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

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