Olympiad Mechanics problem (torque)

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SUMMARY

The forum discussion centers on solving a physics problem involving a pendulum formed by a light wire rod and a mass, where the rod is bent into a hoop and hung on a revolving shaft. The key challenge is to find the equilibrium angle between the rod and the vertical, considering the coefficient of friction (µ) between the shaft and the hoop. Participants emphasize the importance of analyzing torques about the point of contact and correctly positioning the forces to ensure equilibrium, leading to the conclusion that the line of action of the gravitational force (mg) must pass through the point of contact to achieve zero torque.

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  • Familiarity with the concepts of friction, particularly static and kinetic friction.
  • Knowledge of pendulum mechanics and the forces acting on a pendulum system.
  • Ability to apply trigonometric relationships in physics problems.
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  • #31
there are a lot of different interesting motions in this problem
 
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  • #32
IIRC, J.P. Den Hartog discussed this problem in detail in his Mechanical Vibrations text from many years ago.
 
  • #33
Ceva said:
An end of a light wire rod is bent into a hoop of radius r.
This quote, and the associated figure indicate that there is support for a bending moment transfer between the pendulum shaft and the ring. Saying this differently, the pendulum is not pivoted on the ring, but is rather fixed on the ring. This means that there is only one DOF, not two.
 
  • #34
Dr.D said:
IIRC, J.P. Den Hartog discussed this problem in detail in his Mechanical Vibrations text from many years ago.
That is strange. This problem is too simple to discuss it in a monograph in detail.
 
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  • #35
zwierz said:
That is strange. This problem is too simple to discuss it in a monograph in detail.

By George! You are correct. He did not discuss it in detail, but only offered it as a homework problem in such a way that the person working the problem would develop a rather comprehensive discussion of the several possible cases. I was recalling my own detailed write up of this problem.
 
  • #36
Dr.D said:
He did not discuss it in detail, but only offered it as a homework problem in such a way that the person working the problem would develop a rather comprehensive discussion of the several possible cases.
So what are the several possible cases?
 
  • #37
Several different friction models.
 
  • #38
It does not make sense to consider friction models whenever non slipping condition has already been imposed.

The phase portraits of described above system essentially differ from each other for the following four cases ##\epsilon r/g>1,\quad \epsilon r/g=1,\quad 0<\epsilon r/g<1,\quad \epsilon=0##

The center of the ring can rotate about the shaft; it can oscillate near its stable equilibrium; it can even perform asymptotic motions
 
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  • #39
I'll leave you to discuss it with Den Hartog.
 
  • #40
I understand the fact that on an incline the slipping begins at a angle ## \alpha ## s.t tan ## \alpha =
\mu ## , but how can you assocciate that fact to this problem?
 
  • #41
RoloJosh16 said:
I understand the fact that on an incline the slipping begins at a angle ## \alpha ## s.t tan ## \alpha =
\mu ## , but how can you assocciate that fact to this problem?
Are you referring to the original problem in post #1 or to the very different problem zwierz introduced (in violation of forum guidelines!) in post #29?
 
  • #42
haruspex said:
Are you referring to the original problem in post #1 or to the very different problem zwierz introduced (in violation of forum guidelines!) in post #29?

To the original problem.
 
  • #43
haruspex said:
Are you referring to the original problem in post #1 or to the very different problem zwierz introduced (in violation of forum guidelines!) in post #29?

Do you understand what I am asking?
 
  • #44
RoloJosh16 said:
To the original problem.
In the original problem the shaft is turning at constant speed and the system is in steady state, so we are only concerned with kinetic friction.

Edit: but, interestingly, if we define α as tan(α)=μk then the answer can be written as (R+L)sin(θ)=Rsin(α ).
 
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  • #45
RoloJosh16 said:
I understand the fact that on an incline the slipping begins at a angle ## \alpha ## s.t tan ## \alpha =
\mu ## , but how can you assocciate that fact to this problem?
The original problem is similar to having a conveyer belt inclined at angle ##\alpha## with the belt moving upward at a constant speed. Suppose a box is placed on the moving belt and the box happens to stay at rest relative to the earth. Then you can ask for the relation between ##\alpha## and the coefficient of kinetic friction ##\mu_k##.
 
  • #46
TSny said:
The original problem is similar to having a conveyer belt inclined at angle ##\alpha## with the belt moving upward at a constant speed. Suppose a box is placed on the moving belt and the box happens to stay at rest relative to the earth. Then you can ask for the relation between ##\alpha## and the coefficient of kinetic friction ##\mu_k##.

Ahhh, thank you. I was thinking about that relation but didn' t think about a moving surface. The box in that case would be the tiny part of the hoop in contact with the shaft?
 
  • #47
RoloJosh16 said:
Ahhh, thank you. I was thinking about that relation but didn' t think about a moving surface. The box in that case would be the tiny part of the hoop in contact with the shaft?
Yes, that's right.
 

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