A ring of mass m and radius r is allowed to roll down without slipping on an inclined plane having inclination sin−1(110) from the horizontal. The magnitude of acceleration of it's centre of mass is
A
9.8ms−2
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B
4.9ms−2
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C
0.98ms−2
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D
0.49ms−2
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Solution
The correct option is D0.49ms−2 Magnitude of linear acceleration of centre of mass of a body rolling down an inclined plane is given by a, where a=aCM:
⇒a=gsinθ1+K2r2=gsinθ1+Imr2 K= Radius of gyration ⇒a=gsinθ(1+1) ∵I=mr2 for ring, about an axis passing through it's COM ∴a=(9.8×110)(1+1)ms−2=0.49ms−2