Consider an electric dipole of dipole moment \(\vec P\) placed in a uniform electric field \(\vec P\) making an angle Φ with \(\vec P\).The torque \(\vec{\tau}\) = \(\vec P\) x \(\vec E\) tends to rotate the dipole and align it with \(\vec E\).
If the dipole was initially parallel to \(\vec E\), its potential energy is minimum. We arbitrarily assign U0 = 0 to the minimum potential energy for this position. Then, at a position where \(\vec P\) makes an angle θ with \(\vec E\), the potential energy of the dipole is
Uθ = -pE cos θ = - \(\vec P\). \(\vec E\).
A current-carrying coil placed in a magnetic field \(\vec B\) experiences a torque,
\(\vec{\tau}\) \(\vec \mu\) x \(\vec B\)…………. (1)
where \(\vec \mu\) is the magnetic dipole moment of the coil. In analogy with an electric dipole, the potential energy of a magnetic dipole is
Uθ = – μB cos θ = – \(\vec \mu\). \(\vec B\) ……….. (2)
Uθ is also known as orientation energy. A magnetic dipole has its lowest energy ( = – μB cos 0 = – μB) when its dipole moment is lined up with the magnetic field, and has its highest energy ( = – μBcos 180° = + μB) when is directed opposite the field.
Orientations of highest and lowest energy of a magnetic dipole moment in an external magnetic field \(\vec B\)