A condenser of capacity \( C \) is charged to a potential difference of \( V_{1} \). The plates ...

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A condenser of capacity \( C \) is charged to a potential difference of \( V_{1} \). The plates of the condenser are then connected to an ideal inductor of inductance \( L \). The current through the inductor when the potential difference across the condenser reduces to \( V_{2} \) is
a) \( \left(\frac{C\left(V_{1}-V_{2}\right)^{2}}{L}\right)^{\frac{1}{2}} \)
(b) \( \frac{C\left(V_{1}^{2}-V_{2}^{2}\right)}{L} \)
(c) \( \frac{C\left(V_{1}^{2}+V_{2}^{2}\right)}{L} \)
(d) \( \left(\frac{C\left(V_{1}^{2}-V_{2}^{2}\right)}{L}\right)^{\frac{1}{2}} \)
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