Each of two large conducting parallel plates has one sided surface area $A$. If one of the plates is given a charge $Q$ whereas the other is neutral, then the electric field at a point in between the plates is given by

  • A

    $\frac{Q}{A \varepsilon_0}$

  • B

    $\frac{Q}{2 A \varepsilon_0}$

  • C

    $\frac{Q}{4 A \varepsilon_0}$

  • D

    Zero

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