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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. |
`(g sin theta)/((1-MR^2)/I)` |
B. |
`(g sin theta)/((1+I)/(MR^2))` |
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C. |
`(g sin theta)/((1+MR^2)/I)` |
D. |
`(g sin theta)/((1-I)/(MR^2))` |