As the ball has to hit the inclined plane normally, in that position the x-component of velocity will be zero and the velocity will have y-component only.
The ball will hit the incline normally if its parallel component of velocity reduces to zero during the time of flight.
By analyzing this motion along incline, i.e., x-direction,
vx=ux+axt
Here, vx=0,ux=v0cosθ,ax=−gsinα
0=v0cosθ−(gsinα)T⇒T=v0cosθgsinα ....(i)
Also the displacement of the particle in y-direction will be zero. Using
y=uyt+12ayt2⇒0=v0sinθT−12gcosT2
This gives T=2v0sinθgcosα ...(ii)
From (i) and (ii), we have
v0cosθgsinα=2v0sinθgcosα
⇒cosθsinα=2sinθcosα
tanθ=[12cotα]
θ=tan−1(12cotα)
Which is the required angle of projection.