From a uniform circular thin disc of mass $9 \mathrm{M}$ and radius $\mathrm{R}$, a small disc of radius…
- $4 \mathrm{MR}^{2}$
- $3 \mathrm{MR}^{2}$
- $\frac{\mathrm{MR}^{2}}{2}$
- $\mathrm{MR}^{2}$
Solution
The moment of inertia of the complete disc $\mathrm{I}_{1}=\frac{9 \mathrm{MR}^{2}}{2}$ The moment of inertia of the removed disc $=$
$\begin{aligned}
I^{\prime} &=\frac{M}{2}\left(\frac{R}{3}\right)^{2}+M\left(\frac{2 R}{3}\right)^{2}=\frac{M R^{2}}{18}+\frac{4 M R^{2}}{9} \\
&=\frac{M R^{2}}{2}
\end{aligned}$
[Since mass is proportional to area, it is proportional to square of the radius. Since the radius of the removed disc is $\frac{R}{3}$, its mass will be $M$ ]
$\therefore$ Moment of inertia of the remaining disc will be $I_{2}=I_{1}-I^{\prime}=\frac{9 m R^{2}}{2}-\frac{M R^{2}}{2}=4 M R^{2}$Asked in: MHT CET 2020 (13 Oct Shift 1)