(d) Let $\alpha''$ be the angle of projection of the second body
[image:4_image128.emf]
$R = \frac{u^{2}}{g\cos\beta}\lbrack sin(2\alpha - \beta)\rbrack$
Range of both the bodies is same. Therefore,
$\sin(2\alpha - \beta) = \sin{(2\alpha^{''} - \beta)}$
or $2\alpha^{''} - \beta = \pi - (2\alpha - \beta)$
$\alpha^{''} = \frac{\pi}{2} - (\alpha - \beta)$
Now, $T = \frac{2u\sin(\alpha - \beta)}{g\cos\beta}\ and\ T^{''} = \frac{2u\sin{(\alpha^{''} - \beta)}}{g\cos\beta}$
$\therefore\frac{T}{T''} = \frac{\sin{(\alpha - \beta)}}{\sin{(\alpha'' - \beta)}} = \frac{\sin{(\alpha^{\ } - \beta)}}{\sin\left\{ \frac{\pi}{2} - (\alpha^{\ } - \beta) - \beta \right\}}$
$= \frac{\sin{(\alpha^{\ } - \beta)}}{\sin\left( \frac{\pi}{2} - \alpha \right)} = \frac{\sin{(\alpha^{\ } - \beta)}}{\cos\alpha}$