An electric dipole having charges `+q` and `-q` at a separation r. At distance `d gt gt r` along the axis of the dipole , the field is proportional to

A point Q lies on the perpendicular bisector of an electrical dipole of dipole moment p, If the distance of Q from the dipole is r (much larger than the size of the dipole), then electric field at Q is proportional to

A point Q lies on the perpendicular bisector of an electrical dipole of dipole moment p , If the distance of Q from the dipole is r (much larger than the size of the dipole), then electric field at Q is proportional to

A point Q lies on the perpendicular bisector of an electrical dipole of dipole moment p , If the distance of Q from the dipole is r (much larger than the size of the dipole), then electric field at Q is proportional to

An electric dipole vec(P) and a point charge q (gt 0) are located at a separation r as shown. Force on the dipole vec((F)) due to the point charge on the qualitatively dinoted as :

Two equal charges q of opposite sign separated by a distance 2a constitute an electric dipole of dipole moment p . If P is a point at a distance r from the centre of the dipole and the line joining the centre of the dipole to this point makes an angle theta with the axis of the dipole, then then potential at P is given by (r gt gt 2a) where (p = 2 qa)