Question:

A thin circular plate of mass $M$ and radius $R$ has its density varying as $\rho (r) = \rho_0 r$ with $\rho_0$ as constant and $r$ is the distance from its centre. The moment of Inertia of the circular plate about an axis perpendicular to the plate and passing through its edge is $I = aMR^2$. The value of the coefficient $a$ is :

Updated On: Sep 27, 2024
  • $\frac{3}{2}$
  • $\frac{1}{2}$
  • $\frac{3}{5}$
  • $\frac{8}{5}$
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The Correct Option is D

Solution and Explanation

$M= \int^{R}_{0} \rho_{0} r \left(2\pi rdr\right) = \frac{\rho_{0} \times2 \pi \times R^{3}}{3} $
${$\underset{\text{ (MOI about COM) }}{{ I_0 }}$ = \int^{R}_{0} \rho_{0} r (2 \pi rdr) \times r^{2} = \frac{\rho_{0} \times2\pi R^{5}}{5} } $
by parallel axis theorem
$ I = I_{0} + MR^{2} $
$ = \frac{\rho_{0} \times2 \pi R^{5}}{5} + \frac{\rho_{0} \times2\pi R^{3}}{3} \times R^{2} = \rho_{0} 2\pi R^{5} \times\frac{8}{15} $
$ = MR^{2} \times\frac{8}{5} $
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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.