$A$ dipole having dipole moment $p$ is placed in front of a solid uncharged conducting sphere as shown in the diagram. The net potential at point $A$ lying on the surface of the sphere is:

  • A
    $\frac{kp \cos \phi}{r^2}$
  • B
    $\frac{kp \cos^2 \phi}{r^2}$
  • C
    zero
  • D
    $\frac{2kp \cos^2 \phi}{r^2}$

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