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<document xmlns="http://cnx.rice.edu/cnxml" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:bib="http://bibtexml.sf.net/" id="m0023">
  
  <name>Circuits with Capacitors and Inductors</name>

  <metadata>
  <md:version>2.10</md:version>
  <md:created>2000/07/07</md:created>
  <md:revised>2007/05/10 09:23:36.116 GMT-5</md:revised>
  <md:authorlist>
      <md:author id="dhj">
      <md:firstname>Don</md:firstname>
      
      <md:surname>Johnson</md:surname>
      <md:email>dhj@rice.edu</md:email>
    </md:author>
  </md:authorlist>

  <md:maintainerlist>
    <md:maintainer id="dhj">
      <md:firstname>Don</md:firstname>
      
      <md:surname>Johnson</md:surname>
      <md:email>dhj@rice.edu</md:email>
    </md:maintainer>
    <md:maintainer id="liqun">
      <md:firstname>Liqun</md:firstname>
      
      <md:surname>Wang</md:surname>
      <md:email>liqun@rice.edu</md:email>
    </md:maintainer>
    <md:maintainer id="bfite">
      <md:firstname>Benjamin</md:firstname>
      
      <md:surname>Fite</md:surname>
      <md:email>bfite@rice.edu</md:email>
    </md:maintainer>
  </md:maintainerlist>
  
  <md:keywordlist>
    <md:keyword>capacitor</md:keyword>
    <md:keyword>circuit</md:keyword>
    <md:keyword>inductor</md:keyword>
  </md:keywordlist>

  <md:abstract>Introducing when a circuit has capacitors and inductors other than resistors and sources, the impedance concept will be applied.</md:abstract>
</metadata>

  <content>

    <figure id="simpleRCcircuit">
      <name/>
      <media type="image/png" src="circuit5.png"/>
      <caption>
	A simple <m:math><m:ci>RC</m:ci></m:math> circuit.
      </caption>
    </figure>

    <para id="para1">
      Let's consider a circuit having something other than resistors
      and sources. Because of KVL, we know that
      <m:math>
	<m:apply>
	  <m:eq/>
	  <m:ci>
	    <m:msub>
	      <m:mi>v</m:mi>
	      <m:mi>in</m:mi>
	    </m:msub>
	  </m:ci>
	  <m:apply>
	    <m:plus/>
	    <m:ci>
	      <m:msub>
		<m:mi>v</m:mi>
		<m:mi>R</m:mi>
	      </m:msub>
	    </m:ci>
	    <m:ci>
	      <m:msub>
		<m:mi>v</m:mi>
		<m:mi>out</m:mi>
	      </m:msub>
	    </m:ci>
	  </m:apply>
	</m:apply>
      </m:math>.
      The current through the capacitor is given by
      <m:math>
	<m:apply>
	  <m:eq/>
	  <m:ci>i</m:ci>
	  <m:apply>
	    <m:times/>
	    <m:ci>C</m:ci>
	    <m:apply>
	      <m:diff/>
	      <m:bvar>
		<m:ci>t</m:ci>
	      </m:bvar>
	      <m:ci>
		<m:msub>
		  <m:mi>v</m:mi>
		  <m:mi>out</m:mi>
		</m:msub>
	      </m:ci>
	    </m:apply>
	  </m:apply>
	</m:apply>
      </m:math>, and this current equals that passing through the
      resistor. Substituting
      <m:math>
	<m:apply>
	  <m:eq/>
	  <m:ci>
	    <m:msub>
	      <m:mi>v</m:mi>
	      <m:mi>R</m:mi>
	    </m:msub>
	  </m:ci>
	  <m:apply>
	    <m:times/>
	    <m:ci>R</m:ci>
	    <m:ci>i</m:ci>
	  </m:apply>
	</m:apply>
      </m:math>
      into the KVL equation and using the <emphasis>v-i</emphasis>
      relation for the capacitor, we arrive at

      <equation id="eq1">
	<m:math>
	  <m:apply>
	    <m:eq/>
	    <m:apply>
	      <m:plus/>
	      <m:apply>
		<m:times/>
		<m:ci>R</m:ci>
		<m:ci>C</m:ci>
		<m:apply>
		  <m:diff/>
		  <m:bvar>
		    <m:ci>t</m:ci>
		  </m:bvar>
		  <m:ci>
		    <m:msub>
		      <m:mi>v</m:mi>
		      <m:mi>out</m:mi>
		    </m:msub>
		  </m:ci>
		</m:apply>
	      </m:apply>
	      <m:ci>
		<m:msub>
		  <m:mi>v</m:mi>
		  <m:mi>out</m:mi>
		</m:msub>
	      </m:ci>
	    </m:apply>
	    <m:ci>
	      <m:msub>
		<m:mi>v</m:mi>
		<m:mi>in</m:mi>
	      </m:msub>
	    </m:ci>
	  </m:apply>
	</m:math>
      </equation> 
      The input-output relation for circuits involving energy storage
      elements takes the form of an ordinary differential equation,
      which we must solve to determine what the output voltage is for
      a given input. In contrast to resistive circuits, where we
      obtain an <emphasis>explicit</emphasis> input-output relation,
      we now have an <emphasis>implicit</emphasis> relation that
      requires more work to obtain answers.
    </para>

    <!-- This next part will become a segue -->
    
    <para id="para2">At this point, we could learn how to solve differential
      equations. Note first that even finding the differential
      equation relating an output variable to a source is often very
      tedious. The parallel and series combination rules that apply to
      resistors don't directly apply when capacitors and inductors
      occur. We would have to slog our way through the circuit
      equations, simplifying them until we finally found the equation
      that related the source(s) to the output. At
      the turn of the twentieth century, a method was discovered that not only
      made finding the differential equation easy, but also simplified
      the solution process in the most common situation. Although not
      original with him, <link src="http://www.invent.org/hall_of_fame/139.html">Charles
      Steinmetz</link> presented the key paper describing the
      <term>impedance</term> approach in 1893. The impedance concept
      is very important, extending its reach far beyond circuits.
    </para>

  </content>
</document>
