Question on Lagrangian Mechanics

AI Thread Summary
The discussion centers on the flexibility in choosing the Lagrangian for a mechanical system, including the ability to scale time by a constant factor. It highlights that while the Lagrangian can be transformed, such as multiplying by a constant, the equations of motion must remain consistent under these transformations. A key point raised is that if the Lagrangian does not explicitly depend on time, it remains invariant under time translations, which relates to energy conservation. However, scaling time requires adjustments to other parameters, such as the spring constant, to maintain dimensional consistency. Ultimately, the conversation emphasizes the importance of correctly applying transformations to ensure valid physical interpretations.
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:
L = \frac{1}{2}m\dot{q}^2 - kqt

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

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

The E-L equation is
m\ddot{q} + c^3kt = 0
 
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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
 
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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 L = T - V example, it doesn't make any sense that V became bigger but T became way smaller (assuming c > 1) when you changed the time scale. They should stay at the same ratio.

OK, I think I know what the problem is. I think k 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 k, by dividing it by c^3. Then everything has c^2 on the bottom and everyone's happy again. Does that sound right?
 
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Okay.It doesn't really matter.Rescaling

t'=:ct

(adimensional constant,dfan!).

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

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

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

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.
 
I have recently been really interested in the derivation of Hamiltons Principle. On my research I found that with the term ##m \cdot \frac{d}{dt} (\frac{dr}{dt} \cdot \delta r) = 0## (1) one may derivate ##\delta \int (T - V) dt = 0## (2). The derivation itself I understood quiet good, but what I don't understand is where the equation (1) came from, because in my research it was just given and not derived from anywhere. Does anybody know where (1) comes from or why from it the...

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