Question on Lagrangian Mechanics

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Discussion Overview

The discussion revolves around the properties of the Lagrangian in mechanics, particularly focusing on the implications of changing the time scale by a constant factor. Participants explore the validity of such transformations and their effects on the equations of motion derived from the Lagrangian.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant asserts that various transformations, including changing the time scale, can yield a satisfactory Lagrangian for describing motion.
  • Another participant questions the validity of changing the time scale, providing an example where the equations of motion appear to change inconsistently with the original Lagrangian.
  • A third participant clarifies that the invariance of the Lagrangian under time transformations applies only when the Lagrangian does not depend explicitly on time, which is not the case in the initial example.
  • Further discussion highlights that scaling the time should not affect the ratio of kinetic and potential energy, suggesting that the constant \( k \) in the potential energy term may need to be adjusted to maintain dimensional consistency.
  • Another participant proposes that a time rescaling does not modify the Lagrange equations, asserting that the equations of motion remain the same under such transformations.

Areas of Agreement / Disagreement

Participants express differing views on the implications of changing the time scale in the Lagrangian. There is no consensus on the correctness of the initial example or the necessary adjustments to maintain consistency in the equations of motion.

Contextual Notes

Participants note limitations regarding the dependence of the Lagrangian on time and the need for careful consideration of units when scaling parameters. The discussion remains open to interpretation and further exploration of the implications of time rescaling.

kakarukeys
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"There is some freedom as to what we choose for the Lagrangian in a given problem: We can add a constant, multiply by a constant, change the time scale by a multiplicative constant, or add the total time derivative ... Any of these transformations will lead to a Lagrangian that is perfectly satisfactory for describing the motion."

I could not verify the 3rd one. Why is it possible to change the time scale by a constant factor?

For example:
[tex]L = \frac{1}{2}m\dot{q}^2 - kqt[/tex]

The E-L equation is
[tex]m\ddot{q} + kt = 0[/tex]

If we modify the Lagrangian, multiplying all time by constant c
[tex]L = \frac{1}{2c^2}m\dot{q}^2 - ckqt[/tex]

The E-L equation is
[tex]m\ddot{q} + c^3kt = 0[/tex]
 
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http://www.physik.fu-berlin.de/~kleinert/b6/psfiles/conslaw.pdf

I refer to section 6.2 on page 4 of the above link.

If the Lagrangian does NOT depend on time explicitely (which is NOT the case in your example), then this L will be invariant under time-transformations t-->t + e where e is a given constant. This symmetry yields the energy conservation law.

marlon
 
Last edited by a moderator:
marlon said:
http://www.physik.fu-berlin.de/~kleinert/b6/psfiles/conslaw.pdf

If the Lagrangian does NOT depend on time explicitly (which is NOT the case in your example), then this L will be invariant under time-transformations t-->t + e where e is a given constant. This symmetry yields the energy conservation law.

Yeah, but that's translating time, and the excerpt he quoted was about scaling time.

Something's not quite right in kakarukeys' example, but I can't put my finger on it. Certainly it shouldn't matter whether you measure time in seconds or milliseconds. And in your [itex]L = T - V[/itex] example, it doesn't make any sense that [itex]V[/itex] became bigger but [itex]T[/itex] became way smaller (assuming [itex]c > 1[/itex]) when you changed the time scale. They should stay at the same ratio.

OK, I think I know what the problem is. I think [itex]k[/itex] needs to be in units of mass * length / time^3 for the units to come out right. So when you did your scaling, you also needed to scale [itex]k[/itex], by dividing it by [itex]c^3[/itex]. Then everything has [itex]c^2[/itex] on the bottom and everyone's happy again. Does that sound right?
 
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Okay.It doesn't really matter.Rescaling

[tex]t'=:ct[/tex]

(adimensional constant,dfan!).

[tex]L\left(q,\frac{dq}{dt'},t'\right)=\frac{m}{2}\left(\frac{dq}{dt'}\right)^{2}-kqt'[/tex]

It can be easily proven that a time rescaling doesn't modify the Lagrange equation(s),so it looks (for this 1D-case)

[tex]\frac{\partial L}{\partial q}-\frac{d}{dt'}\left(\frac{\partial L}{\partial \left(\frac{dq}{dt'}\right)}\right) =0[/tex]

and so,in the rescaled variables,the equation of motion is the same...

We all know that time inversion is a weird (for relativistic systems,classical & quantum fields) example of a time-rescaling.

Daniel.
 

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