A thin rod of mass $m$ and length $l$ is oscillating about horizontal axis through its one end. Its maximum angular speed is $\omega$. Its centre of mass will rise upto maximum height :-
A thin rod of mass $m$ and length $l$ is oscillating about horizontal axis through its one end. Its maximum angular speed is $\omega$. Its centre of mass will rise upto maximum height :-
- A
$\frac{1}{6} \frac{l \omega}{g}$
- B
$\frac{1}{2} \frac{l^2 \omega^2}{g}$
- C
$\frac{1}{6} \frac{l^2 \omega^2}{g}$
- D
$\frac{1}{3} \frac{l^2 \omega^2}{g}$
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