If the velocity of projection be v and mass of the projectile be m, then \(K = \frac{1}{2}mv^2\)
∵ The projectile attains maximum range, therefore angle of projection will be θ = 45°.
∴ At the time of projection,
\(v_x = v\cos45^\circ = \frac{v}{\sqrt{2}}\) (horizontal velocity)
and vy = v sin 45° = \(\frac{v}{\sqrt{2}}\) (vertical velocity)
∵ The horizontal velocity vx remains unchanged and at heighest point, vy becomes zero. Only vx remains there.
∴ Kinetic energy at highest point,
\(K' = \frac{1}{2}mv_x{}^2 = \frac{1}{2}m(\frac{v}{\sqrt{2}})^2 = \frac{1}{2}\ \frac{mv^2}{2}\)
or \(K' =\frac{K}{2}\)
or K' = 0.5 K