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Update lecture-09.html
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jcponce committed Aug 2, 2023
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Expand Up @@ -133,11 +133,77 @@ <h4>1 Ordinary Differential Equations</h4>
<p><strong>1.6.2 Worked-out example: RL circuit</strong></p>
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<p>
<span>The voltage drop due to the inductor is $\ds L\dif{J}{t}$ where $L$ is
the inductance (in Henries).
</span>
</p>
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<p>
<span>According to <span id="rr">Kirchhoff's Law</span> the sum of the voltage drops is equal
to the supplied voltage $E(t)$ (in Volts).
</span>
<span class="fragment" data-fragment-index="0">
Hence
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<p>
<span class="fragment" data-fragment-index="0">
$\ds L\dif{J}{t}+RJ=E(t). \qquad (*)$
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</p>
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<img style="width: 30%;" src="images/lect-09/circuit.png">
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<br/><br/><br/>
</section>

</section>

<section>

<section data-auto-animate>
<h4>1 Ordinary Differential Equations</h4>
<div id="sbt">
<p><strong>1.6.2 Worked-out example: RL circuit</strong></p>
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<p>
<span>
<strong>
Example:
</strong>
Suppose in an RL circuit a battery supplies a
constant voltage of 80V, the inductance is 2H and the resistance is
$10\Omega$.
(i) Find an expression for $J(t),$ and (ii)
determine the the current after 1 second if $J(0)=0.$
</span>
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Expand All @@ -157,6 +223,8 @@ <h4>1 Ordinary Differential Equations</h4>
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<br/><br/><br/>
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