Simplifying Equations of Motion for a Bead Sliding on a Parabolic Wire

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Discussion Overview

The discussion revolves around deriving the Lagrangian for a bead sliding down a frictionless parabolic wire described by the equation y=ax^2. Participants explore how to express the Lagrangian in terms of the variable x alone, considering the constraint imposed by the parabolic shape, and seek to simplify the equations of motion for small oscillations.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant seeks to derive the Lagrangian L=1/2m(x')^2(1 + 4a^2x^2) - mgax^2 from the initial form L=1/2m(x')^2 + 1/2m(y')^2 - mgy.
  • Another participant identifies the constraint as y=ax^2, suggesting substitution to simplify the Lagrangian.
  • A participant questions how the term 1/2m(x')^2 * 4ax^2 arises, indicating confusion about the inclusion of x' in that term.
  • One participant challenges the correctness of the derivative y'=2ax, implying a potential misunderstanding.
  • A later reply corrects the derivative, stating that the correct form is y' = 2ax dx/dt = 2ax x', emphasizing the use of the chain rule.

Areas of Agreement / Disagreement

Participants express differing views on the correctness of the derivative and the derivation of terms in the Lagrangian. There is no consensus on the simplification process or the interpretation of the constraint force.

Contextual Notes

Participants have not fully resolved the implications of the constraint or the mathematical steps involved in deriving the Lagrangian. The discussion reflects uncertainty regarding the treatment of derivatives in the context of the problem.

Ed Quanta
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So a bead slides down a frictionless parabolic wire of shape y=ax^2. I have to express the Lagrangian in terms of x and y. Then I have to use the constraint equation to express this solely in terms of x. Then I have to find the equations of motion, and simplify them for small oscillations.

How do I get from

L=1/2m(x')^2 + 1/2m(y')^2 - mgy

to

L=1/2m(x')^2(1 + 4a^2x^2) -mgax^2 ?

And in this specific example I am having trouble seeing what the constraint force or constraint potential is. It seems to that we know that the force of gravity is present and acting in the negative y direction, and we are told there is no force of friction, so what is the constraint?
 
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You have two degrees of freedom, x and y, and one constraint, so you are left with one degree of freedom. Your bead has to roll on a parabola with equation y=ax^2, so (surprise, surprise), the constraint is y=ax^2. Simply substitute y and you'll get the correct lagrangrian.
 
Yes, but since y'=2ax, how do you come up with the term 1/2m(x')^2 *4ax^2? In other words, how does a term of x' end up in there? And I am not talking about the term 1/2m(x')^2 *1 which is also present in the Lagrangian.
 
since y'=2ax

I don't think that's true...
 
Originally posted by Ed Quanta
Yes, but since y'=2ax, how do you come up with the term 1/2m(x')^2 *4ax^2? In other words, how does a term of x' end up in there? And I am not talking about the term 1/2m(x')^2 *1 which is also present in the Lagrangian.

You've made an error in taking the derivative. Yo didn't take the derivative with respect to time, you took the derivative with respect to x. The correct derivative is obtained using the chaing rule. The result is

y' = dy/dt = 2ax dx/dt = 2ax x'
 
Stupid stupid me
 

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