Work Done to Rotate the Dipole in an Electric Field
1: Work Done Formula
The work done \( W \) to rotate an electric dipole from an initial angle \( \theta_1 \) to a final angle \( \theta_2 \) in a uniform electric field is given by:
\[
W = -\int_{\theta_1}^{\theta_2} \vec{\tau} \cdot d\vec{\theta}
\]
where:
- \( \vec{\tau} = pE \sin\theta \) is the torque on the dipole,
- \( p \) is the dipole moment,
- \( E \) is the electric field.
2: Work Done to Rotate from Stable to Unstable Equilibrium
For stable equilibrium: \( \theta_1 = 0^\circ \) (where \( \cos \theta = 1 \)),
For unstable equilibrium: \( \theta_2 = 180^\circ \) (where \( \cos \theta = -1 \)).
Thus, the work done to rotate the dipole is:
\[
W = -\int_{0}^{180^\circ} pE \cos\theta \, d\theta = 2pE
\]
Thus, the correct answer is:
\[
\boxed{(A) \, 2pE}
\]