Lagrange equations of a spinning parabola

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SUMMARY

The discussion focuses on deriving the Lagrangian for a bead of mass m sliding on a parabolic wire, defined by the equation z = kρ², while rotating with a constant angular velocity ω. Participants emphasize the importance of using cylindrical polar coordinates and correctly identifying the kinetic and potential energy terms in the Lagrangian, specifically noting that the potential energy should be expressed as mgz. The correct approach involves expressing the coordinates x(t), y(t), and z(t) in terms of the generalized coordinate ρ and differentiating them to find the velocity.

PREREQUISITES
  • Cylindrical polar coordinates
  • Lagrangian mechanics
  • Basic calculus and differentiation
  • Understanding of kinetic and potential energy in classical mechanics
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  • Study the derivation of the Lagrangian in cylindrical coordinates
  • Learn about the equations of motion derived from the Lagrangian
  • Explore examples of Lagrangian mechanics applied to rotating systems
  • Investigate the implications of potential energy in different coordinate systems
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Students and educators in classical mechanics, particularly those studying Lagrangian dynamics and rotational motion, will benefit from this discussion.

tehdiddulator
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Homework Statement



Consider a bead of mass m sliding without friction on a wire that is bent in the shape of a parabola and is being spun with constant angular velocity ω about its vertical axis. Use cylindrical polar coordinates and let the equation of the parabola be ##z = kρ^{2}##. Write down the lagrangian in terms of ρ as the generalized coordinate. Find the equation of motion.

Homework Equations



$$L = T-U = \frac{1}{2}mv^2-mgy$$

The Attempt at a Solution



I just need a hint on how to set up the kinetic energy of the parabola, maybe someone can explain it in a different way that would push me in the right direction.

Also, sorry if this isn't considered advanced physics. This is a classical mechanics class (upper level at my school) and it seems like a gray area for me.
Thanks!
 
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you need to change your coordinates to suit the problem better
 
tehdiddulator said:

Homework Statement



Consider a bead of mass m sliding without friction on a wire that is bent in the shape of a parabola and is being spun with constant angular velocity ω about its vertical axis. Use cylindrical polar coordinates and let the equation of the parabola be ##z = kρ^{2}##. Write down the lagrangian in terms of ρ as the generalized coordinate. Find the equation of motion.

Homework Equations



$$L = T-U = \frac{1}{2}mv^2-mgy$$

The Attempt at a Solution



I just need a hint on how to set up the kinetic energy of the parabola, maybe someone can explain it in a different way that would push me in the right direction.
A straightforward method is to write down expressions for x(t), y(t), and z(t) and then differentiate them with respect to time. For example, ##x(t) = \rho\cos \phi##, so
$$\dot{x}(t) = \dot{\rho}\cos \phi - \rho\sin\phi \,\dot{\phi}.$$ When you have all three, plug them into ##v^2 = \dot{x}(t)^2 + \dot{y}(t)^2 + \dot{z}(t)^2##.

By the way, I think the potential term in the Lagrangian should be mgz, not mgy.

Also, sorry if this isn't considered advanced physics. This is a classical mechanics class (upper level at my school) and it seems like a gray area for me.
Thanks!
It's in the right place.
 
Ah, I suppose I should add in the major fact that they want it in terms of the generalized coordinate rho. I can try and find/make a picture of the graph if it helps.

and yes, you are correct, the potential would be mgz.
 
The expression you end up with will be in terms of ##\rho##.
 
Everything worked out properly! Thanks a bunch for your help.
 

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