(c) $h = - vt_{1} + \frac{1}{2}gt_{1}^{2}$ or $\frac{h}{t_{1}} = - v + \frac{1}{2}gt_{1}$ …(i)
$h = vt_{2} + \frac{1}{2}gt_{1}^{2}$ or $- \frac{h}{t_{2}} = - v + \frac{1}{2}gt_{2}$ …(ii)
$\therefore\ \ \frac{h}{t_{1}} + \frac{h}{t_{2}} = \frac{1}{2}g(t_{1} + t_{2})$
or $h = \frac{1}{2}gt_{1}t_{2}$
For falls under gravity from the top of the tower
$h = \frac{1}{2}gt^{2}$
$\therefore\ \frac{1}{2}gt_{1}t_{2} = \frac{1}{2}gt^{2} \Rightarrow t = \sqrt{t_{1}t_{2}}$