(a) Consider an electric dipole placed in a uniform electric field of strength E in such a way that its dipole moment vector p makes an angle q with the direction of vector E. The charges of dipole are - q and + q at separation 2l the dipole moment of electric dipole,
p = q.2l ...(1)
Force: The force on charge + q is, vector F1 = qvector vector E, along the direction of field vector E
The force on charge - q is, vector F2 = qE, opposite to the direction of field vector E
Obviously forces vector F and vector F are equal in magnitude but opposite in direction; hence net force on electric dipole in uniform electric field is
F = F1 - F2 = qE - qE = 0 (zero)
As net force on electric dipole is zero, so dipole does not undergo any translatory motion.
Torque: The forces vector F1 and vector F2 form a couple (or torque) which tends to rotate and align the dipole along the direction of electric field. This couple is called the torque and is denoted by τ.
∴ torque τ = magnitude of one force x perpendicular distance between lines of action of forces
= qE(BN) = qE(2lsinθ)
=(θ2l)Esinθ
= pEsinθ[using (1)] ....(2)
Clearly, the magnitude of torque depends on orientation (θ) of the electric dipole relative to electric field. Torque (τ) is a vector quantity whose direction is perpendicular to both vector p and vector E.
In vector form vector τ = vector p x vector E ...(3)
Thus, if an electric dipole is placed in an electric field in oblique orientation, it experiences no force but experiences a torque. The torque tends to align the dipole moment along the direction of electric field.
Maximum Torque: For maximum torque sinθ should be the maximum. As the maximum value of sinθ =1 when θ = 90°
∴ Maximum Torque,τmax = pE