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Question: A heavy ring of mass m is clamped on the periphery of a light circular disc. A small particle having...

A heavy ring of mass m is clamped on the periphery of a light circular disc. A small particle having equal mass is damped at the centre of the disc. The system is rotated in such a way that the centre moves in a circle of radius r with a uniform speed vv . We conclude that the external force …
A. mv2r\dfrac{{m{v^2}}}{r} ,Must be acting on the central particle.
B. 2mv2r\dfrac{{2m{v^2}}}{r} ,Must be acting on the central particle.
C. 2mv2r\dfrac{{2m{v^2}}}{r} ,Must be acting on the system.
D. mv2r\dfrac{{m{v^2}}}{r}, Must be acting on the ring.

Explanation

Solution

To find out the force on the system of particles , first treat the bodies of the system as a whole system then apply the formula on the centre of mass of the system. Here total of mass 2m is moving with velocity ( v ) so the centrifugal force on the system of particle is FC=msystem(velocity)2radius  ofc.o.m{F_C} = \dfrac{{{m_{system}}{{(velocity)}^2}}}{{radius\;ofc.o.m}}.

Complete Step by step solution :
The situation is shown here

FC{F_C}

Let us consider the heavy ring of mass m is clamped on the periphery of a light circular disc and a small particle having equal mass is damped at the centre of the disc as a system. Then the centre of mass of the system has a total of mass 2m.

Now, it is given that the centre of mass moves with velocity v in a circle , so due to this circular motion of the centre of mass there will be a centrifugal force .
FC=msystem(velocity)2radius  ofc.o.m\Rightarrow {F_C} = \dfrac{{{m_{system}}{{(velocity)}^2}}}{{radius\;ofc.o.m}}
Putting the values msystem=2m{m_{system}} = 2m; velocity=vvelocity = v; radius  ofc.o.m=rradius\;ofc.o.m = r
FC=2mv2r\Rightarrow {F_C} = \dfrac{{2m{v^2}}}{r}
Since, 2mv2r\dfrac{{2m{v^2}}}{r} ,Must be acting on the system as a centrifugal force ,

Hence option ( C ) is the correct answer.

Note:
When a body moves in a circular motion there acts a force due to which the particle still continues its path in a circle and this force is constant in nature if the velocity of the body is constant and called as centripetal force.
The value of the centripetal force is
Fcentripetal=mbody(velocity)2radius  ofcircle{F_{centripetal}} = \dfrac{{{m_{body}}{{(velocity)}^2}}}{{radius\;of circle}}.