(c) Refer figure when the velocity vector makes an angle $\alpha$ with the horizontal, the component of acceleration, perpendicular to velocity, $ie,$ the centripetal acceleration is $g\cos\alpha$. As horizontal component of velocity remains unchanged in angular projection of projectile, hence
[image:4_image86.emf]
$v\cos{\alpha = u\cos\theta}\ $or $v = \frac{u\cos\theta}{\cos\alpha}$
As, $g\cos\alpha$ provides centripetal acceleration, hence
$g\cos\alpha = \frac{v^{2}}{r}\ $ or $\frac{v^{2}}{g\cos\alpha} = \frac{u^{2}\cos^{2}\theta}{g\cos^{3}\alpha}$