Question:

A thin circular ring of mass m and radius R is rotating about its axis perpendicular to the plane of the ring with a constant angular velocity $\omega$. Two point particles each of mass M are attached gently to the opposite ends of a diameter of the ring. The ring now rotates with an angular velocity $\omega /2$. Then, the ratio m/M is

Updated On: Mar 4, 2024
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  • $\frac{1}{2}$
  • $\sqrt{2}$
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The Correct Option is B

Solution and Explanation

$\because$ Momentum before particle is attached to the ring, $=I \omega=m R^{2} \omega$
Momentum after two particle is attached to the ring,
$=I \omega / 2+\left(\mu x^{2}\right) \omega / 2$
Here, $\mu=\frac{M \cdot M}{M+M}=\frac{M}{2}$ and $x=2 R$
So, $I \frac{\omega}{2}+\left(\mu x^{2}\right) \frac{\omega}{2} =\left[m R^{2}+\frac{M}{2}\left(4 R^{2}\right)\right] \frac{\omega}{2}$
$=\left[m R^{2}+2 M R^{2}\right] \frac{\omega}{2}$
According law of conservation of momentum, (momentum before) $=$ (momentum after) $\Rightarrow m R^{2} \omega=\left(m R^{2}+2 M R^{2}\right) \frac{\omega}{2}$
$\Rightarrow 2 m R^{2}=m R^{2}+2 M R^{2}$
So $\frac{m}{M}=2$
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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.