An electric dipole consists of two small particles. Each has mass m but opposite electric charge ±q. They are separated by a light, non-conducting rod of length l. The dipole is placed in a uniform electric field E such that it forms an angle θ to the field, then is released. Its initial angular acceleration about its centre of mass is given by
a) ml2qEcosθ; b) ml2qEsinθ; c) mqElcosθ;
d) mqElsinθ; e) ml2qEsinθ.
[Figure: Electric dipole at angle θ to uniform electric field E]