A bar magnet is initially at right angles to a uniform magnetic field. The magnet is rotated till the torque acting on it becomes one-half of its initial value. The angle through which the bar magnet is rotated is:
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Torque on a magnetic dipole in a magnetic field is maximum when it’s perpendicular to the field. If torque becomes half, solve \( \sin \theta = \frac{1}{2} \).
The torque \( \tau \) on a magnetic dipole in a magnetic field is given by:
\[
\tau = MB \sin\theta
\]
where:
- \( M \) is magnetic moment
- \( B \) is magnetic field
- \( \theta \) is the angle between \( \vec{M} \) and \( \vec{B} \)
Initially, \( \theta = 90^\circ \Rightarrow \tau_0 = MB \sin 90^\circ = MB \)
We are told:
\[
\tau = \frac{1}{2} \tau_0 = \frac{1}{2} MB
\]
Then:
\[
MB \sin \theta = \frac{1}{2} MB \Rightarrow \sin \theta = \frac{1}{2}
\Rightarrow \theta = 30^\circ
\]
So, the magnet is rotated from \( 90^\circ \) to \( 60^\circ \), hence angle rotated is:
\[
90^\circ - 30^\circ = 60^\circ
\]
Final answer: \( 60^\circ \)