Angular Momentum and Point of Application in Rolling Motion

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The discussion focuses on the application of angular momentum in rolling motion, particularly regarding the choice of reference points for calculating torque. One method involves taking the origin at the center of mass, while another suggests using the point of contact with the ground, which is instantaneously at rest. Participants express uncertainty about the validity of using an accelerating reference frame and whether it affects angular momentum calculations. The conversation highlights the importance of clearly defining the reference point and its implications on the analysis of rotational dynamics. Understanding these concepts is crucial for solving related physics problems effectively.
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Homework Statement


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Homework Equations


Angular momentum


The Attempt at a Solution


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So I have my work shown in the two pictures. rm, rf denote the position vectors to the center of mass and point of application of force respectively (with respect to the chosen origin of course). Is this the way to do it? I've seen a way done by some others where they take the origin of the coordinate system to be instantaneously co - moving with the point on the ball that is in contact with the ground (so that again torque will vanish with respect to this origin because it acts at the origin itself) and use the exact same terms for the final and initial angular momentum. This frame will however be accelerating with respect to a fixed coordinate system due to friction but is angular momentum unaffected by this?
 
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It's a bit hard to comment on the other approach without seeing it in detail.
 
Is my method correct however? Also there wasn't any difference at all in the other approach other than the fact that the reference point is taken to be the point of contact of the ball with the ground. The equations are then written the same way. I was just wondering if that was allowed because such a reference point would be decelerating with respect to a fixed one.
 
PhizKid said:
Is my method correct however?
I believe it is, and a quite interesting one too.
Also there wasn't any difference at all in the other approach other than the fact that the reference point is taken to be the point of contact of the ball with the ground. The equations are then written the same way. I was just wondering if that was allowed because such a reference point would be decelerating with respect to a fixed one.
It's still unclear without seeing the details. I often take moments about a point of contact, but treating it only as the instantaneous point of contact. That's not the same as using an accelerating point as the origin of a reference frame. Even in the latter case, it might happen to be valid, but probably should be supported by some argument as to why it is valid.
 
Could you explain how you would do it with the way you mentioned by keeping the origin instantaneously at rest with respect to the point of contact. Thanks haruspex!
 
PhizKid said:
Could you explain how you would do it with the way you mentioned by keeping the origin instantaneously at rest with respect to the point of contact. Thanks haruspex!
No, I didn't necessarily mean for this problem. I meant rotational dynamics problems in general. For a rolling ball or disc, the point of contact is instantaneously at rest, and that's often a useful place to take moments about.
 
If I'm not mistaken, when you say the point to take the moment about that is not the same thing as the origin of the coordinate system is it?
 
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