A stationary horizontal disc is free to rotate
about its axis. When a torque is applied on it,
its kinetic energy as a function of $\theta $, where $\theta $
is the angle by which it has rotated, is given as
k$\theta $2. If its moment of inertia is I then the
angular acceleration of the disc is :
${k \over {4I}}\theta $
${k \over {I}}\theta $
${k \over {2I}}\theta $
${2k \over {I}}\theta $
Solution
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