Foundation
Physics
Center of Mass
Constrained Relation
Constrained Motion
Question

A point object of mass m is slipping down on a smooth hemispherical body of mass M and radius R. The point object is tied to a wall with an ideal string as shown. At a certain instant, speed of the hemisphere is v and its acceleration is a. Then speed vp and acceleration aP of a particle has value (Assume all the surfaces in contact are frictionless)

aP = a

aP=[(v2R)+(a32)]2+(a2)2

VP = v sin 60°

VP = v

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Solution
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x + Rθ = constant

dxdt+Rdθdt=0

∴ω=dθdt=vR

α=dωdt=aR

At θ = 60°,

∴VP = v and aP =(a32+v2R)2+(a2)2