I Derivation of Euler-Lagrange equation with change of coordinates

AI Thread Summary
The discussion centers on the inclusion of the term ##\frac{\partial L}{\partial t}\frac{\partial t}{\partial \dot{q_m}}## in the Euler-Lagrange equation, questioning its necessity given that time ##t## does not depend on the coordinates. Participants clarify that while transformations can introduce time dependence in coordinates, time itself remains independent in Hamilton's principle of least action. The conversation highlights that the Euler-Lagrange equations are form-invariant under arbitrary diffeomorphisms, reinforcing that the term in question does not apply. It is emphasized that the partial derivatives involving time and coordinates must consider their independence, leading to the conclusion that the term is not relevant in this context. The discussion ultimately confirms that the structure of the equations does not require the inclusion of the debated term.
Happiness
Messages
686
Reaction score
30
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?

image.png
 
Last edited:
Physics news on Phys.org
##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.
 
  • Like
Likes Happiness
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
$$q^{\prime k}=Q^k(q,t).$$
 
  • Like
Likes Happiness
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.
 
  • Like
Likes Happiness
  • #15
There is no such term! It doesn't even make any sense, or how do you define it?
 
Back
Top