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<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/">Solving Circuits with Impedances</name>

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      <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>
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      <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>
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    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">circuit</md:keyword>
    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">impedance</md:keyword>
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  <md:abstract xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Introducing the advantages of using impedance and how to use it.</md:abstract>
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<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"> As we unfold the impedance story, we'll see that the
powerful use of impedances suggested by <link xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" src="http://www.invent.org/hall_of_fame/139.html">Steinmetz</link>
greatly simplifies solving circuits, alleviates us from solving
differential equations, and suggests a general way of thinking about
circuits. Because of the importance of this approach, let's go over
how it works.  </para>


<list 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="enumerated" id="list1"> <item xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/"> Even though it's not,
      pretend the source is a complex exponential. We do this because
      the impedance approach simplifies finding how input and output
      are related. If it were a voltage source having voltage
      <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:ci type="fn">p</m:ci>
	      <m:ci>t</m:ci>
	    </m:apply>
	</m:apply>
      </m:math>
     (a pulse), still let   
      <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:times/>
	      <m:ci>
		<m:msub>
		  <m:mi>V</m:mi>
		  <m:mi>in</m:mi>
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		<m:apply>
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		  <m:imaginaryi/>
		  <m:cn>2</m:cn>
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		  <m:ci>f</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:apply>
	</m:math>.
     We'll learn how to "get the pulse back" later.
     </item>
      <item xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/"> With a source equaling a complex exponential,
     <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/">all </emphasis>variables in a linear circuit will also
     be complex exponentials having the <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/">same
     </emphasis>frequency. The circuit's only remaining "mystery" is
     what each variable's complex amplitude might be. To find these,
     we consider the source to be a complex number (
      <m:math>
	 <m:ci>
	  <m:msub>
	    <m:mi>V</m:mi>
	    <m:mi>in</m:mi>
	  </m:msub>
	</m:ci>
      </m:math> here) and the elements to be impedances.
     </item>
      <item xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/"> We can now solve using series and parallel combination
     rules how the complex amplitude of any variable relates to the
     sources complex amplitude.</item>
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<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"> A common error in using impedances is to keep the
time-dependent part, the complex exponential, in the fray. The entire
point of using impedances is to get rid of them <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/">in writing
circuit equations and in the subsequent algebra</emphasis>. The
complex exponentials are there <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/">implicitly
</emphasis>(they're behind the scenes). Only after we find the result
do we raise the curtain and put things back to together again. In
short, <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/">when solving circuits using impedances, </emphasis>
    <m:math>
      <m:ci>t</m:ci>
    </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/">should not appear except for the beginning and end</emphasis>.
</para>
 

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