$A$ spherical uniform body of radius $R$,mass $M$,and moment of inertia $I$ rolls down (without slipping) on an inclined plane making an angle $\theta$ with the horizontal. Then its acceleration is

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

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