Bead on a rotating wire - holonomic or not?

In summary: Btw, back to the OP: the first case (wire rotating about an axis perpendicular to its plane) is clearly not time... dependent.
  • #1
bitty
14
0

Homework Statement


We have a bead sliding on a frictionless hoop oriented vertically. First the hoop rotates about its center with rotation axis perpendicular to its plane.

Second, the hoop rotates about a vertical axis as well.
In both of these cases, are the constraints holonomic or nonholonomic? Are the time dependent or independent?


Homework Equations





The Attempt at a Solution


In both cases the constraints are time dependent because they depend on the rotational velocity. In the first case, it is holonomic - you can define the bead's position in terms of time and the generalized coordinates.

However, I'm not sure about the second case. I think it might be holonomic as well, because we should be able to describe its constraints knowing only the hoop's equations of motion. The hoop has 2 degrees of freedom, theta and phi, and we define an origin we should be able to describe the particle's location at any time using just theta and phi.
Am I correct in my argument that the constraints in both cases are holonomic?

This question has my confidence completely stumped!
 
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  • #2
bitty said:
we should be able to describe the particle's location at any time using just theta and phi.
Well, not the particle's exact location, but the constraints on it, yes. I agree they're both holonomic, though I'd never heard of the term until I saw this post :-).
 
  • #3
If the bead were sliding with friction, would the constraint turn from holonomic to non-holonomic?
 
  • #4
Mistro116 said:
If the bead were sliding with friction, would the constraint turn from holonomic to non-holonomic?
Not as I understand it. We are only concerned with the constraints on its location, right? I.e., where it physically could be. I don't see how friction changes that.
An example of a non-holonomic constraint would be an object moving on a curved surface, held down by gravity. Whether it stays on the surface would then depend on velocity.
I confess to being uneasy about this though. Even in the first case of the OP, whether it can reach the top of the hoop is limited by KE, so whether it's holonomic seems to depend on which constraints you choose to consider.
 
  • #5
Holonomic constraints corresponds to case where eqn. are integrable.In case of friction,where the particle must also have to satisfy the eqn of surface,it turns out to be non holonomic.
 
  • #6
andrien said:
Holonomic constraints corresponds to case where eqn. are integrable.In case of friction,where the particle must also have to satisfy the eqn of surface,it turns out to be non holonomic.
Very surprised by that... what has integrability of the equation to do with the nature of the constraints? Is there a URL reference you can post?
 
  • #7
haruspex said:
Very surprised by that... what has integrability of the equation to do with the nature of the constraints? Is there a URL reference you can post?

There are a plenty of refrences.Why don't you start with wikipedia like here
http://en.wikipedia.org/wiki/Nonholonomic_system
If you want a book ,then 'Dynamics vol.2 by a.s. ramsey' or any other like of routh or whittaker has also given it in detail.
 
  • #8
andrien said:
There are a plenty of refrences.Why don't you start with wikipedia like here
http://en.wikipedia.org/wiki/Nonholonomic_system
If you want a book ,then 'Dynamics vol.2 by a.s. ramsey' or any other like of routh or whittaker has also given it in detail.
The reference I found was http://en.wikipedia.org/wiki/Holonomic_constraints, which gives a rather different impression.
The reference you give also results in a different answer for the second part of the OP: http://en.wikipedia.org/wiki/Nonholonomic_system#The_Foucault_Pendulum
 
  • #9
haruspex said:
The reference I found was http://en.wikipedia.org/wiki/Holonomic_constraints, which gives a rather different impression.
The reference you give also results in a different answer for the second part of the OP: http://en.wikipedia.org/wiki/Nonholonomic_system#The_Foucault_Pendulum
Your question was about the non-integrability relation to non-holonomic constraint which is clearly shown by the relation given on wiki.So far as the op question is concerned,I don't see any disagreement.I would like to know about that different impression.
 
  • #10
andrien said:
Your question was about the non-integrability relation to non-holonomic constraint which is clearly shown by the relation given on wiki.So far as the op question is concerned,I don't see any disagreement.I would like to know about that different impression.
The mention of integrability at the reference I found only says "if it's integrable then [constraints satisfying ... are holonomic]". It doesn't make integrability a requirement for holonomicity.
But maybe you can explain it to me this way: what constraint on the particle derives from the friction? The friction does not affect the set of places the bead can be at a point in time, and I don't know what other constraints one is supposed to consider.

Btw, back to the OP: the first case (wire rotating about an axis perpendicular to its plane) is clearly not time dependent.
 
  • #11
haruspex said:
The mention of integrability at the reference I found only says "if it's integrable then [constraints satisfying ... are holonomic]". It doesn't make integrability a requirement for holonomicity.
But maybe you can explain it to me this way: what constraint on the particle derives from the friction? The friction does not affect the set of places the bead can be at a point in time, and I don't know what other constraints one is supposed to consider.

Btw, back to the OP: the first case (wire rotating about an axis perpendicular to its plane) is clearly not time dependent.
Friction does not affect the situation here.But in a case,where a sphere rolls on a frictional surface.The point of contact must satisfy the zero velocity condition.With respect to which One can write the kinetic energy in terms of three euler angles θ,∅,ψ but the resulting eqn which one get by applying lagrange's eqn. will be incorrect because of non-holonomicity condition of eqn of rolling.In similar cases,one finds that when non-holonomic constraints are imposed,the number of variables used to describe eqn of motion are always greater than the numbers of degrees of freedom.Non-holonomic constraint also don't do work but they just involves a differential relation between velocities(generalised components) and generalised coordinates which can not be integrated because if they will ,then it will be possible to reduce the number of variables and system attains a holonomic state.
I do not want to continue this discussion further.
 
  • #12
andrien said:
Friction does not affect the situation here.But in a case,where a sphere rolls on a frictional surface.The point of contact must satisfy the zero velocity condition.
OK, so if it were static friction then it would be non-holonomic.
Thanks.
 

FAQ: Bead on a rotating wire - holonomic or not?

Is the bead on a rotating wire a holonomic or non-holonomic system?

The bead on a rotating wire is a holonomic system. This means that the position of the bead can be fully described by the position of its coordinates on the wire and the angle of rotation. The constraints of the system do not depend on the velocity or acceleration of the bead.

How does the bead's position change as the wire rotates?

As the wire rotates, the bead will move along the wire and also rotate around the wire. The position of the bead will depend on the angle of rotation of the wire and the initial position of the bead.

Can the bead on a rotating wire exhibit chaotic behavior?

Yes, the bead on a rotating wire can exhibit chaotic behavior. This is due to the nonlinearity of the system and its sensitivity to initial conditions. A small change in the initial position or velocity of the bead can lead to drastically different outcomes over time.

How does the radius of the wire affect the motion of the bead?

The radius of the wire affects the motion of the bead by changing the curvature of the wire and the centripetal force acting on the bead. A smaller radius will result in a tighter curve and a larger centripetal force, while a larger radius will result in a more gradual curve and a smaller centripetal force.

Can this system be used to model real-world phenomena?

Yes, the bead on a rotating wire has been used to model a variety of real-world phenomena such as the motion of a satellite orbiting the Earth and the motion of a pendulum. It can also be used to study the behavior of mechanical systems and the principles of rotational motion.

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