Derivation of Euler-Lagrange equation with change of coordinates

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Discussion Overview

The discussion revolves around the derivation of the Euler-Lagrange equation, particularly focusing on the implications of changing coordinates and the role of time in the Lagrangian formulation. Participants explore whether certain terms should be included in the equations based on the dependence of the Lagrangian on time and the coordinates.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants question why the term ##\frac{\partial L}{\partial t}\frac{\partial t}{\partial \dot{q_m}}## is not included in the Euler-Lagrange equation, suggesting that ##L## could depend on ##t## explicitly.
  • Others assert that ##t## does not depend on the coordinates and is not varied in Hamilton's principle of least action.
  • There is a discussion about the implications of a particle traveling at constant velocity, with some participants expressing confusion about whether ##t## depends on ##x## in this context.
  • Some participants propose that transformations from one set of generalized coordinates to another can depend explicitly on time, particularly in non-inertial frames, but maintain that this does not affect the variation in Hamilton's principle.
  • Concerns are raised about the form-invariance of the Euler-Lagrange equations under coordinate transformations, with references to specific equations and terms that may be omitted in proofs.
  • Participants express uncertainty about the implications of certain partial derivatives, particularly regarding the independence of ##t## and its relationship to other variables.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether the term ##\frac{\partial L}{\partial t}\frac{\partial t}{\partial \dot{q_m}}## should be included in the Euler-Lagrange equation. Multiple competing views remain regarding the dependence of ##t## on the coordinates and the implications of various transformations.

Contextual Notes

Some participants note that the relationship between partial derivatives is not straightforward and depends on the specific functions and variables involved in the transformation. There are also references to specific equations (e.g., (5.41)) that are not fully explained in the discussion.

Happiness
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Why isn't ##\frac{\partial L}{\partial t}\frac{\partial t}{\partial \dot{q_m}}## included in (5.41), given that ##L## could depend on ##t## explicitly?

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##t## does not depend on the coordinates.
 
And also ##t## is not varied in Hamilton's principle of least action.
 
Orodruin said:
##t## does not depend on the coordinates.

Suppose ##(\frac{\partial x}{\partial t})_{y,z}\neq0##. Doesn't that imply ##(\frac{\partial t}{\partial x})_{y,z}=((\frac{\partial x}{\partial t})_{y,z})^{-1}\neq0##?
 
Happiness said:
Suppose ##(\frac{\partial x}{\partial t})_{y,z}\neq0##. Doesn't that imply ##(\frac{\partial t}{\partial x})_{y,z}=((\frac{\partial x}{\partial t})_{y,z})^{-1}\neq0##?
"##t## does not depend on the coordinates" ## \Leftrightarrow (\frac{\partial x}{\partial t})_{y,z}=0##!
 
Shayan.J said:
"##t## does not depend on the coordinates" ## \Leftrightarrow (\frac{\partial x}{\partial t})_{y,z}=0##!

Suppose a particle travels at constant velocity, i.e., ##x=vt##. Then ##\frac{\partial x}{\partial t}=v\neq0##. So does ##t## depends on ##x##? I'm confused.
 
Happiness said:
Suppose a particle travels at constant velocity, i.e., ##x=vt##. Then ##\frac{\partial x}{\partial t}=v\neq0##. So does ##t## depends on ##x##? I'm confused.
You are considering a transformation taking x to q and t to t. Regardless of what transformation you have done, t only depends on t.
 
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Well, of course you can have transformations from one set of generalized coordinates to another that depends explicitly on time. That's, e.g., useful if you want to describe the motion in non-inertial frames starting from the physics in an inertial frame. Still this has nothing to do with the variation, because by definition in Hamilton's principle time is not varied.

It turns out immidiately that the Euler-Lagrange equations are forminvariant under arbitrary diffeomorphisms
$$q^{\prime k}=Q^k(q,t).$$
 
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Indeed, the new coordinates may depend explicitly on time by (5.38) below.

In that case, should ##\frac{\partial L}{\partial t}\frac{\partial t}{\partial\dot{q_m}}## be included in (5.41)?

Screen Shot 2016-07-28 at 10.38.56 pm.png
 
  • #10
Happiness said:
In that case, should ∂L∂t∂t∂˙qm∂L∂t∂t∂qm˙\frac{\partial L}{\partial t}\frac{\partial t}{\partial\dot{q_m}} be included in (5.41)?
No, t still does not depend on the coordinates.
 
  • #11
I don't know what Eq. (5.41) is, but you should get the form-invariant Euler-Lagrange equations also in the new coordinates, i.e., you have given
$$L'(q,\dot{q},t)=L[x(q,t);\dot{x}(q,t),t].$$
where
$$\dot{x}^i=\dot{q}^k \frac{\partial x^i}{\partial q^k}+\partial_t x^i.$$
In this equation the ##\partial_t x^i## means the derivative of the explicit time dependence of ##x^i(q,t)##.

Then the equations of motion in the new coordinates read
$$\frac{\partial L'}{\partial q^k}-\frac{\mathrm{d}}{\mathrm{d} t} \frac{\partial L'}{\partial \dot{q}^k}=0.$$
 
  • #12
Orodruin said:
No, t still does not depend on the coordinates.

Does that mean ##\frac{\partial t}{\partial\dot{q_m}}=0## and ##\frac{\partial t}{\partial q_m}=0##? Why?

Clearly, ##\frac{\partial q_m}{\partial t}\neq0##.
 
  • #13
vanhees71 said:
I don't know what Eq. (5.41) is, but you should get the form-invariant Euler-Lagrange equations also in the new coordinates, i.e., you have given
$$L'(q,\dot{q},t)=L[x(q,t);\dot{x}(q,t),t].$$
where
$$\dot{x}^i=\dot{q}^k \frac{\partial x^i}{\partial q^k}+\partial_t x^i.$$
In this equation the ##\partial_t x^i## means the derivative of the explicit time dependence of ##x^i(q,t)##.

Then the equations of motion in the new coordinates read
$$\frac{\partial L'}{\partial q^k}-\frac{\mathrm{d}}{\mathrm{d} t} \frac{\partial L'}{\partial \dot{q}^k}=0.$$

What you wrote is claim 5.2, where (5.41) is found. But the proof seems to omit the term ##\frac{\partial L}{\partial t}\frac{\partial t}{\partial\dot{q_m}}## in (5.41).

Screen Shot 2016-07-28 at 11.00.16 pm.png
 
  • #14
Happiness said:
Does that mean ##\frac{\partial t}{\partial\dot{q_m}}=0## and ##\frac{\partial t}{\partial q_m}=0##? Why?

Clearly, ##\frac{\partial q_m}{\partial t}\neq0##.
In general, for partial derivatives, ##\partial x^i/\partial y^j## is not equal to the reciprocal of ##\partial y^j/\partial x^i##. You need to consider what these functions actually are functions of and what variable change you are considering. In this case you are keeping t as an independent variable and its parial derivative wrt anything else is zero.
 
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  • #15
There is no such term! It doesn't even make any sense, or how do you define it?
 

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