1. Force on +q, F+ = +qE (along the direction of electric field)
Force on -q, F = -qE (Opposite to the direction of electronic field)
2. Net force on the system is zero.
3.

Consider an electric dipole of dipole moment P = 2aq kept in a uniform external electric field, inclined at an angle θ to the field direction. torque = any one force × perpendicular
distance τ = qE × 2 a sin θ
Since P = 2aq
τ = p E sin θ
Vectorialy
\(\overrightarrow \tau = \overrightarrow P \times \overrightarrow E\)
4. In nonuniform electric field, total force is not zero. Hence the dipole undergoes for both translational and rotational motion.