A rod AB of length L and mass M is free to move on a frictionless horizontal surface is moving with a velocity v as shown in fig. End B of rod AB strikes end of wall. Assuming elastic impact, angular velocity of rod AB just after impact is
L-conservation⇒MvcmML212ω=MvL2⇒vcm+ωL6=vP-conservation⇒ωL2−vcm=v⇒ω(L2+L6)=2v∴ω=3vL