A stone is projected from a horizontal plane. It attains maximum height H and strikes a stationary smooth wall and falls on the ground vertically below the maximum height. Assume the collision to be elastic. The height of the point on the wall where ball will strike is
3H4
u sinθ=√2gH
T=2u sinθg=2√2gHg
The horizontal distance covered
T=t1+t2
2usinθg=(R2+x)u cosθ+xu cosθ⇒R=R2+x+x⇒x=R4
t1=3R4u cosθ=342√2gH
=32√2Hg
=3√H2g
h=u sinθ×t1−12gt21
=√2gH×3√H2g−12g×9H2g
=3H−9H4=3H4