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Q. A thin non-conducting disc of radius $R$ is rotating clockwise (see figure) with an angular velocity $\omega$ about its central axis, which is perpendicular to its plane. Both its surfaces carry +ve charges of uniform surface density. Half the disc is in a region of a uniform, unidirectional magnetic field $B$ parallel to the plane of the disc, as shown. Then,Physics Question Image

Moving Charges and Magnetism

Solution:

$\vec{\tau}=\vec{M} \times \vec{B}=\frac{I A}{2}(-\hat{k}) \times B(-\hat{j})=\frac{I A B}{2}(-\hat{i})$ (leftward)