Question:

A solid sphere of mass M, radius R and having moment of inertia about an axis passing through the centre of mass as I, is recast into a disc of thickness t, whose moment of inertia about an axis passing through its edge and perpendicular to its plane remains I. Then, radius of the disc will be

Updated On: Jul 6, 2022
  • $\frac{2R}{\sqrt{15}}$
  • $R\sqrt{\frac{2}{15}}$
  • $\frac{4R}{\sqrt{15}}$
  • $\frac{R}{4}$
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The Correct Option is A

Solution and Explanation

Moment of inertia of solid sphere of mass M and radius R about an axis passing through the centre of mass is $I=\frac{2}{5}MR^{2}$. Let the radius of the disc is $r.$ Moment of inertia of circular disc of radius $r$ and mass $M$ about an axis passing through the centre of mass and perpendicular to its plane $=\frac{1}{2}Mr^{2}$ Using theorem of parallel axes, moment of inertia of disc about its edge is $I '=\frac{1}{2}Mr^{2}+Mr^{2}=\frac{3}{2}Mr^{2}$ Given, $I = I ? $\therefore \frac{2}{5}MR^{2}=\frac{3}{2}Mr^{2}$ or $r^{2}=\frac{4}{15}R^{2}$ or $r=\frac{2R}{\sqrt{15}}$
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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.