Noether's Theorem: Julien's Calculation Mistake?

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Discussion Overview

The discussion revolves around Noether's theorem, specifically focusing on the calculation of variations in symmetry and the potential mistakes in a teacher's script regarding the definitions of these variations. Participants explore the implications of different definitions and their effects on calculations related to symmetry variations.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Julien presents a calculation based on a teacher's script regarding the variation of symmetry in Noether's theorem, questioning the accuracy of the script.
  • Some participants note that the definitions of ##\Delta q_a## and ##\delta q_a## in the script appear incompatible or require clarification.
  • Julien suggests that the teacher may have made a mistake and proposes a potential correction regarding the definitions of the variations.
  • Another participant points out that the definitions used by Julien differ from those implied in the teacher's script, which may lead to confusion in the calculations.
  • Julien revises his calculations based on feedback, leading to a realization about the definitions and their implications for the results.

Areas of Agreement / Disagreement

Participants express differing interpretations of the definitions of the variations in the context of Noether's theorem. There is no consensus on the correctness of the teacher's script, and the discussion remains unresolved regarding the implications of these definitions on Julien's calculations.

Contextual Notes

Participants highlight that the definitions of ##\Delta q## and ##\delta q## are crucial for the calculations, and the ambiguity in the teacher's script may lead to different interpretations and results. The discussion reflects the complexity of the topic and the need for clarity in definitions.

JulienB
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Hi everybody! I'm currently studying Noether's theorem, but I'm a bit stuck around a stupid line of calculation for the variation of the symmetry. The script of my teacher says (roughly translated from German, equations left as he wrote them):

"V.2. Noether Theorem

How does the action change under arbitrary variations of the path and of the time?

##t' = t + \tau (t)##; ##q_a ' (t') = q_a (t) + \Delta q_a (t)##

where ##\tau## and ##\Delta q_a## are arbitrary functions, which must not be equal zero at the boundaries. For the variation of ##q_a## by a fixed time ##q_a ' (t') = q_a (t) + \delta q_a (t)##, we find a relation between the variations ##\delta q_a## and ##\Delta q_a##:

##q_a ' (t') = q_a ' (t + \tau (t) = q_a ' (t) + \tau (t) \dot{q}_a (t)##
##= q_a (t) + \delta q_a (t) + \tau (t) \dot{q}_a (t)##
##\overset{!}{=} q_a (t) + \Delta q_a (t)##
##\implies \delta q_a (t) = \Delta q_a (t) - \tau (t) \dot{q}_a (t)##"

However, here is what I got when trying to repeat his steps:

##\delta q (t) = q ' (t') - q (t)##
##= q' (t + \tau (t)) - q(t) = q'(t) + \tau (t) \dot{q} ' (t) - q(t)##
##= q(t) + \Delta q(t) + \tau (t) \dot{q} ' (t) - q(t)##
##= \Delta q(t) + \tau (t) \dot{q} ' (t)##

That's close but not quite the same. He (very!) often makes little mistakes in his script, so I wondered if that was one of them. If not, I would be very grateful if someone could explain me when I went wrong :)Thank you very much in advance for your answers.Julien.
 
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JulienB said:
##q_a ' (t') = q_a (t) + \Delta q_a (t)##
##q_a ' (t') = q_a (t) + \delta q_a (t)##
These two definitions are incompatible (or equivalent - meaning ##\Delta q_a = \delta q_a## by definition). I assume that you intend for one to have ##q_a'(t)## on the LHS (or ##t'## instead of ##t## on the RHS). Without knowing which is which, it will be difficult to help you.
 
Hi @Orodruin and thank you for your answer. Those definitions unfortunately come straight out of my teacher's script... I would assume that my teacher made a mistake and -without much certainty- that ##q_a ' (t) = q_a (t) + \Delta q_a (t)## (then it would be the definition of a translation) and that ##\delta q_a (t) = q_a ' (t') - q_a(t)## (the symmetry variation). Does that seem correct to you? Unfortunately, I already used the known definitions of translation and time translation in my calculations, and I got a ##+## instead of a ##-##.

Thanks a lot in advance.Julien.
 
JulienB said:
Hi @Orodruin and thank you for your answer. Those definitions unfortunately come straight out of my teacher's script... I would assume that my teacher made a mistake and -without much certainty- that ##q_a ' (t) = q_a (t) + \Delta q_a (t)## (then it would be the definition of a translation) and that ##\delta q_a (t) = q_a ' (t') - q_a(t)## (the symmetry variation). Does that seem correct to you? Unfortunately, I already used the known definitions of translation and time translation in my calculations, and I got a ##+## instead of a ##-##.
Well, then the result depends on which of the ##\Delta q## and ##\delta q## you change the definition for.
 
I mean, judging from your teacher's script, he has ##q'(t) = q(t) + \delta q## and ##q'(t') = q(t) + \Delta q##. This also rhymes with the statement that ##\delta q## is the fixed time variation. You are using the opposite definition.
 
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@Orodruin In my teacher's script, both definitions are written as ##q' (t')##... Okay, I rewrite my whole development following your advice:

We consider the following transformation:
##t' = t + \tau (t)##, ##q' (t) = q(t) + \delta q(t)##

We want to know what is the symmetry variation, defined as:
##\Delta q = q' (t') - q(t)##
(transformed coordinate - original coordinate)

So:

##\Delta q = q' (t + \tau) - q(t)##
##= q'(t) + \tau \cdot \dot{q} ' (t) - q(t)##
##= q(t) + \delta q(t) + \tau (t) \dot{q} (t) - q(t)##
##= \delta q(t) + \tau (t) \dot{q} (t)##

##\implies \delta q(t) = \Delta q(t) - \tau (t) \dot{q} (t)##

Indeed, that works now.. Raah sorry for that, I get it now.Thanks for your help!Julien.
 
JulienB said:
In my teacher's script, both definitions are written as q' (t')...
Yes, but the text itself "For the variation of qa by a fixed time" and the way he is using it in the equations suggests the definition in my previous post is what is intended.
 
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