A thin rod of length $L$ and mass $M$ is bent at its midpoint into two halves so that the angle between them…
- $\frac{M L^2}{24}$
- $\frac{M L^2}{12}$
- $\frac{M L^2}{6}$
- $\frac{\sqrt{2} M L^2}{24}$
Solution

Moment of inertia of each part through its one end
$=\frac{1}{3}\left(\frac{M}{2}\right)\left(\frac{L}{2}\right)^2$
Hence, net moment of inertia through its middle point $O$ is
$\begin{aligned}
I & =\frac{1}{3}\left(\frac{M}{2}\right)\left(\frac{L}{2}\right)^2+\frac{1}{3}\left(\frac{M}{2}\right)\left(\frac{L}{2}\right)^2 \\
& =\frac{1}{3}\left[\frac{M L^2}{8}+\frac{M L^2}{8}\right]=\frac{M L^2}{12}
\end{aligned}$ .
Asked in: NEET 2008 (Screening)