$A$ disc is given an angular velocity $\omega_0$ as shown in the figure and is kept on an inclined plane of inclination $\theta$ having a coefficient of friction $\mu = \tan \theta$. If the initial acceleration of the centre of mass is $a$ and the angular acceleration is $\alpha$,then:

  • A
    $\alpha R = a$
  • B
    $2\alpha R = a$
  • C
    $\alpha R = g \sin \theta$
  • D
    $\alpha R = 2 g \sin \theta$

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