Why is angular momentum conserved?

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SUMMARY

The discussion centers on the conservation of angular momentum during an instantaneous collision, as presented in David Morin's Classical Mechanics. The key point is that while torque from gravity acts on the system, its effect is negligible during the brief moment of collision. Morin emphasizes that the time frame of the collision is too short for any significant transfer of angular momentum, allowing the angular momentum to remain conserved despite the presence of torque due to gravity.

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Abhishek11235
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So,this is problem from David Morin's Classical Mechanics(Screenshot 1). I solved the problem. Then I went to see the solution in manual hoping for out of box thinking. As in screenshot 2 is solution by Morin. My question is why he conserves angular momentum about the point (R-h) below C.M? There is torque due to its own weight. Actually I want to understand meaning of the statement he has written in bracket.

If texts is small here is what he has written:
"torque from gravity will be relevant during the subsequent rising-up motion. But during the instantaneous collision, L does not change."
Screenshot_2019-02-15-23-46-47.jpeg
Screenshot_2019-02-15-23-52-23.jpeg
 

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You are looking at a collision that is being modeled as instantaneous. As long as this is a good approximation is appropriate, the time of the collision is too short for the torque to transfer any relevant angular momentum to the system.
 
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The argument is that although there is a torque due to gravity while the ball is rotating about the corner, the time required for the ball to go over the corner is short enough so that the angular momentum does not change appreciably.
 
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