A small block slides with velocity 0.5√gr on the horizontal friction less surface as shown in the figure. The block leaves the surface at point C. The angle θ in the figure is:
Vertical displacement, s=r(1−cosθ)
Apply kinematic equation,
V2=u2+2as=[(0.5√gr)2+2gr(1−cosθ)]
Kinetic energy = Potential Energy
12mv2=mgr(1−cosθ)
v2=2gr(1−cosθ).........(1)
Normal reaction on block
N=mgcosθ−mv2r
0=mgcosθ−mv2r
0=mgcosθ−m(0.5√gr)2+2gr(1−cosθ)r
0=mgcosθ−2.25mg+2mgcosθ
cosθ=34
θ=cos−1(34)
Hence, at angle cos−1(34) , block will leave the surface.