graphing Motion]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:momentum Momentum]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:momentum_principle The Momentum Principle]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:acceleration Acceleration &amp;amp; The Change in Momentum]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:motionPredict Applying the Momentum Principle]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:constantF Constant Force Motion]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:iterativePredict Iterative Prediction of Motion]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:mp_multi The Momentum Principle in Multi-particle Systems]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:angular_motivation Why Angular Momentum?]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:ang_momentum Angular Momentum]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:L_principle Net Torque &amp;amp; The Angular Momentum Principle]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:L_conservation Angular Momentum Conservation]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Week 3===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours \&lt;br /&gt;
mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Analytic Prediction with a Constant Force=====&lt;br /&gt;
&amp;lt;div \&lt;br /&gt;
class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Analytical Prediction]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Iterative Prediction with a Varying Force=====&lt;br /&gt;
&amp;lt;div \&lt;br /&gt;
class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Predicting Change in multiple dimensions]]&lt;br /&gt;
*[[Spring Force]]&lt;br /&gt;
*[[Hooke’s Law]]&lt;br /&gt;
*[[Simple Harmonic Motion]]&lt;br /&gt;
*[[Iterative Prediction of Spring-Mass System]]&lt;br /&gt;
*[[Terminal Speed]]&lt;br /&gt;
*[[Determinism]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:drag Drag]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:gravitation Non-constant Force: Newtonian Gravitation]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:ucm Uniform Circular Motion]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:impulseGraphs Impulse Graphs]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:springMotion Non-constant Force: Springs &amp;amp; Spring-like Interactions]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:friction Contact Interactions: The Normal Force &amp;amp; Friction]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Week 4===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours \&lt;br /&gt;
mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Fundamental Interactions=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Gravitational Force]]&lt;br /&gt;
*[[Electric Force]]&lt;br /&gt;
*[[Reciprocity]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:gravitation Non-constant Force: Newtonian Gravitation]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Week 5===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours \&lt;br /&gt;
mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Conservation of Momentum=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Conservation of Momentum]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=====Properties of Matter=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Kinds of Matter]]&lt;br /&gt;
**[[Ball and Spring Model of Matter]]&lt;br /&gt;
*[[Density]]&lt;br /&gt;
*[[Length and Stiffness of an Interatomic Bond]]&lt;br /&gt;
*[[Young’s Modulus]]&lt;br /&gt;
*[[Speed of Sound in Solids]]&lt;br /&gt;
*[[Malleability]]&lt;br /&gt;
*[[Ductility]]&lt;br /&gt;
*[[Weight]]&lt;br /&gt;
*[[Hardness]]&lt;br /&gt;
*[[Boiling Point]]&lt;br /&gt;
*[[Melting Point]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:model_of_a_wire Modeling a Solid Wire: springs in series and parallel]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Week 6===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours \&lt;br /&gt;
mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Identifying Forces=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Free Body Diagram]]&lt;br /&gt;
*[[Compression or Normal Force]]&lt;br /&gt;
*[[Tension]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Curving Motion=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Curving Motion]]&lt;br /&gt;
*[[Centripetal Force and Curving Motion]]&lt;br /&gt;
*[[Perpetual Freefall (Orbit)]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:gravitation Non-constant Force: Newtonian Gravitation]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:grav_accel Gravitational Acceleration]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:ucm Uniform Circular Motion]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:freebodydiagrams Free Body Diagrams]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:curving_motion Curved Motion]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Week 7===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours \&lt;br /&gt;
mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Energy Principle=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[The Energy Principle]]&lt;br /&gt;
*[[Conservation of Energy]]&lt;br /&gt;
*[[Kinetic Energy]]&lt;br /&gt;
*[[Work]]&lt;br /&gt;
*[[Power (Mechanical)]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:define_energy What is Energy?]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:point_particle The Simplest System: A Single Particle]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:work Work: Mechanical Energy Transfer]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:energy_cons Conservation of Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:potential_energy Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:grav_and_spring_PE (Near Earth) Gravitational and Spring Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:force_and_PE Force and Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:newton_grav_pe Newtonian Gravitational Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:spring_PE Spring Potential Energy]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 8===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours \&lt;br /&gt;
mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Work by Non-Constant Forces=====&lt;br /&gt;
&amp;lt;div \&lt;br /&gt;
class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Work Done By A Nonconstant Force]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Potential Energy=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Potential Energy]]&lt;br /&gt;
*[[Potential Energy of Macroscopic Springs]]&lt;br /&gt;
*[[Spring Potential Energy]]&lt;br /&gt;
**[[Ball and Spring Model]]&lt;br /&gt;
*[[Gravitational Potential Energy]]&lt;br /&gt;
*[[Energy Graphs]]&lt;br /&gt;
*[[Escape Velocity]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:work_by_nc_forces Work Done by Non-Constant Forces]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:potential_energy Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:grav_and_spring_PE (Near Earth) Gravitational and Spring Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:rest_mass Changes of Rest Mass Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:force_and_PE Force and Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:newton_grav_pe Newtonian Gravitational Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:grav_pe_graphs Graphing Energy for Gravitationally Interacting Systems]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:spring_PE Spring Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:power Power: The Rate of Energy Change]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:energy_dissipation Dissipation of Energy]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Week 9===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours \&lt;br /&gt;
mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Multiparticle Systems=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Center of Mass]]&lt;br /&gt;
*[[Multi-particle analysis of Momentum]]&lt;br /&gt;
*[[Momentum with respect to external Forces]]&lt;br /&gt;
*[[Potential Energy of a Multiparticle System]]&lt;br /&gt;
*[[Work and Energy for an Extended System]]&lt;br /&gt;
*[[Internal Energy]]&lt;br /&gt;
**[[Potential Energy of a Pair of Neutral Atoms]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:mp_multi The Momentum Principle in Multi-particle Systems]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:center_of_mass Center of Mass Motion]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:center_of_mass Center of Mass Motion]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:energy_sep Separating Energy in Multi-Particle Systems]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Week 10===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours \&lt;br /&gt;
mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Choice of System=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[System &amp;amp; Surroundings]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Thermal Energy, Dissipation and Transfer of Energy=====&lt;br /&gt;
&amp;lt;div \&lt;br /&gt;
class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Thermal Energy]]&lt;br /&gt;
*[[Specific Heat]]&lt;br /&gt;
*[[Heat Capacity]]&lt;br /&gt;
*[[Specific Heat Capacity]]&lt;br /&gt;
*[[First Law of Thermodynamics]]&lt;br /&gt;
*[[Second Law of Thermodynamics and Entropy]]&lt;br /&gt;
*[[Temperature]]&lt;br /&gt;
*[[Predicting Change]]&lt;br /&gt;
*[[Energy Transfer due to a Temperature Difference]]&lt;br /&gt;
*[[Transformation of Energy]]&lt;br /&gt;
*[[The Maxwell-Boltzmann Distribution]]&lt;br /&gt;
*[[Air Resistance]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Rotational and Vibrational Energy=====&lt;br /&gt;
&amp;lt;div \&lt;br /&gt;
class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Translational, Rotational and Vibrational Energy]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:grav_and_spring_PE (Near Earth) Gravitational and Spring Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:rest_mass Changes of Rest Mass Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:newton_grav_pe Newtonian Gravitational Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:grav_pe_graphs Graphing Energy for Gravitationally Interacting Systems]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:escape_speed Escape Speed]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:spring_PE Spring Potential Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:internal_energy Internal Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:system_choice Choosing a System Matters]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:energy_dissipation Dissipation of Energy]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 11===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours \&lt;br /&gt;
mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Different Models of a System=====&lt;br /&gt;
&amp;lt;div \&lt;br /&gt;
class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Real Systems]]&lt;br /&gt;
*[[Point Particle Systems]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=====Models of Friction=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Friction]]&lt;br /&gt;
*[[Static Friction]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:system_choice Choosing a System Matters]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:energy_dissipation Dissipation of Energy]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Week 12===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours \&lt;br /&gt;
mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Collisions=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Newton’s Third Law of Motion]]&lt;br /&gt;
*[[Collisions]]&lt;br /&gt;
*[[Elastic Collisions]]&lt;br /&gt;
*[[Inelastic Collisions]]&lt;br /&gt;
*[[Maximally Inelastic Collision]]&lt;br /&gt;
*[[Head-on Collision of Equal Masses]]&lt;br /&gt;
*[[Head-on Collision of Unequal Masses]]&lt;br /&gt;
*[[Scattering: Collisions in 2D and 3D]]&lt;br /&gt;
*[[Rutherford Experiment and Atomic Collisions]]&lt;br /&gt;
*[[Coefficient of Restitution]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:collisions Colliding Objects]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:center_of_mass Center of Mass Motion]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:center_of_mass Center of Mass Motion]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:rot_KE Rotational Kinetic Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:pp_vs_real Point Particle and Real Systems]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:colliding_systems Collisions]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Week 13===&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours \&lt;br /&gt;
mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Rotations=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Rotation]]&lt;br /&gt;
*[[Angular Velocity]]&lt;br /&gt;
*[[Eulerian Angles]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
=====Angular Momentum=====&lt;br /&gt;
&amp;lt;div class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Total Angular Momentum]]&lt;br /&gt;
*[[Translational Angular Momentum]]&lt;br /&gt;
*[[Rotational Angular Momentum]]&lt;br /&gt;
*[[The Angular Momentum Principle]]&lt;br /&gt;
*[[Angular Momentum Compared to Linear Momentum]]&lt;br /&gt;
*[[Angular Impulse]]&lt;br /&gt;
*[[Predicting the Position of a Rotating System]]&lt;br /&gt;
*[[Angular Momentum of Multiparticle Systems]]&lt;br /&gt;
*[[The Moments of Inertia]]&lt;br /&gt;
*[[Moment of Inertia for a cylinder]]&lt;br /&gt;
*[[Right Hand Rule]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:rot_KE Rotational Kinetic Energy]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:angular_motivation Why Angular Momentum?]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:ang_momentum Angular Momentum]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:L_principle Net Torque &amp;amp; The Angular Momentum Principle]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:L_conservation Angular Momentum Conservation]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
===Week 14===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
=====Analyzing Motion with and without Torque=====&lt;br /&gt;
&amp;lt;div \&lt;br /&gt;
class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Torque]]&lt;br /&gt;
*[[Torque 2]]&lt;br /&gt;
*[[Systems with Zero Torque]]&lt;br /&gt;
*[[Systems with Nonzero Torque]]&lt;br /&gt;
*[[Torque vs Work]]&lt;br /&gt;
*[[Gyroscopes]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:discovery_of_the_nucleus Discovery of the Nucleus]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:torque Torques Cause Changes in Rotation]&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:L_principle Net Torque &amp;amp; The Angular Momentum Principle]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 15===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====Student Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
=====Introduction to Quantum Concepts=====&lt;br /&gt;
&amp;lt;div \class=“mw-collapsible-content”&amp;gt;&lt;br /&gt;
*[[Bohr Model]]&lt;br /&gt;
*[[Energy graphs and the Bohr model]]&lt;br /&gt;
*[[Quantized energy levels]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====Expert Content====&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible \&lt;br /&gt;
mw-collapsed”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* [http://p3server.pa.msu.edu/coursewiki/doku.php?id=183_notes:discovery_of_the_nucleus Discovery of the Nucleus]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div style=“float:left; width:30%; padding:1%;”&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Physics 2==&lt;br /&gt;
===Week 1===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====3D Vectors====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Vectors]]&lt;br /&gt;
*[[Right-Hand Rule]]&lt;br /&gt;
*[[Right Hand Rule]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Electric field]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;CLAIMED BY DIPRO CHAKRABORTY&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Electric force====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
*[[Electric Force]] Claimed by Amarachi Eze&lt;br /&gt;
*[[Lorentz Force]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====Electric field of a point particle====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Point Charge]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Bold text&#039;&#039;&#039;====Superposition====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Superposition Principle]]&lt;br /&gt;
*[[Superposition principle]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Dipoles====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Electric Dipole]]&lt;br /&gt;
*[[Magnetic Dipole]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 2===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Interactions of charged objects====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Electric Field]]&lt;br /&gt;
*[[Electric Potential]]&lt;br /&gt;
*[[Electric Force]]&lt;br /&gt;
*[[Lorentz Force]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Tape experiments====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Polarization]]&lt;br /&gt;
