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A rod of length $l$ is held vertically stationary with its lower end located at a point $\mathrm{P}$, on the horizontal plane. When the rod is released to topple about $\mathrm{P}$, the velocity of the upper end of the rod with which it hits the ground is
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Verified Answer
The correct answer is:
$\sqrt{3 \mathrm{~g} l}$
Here, potential energy of the metre stick will be converted into rotational kinetic energy.

Because centre of gravity of stick lies at the middle of the rod,
PE of metre stick $=\frac{m g l}{2}$
Rotational kinetic energy $E=\frac{1}{2} I \omega^{2}$
$I$ about point $A=\frac{m l^{2}}{3}$.
By law of conservation of energy
$$
m g\left(\frac{l}{2}\right)=\frac{1}{2} I \omega^{2}=\frac{1}{2} \frac{m l^{2}}{3}\left(\frac{v_{B}}{l}\right)^{2}
$$
By solving, we get $v_{B}=\sqrt{3 g l}$

Because centre of gravity of stick lies at the middle of the rod,
PE of metre stick $=\frac{m g l}{2}$
Rotational kinetic energy $E=\frac{1}{2} I \omega^{2}$
$I$ about point $A=\frac{m l^{2}}{3}$.
By law of conservation of energy
$$
m g\left(\frac{l}{2}\right)=\frac{1}{2} I \omega^{2}=\frac{1}{2} \frac{m l^{2}}{3}\left(\frac{v_{B}}{l}\right)^{2}
$$
By solving, we get $v_{B}=\sqrt{3 g l}$
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