Rope Slipping in Pulley System: Does ##\ddot{l} = 0##?

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Discussion Overview

The discussion revolves around the assumptions and implications of a derivation related to a pulley system, specifically questioning whether the rope slips and how that affects the equation ##\ddot{l} = 0##. Participants explore the applicability of the equation across different pulley configurations and coordinate systems, as well as the implications of rope slipping on the constraints of the system.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants question whether the derivation assumes the rope does not slip, suggesting that if it does, there is no guarantee that ##\ddot{l} = 0##.
  • Others argue that the primary assumption is that the rope does not stretch, and they do not see how slipping is relevant to the derivation.
  • Concerns are raised about whether the equation applies to all pulley systems, particularly in cases where the dimensions of the system vary, such as when ##|h| > |X|##.
  • Participants discuss the implications of slipping, noting that if the rope slips, the length of the section of the rope terminating at the pull point is no longer constant.
  • There is a distinction made between slipping of the rope with respect to the hand versus slipping along the pulleys, with some clarification on how to interpret the position of the rope.
  • Some participants express curiosity about the effects of using a coordinate system with negative values, questioning if it would complicate the problem unnecessarily.
  • It is suggested that while using a coordinate system with negative values could be cumbersome, the physical constraint of the rope's length being constant remains unchanged.

Areas of Agreement / Disagreement

Participants generally do not reach a consensus on the relevance of slipping to the derivation, and multiple competing views remain regarding the implications of different coordinate systems and the assumptions made in the derivation.

Contextual Notes

Participants note that the discussion involves assumptions about the behavior of the rope, the implications of slipping, and the choice of coordinate systems, which may affect the interpretation of the equations involved.

PFuser1232
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In this derivation (see attached image), does the author assume that the rope doesn't slip? Because if it does, then there is no guarantee that ##\ddot{l} = 0##, right?
Also, does this equation apply to all pulley systems where one pulley is fixed and the other is allowed to move? For example, would this equation still hold for an arrangement where ##|h| > |X|##?
Also, would this equation hold if we were to choose a coordinate system where ##x## and ##X## are both negative?
 

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MohammedRady97 said:
In this derivation (see attached image), does the author assume that the rope doesn't slip? Because if it does, then there is no guarantee that l¨=0\ddot{l} = 0, right?
What the author assumes is that the rope doesn't stretch. I don't see how slipping is relevant.

MohammedRady97 said:
Also, does this equation apply to all pulley systems where one pulley is fixed and the other is allowed to move? For example, would this equation still hold for an arrangement where |h|>|X||h| > |X|? Also, would this equation hold if we were to choose a coordinate system where xx and XX are both negative?
Rather than try to apply this equation to other situations, just understand the logic of the derivation--then you can derive your own equation.
 
Doc Al said:
What the author assumes is that the rope doesn't stretch. I don't see how slipping is relevant.Rather than try to apply this equation to other situations, just understand the logic of the derivation--then you can derive your own equation.

If the rope slips then the length of the section of the rope which terminates at the point where the rope is pulled is no longer constant.
 
MohammedRady97 said:
If the rope slips then the length of the section of the rope which terminates at the point where the rope is pulled is no longer constant.
I'm not sure what you mean. That section is labeled as "x" in the diagram; it's not constant.
 
Doc Al said:
I'm not sure what you mean. That section is labeled as "x" in the diagram; it's not constant.

If the grip isn't firm enough, the rope would begin to slip. This change in ##x## isn't accounted for in the constraint equation, right? For example, if someone were to move their hand up and down the rope without actually pulling it we would end up with a change in ##x## without a corresponding change in ##X##.
 
MohammedRady97 said:
If the grip isn't firm enough, the rope would begin to slip. This change in ##x## isn't accounted for in the constraint equation, right? For example, if someone were to move their hand up and down the rope without actually pulling it we would end up with a change in ##x## without a corresponding change in ##X##.
Ah... you're talking about slipping of the rope with respect to the hand! (I thought you meant slipping along the pulleys.) Just think of x as the position of the rope, not the hand. Sure, if you want x to represent the position of the hand, then you'll have to assume no slipping. But the relationship really has to do with the position of the rope, not the hand.
 
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MohammedRady97 said:
If the grip isn't firm enough, the rope would begin to slip. This change in ##x## isn't accounted for in the constraint equation, right?
Doc Al said:
Ah... you're talking about slipping of the rope with respect to the hand! (I thought you meant slipping along the pulleys.) Just think of x as the position of the rope, not the hand. Sure, if you want x to represent the position of the hand, then you'll have to assume no slipping. But the relationship really has to do with the position of the rope, not the hand.

This is clear now, thanks!
I'm still curious as to whether reversing the coordinate system used would make a difference though. I know we chose a coordinate system where the coordinates of all parts of the pulley system are positive for convinience, but what happens when we use a coordinate system where the coordinates are negative? Also, should I even bother? I always get bogged down in trying to understand what would happen if a fairly simple problem were much more complicated. Will doing so improve my understanding of the subject, or will it just backfire and prevent me from making progress?
 
MohammedRady97 said:
but what happens when we use a coordinate system where the coordinates are negative?
The physical constraint will be the same: the length of the rope is a constant.

MohammedRady97 said:
Also, should I even bother? I always get bogged down in trying to understand what would happen if a fairly simple problem were much more complicated. Will doing so improve my understanding of the subject, or will it just backfire and prevent me from making progress?
It's hard to generalize. Often it helps, as long as you get the physics right. Other times it's a waste.

Perhaps a better strategy might be to actually try a more complicated problem and see if you can apply the same principles as in the simple one.
 
Doc Al said:
The physical constraint will be the same: the length of the rope is a constant.It's hard to generalize. Often it helps, as long as you get the physics right. Other times it's a waste.

Perhaps a better strategy might be to actually try a more complicated problem and see if you can apply the same principles as in the simple one.

If we wish to apply the physical constraint (that is constant length) in a coordinate system where all parts of the pulley system have negative coordinates we would have to use absolute values, but since dealing with absolute values is annoying, we're better off sticking to a coordinate system where each part has positive coordinates, right?
 
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MohammedRady97 said:
we're better off sticking to a coordinate system where each part has positive coordinates, right?
That would be my choice. Choose a coordinate system that makes the problem as easy as possible.

Regardless of coordinate system chosen, the length will still be a positive quantity. (Though expressing it might be cumbersome.)
 
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Doc Al said:
That would be my choice. Choose a coordinate system that makes the problem as easy as possible.

Regardless of coordinate system chosen, the length will still be a positive quantity. (Though expressing it might be cumbersome.)

Thanks Doc!
 

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