A projectile is fired at an angle θ with the horizontal. The condition under which it lands perpendicular on the fixed inclined plane with inclination α as shown in figure is,
To strike the plane perpendicularly, Final velocity along the plane is zero.
Along the inclined plane, we have,
i.e u cos (θ - α) = g sin αt ⇒ (1)
Also, the range of the projectile over the inclined plane is,
t = 2usin(θ−α)gcosα⇒ (2)
∴ u cot (θ - α) = 2 tan α × u
∴cot (θ - α) = 2 tan α