A particle of mass 'm' is projected with velocity 'u' at an angle θ with horizontal. During the period when the particle descends from highest point to the position where its velocity vector makes an angle θ2 with horizontal, work done by the gravity force is
12m⎡⎣(ucosθcosθ2)2−(ucosθ)2⎤⎦
12mu2cos2θ(1cos2θ2−1)
=12mu2cos2θ(1−cos2θ2cos2θ2)
=12mu2cos2θtan2θ2