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Question

Physics Question on System of Particles & Rotational Motion

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

A

τL38π2 \frac{ \tau L^3}{ 8 {\pi}^2}

B

τL31116π2 \frac{ \tau L^3}{1116 {\pi}^2}

C

5τL316π2 \frac{ 5 \tau L^3}{ 16 {\pi}^2}

D

3τL38π2 \frac{ 3\tau L^3}{ 8 {\pi}^2}

Answer

3τL38π2 \frac{ 3\tau L^3}{ 8 {\pi}^2}

Explanation

Solution

Mass of the ring M = τ\tauL. Let R be the radius of the ring, then
L = 2n R or R = L2π\frac{L}{2 \pi }
Moment of inertia about an axis passing through O and parallel to XX 'will be
I0=12MR2\, \, \, \, \, \, \, \, \, \, \, I_0 = \frac{1}{2} MR^2
Therefore, moment of inertia about XX' (from parallel axis theorem) will be given by
IXX=12MR2+MR2=32MR2\, \, \, I_{XX ' } = \frac{ 1}{2} MR^2 +MR^2 = \frac{3}{2} MR^2
Substituting values of M and R
IXX=32(τL)(L2π2)=3τL38π2\, \, \, \, \, I_ { XX ' } = \frac{ 3}{2} (\tau L) \bigg( \frac{ L^2}{{\pi}^2} \bigg) = \frac{ 3 \tau L^3}{ 8 {\pi}^2}