*[[Electric Polarization]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Polarization====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Polarization]]&lt;br /&gt;
*[[Electric Polarization]]&lt;br /&gt;
*[[Polarization of an Atom]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 3===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Insulators====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Insulators]]&lt;br /&gt;
*[[Potential Difference in an Insulator]]&lt;br /&gt;
*[[Charged Conductor and Charged Insulator]]&lt;br /&gt;
*[[Charged conductor and charged insulator]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Conductors====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Conductivity]]&lt;br /&gt;
*[[Charge Transfer]]&lt;br /&gt;
*[[Resistivity]]&lt;br /&gt;
*[[Polarization of a conductor]]&lt;br /&gt;
*[[Charged Conductor and Charged Insulator]]&lt;br /&gt;
*[[Charged conductor and charged insulator]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Charging and discharging====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Charge Transfer]]&lt;br /&gt;
*[[Electrostatic Discharge]]&lt;br /&gt;
*[[Charged Conductor and Charged Insulator]]&lt;br /&gt;
*[[Charged conductor and charged insulator]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 4===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Field of a charged rod====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Charged Rod]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Field of a charged ring/disk/capacitor====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Charged Ring]]&lt;br /&gt;
*[[Charged Disk]]&lt;br /&gt;
*[[Charged Capacitor]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Field of a charged sphere====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Charged Spherical Shell]]&lt;br /&gt;
*[[Field of a Charged Ball]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 5===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Potential energy====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Potential Energy]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Electric potential====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Electric Potential]]&lt;br /&gt;
*[[Path Independence of Electric Potential]]&lt;br /&gt;
*[[Potential Difference Path Independence, claimed by Aditya Mohile]] &lt;br /&gt;
*[[Potential Difference in a Uniform Field]]&lt;br /&gt;
*[[Potential Difference of Point Charge in a Non-Uniform Field]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Sign of Potential Difference====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Sign of Potential Difference]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Potential at a single location====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Electric Potential]]&lt;br /&gt;
*[[Potential Difference at One Location]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Path independence and round trip potential====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Path Independence of Electric Potential]]&lt;br /&gt;
*[[Potential Difference Path Independence, claimed by Aditya Mohile]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 6===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Electric field and potential in an insulator====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Potential Difference in an Insulator]]&lt;br /&gt;
*[[Electric Field in an Insulator]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Moving charges in a magnetic field====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Magnetic Field]]&lt;br /&gt;
*[[Magnetic Force]]&lt;br /&gt;
*[[Lorentz Force]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Biot-Savart Law====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Biot-Savart Law]]&lt;br /&gt;
*[[Biot-Savart Law for Currents]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Moving charges, electron current, and conventional current====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Moving Point Charge]]&lt;br /&gt;
*[[Current]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 7=== Claimed by Diem Tran&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Magnetic field of a wire====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Magnetic Field of a Long Straight Wire]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Magnetic field of a current-carrying loop====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Magnetic Field of a Loop]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Magnetic dipoles====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Magnetic Dipole Moment]]&lt;br /&gt;
*[[Bar Magnet]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Atomic structure of magnets====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Atomic Structure of Magnets]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 8===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Steady state current====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Steady State]]&lt;br /&gt;
*[[Non Steady State]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Node rule====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Node Rule]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Electric fields and energy in circuits====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Series circuit]] &lt;br /&gt;
*[[Node Rule]]&lt;br /&gt;
*[[Loop Rule]]&lt;br /&gt;
*[[Electric Potential Difference]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Macroscopic analysis of circuits====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Series Circuits]]&lt;br /&gt;
*[[Parallel CIrcuits]]&lt;br /&gt;
*[[Parallel Circuits vs. Series Circuits*]]&lt;br /&gt;
*[[Loop Rule]]&lt;br /&gt;
*[[Node Rule]]&lt;br /&gt;
