A uniform disc of mass $\mathrm{M}$ and radius $\mathrm{R}$ rolls without slipping down a plane inclined at an angle $\theta$ with the horizontal.
The magnitude of torque acting on the disc is
$\{\mathrm{A}\} \mathrm{MgR}$
$\{\mathrm{B}\} \mathrm{MgR} \sin \theta$
$\{\mathrm{C}\}[(2 \mathrm{MgR} \sin \theta) / 3]$
$\{\mathrm{D}\}[(\mathrm{MgR} \sin \theta) / 3]$