<?xml version="1.0" encoding="utf-8" standalone="no"?>
<!DOCTYPE document PUBLIC "-//CNX//DTD CNXML 0.5 plus MathML//EN" "http://cnx.rice.edu/cnxml/0.5/DTD/cnxml_mathml.dtd">
<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="m0025">

  <name xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Impedance</name>

  <metadata xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
  <md:version xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">2.6</md:version>
  <md:created xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">2000/07/07</md:created>
  <md:revised xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">2004/08/10 08:09:52.758 GMT-5</md:revised>
  <md:authorlist xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
      <md:author xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="dhj">
      <md:firstname xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Don</md:firstname>
      
      <md:surname xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Johnson</md:surname>
      <md:email xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">dhj@rice.edu</md:email>
    </md:author>
  </md:authorlist>

  <md:maintainerlist xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
    <md:maintainer xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="liqun">
      <md:firstname xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Liqun</md:firstname>
      
      <md:surname xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Wang</md:surname>
      <md:email xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">liqun@rice.edu</md:email>
    </md:maintainer>
    <md:maintainer xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="dhj">
      <md:firstname xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Don</md:firstname>
      
      <md:surname xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Johnson</md:surname>
      <md:email xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">dhj@rice.edu</md:email>
    </md:maintainer>
  </md:maintainerlist>
  
  <md:keywordlist xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">impedance</md:keyword>
  </md:keywordlist>

  <md:abstract xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Introducing what is the impedance, and why and where to use it.</md:abstract>
</metadata>
  <content xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">


    
    <para xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="para1"> 
      <emphasis xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">The major consequence of assuming complex exponential
	voltage and currents is that the ratio </emphasis> 
      <m:math>
	<m:apply>
	  <m:eq/>
	  <m:ci>Z</m:ci>
	  <m:apply>
	    <m:divide/>
	    <m:ci>V</m:ci>
	    <m:ci>I</m:ci>
	  </m:apply>
	</m:apply>
      </m:math>
      <emphasis xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">for each element does not depend on time</emphasis>. This
      quantity is known as the element's <term xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">impedance</term>.
    </para>


    <figure xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="basicelements">
      <name xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/"/>      
      <subfigure xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
	<media xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" type="image/png" src="resistor.png"/>
	<caption xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Resistor:  
	  <m:math>
	    <m:apply>
	      <m:eq/>
	      <m:ci>
		<m:msub>
		  <m:mi>Z</m:mi>
		  <m:mi>R</m:mi>
		</m:msub>
	      </m:ci>
	      <m:ci>R</m:ci>
	    </m:apply>
	  </m:math> 
	</caption>
      </subfigure>
      <subfigure xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
	<media xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" type="image/png" src="capacitor.png"/>
	<caption xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
	  Capacitor:  
	  <m:math>
	    <m:apply>
	      <m:eq/>
	      <m:ci>
		<m:msub>
		  <m:mi>Z</m:mi>
		  <m:mi>C</m:mi>
		</m:msub>
	      </m:ci>
	      <m:apply>
		<m:divide/>
		<m:cn>1</m:cn>
		<m:apply>
		  <m:times/>
		  <m:imaginaryi/>
		  <m:cn>2</m:cn>
		  <m:pi/>
		  <m:ci>f</m:ci>
		  <m:ci>C</m:ci>
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:math>
	</caption>
      </subfigure>
      <subfigure xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
	<media xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" type="image/png" src="inductor.png"/>
	<caption xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
	  Inductor:  
	  <m:math>
	    <m:apply>
	      <m:eq/>
	      <m:ci>
		<m:msub>
		  <m:mi>Z</m:mi>
		  <m:mi>L</m:mi>
		</m:msub>
	      </m:ci>
	      <m:apply>
		<m:times/>
		<m:imaginaryi/>
		<m:cn>2</m:cn>
		<m:pi/>
		<m:ci>f</m:ci>
		<m:ci>L</m:ci>
	      </m:apply>
	    </m:apply>
	  </m:math>
	</caption>
      </subfigure> 
    </figure>


    <para xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="para2">
      The impedance is, in general, a complex-valued,
      frequency-dependent quantity. For example, the magnitude of the
      capacitor's impedance is inversely related to frequency, and has
      a phase of
      <m:math>
	<m:apply>
	  <m:minus/>
	  <m:apply>
	    <m:divide/>
	    <m:pi/>
	    <m:cn>2</m:cn>
	  </m:apply>
	</m:apply>
      </m:math>.  This observation means that if the current is a
      complex exponential and has constant amplitude, the amplitude of
      the voltage decreases with frequency.  </para>

