Question:

A thin uniform circular disc of mass M and radius R is rotating in a horizontal plane ahout an axis passing through its centre and perpendicular to the plane with an angular velocity $\omega$ Another disc of same mass hut half the radius is gently placed over it coaxially. The angular speed o f the composite disc will be

Updated On: Jul 6, 2022
  • $\frac{5}{4}\omega$
  • $\frac{4}{5}\omega$
  • $\frac{2}{5}\omega$
  • $\frac{5}{2}\omega$
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The Correct Option is B

Solution and Explanation

$I_1\omega_1=(I_1+I_2)\omega_2$ $\left[\frac{MR^2}{2}\right]\omega=\left[\frac{MR^2}{2}+\frac{M\left(\frac{R}{2}\right)^2}{2}\right]\omega^2$ $=\left[\frac{MR^2}{2}+\frac{MR^2}{8}\right]\omega_2=\left[\frac{5MR^2}{8}\right]$ $\omega_2=\frac{4}{5}\omega$
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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.