Question:

A solid sphere is rotating about a diameter at an angular velocity $ \omega . $ If it coots so that its radius reduces to $ \frac{1}{n} $ of its original value, its angular velocity becomes

Updated On: Jul 14, 2022
  • $ \frac{\omega }{n} $
  • $ \frac{\omega }{{{n}^{2}}} $
  • $ n\omega $
  • $ {{n}^{2}}\omega $
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The Correct Option is D

Solution and Explanation

From law of conservation of angular momentum, if no external torque is acting upon a body rotating about an axis, then the angular momentum of the body remains constant that is $J=I \omega$ Also, $I=\frac{2}{5} M R^{2}$ for a solid sphere. Given, $ R_{1}=R, R_{2}=\frac{R}{n} $ $\therefore \frac{2}{5} M R^{2} \omega_{1}=\frac{2}{5} M\left(\frac{R}{n}\right)^{2} \times \omega_{2} $ $\Rightarrow \omega_{2}=n^{2} \omega_{1} $ $=m^{2} \omega$
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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.