(c) We know that range of projectile is same for complementary angles $ie,$ for $\theta\ and\ (90{^\circ} - \theta).$
$\therefore\ T_{1} = \frac{2u\sin\theta}{g}$
$T_{2} = \frac{2u\sin(90{^\circ} - \theta)}{g} = \frac{2u\cos\theta}{g}$
$and\ \ \ R = \frac{u^{2}\sin\theta}{g}$
$Therefore,\ \ T_{1}T_{2} = \frac{2u\sin\theta}{g} \times \frac{2u\cos\theta}{g}$
$= \frac{{2u}^{2}(2\sin{\theta\cos{\theta)}}}{g^{2}}$
$= \frac{{2u}^{2}(2\sin{\theta)}}{g^{2}} = \frac{2R}{g}$
$\therefore\ T_{1}T_{2} \propto R$