Question:

A thin wire of length L and uniform linear mass density p is bent into a circular loop with centre at O as shown. The moment of inertia of the loop about the axis XX ' is

Updated On: Jun 14, 2022
  • $ \frac{ \tau L^3}{ 8 {\pi}^2}$
  • $ \frac{ \tau L^3}{1116 {\pi}^2}$
  • $ \frac{ 5 \tau L^3}{ 16 {\pi}^2}$
  • $ \frac{ 3\tau L^3}{ 8 {\pi}^2}$
Hide Solution
collegedunia
Verified By Collegedunia

The Correct Option is D

Solution and Explanation

Mass of the ring M = $\tau$L. Let R be the radius of the ring, then
L = 2n R or R = $\frac{L}{2 \pi }$
Moment of inertia about an axis passing through O and parallel to XX 'will be
$ \, \, \, \, \, \, \, \, \, \, \, I_0 = \frac{1}{2} MR^2$
Therefore, moment of inertia about XX' (from parallel axis theorem) will be given by
$ \, \, \, I_{XX ' } = \frac{ 1}{2} MR^2 +MR^2 = \frac{3}{2} MR^2$
Substituting values of M and R
$ \, \, \, \, \, I_ { XX ' } = \frac{ 3}{2} (\tau L) \bigg( \frac{ L^2}{{\pi}^2} \bigg) = \frac{ 3 \tau L^3}{ 8 {\pi}^2}$
Was this answer helpful?
0
0

Top Questions on System of Particles & Rotational Motion

View More Questions

Questions Asked in JEE Advanced exam

View More Questions

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.