Rope on Table Kleppner-Mechanics

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SUMMARY

The discussion focuses on a physics problem involving a rope of mass M and length l on a frictionless table, with a portion l0 hanging through a hole. Participants analyze the dynamics of the rope, particularly the assumptions regarding its configuration and the implications for deriving the correct ordinary differential equations (ODEs). Key points include the conservation of work and the effects of momentum transfer as the rope moves through the hole, leading to different interpretations of the system's behavior.

PREREQUISITES
  • Understanding of classical mechanics, specifically linear momentum and energy conservation.
  • Familiarity with ordinary differential equations (ODEs) and their applications in physics.
  • Knowledge of the dynamics of systems involving tension and frictionless surfaces.
  • Experience with problem-solving in physics, particularly in analyzing motion and forces.
NEXT STEPS
  • Study the derivation of ODEs in classical mechanics, focusing on systems with variable mass.
  • Explore the concept of conservation of energy in dynamic systems, particularly in relation to momentum transfer.
  • Investigate the effects of different boundary conditions on the motion of objects, such as the rope in this scenario.
  • Learn about the application of calculus in physics, specifically in solving problems involving integrals of forces over time.
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Students and educators in physics, particularly those studying mechanics, as well as anyone interested in the mathematical modeling of dynamic systems involving ropes and forces.

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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

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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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