What is the radius of curvature of the parabola traced out by the projectile in the previous problem at a point where the particle velocity makes an angle θ2 with the horizontal ?
Let 'v' the velocity at the point where it makes an angle θ2 with horizontal.
The horizontal component remains unchanged.
So, v cos(θ2)=u cos θ
⇒ v=u cos θcos(θ2) ...(i)
From figure, mg cos(θ2)=mv2r
⇒ r=v2g cos(θ2)
Putting the value of 'v' from equation (i)
r=v2 cos2 θg cos2(θ2)