$A$ spherical object of mass $M$ and radius $R$ has a moment of inertia $I$ about its axis. If this object rolls down an inclined plane of angle $\theta$ without slipping,its acceleration is given by:

  • A
    $\frac{g \sin \theta}{1 - \frac{M R^2}{I}}$
  • B
    $\frac{g \sin \theta}{1 + \frac{I}{M R^2}}$
  • C
    $\frac{g \sin \theta}{1 + \frac{M R^2}{I}}$
  • D
    $\frac{g \sin \theta}{1 - \frac{I}{M R^2}}$

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