An electric dipole of moment $p$ is placed in the position of stable equilibrium in a uniform electric field of intensity $E$. It is rotated through an angle $\theta$ from the initial position. The potential energy of the electric dipole in the final position is

  • A
    $pE \cos \theta$
  • B
    $pE \sin \theta$
  • C
    $pE(1 - \cos \theta)$
  • D
    $-pE \cos \theta$

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