A thin uniform bar of length l and mass 8 m lies on a smooth horizontal table. Two point masses m and 2 m are moving in the same horizontal plane from opposite sides of the bar with speeds 2v and v respectively. The masses stick to the bar after collision
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Moment of inertia= I = Ml^2 / 12
As per angular momentum's conservation law:
τ = dL / dt
Torque = 0
dL / dt = zero
L = constant
Ang. momentum would be conserved if torque is 0
Center of masses of system from zero
= 8m x 0 + m (L/3) - 2m ( L/6 )
Center of masses = 0
As angular momentum is conserved:
Li=Lf
Li = m (2v) x ( L/3) + 2mv x ( L/6 )
Lf = [ (8m) L^2 / 12 + m (L/3)^2 + m (L/6)^2 ω
= { 2/3 mL^2 + mL^2 / 9 + mL^2 / 18 } ω
= 5/6 mL^2 ω
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