(b) Let $\alpha^{''}$ be the angle of projection of the second body
[image:4_image145.emf]
$R = \frac{u^{2}}{gcos^{2}\beta}\left\lbrack \sin(2\alpha - \beta) - sin\beta \right\rbrack$
Range of both the body is same. Therefore
$\sin(2\alpha - \beta) = sin\left( 2\alpha^{''} - \beta \right)$
$or\ 2\alpha^{''} - \beta = \pi - (2\alpha - \beta)$
$\alpha^{''} = \frac{\pi}{2} - (\alpha - \beta)$
$Now,\ \ \ \ T = \frac{2u\sin(\alpha - \beta)}{gcos\beta}\ and\ T^{''} = \frac{2u\sin\left( \alpha^{''} - \beta \right)}{gcos\beta}$
$\therefore\ \frac{T}{T^{''}} = \frac{\sin(\alpha - \beta)}{\sin\left( \alpha^{''} - \beta \right)} = \frac{\sin(\alpha - \beta)}{\sin\left\{ \frac{\pi}{2} - (\alpha - \beta) - \beta \right\}}$
$\frac{\sin(\alpha - \beta)}{\sin\left( \frac{\pi}{2} - \alpha \right)} = \frac{\sin(\alpha - \beta)}{cos\alpha}$