*[[Resistors*]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 9===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Electric field and potential in circuits with capacitors====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Charging and Discharging a Capacitor]]&lt;br /&gt;
*[[RC Circuit]] *CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
*[[R Circuit]]&lt;br /&gt;
*[[AC and DC]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Magnetic forces on charges and currents====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Magnetic Force]]&lt;br /&gt;
*[[Lorentz Force]]&lt;br /&gt;
*[[Applying Magnetic Force to Currents]]&lt;br /&gt;
*[[Magnetic Force in a Moving Reference Frame]]&lt;br /&gt;
*[[Right-Hand Rule]]&lt;br /&gt;
*[[Analysis of Railgun vs Coil gun technologies]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Electric and magnetic forces====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Electric Force]]&lt;br /&gt;
*[[Magnetic Force]]&lt;br /&gt;
*[[Lorentz Force]]&lt;br /&gt;
*[[VPython Modelling of Electric and Magnetic Forces]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Velocity selector====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Lorentz Force]]&lt;br /&gt;
*[[Combining Electric and Magnetic Forces]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 10===&lt;br /&gt;
&lt;br /&gt;
====Student Content====&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
==== Hall Effect ====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Hall Effect]]&lt;br /&gt;
*[[Motional Emf]]&lt;br /&gt;
*[[Magnetic Force]]&lt;br /&gt;
*[[Magnetic Torque]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 13===&lt;br /&gt;
&amp;lt;div class=“toccolours mw-collapsible mw-collapsed”&amp;gt;&lt;br /&gt;
==== Changing Field Patterns ====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Faraday&#039;s Law - claimed by duql1030]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Physics 3==&lt;br /&gt;
&lt;br /&gt;
===Week 1===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Classical Physics====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 2===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Special Relativity====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Frame of Reference]]&lt;br /&gt;
*[[Einstein&#039;s Theory of Special Relativity]]&lt;br /&gt;
*[[Time Dilation]]&lt;br /&gt;
*[[Einstein&#039;s Theory of General Relativity]]&lt;br /&gt;
*[[Albert A. Micheleson &amp;amp; Edward W. Morley]]&lt;br /&gt;
*[[Magnetic Force in a Moving Reference Frame]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 3===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Photons====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Spontaneous Photon Emission]]&lt;br /&gt;
*[[Light Scattering: Why is the Sky Blue]]&lt;br /&gt;
*[[Lasers]]&lt;br /&gt;
*[[Electronic Energy Levels and Photons]]&lt;br /&gt;
*[[Quantum Properties of Light]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 4===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Matter Waves====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Wave-Particle Duality]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 5===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Wave Mechanics====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Standing Waves]]&lt;br /&gt;
*[[Wavelength]]&lt;br /&gt;
*[[Wavelength and Frequency]]&lt;br /&gt;
*[[Mechanical Waves]]&lt;br /&gt;
*[[Transverse and Longitudinal Waves]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 6===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Rutherford-Bohr Model====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Rutherford Experiment and Atomic Collisions]]&lt;br /&gt;
*[[Bohr Model]]&lt;br /&gt;
*[[Quantized energy levels]]&lt;br /&gt;
*[[Energy graphs and the Bohr model]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 7===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====The Hydrogen Atom====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Quantum Theory]]&lt;br /&gt;
*[[Atomic Theory]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 8===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Many-Electron Atoms====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Quantum Theory]]&lt;br /&gt;
*[[Atomic Theory]]&lt;br /&gt;
*[[Pauli exclusion principle]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 9===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Molecules====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 10===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Statistical Physics====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 11===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Condensed Matter Physics====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 12===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====The Nucleus====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 13===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Nuclear Physics====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Nuclear Fission]]&lt;br /&gt;
*[[Nuclear Energy from Fission and Fusion]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Week 14===&lt;br /&gt;
&amp;lt;div class=&amp;quot;toccolours mw-collapsible mw-collapsed&amp;quot;&amp;gt;&lt;br /&gt;
====Particle Physics====&lt;br /&gt;
&amp;lt;div class=&amp;quot;mw-collapsible-content&amp;quot;&amp;gt;&lt;br /&gt;
*[[Elementary Particles and Particle Physics Theory]]&lt;br /&gt;
*[[String Theory]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
	<entry>
		<id>http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22448</id>
		<title>RC Circuit</title>
		<link rel="alternate" type="text/html" href="http://www.physicsbook.gatech.edu/index.php?title=RC_Circuit&amp;diff=22448"/>
		<updated>2016-04-17T20:42:14Z</updated>

