
(d) From law of conservation of energy, potential energy of fall gets converted to kinetic energy.
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$\therefore\ \ PE = KE$
$mgh = \frac{1}{2}{mv}^{2}$
$or\ \ v = \sqrt{2gh}\ \ \ldots.(i)$
Also, the horizontal component of force is equal centrifugal force.
$\therefore\ \ \ mg\cos{\theta = \frac{{mv}^{2}}{R}\ \ldots(ii)}$
From Eq. (i)
$\therefore\ \ \ mg\cos{\theta = \frac{2mgh}{R}\ \ldots(iii)}$
From $\mathrm{\Delta}\ AOB,$
$\ \cos{\theta = \frac{(R - h}{R}\ }$
$\Longrightarrow \ \ mg\left( \frac{(R - h)}{R} \right) = \frac{2mgh}{R}$
$\Longrightarrow \ \ 3h = R$
$\Longrightarrow h = \frac{R}{3}$