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 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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