A weird answer -- Lagrangian mechanics

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Discussion Overview

The discussion revolves around a problem in Lagrangian mechanics involving a ball connected to a rotating vertical pole via a massless string. Participants explore the implications of the equations derived from the Lagrangian and the resulting equations of motion, particularly focusing on the behavior of the angular velocity and the angle of the string.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant presents the Lagrangian for the system and derives an equation of motion that suggests a dependency on the angle θ, leading to confusion about the expected behavior of φ.
  • Another participant suggests setting the angular velocity φ' as a constant in the Lagrangian to simplify the analysis.
  • A different participant reiterates the need to treat φ' as a constant, indicating that it is a constraint rather than a degree of freedom.
  • There is a correction from one participant regarding a previous statement about the angle θ, clarifying that they meant θ=π/2 instead of π/4.
  • Several participants emphasize the importance of enforcing the condition that φ' is constant in their calculations.

Areas of Agreement / Disagreement

Participants generally agree on the necessity of treating φ' as a constant, but there remains some confusion regarding the implications of the derived equations and the behavior of the system. The discussion does not reach a consensus on the interpretation of the results.

Contextual Notes

The discussion highlights potential limitations in understanding the constraints of the system and the assumptions made in the derivation of the equations of motion. There are unresolved aspects regarding the implications of the derived equations and their physical interpretation.

Andreas C
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Just refer to my profile picture to see what the issue is! :biggrin:

Here's the problem: a ball of mass m is connected to a vertical pole with an inextensible, massless string of length r. The angle between the string and the pole is θ. The pole rotates around the z axis with a constant angular velocity $$\dotφ$$

We can easily determine the following equations:
$$x=r*sinθ*cosφ$$ $$y=r*sinθ*sinφ$$ $$z=r(1-cosθ)$$

Now I determined that the pesky Lagrangian is equal to the following:
$$L=\frac{mr^2}{2}(\dot\theta^2+\dot\phi^2sin^2\theta)+mgr(1-cos\theta)$$

So, where's the issue? Well, solving the Euler-Lagrange equations we find this:
$$mr^2\ddot\phi sin\theta+2mr^2\dot\phi\dot\theta cos\theta sin\theta=0$$

Which means that
$$\ddot\phi=-\frac{2\dot\phi\dot\theta}{tan\theta}$$

That's a really odd result. φ' is supposed to be constant, so φ''=0. But here we can see that φ'' can only be 0 if either φ' or θ' are 0, or if θ=π/4. Weird.

Am I missing something (I obviously am, it's a rhetorical question)?
 
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You have to set
$$x=r \cos (\omega t) \sin \theta, \quad y=r \sin(\omega t) \sin \theta, \quad z=r (1-\cos \theta),$$
evaluate ##T=m \dot{\vec{x}}^2/2## and then derive the equation of motion for ##\theta## via the Euler-Lagrange equations.
 
vanhees71 said:
You have to set ##\dot{\phi}=\omega=\text{const}## in the Lagrangian. Then you can evaluate the EoM for ##\theta##.

So I don't have to solve the Euler-Lagrange equations for φ and ##\dotφ## all?
 
I've reformulated my suggestion a bit, but it's of course finally the same. If I understand your problem right, it's forced to have a rotation with constant angular velocity ##\omega=\dot{\phi}## around the ##z## axis. That's a constraint rather than a degree of freedom.
 
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vanhees71 said:
I've reformulated my suggestion a bit, but it's of course finally the same. If I understand your problem right, it's forced to have a rotation with constant angular velocity ##\omega=\dot{\phi}## around the ##z## axis. That's a constraint rather than a degree of freedom.

Ah ok! Thanks!
 
Oh whoops, in my original post I meant "if θ was π/2", not π/4.
 
As I said, you must enforce that ##\dot{\phi}=\text{const}##!
 
vanhees71 said:
As I said, you must enforce that ##\dot{\phi}=\text{const}##!

Yeah, yeah, I did that, and I got a result that makes sense. I was just saying...
 

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