    
    <para xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="para3"> Let's consider Kirchoff's circuit laws. When
      voltages around a loop are all complex exponentials of the same
      frequency, we have
      <equation xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="eq1">
	<m:math>
	  <m:apply>
	    <m:eq/>
	    <m:apply>
	      <m:sum/>
	      <m:bvar>
		<m:ci>n</m:ci>
	      </m:bvar>
	      <m:domainofapplication>
		<m:ci>n</m:ci>
	      </m:domainofapplication>
	      <m:apply>
		<m:ci>
		  <m:msub>
		    <m:mi>v</m:mi>
		    <m:mi>n</m:mi>
		  </m:msub>
		</m:ci>
	      </m:apply>
	    </m:apply>
	    <m:apply>
	      <m:sum/>
	      <m:bvar>
		<m:ci>n</m:ci>
	      </m:bvar>
	      <m:domainofapplication>
		<m:ci>n</m:ci>
	      </m:domainofapplication>
	      <m:apply>
		<m:times/>
		<m:ci>
		  <m:msub>
		    <m:mi>V</m:mi>
		    <m:mi>n</m:mi>
		  </m:msub>
		</m:ci>
		<m:apply>
		  <m:exp/>
		  <m:apply>
		    <m:times/>
		    <m:imaginaryi/>
		    <m:cn>2</m:cn>
		    <m:pi/>
		    <m:ci>f</m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:apply>
	    <m:cn>0</m:cn>
	  </m:apply>
	</m:math>
      </equation>
      which means
      <equation xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="eq2">
	<m:math>
	  <m:apply>
	    <m:eq/>
	    <m:apply>
	      <m:sum/>
	      <m:bvar>
		<m:ci>n</m:ci>
	      </m:bvar>
	      <m:domainofapplication>
		<m:ci>n</m:ci>
	      </m:domainofapplication>
	      <m:apply>
		<m:ci>
		  <m:msub>
		    <m:mi>v</m:mi>
		    <m:mi>n</m:mi>
		  </m:msub>
		</m:ci>
	      </m:apply>
	    </m:apply>
	    <m:cn>0</m:cn>
	  </m:apply>
	</m:math>
      </equation>

      <emphasis xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">the complex amplitudes of the voltages obey
      KVL</emphasis>. We can easily imagine that the complex
      amplitudes of the currents obey KCL.  </para>


    <para xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="para4"> What we have discovered is that source(s)
      equaling a complex exponential of the same frequency forces all
      circuit variables to be complex exponentials of the same
      frequency. Consequently, the ratio of voltage to current for
      each element equals the ratio of their complex amplitudes, which
      depends only on the source's frequency and element values. This
      situation occurs because the circuit elements are linear and
      time-invariant. For example, suppose we had a circuit element
      where the voltage equaled the square of the current:
      <m:math>
	<m:apply>
	  <m:eq/>
	  <m:apply>
	    <m:ci type="fn">v</m:ci>
	    <m:ci>t</m:ci>
	  </m:apply>
	  <m:apply>
	    <m:times/>
	    <m:ci>K</m:ci>
	    <m:apply>
	      <m:power/>
	      <m:apply>
		<m:ci type="fn">i</m:ci>
		<m:ci>t</m:ci>
	      </m:apply>
	      <m:cn>2</m:cn>
	    </m:apply>
	  </m:apply>
	</m:apply>
      </m:math>. If  
      <m:math>
	<m:apply>
	  <m:eq/>
	  <m:apply>
	    <m:ci type="fn">i</m:ci>
	    <m:ci>t</m:ci>
	  </m:apply>
	  <m:apply>
	    <m:times/>
	    <m:ci>I</m:ci>
	    <m:apply>
	      <m:exp/>
	      <m:apply>
		<m:times/>
		<m:imaginaryi/>
		<m:cn>2</m:cn>
		<m:pi/>
		<m:ci>f</m:ci>
		<m:ci>t</m:ci>
	      </m:apply>
	    </m:apply>
	  </m:apply>
	</m:apply>
      </m:math>,
      <m:math>
	<m:apply>
	  <m:eq/>
	  <m:apply>
	    <m:ci type="fn">v</m:ci>
	    <m:ci>t</m:ci>
	  </m:apply>
	  <m:apply>
	    <m:times/>
	    <m:ci>K</m:ci>
	    <m:apply>
	      <m:power/>
	      <m:ci>I</m:ci>
	      <m:cn>2</m:cn>
	    </m:apply>
	    <m:apply>
	      <m:exp/>
	      <m:apply>
		<m:times/>
		<m:imaginaryi/>
		<m:cn>2</m:cn>
		<m:pi/>
		<m:cn>2</m:cn>
		<m:ci>f</m:ci>
		<m:ci>t</m:ci>
	      </m:apply>
	    </m:apply>
	  </m:apply>
	</m:apply>
      </m:math>, meaning that voltage and current no longer had the
      same frequency and that their ratio was time-dependent.
    </para>


    <para xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="para5">
      Because  for  linear  circuit  elements  the  complex  amplitude  of
      voltage is proportional to the complex amplitude of current—
      <m:math>
	<m:apply>
	  <m:eq/>
	  <m:ci>V</m:ci>
	  <m:apply>
	    <m:times/>
	    <m:ci>Z</m:ci>
	    <m:ci>I</m:ci>
	  </m:apply>
	</m:apply>
      </m:math> —circuit
      elements behave as if they were resistors, where instead of
      resistance, we use impedance. Because complex amplitudes for
      voltage and current also obey Kirchoff's laws, we can solve
      circuits using voltage and current divider and the series and
      parallel combination rules by considering the elements to be
      impedances.
    </para>


  </content>
</document>
