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  <resource>
  <id>6677</id>
  <path>/www/nrich/html/content/id/6677/</path>
  <resourceTypeID>1</resourceTypeID>
  <last_published>2011-02-01T00:00:01</last_published>
  <indexXML>&lt;?xml version=&quot;1.0&quot; encoding=&quot;UTF-8&quot;?&gt;
&lt;mdoxml version=&quot;1.0&quot;&gt;&lt;br&gt;&lt;/br&gt;
&lt;ul id=&quot;stemLinks&quot;&gt;
&lt;li&gt;&lt;a href=&quot;http://nrich.maths.org/8690&quot;&gt;Warm-up&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;&lt;a href=&quot;http://nrich.maths.org/6669&quot;&gt;Try this next&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;&lt;a href=&quot;http://nrich.maths.org/6667&quot;&gt;Think higher&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;&lt;a href=&quot;http://nrich.maths.org/6661&quot;&gt;Read: mathematics&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;&lt;a href=&quot;http://en.wikipedia.org/wiki/Inductors&quot;&gt;Read: science&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;&lt;a href=&quot;http://en.wikipedia.org/wiki/Impedance_matching&quot;&gt;Explore further&lt;/a&gt;&lt;/li&gt;
&lt;/ul&gt;
&lt;div&gt; &lt;/div&gt;
&lt;br&gt;&lt;/br&gt;
&lt;p&gt;An AC generator of rms voltage E is connected in series with two reactive impedances,&lt;br&gt;&lt;/br&gt;
$Z_1$ and $Z_2$, as shown below:&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\theta$ is the argument of $Z_1$ and $\phi$ is the argument of $Z_2$.&lt;br&gt;&lt;/br&gt;
&lt;mdo:image alt=&quot;&quot; height=&quot;242&quot; src=&quot;Problem4.jpg&quot; width=&quot;382&quot;&gt;&lt;/mdo:image&gt;&lt;br&gt;&lt;/br&gt;
Find the power dissipated in $Z_2$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
If the phase of $Z_2$ ($\phi$) is fixed whilst allowing the magnitude to vary, find the relationship between $Z_1$ and $Z_2$ when we achieve maximum power transfer to $Z_2$.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
 &lt;/p&gt;&lt;/mdoxml&gt;</indexXML>
  <solutionXML>&lt;?xml version=&quot;1.0&quot; encoding=&quot;UTF-8&quot;?&gt;
&lt;mdoxml version=&quot;1.0&quot;&gt;&lt;br&gt;&lt;/br&gt;
Part 1:&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
 $P = IV$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
I = $\frac{E}{Z_1 + Z_2} = \frac{E}{Z_1cos\theta + Z_2cos\phi +
i(Z_1sin\theta + Z_2sin\phi)}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
|I| = $\frac{E}{\sqrt{(Z_1cos\theta + Z_2cos\phi)^2 + (Z_1sin\theta
+ Z_2sin\phi)^2}}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
The real power transferred to $Z_2$: P = I^2 R&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
P = $ I^2 Z_2cos \phi = \frac{E^2 Z_2cos \phi}{Z_1^2 + Z_2^2 +
2Z_1Z_2(cos \theta cos \phi + sin \theta \phi)}$= $ \frac{E^2
Z_2cos \phi}{Z_1^2 + Z_2^2 + 2Z_1Z_2cos( \theta - \phi )} $&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
Part 2:&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
To find the maximum power; we can differentiate the power
expression with respect to $Z_2$ and set the derivative equal to
zero.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\frac{dP}{dZ_2} = \frac{d}{dZ_2}\frac{E^2 Z_2cos \phi}{Z_1^2 +
Z_2^2 + 2Z_1Z_2cos( \theta - \phi )}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
Let U = $E^2 Z_2cos \phi$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
Let V = $ Z_1^2 + Z_2^2 + 2Z_1Z_2cos( \theta - \phi ) $&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$\frac{dP}{dZ_2} = \frac{VU' - UV'}{V^2}$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
V' = $ 2Z_2 + 2Z_1 cos ( \theta - \phi)$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
U' = $E^2 cos \phi$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
Substituting thses values into the expression and setting it equal
to zero we find that:&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
$Z_1 = Z_2$&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
For maximum power transfer between load and source we must
therefore match the internal impedance of the load with the
impedance of the source&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;&lt;/mdoxml&gt;</solutionXML>
  <noteXML/>
  <clueXML>&lt;?xml version=&quot;1.0&quot; encoding=&quot;UTF-8&quot;?&gt;
&lt;mdoxml version=&quot;1.0&quot;&gt;&lt;br&gt;&lt;/br&gt;
This problem makes use of the concepts of AC generators and RMS
(root-mean-square) voltage.You will also need to be familiar with
complex numbers in order to attempt this problem.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;
You  may  wish to read our articles on &lt;a href=&quot;http://nrich.maths.org/6661&amp;amp;part=&quot;&gt;AC/DC circuits&lt;/a&gt; for
the background physics and mathematics required.&lt;br&gt;&lt;/br&gt;
&lt;br&gt;&lt;/br&gt;&lt;/mdoxml&gt;</clueXML>
  <canonXML/>
  <end_user_role>2</end_user_role>
  <difficulty>5</difficulty>
  <keystage1>0</keystage1>
  <keystage2>0</keystage2>
  <keystage3>0</keystage3>
  <keystage4>0</keystage4>
  <keystage4plus>1</keystage4plus>
  <title>Impedance can be complex!</title>
  <description>Put your complex numbers and calculus to the test with this
impedance calculation.</description>
  <spec_group>Applications
    <specifier>engineering</specifier>
  </spec_group>
  <spec_group>Pre-Calculus and Calculus
    <specifier>Differentiation</specifier>
  </spec_group>
  <spec_group>Pre-Calculus and Calculus
    <specifier>Complex analysis</specifier>
  </spec_group>
  <spec_group>Advanced Algebra
    <specifier>Complex numbers</specifier>
  </spec_group>
  <spec_group>Applications
    <specifier>engineering</specifier>
  </spec_group>
  <spec_group>Admin
    <specifier>Individual</specifier>
  </spec_group>
</resource>