A hemisphere of radius r and of mass 4m is free to slide with its base on a smooth horizontal table. A particle of mass m is placed on the top of the hemisphere. The angular velocity of the particle relative to hemisphere at an angular displacement , when velocity of hemisphere has become v is
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Let the hemisphere be moved by a distance of x through angle θ. CM remains same as there are no forces acting horizontally
m(Rsinθ−x)=Mx
mRsinθ=(M=m)x
Differentiating,
mRωcosθ=(M+m)v
wherev=xandω=θ.
wkt,M=4m
ω=
Rcosθ
5v
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