(d) The particle is moving in circular path
From the figure, $mg = R\sin\theta\ \ \ \ \ \ \ldots(i)$
$\frac{mv^{2}}{r} = \ \ R\cos\theta\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ldots(ii)$
From equation (i) and (ii) we get
$\tan\theta = \frac{rg}{v^{2}}$ but $\tan\theta = \frac{r}{h}$
$\therefore h = \frac{v^{2}}{g} = \frac{(0.5)^{2}}{10} = 0.025m = 2.5\ cm$