Question:

A circular hole of diameter $R$ is cut from a disc of mass $M$ and radius $R$; the circumference of the cut passes through the centre of the disc. The moment of inertia of the remaining portion of the disc about an axis perpendicular to the disc and passing through its centre is

Updated On: Jul 5, 2022
  • $\left(\frac{15}{32}\right)MR^{2}$
  • $\left(\frac{1}{8}\right)MR^{2}$
  • $\left(\frac{3}{8}\right)MR^{2}$
  • $\left(\frac{13}{32}\right)MR^{2}$
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The Correct Option is D

Solution and Explanation

M.I. of complete disc about its centre $O$. $I_{Total}=\frac{1}{2}MR^{2} \, ...\left(i\right)$ Mass of circular hole $\left(removed\right)$ $=\frac{M}{4}\left(As\,M=\pi R^{2}\,t \therefore M\,\propto\,R^{2}\right)$ M.I. of removed hole about its own axis $=\frac{1}{2}\left(\frac{M}{4}\right)\left(\frac{R}{2}\right)^{2}=\frac{1}{32} \,MR^{2}$ $M.I.$ of removed hole about $O'$ $I_{removed hole }=I_{cm}+mx^{2}$ $=\frac{MR^{2}}{32}+\frac{M}{4}\left(\frac{R}{2}\right)^{2}$ $=\frac{MR^{2}}{32}+\frac{MR^{2}}{16}=\frac{3MR^{2}}{32}$ $M.I.$ of complete disc can also be written as $I_{Total}=I_{removed hole}+I_{remaining disc}$ $I_{Total}=\frac{3MR^{2}}{32}+I_{remaining disc}\, ...\left(ii\right)$ From e $\left(i\right)$ and $\left(ii\right),$ $\frac{1}{2}MR^{2}=\frac{3MR^{2}}{32}+I_{remaining disc}$ $\Rightarrow I_{remaining disc}$ $=\frac{MR^{2}}{2}-\frac{3MR^{2}}{32}=\left(\frac{13}{32}\right)MR^{2}$
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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.