An electric dipole is placed in a non-uniform electric field. Then the electric force on the dipole depends upon
orientation of the dipole moment of the dipole.
orientation of the dipole and the rate at which the field is changing in space.
dipole moment of the dipole and the rate at which the field is changing in space.
orientation of dipole, dipole moment and the rate at which the field is changing in space.
If px→, py→ and pz →are the components of dipole moment and Ex→ , Ey→ and Ez→ are the components of electric field , then
Fnet→=∇→p→.E→=px∂Ex∂xi^+py∂Ey∂yj^+pz∂Ez∂zk^