A parallel plate capacitor has plates with area $A$ and separation $d$. A battery charges the plates to a potential difference $V_0$. The battery is then disconnected and a dielectric slab of thickness $d$ is introduced. The ratio of energy stored in the capacitor before and after slab is introduced, is

  • A

    $K$

  • B

    $\frac{1}{K}$

  • C

    $\frac{A}{{{d^2}K}}$

  • D

    $\frac{{{d^2}K}}{A}$

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