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Its downward component is L, its horizontal component is R (the radius of the
pulley).
No external torque means angular momentum is conserved.
Wait, what if we don't use a pulley, just a frictionless hook? If R=0, the
angular momentum is already zero without putting any constraint on v.
Oh, but notice that if this problem really needs conservation of angular
momentum to do it correctly, it shouldn't be appear in the book in the section
dealing with linear momentum.
pulling on a rope is the easiest way to handle the problem after all.