(I) Let an electric dipole be placed in a uniform electric field →E, making an angle θ with the field. Force on charge +q →F+q = +q →E (along →E). Force on charge −q →F−q = −q →E (opposite to →E). As two equal and opposite forces are acting on the dipole, therefore net force →F = 0.
(ii) We know that work done in rotating an electric dipole from θ1 to θ2 (where θ1 is the angle of the dipole with the electric field) is given by, W = pE(cosθ1 − cosθ2). Now given θ1 = 0, θ2 = 180°. Therefore, W = pE(cos0 − cos180) = 2pE