Question on the work done while charging up a capacitor.

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SUMMARY

The work done while charging a capacitor is accurately represented by the equation dW=(V+dV)dQ, where V is the voltage across the capacitor and dQ is the infinitesimal charge added. This equation accounts for the change in voltage dV as the charge is transferred, which is crucial since the voltage is not constant during the charging process. The misconception arises from applying the equation V=W/Q without recognizing that it only holds when voltage is constant, which is not the case for a charging capacitor.

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So the work done when charging up a capacitor is ##dW=VdQ##
However, when we add a charge ##dQ## to the capacitor, ##V## also changes accordingly, so I was wondering why the work done wasn't written as ##dW=VdQ+QdV## (one that also takes into account t he change in ##V##).

Thanks in advance.
 
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I think the correct equation for dW is ##dW=(V+dV)dQ=VdQ+dVdQ##. This is because the voltage changes to V+dV but remains constant and equal to V+dV as the charge dQ moves from one plate of the capacitor to the other.

But when we do a single (not double) integration on dVdQ the result is 0. That is ##\int dVdQ=0## I can expand for this if you want.

EDIT: Why the equation you wrote is not correct for the case of a charging capacitor:

It all starts from the equation ##V=W/Q##. If this equation was correct in all cases then we could simply handle it as follows ##W=VQ## and differentiating using the product rule of differentiation (and omitting the denominators ##dt##) we ll end up with ##dW=VdQ+QdV##. So at first place it seems that the equation you wrote is correct.

However the mistake lies at our starting point: The equation ##V=W/Q## does not hold for the case of a charging capacitor. This equation is true only if the voltage V is constant and independent of time t or the charge Q (as to why this is true we ll have to go back to electrostatics and studying the motion of a charged point particle which moves between two points of an electrostatic field that have potential difference V). In the case of a charging capacitor V is not constant in time and it depends on the charge Q in the capacitor plates, so this equation does not hold.

It holds though if we apply it for an infinitesimal time interval ##(t,t+dt)## for which we consider the voltage constant and equal to ##V## (or ##V+dV## as I wrote above). Then the infinitesimal work ##dW## for this infinitesimal time interval ##dt## during which the charge dQ moves from one plate of the capacitor to the other, is ##dW=(V+dV)dQ##. And from here we go back at the start of my message...
 
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