Rope on Table Kleppner-Mechanics

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Homework Help Overview

The discussion revolves around a physics problem involving a rope of mass M and length l on a frictionless table, with a portion hanging through a hole. The original poster seeks to find a general solution for the length of rope through the hole over time, x(t), and has encountered discrepancies with the differential equation presented in the reference material by Kleppner.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants explore the implications of the rope's configuration on the problem, questioning whether the rope lies in a heap or a straight line. They discuss the effects of tension and the motion of different parts of the rope, as well as the assumptions regarding momentum and energy conservation.

Discussion Status

The discussion is ongoing, with participants raising various interpretations of the problem setup and its implications for the differential equations involved. Some have suggested that the conservation of work may play a role in how the rope interacts with the hole, while others are still clarifying the assumptions regarding the motion of the rope.

Contextual Notes

There are uncertainties regarding the configuration of the rope and how it interacts with the hole, which may affect the resulting equations of motion. Participants are also considering the implications of different assumptions on the forces acting on the rope.

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Homework Statement


A rope of mass M and length l lies on a frictionless table, with a short portion, l0 hanging through a hole. Initially the rope is at rest. a. Find a general solution for x(t), the length of rope through the hole.

Homework Equations



UPLOADED

The Attempt at a Solution


Solution uploaded. Where did I go wrong! My differential equation is different than Kleppner's.
Thanks

UPLOADED
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What is P ?
 
BvU said:
What is P ?
Linear Momentum going down positive
 
That the only thing that moves ?
 
BvU said:
That the only thing that moves ?
Rope on table moving along horizontally not down so yes
I am summing momentum along the vertical direction
 
So where does the motion of the horizontal part of the rope come from :rolleyes: ? Spontaneity ?
 
MARX said:
A rope of mass M and length l lies on a frictionless table
It is unclear whether it lies in a formless heap or in a straight line. If in a line then it is unclear exactly how it passes through the hole. You have assumed a heap. Can you find a different assumption which matches the book equation?
 
I am still not sure from replies either way what difference it makes?
are you suggesting there is also Tension Up on top of the moving piece? needs factored to the force? would it not be zero anyways if we consider the nonmoving part of the rope ie no forces there HORIZANTALLY so T = 0 ? and no friction so rope should slide towards hole freely?
 
MARX said:
the nonmoving part of the rope
If the portion on the table is straight then there are no nonmoving (indeed, no non-accelerating) parts.
 
  • #10
haruspex said:
If the portion on the table is straight then there are no nonmoving (indeed, no non-accelerating) parts.
Thank you. I see. You are correct. But now the question is how do I find ∫ F dt between t and t+dt
 
  • #11
MARX said:
Thank you. I see. You are correct. But now the question is how do I find ∫ F dt between t and t+dt
As I mentioned in post #7, if the tabletop portion is straight there is still a question mark over exactly how it passes through the hole.
Most likely, the question setter assumes work is conserved. E.g. imagine a hole in the form of a smooth tube bent into an arc, horizontal at the top and vertical below. In this way, the horizontal momentum of the rope across the table gets converted into vertical momentum without KE loss.
At the other extreme, as each dx of rope reaches the top of the hole it effectively slams into a wall, losing all its momentum and KE.
These scenarios will lead to different ODEs.
 
  • #12
haruspex said:
As I mentioned in post #7, if the tabletop portion is straight there is still a question mark over exactly how it passes through the hole.
Most likely, the question setter assumes work is conserved. E.g. imagine a hole in the form of a smooth tube bent into an arc, horizontal at the top and vertical below. In this way, the horizontal momentum of the rope across the table gets converted into vertical momentum without KE loss.
At the other extreme, as each dx of rope reaches the top of the hole it effectively slams into a wall, losing all its momentum and KE.
These scenarios will lead to different ODEs.
Got it. Ok thanks so much.
 

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