
A uniform circular disc of radius ' R ' and mass ' M ' is rotating about an axis perpendicular to its plane…

- $\frac{7}{32} \mathrm{MR}^2$
- $\frac{9}{32} \mathrm{MR}^2$
- $\frac{17}{32} \mathrm{MR}^2$
- $\frac{13}{32} \mathrm{MR}^2$
Solution
The moment of inertia of a uniform circular disc of mass \(M\) and radius \(R\) about its central axis (perpendicular to its plane) is given by:
\(I_{\text {original }}=\frac{1}{2} M R^2\)
Step 2: Moment of Inertia of the Removed Part
The removed part is a smaller disc of radius \(R / 2\).
Since, the original disc has uniform mass distribution, the mass of the smaller disc (proportional to its area) is:
The moment of inertia of a smaller disc about its own center is:
\(\begin{gathered}
M_{\text {removed }}=M \times \frac{\pi(R / 2)^2}{\pi R^2}=M \times \frac{1}{4}=\frac{M}{4} \\
I_{\text {removed,center }}=\frac{1}{2} M_{\text {removed }}\left(\frac{R}{2}\right)^2 \\
I_{\text {removed opeter }}=\frac{1}{2} \times \frac{M}{4} \times \frac{R^2}{4}=\frac{1}{32} M R^2
\end{gathered}\)
\(\begin{gathered}
I_{\text {removed }}=I_{\text {removed,ceater }}+M_{\text {removed }} d^2 \\
I_{\text {remored }}=\frac{1}{32} M R^2+\left(\frac{M}{4} \times \frac{R^2}{4}\right) \\
I_{\text {removed }}=\frac{1}{32} M R^2+\frac{1}{16} M R^2 \\
I_{\text {removed }}=\frac{1}{32} M R^2+\frac{2}{32} M R^2=\frac{3}{32} M R^2
\end{gathered}\)
Step 3: Moment of Inertia of the Remaining Part
The moment of inertia of the remaining part is:
\(\begin{gathered}
I_{\text {remaining }}=I_{\text {original }}-I_{\text {removed }} \\
I_{\text {remaining }}=\frac{1}{2} M R^2-\frac{3}{32} M R^2 \\
I_{\text {rvmaining }}=\frac{16}{32} M R^2-\frac{3}{32} M R^2 \\
I_{\text {remaining }}=\frac{13}{32} M R^2
\end{gathered}\)
Asked in: JEE Main 2025 (22 Jan Shift 1)