The torque \( \boldsymbol{\tau} \) experienced by a magnetic dipole moment \( \mathbf{m} \) placed in a magnetic field \( \mathbf{B} \) is given by the vector cross product:
\[
\boldsymbol{\tau} = \mathbf{m} \times \mathbf{B}.
\]
This torque arises because the magnetic dipole tends to align itself with the external magnetic field. The magnitude of the torque is:
\[
|\boldsymbol{\tau}| = m B \sin \theta,
\]
where \( \theta \) is the angle between the magnetic moment \( \mathbf{m} \) and the magnetic field \( \mathbf{B} \).
The direction of the torque is perpendicular to the plane formed by \( \mathbf{m} \) and \( \mathbf{B} \), following the right-hand rule.
Physically, this torque causes the magnetic dipole to rotate, reducing the angle \( \theta \) until \( \mathbf{m} \) aligns parallel to \( \mathbf{B} \), minimizing the potential energy of the system.