		<summary type="html">&lt;p&gt;Mrussell38: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CLAIMED BY MARK RUSSELL SPRING 2016&lt;br /&gt;
&lt;br /&gt;
==The Main Idea==&lt;br /&gt;
&lt;br /&gt;
The figure below shows a capacitor, ( C ) in series with a resistor, ( R ) forming a RC Charging Circuit connected across a DC battery supply ( Vs ) via a mechanical switch. When the switch is closed, the capacitor will gradually charge up through the resistor until the voltage across it reaches the supply voltage of the battery. The manner in which the capacitor charges up is also shown below.&lt;br /&gt;
[[File:rc1.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
Let us assume left, that the capacitor, C is fully “discharged” and the switch (S) is fully open. These are the initial conditions of the circuit, then t = 0, i = 0 and q = 0. When the switch is closed the time begins at t = 0 and current begins to flow into the capacitor via the resistor.&lt;br /&gt;
&lt;br /&gt;
Since the initial voltage across the capacitor is zero, ( Vc = 0 ) the capacitor appears to be a short circuit to the external circuit and the maximum current flows through the circuit restricted only by the resistor R. &lt;br /&gt;
&lt;br /&gt;
As the capacitor charges up, the potential difference across its plates slowly increases with the actual time taken for the charge on the capacitor to reach its maximum possible voltage. The maximum voltage the capacitor reaches is equal to the voltage supply of the battery. Once the potential difference across the plates of the capacitor equals the battery&#039;s voltage supply, current will stop flowing through the circuit. This is known as the steady state of an RC circuit; it is reached when time goes to infinity.&lt;br /&gt;
===A Mathematical Model===&lt;br /&gt;
&lt;br /&gt;
ΔV = I * R&lt;br /&gt;
&lt;br /&gt;
Q=CV&lt;br /&gt;
&lt;br /&gt;
[[File:images.png|100px|thumb|left|]]&lt;br /&gt;
Node Rule-Current is assigned (positive or negative) quantity reflecting direction towards or away from a node. &lt;br /&gt;
This principle can be solved by adding all the currents up to equal 0. The Node Rule is important to RC Circuits &lt;br /&gt;
because finding the current flow in the different states of an RC Circuit often relies on nodes when the &lt;br /&gt;
capacitor is in parallel.&lt;br /&gt;
[[File:images2.jpeg|100px|thumb|right|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Loop Rule-Similar to the node rule; however, the voltage jumps and drops are added up around the circuit to equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
&lt;br /&gt;
===Simple===&lt;br /&gt;
[[File:RCcircuitSimple.gif|100px|thumb|left|]]&lt;br /&gt;
In the steady state what is the potential difference across the plates of the capacitor? The circuit has a resistor, R, capacitor, C, and battery, Vs.&lt;br /&gt;
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Solution: The key concept in this problem is that in the steady state time is approaching infinity. In an RC circuit as time approaches infinity, the current is 0 because the potential difference across the capacitor equals that of the battery. Therefore, the potential difference across the plates of the capacitor equals Vs.&lt;br /&gt;
===Difficult===&lt;br /&gt;
The circuit below has been in position a for a long time. At time t = 0 the switch is thrown to position b. DATA: Vb = 12 V, C = 10 mF, R = 20 W&lt;br /&gt;
[[File:rccircuit.gif|200px|thumb|left|]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
a.) What is the current through the resistor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
The circuit is in a steady state so I = 0&lt;br /&gt;
&lt;br /&gt;
b.) What is the current through the resistor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: I = V/R I = 0.6 amps since the capacitor has a potential difference and is creating the current.&lt;br /&gt;
&lt;br /&gt;
c.) What is the charge across the capacitor just BEFORE the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Q = CV&lt;br /&gt;
Q = 120 mC&lt;br /&gt;
&lt;br /&gt;
d.) What is the charge on the capacitor just AFTER the switch is thrown?&lt;br /&gt;
&lt;br /&gt;
Solution: Charge does not change instantaneously &lt;br /&gt;
Q = 120mC&lt;br /&gt;
==Connectedness==&lt;br /&gt;
#How is this topic connected to something that you are interested in?&lt;br /&gt;
:: RC Circuits can be used in musical instruments such as guitars and amplifiers. I play the guitar so it is cool to see how the guitar actually works.&lt;br /&gt;
#How is it connected to your major?&lt;br /&gt;
:: Mechanical Engineering requires the use of many electronics and learning how various circuits work is necessary for creating new parts and machines.&lt;br /&gt;
#Is there an interesting industrial application?&lt;br /&gt;
RC circuits can be used in many industrial areas to allow certain frequencies to pass through a circuit.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
===Further reading===&lt;br /&gt;
[[Charge in a RC Circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Current in a RC circuit]]&lt;br /&gt;
&lt;br /&gt;
[[Loop Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Node Rule]]&lt;br /&gt;
&lt;br /&gt;
[[Current]]&lt;br /&gt;
&lt;br /&gt;
===External links===&lt;br /&gt;
&lt;br /&gt;
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/rcimp.html&lt;br /&gt;
&lt;br /&gt;
http://www.allaboutcircuits.com/textbook/alternating-current/chpt-4/series-resistor-capacitor-circuits/&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
http://www.electronics-tutorials.ws/rc/rc_1.html&lt;br /&gt;
&lt;br /&gt;
https://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/examples.html&lt;br /&gt;
&lt;br /&gt;
[[Category:Simple Circuits]]&lt;/div&gt;</summary>
		<author><name>Mrussell38</name></author>
	</entry>
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