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Q. A magnet of dipole moment $m$ is aligned in equilibrium position in a magnetic field of intensity $B$. The work done to rotate it through an angle $\theta$ in the magnetic field is

Magnetism and Matter

Solution:

Work done $W=\int\limits_{0}^{\theta} m B \sin \theta d \theta=m B(1-\cos \theta)$
$(\text { as } \Delta W=\tau d \theta=m B \sin \theta d \theta)$