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A round uniform body of radius \( R \), mass \( M \), and moment of inertia \( I \) rolls down (without slipping) in an inclined plane making an angle \( \theta \) with the horizontal. Then, its acceleration is
(A) \( \frac{g \sin \theta}{1+\left(I / M R^{2}\right)} \)
(B) \( \frac{g \sin \theta}{1+\left(M R^{2} / I\right)} \)
(C) \( \frac{g \sin \theta}{1-\left(I / M R^{2}\right)} \)
(D) \( \frac{g \sin \theta}{1-\left(M R^{2} / I\right)} \)
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