A solid cylinder of mass M and radius R rolls down an inclined plane of height h without slipping. The speed of its centre when it reaches the bottom is.
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Work-energy theorem, Mgh=21Mv2+21Iw2
For solid cylinder, I=21MR2
Also v=Rw (due to pure rolling)
Thus Mgh=21Mv2+21×21MR2w2
$$\implies v= \sqrt{\dfrac{4}{3}gh}$$
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