The electric potential at a point on the axis of an electric dipole depends on the distance $r$ of the point from the dipole as

  • A
    $ \propto \frac{1}{r} $
  • B
    $ \propto \frac{1}{r^2} $
  • C
    $ \propto r $
  • D
    $ \propto \frac{1}{r^3} $

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