NOTE: We could either:

It is easier in this example to do the second method. In many examples, it is easier to do the first method.

For the first loop, we have:


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For the second loop, we have:


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Substituting (2) into (1) gives:


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Next we take the Laplace Transform of both sides.

Note:

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In this example, $q_{0}=0$. So MATH


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Now taking Inverse Laplace:

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And using result (2) from above, we have:

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For charge on the capacitor, we first need voltage across the capacitor:

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So, since $V_{C}=\dfrac{q}{C}$, we have:

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Graph of q(t):


10_lap_app3_18pt__19.png