$A$ capacitor of capacity $C$ is charged to a potential difference of $V_1$. The plates of the capacitor are then connected to an ideal inductor of inductance $L$. The current through the inductor when the potential difference across the capacitor reduces to $V_2$ is

  • A
    $[\frac{C(V_1 - V_2)^2}{L}]^{1/2}$
  • B
    $\frac{C(V_1^2 - V_2^2)}{L}$
  • C
    $\frac{C(V_1^2 + V_2^2)}{L}$
  • D
    $[\frac{C(V_1^2 - V_2^2)}{L}]^{1/2}$

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