Step 1: The torque \( \tau \) experienced by a magnetic dipole in a uniform magnetic field is given by:
\[
\tau = \vec {m} \times \vec{B}
\]
where \( \vec {m} \) is the magnetic moment and \( \vec {B} \) is the magnetic field.
Step 2: The cross product indicates that the torque is perpendicular to both \(\vec m \) and \( \vec B \), leading to rotational motion.