Question:

A merry-go-round, made of a ring-like platform of radius $R$ and mass $M$, is revolving with angular speed $\omega$. $A$ person of mass $M$ is standing on it. At one instant, the person jumps off the round, radially away from the centre of the round. The speed of the round afterwards is

Updated On: Jul 5, 2022
  • $2\omega$
  • $\omega$
  • $\frac{\omega}{2}$
  • $0$
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The Correct Option is A

Solution and Explanation

Here angular momentum is converted $L _{ i }= L _{ f }$ $\left( I _{\text {ring }}+ M R ^{2}\right) \omega=\left( L _{\text {man }}+ L _{\text {ring }}\right) \omega' \,\,\,L _{\text{man}}= L _{\text {ring }}$ [A man is assumed to at circumstances of ring and is final angular speed of ring after men jump off] $\left( M R ^{2}+ M R ^{2}\right) \omega= O + M R ^{2} \omega '$ $2 \omega=\omega'$
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Concepts Used:

System of Particles and Rotational Motion

  1. The system of particles refers to the extended body which is considered a rigid body most of the time for simple or easy understanding. A rigid body is a body with a perfectly definite and unchangeable shape.
  2. The distance between the pair of particles in such a body does not replace or alter. Rotational motion can be described as the motion of a rigid body originates in such a manner that all of its particles move in a circle about an axis with a common angular velocity.
  3. The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.