Suppose a body of mass $M$ and radius $R$ is allowed to roll on an inclined plane without slipping from its topmost point $A$. The acceleration of the body down the plane is given by (where $\beta = 1 + \frac{I}{MR^2}$):

  • A
    $g \sin \theta$
  • B
    $g$
  • C
    $\beta g \sin \theta$
  • D
    $\frac{g \sin \theta}{\beta}$

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