The particle has circular path before it passes AB second time during its upward motion. Let the particle have circular path at ′P′ and V be its velocity at P.
Applying conservation of energy at P and at the lowest point gives:
12mu2=12mv2+mgL(1+sinθ)
At point P
T+mgsinθ=mv22
and when T=0
2gsinθ=v2
After moving in a circular path, the particle moves along a parabolic trajectory. Since the velocity of the particle when it crosses AB is horizontal. Therefore, it is passing through its highest point in the parabolic path. Thus, half of the range of this parabolic path Lcosθ=L8
Projection angle of the particle at P
=90°−θ
∴ minimum range
=v2sin2(90−θ)g∴12v2sin2(90−θ)g=Lcosθ−L8
⇒cosθ=12⇒θ=60°
Using the above equations:
u= ⎷(4+3√32)gL