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Q. A thin uniform rod of length $l$ and mass $m$ is swinging freely about a horizontal axis passing through its end. Its maximum angular speed is $\omega$. Its centre of mass rises to a maximum height of

AIEEEAIEEE 2009System of Particles and Rotational Motion

Solution:

$T.E_{i}=T.E_{f}$
$\frac{1}{2}I\omega^{2}=mgh$
$\frac{1}{2}\times\frac{1}{3}m\ell^{2}\omega^{2}=mgh \Rightarrow h=\frac{1}{6} \frac{\ell^{2}\omega^{2}}{g}$

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