To determine the energy required to rotate an electric dipole in a uniform electric field, we need to understand the concept of potential energy for an electric dipole. The potential energy \( U \) of a dipole with dipole moment \( \mathbf{p} \) that makes an angle \( \theta \) with a uniform electric field \( \mathbf{E} \) is given by the formula:
U = -\mathbf{p} \cdot \mathbf{E} = -pE \cos \theta
Initially, the dipole is aligned parallel to the electric field, which means the angle \( \theta \) is \( 0^\circ \). Therefore, the initial potential energy \( U_i \) is:
U_i = -pE \cos 0^\circ = -pE
When the dipole is rotated by \( 90^\circ \), the angle \( \theta \) becomes \( 90^\circ \). The potential energy \( U_f \) at this position is:
U_f = -pE \cos 90^\circ = 0
The work done or the energy required to rotate the dipole from its initial position to the final position is the change in potential energy, given by:
\Delta U = U_f - U_i = 0 - (-pE) = pE
Thus, the energy required to rotate the dipole by \( 90^\circ \) is pE, which matches the correct answer.
Hence, the correct answer is:
pE