The only proof I've seen of Conservation of Angular Momentum assumes that the internal forces of the system act along the line joining particles i and j (i.e. - all internal forces are central.) Can we prove Conservation of Angular Momentum without this assumption?
If not, how can we apply conservation of angular momentum to systems that involve collisions, such as the following:
A uniform circular turntable is at rest in the $xy$ plane and is mounted on a frictionless axle, which lies along the vertical $ z$ axis. I throw a lump of putty (mass $m$) with speed $v$ toward the edge of the turntable. When the putty hits the turntable, it sticks to the edge, and the two rotate together with angular velocity $\omega.$ Find $\omega.$