An electric dipole is composed of two electric charges with opposite signs brought very close together. An ideal electric dipole is one in which the two charges are only infinitesimally separated. Equations defined particularly for electric dipoles are defined in terms of the electric dipole moment
The electric dipole moment for two charges and separated by a displacement vector is
If an electric dipole is placed in an external electric field the charges will feel forces in opposite directions by virtue of their opposite signs, causing a rotation if the two charges remain bound to one another. Hence, the forces actually manifest themselves as a torque.
Since the torque is largest when is perpendicular to and decreases as the two vectors become more parallel, it is best modeled as the cross product between the two vectors.
The torque on a dipole placed in an external field is
Two charges and are placed at and respectively in an external field What is the torque on the dipole?
In order to evaluate the cross product, write down the dipole.
Now evaluate the cross product.
The dipole wants to rotate until its moment points in the same direction as the external electric field. This orientation thus represents the potential minimum, and the potential energy increases as the angle between the dipole moment and the external field increases.
How much work is required to flip an electric dipole from its potential minimum to an orientation antiparallel to the external field?
Recall that work is defined in terms of potential energy according to the work-energy theorem.
- Geek3, . VFPt dipole animation electric. Retrieved June 8, 2016, from https://commons.wikimedia.org/wiki/File:VFPt_dipole_animation_electric.gif