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

  • 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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