A weird answer -- Lagrangian mechanics

AI Thread Summary
The discussion centers on a problem involving a ball connected to a rotating pole via a string, analyzed using Lagrangian mechanics. The derived Lagrangian leads to an unexpected equation of motion for the angle φ, suggesting that φ' should be constant, yet the solution indicates that φ'' can only be zero under specific conditions. Participants clarify that the constant angular velocity of the pole introduces a constraint rather than an additional degree of freedom. The conversation emphasizes the necessity of enforcing the constant angular velocity in the Lagrangian formulation. Ultimately, the issue is resolved by correctly applying the constraints in the equations of motion.
Andreas C
Messages
196
Reaction score
20
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)?
 
Physics news on Phys.org
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.
 
  • Like
Likes Andreas C
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...
 
Back
Top