The potential energy of a dipole in a uniform field is \( U = -p E \cos \theta \), where \( p \) is the
dipole moment, \( E \) is the field strength, and \( \theta \) is the angle between \( p \) and \( E \).
The energy is minimum when \( \cos \theta = 1 \), i.e., \( \theta = 0^\circ \), meaning the dipole aligns
with the field. At this position, the torque (\( \tau = p E \sin \theta \)) is zero, and the system is in
stable equilibrium, minimizing the potential energy.
The field exerts maximum torque
The dipole moment cancels the field
The field becomes non-uniform
The torque is zero at alignment