Question about n rotating parallel cylinders

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Discussion Overview

The discussion revolves around the behavior of n identical vertical cylinders rotating around their axes when brought into contact with each other. Participants explore the implications of angular momentum, energy dissipation, and the effects of friction in both ideal and practical scenarios, including the potential for different configurations such as toothwheels.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that for even n, the cylinders come to rest, while for odd n, they end up with counter-rotating velocities, with angular momentum and kinetic energy reduced to specific fractions of their initial values.
  • Others argue that the total angular momentum of the system remains conserved during the interaction, despite changes in individual cylinder velocities.
  • There is a suggestion that energy is dissipated through friction and heat when the cylinders touch, but the exact mechanism of energy loss remains unclear, especially in the context of different configurations like toothwheels.
  • A participant questions the clarity of the original post regarding the fixed position of the cylinders relative to the Earth, which affects the overall momentum transfer.
  • Some participants discuss the implications of the cylinders forming a "snowmanular" shape and how this affects their motion and interaction.
  • Concerns are raised about the behavior of the system if the cylinders were to misalign, particularly in terms of locking mechanisms if they were gears.

Areas of Agreement / Disagreement

Participants express multiple competing views on how angular momentum and energy are conserved or dissipated in the system. The discussion remains unresolved regarding the exact fate of the energy and the implications of different configurations.

Contextual Notes

Limitations include assumptions about the nature of friction, the fixed position of the cylinders, and the potential for misalignment during interaction. The discussion does not resolve how these factors influence the overall behavior of the system.

Prishon
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There are n vertical identical parallel identical cilinders rotating around their length axes with the same angular velocity. The are somehow fixed wrt to Earth and brought together (on a rail?). After the contact there is no slipping and the cilinders are coupled to their neighbor cilinders. It is easy to see the cilinders end up as follows:

For even n there is no rotation anymore. All cilinders are at rest.

For uneven n the cilinders end up with contrary velocities. If there are n cilinders in contact then the absolute value of their angular velocities will be 1/n of the initial value.

For example, 3 cilinders (assuming their mass and initial angular velocities are 1) end up with angular momentum 1/3 and kinetic energy of 1/9 of the initial value.

But how is the energy dissipated? 1/9 of the momentum and energy are left in the cilinders. The rest of the momentum has flown into Earth. But where has the energy gone. Not into the Earth(well a very small part). Has it gone by friction? But what if the cilinders were toothwheels?
 
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If there are n identical cylinders and each has angular momentum of p, then the total angular momentum (be they apart or brought together) is n*p. That or external torque was applied, but you don't indicate that.

So if two of them are brought together, they'll form a sort of spinning snowmanular-cylinder shape (yes, that's a word now). The energy went away via friction/heat when they touched but the momentum must remain, so the joined figure must still rotate with the original combined angular momentum.
 
Halc said:
If there are n identical cylinders and each has angular momentum of p, then the total angular momentum (be they apart or brought together) is n*p. That or external torque was applied, but you don't indicate that.

So if two of them are brought together, they'll form a sort of spinning snowmanular-cylinder shape (yes, that's a word now). The energy went away via friction/heat when they touched but the momentum must remain, so the joined figure must still rotate with the original combined angular momentum.
Can you provide a reference or link for "snowmanular"?
 
kuruman said:
Can you provide a reference or link for "snowmanular"?
The momentum of say 3 cilinders is not the same before and after. In the beginning they all 3 rotate say clocjwise (with omega say 1) and afterwards they rotate with omega 1/3, tbe middle one anti-clickwise, as it must be since they are oushed against one another.
 
Halc said:
If there are n identical cylinders and each has angular momentum of p, then the total angular momentum (be they apart or brought together) is n*p. That or external torque was applied, but you don't indicate that.

So if two of them are brought together, they'll form a sort of spinning snowmanular-cylinder shape (yes, that's a word now). The energy went away via friction/heat when they touched but the momentum must remain, so the joined figure must still rotate with the original combined angular momentum.
They are pushed together in fixed position wrt to the Earth. Didn't I mention?
 
kuruman said:
Can you provide a reference or link for "snowmanular"?
This question comes forth if I search the net for that word...:)
 
Prishon said:
The momentum of say 3 cilinders is not the same before and after. In the beginning they all 3 rotate say clocjwise (with omega say 1) and afterwards they rotate with omega 1/3, tbe middle one anti-clickwise, as it must be since they are oushed against one another.
So you have three cylinders spinning about their axes that are brought together to touch and look from above like this OOO Correct?
Then because of friction, their surfaces will eventually stop moving relative to each other, correct?
While they are in contact, the angular momentum of the three-cylinder system about the axis of the middle cylinder is conserved because there is no external torque acting on this system about that axis, correct?
If all of the above is correct, what kind of motion do you think the three-cylinder system is going to undergo? Remember, no cylinder can spin independently about its own axis because friction has put a stop to that.
 
kuruman said:
So you have three cylinders spinning about their axes that are brought together to touch and look from above like this OOO Correct?
Then because of friction, their surfaces will eventually stop moving relative to each other, correct?
While they are in contact, the angular momentum of the three-cylinder system about the axis of the middle cylinder is conserved because there is no external torque acting on this system about that axis, correct?
If all of the above is correct, what kind of motion do you think the three-cylinder system is going to undergo? Remember, no cylinder can spin independently about its own axis because friction has put a stop to that.
Almost right! But the whole system can' t rotate. That system is fixed wrt to Earth. So momentum is tranferred to the Earth.
 
kuruman said:
So you have three cylinders spinning about their axes that are brought together to touch and look from above like this OOO
See? That's a snowman shape, except rotated on its side. Extend it in 3D and it's a snowmanular cylinder.
Sheesh, you guys need to lighten up.

Prishon said:
But the whole system can' t rotate. That system is fixed wrt to Earth. So momentum is tranferred to the Earth.
Oh. That wasn't clear from the OP.
 
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  • #10
Three identical cilinders (with fixed axes wrt to Earth) are identically rotating. When brought together (say on a rail) they end up with 1/3 of their initial rotational velocity. The middle one obviously rotating contra the others. They end up with 1/9 of initial momentum and kinetic energy.

Four (or 6,8,10, etc.) end up with zero velocity.

Uneven numbers end up with 1/n velocity.
 
  • #11
Prishon said:
But where has the energy gone. Not into the Earth(well a very small part). Has it gone by friction? But what if the cilinders were toothwheels?
So long as the cylinders remain counter-rotating and in line, all is OK.
But during the crush, when any three get out of line and form a triangle, the teeth will mesh and those three gears will lock together, then groups of three will lock, and so on.

This is a similar problem to the over-speed failure of a flat, circular disk flywheel breaking into three equal 120° pie-slices. What is the rate of rotation increase of the fragments, each of which has a lower moment of inertia than the original wheel.
 
  • #12
Baluncore said:
So long as the cylinders remain counter-rotating and in line, all is OK.
But during the crush, when any three get out of line and form a triangle, the teeth will mesh and those three gears will lock together, then groups of three will lock, and so on.

This is a similar problem to the over-speed failure of a flat, circular disk flywheel breaking into three equal 120° pie-slices. What is the rate of rotation increase of the fragments, each of which has a lower moment of inertia than the original wheel.
But they stay in line always. Their axes are fixed wrt Earth (they can only be brought together on one line; they always stay in line, no trianglez).
 

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