Two parallel disks each having radius $R$ are separated by a distance $l$. The surface charge densities are $\sigma$ and $-\sigma$. The electric field at point $P$,a large distance $r$ along the axis of the disks is:

  • A
    $\frac{{\sigma {R^2}l}}{{{\varepsilon _0}{r^3}}}$
  • B
    $\frac{{2\sigma {R^2}l}}{{{\varepsilon _0}{r^3}}}$
  • C
    $\frac{{\sigma {R^2}l}}{{4{\varepsilon _0}{r^3}}}$
  • D
    $\frac{{\sigma {R^2}l}}{{2{\varepsilon _0}{r^3}}}$

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