Variance of the EM wave equation under Galilean transformation

Click For Summary

Discussion Overview

The discussion revolves around the invariance of the electromagnetic (EM) wave equation under Galilean transformations. Participants explore the implications of applying Galilean transformations to plane waves and whether these transformations maintain the validity of Maxwell's equations in different reference frames. The conversation touches on theoretical aspects, mathematical reasoning, and the foundational principles of electrodynamics.

Discussion Character

  • Debate/contested
  • Mathematical reasoning
  • Technical explanation

Main Points Raised

  • One participant suggests writing down a simple plane wave and applying the Galilean transformation to check if it satisfies Maxwell's equations in vacuum, assuming the speed of light is constant in the ether frame.
  • Another participant argues that the EM wave equation is not invariant under Galilean transformation because the speed of the wave changes from ##c## to ##c - v##.
  • Concerns are raised about the assumption that the wavenumber ##k## remains unchanged during the transformation, with some participants questioning the justification of this assumption.
  • It is proposed that the frequency of an EM wave depends on the source, leading to the conclusion that while frequency remains the same in both frames, the wavenumber does not.
  • One participant posits that if the plane wave solution is shown to be invariant, then by the superposition principle, all solutions of the EM wave equation would also be invariant under Galilean transformation.
  • Another participant emphasizes that the critical question is whether the transformed fields satisfy Maxwell's equations in both reference frames.
  • Clarifications are made regarding whether the discussion pertains to Maxwell's equations of electrodynamics or the wave equation derived from them.
  • It is noted that the wave equation derived from Maxwell's equations is not satisfied by waves moving at speeds other than ##c##.
  • A participant highlights the challenge of defining Galilean transformations in a way that preserves the form of Maxwell's equations, suggesting that this difficulty led to the development of Lorentz transformations.

Areas of Agreement / Disagreement

Participants express disagreement regarding the invariance of the EM wave equation under Galilean transformations, with some asserting it is invariant while others contend it is not. The discussion remains unresolved as multiple competing views are presented.

Contextual Notes

Participants acknowledge the complexity of the assumptions involved in applying Galilean transformations to electromagnetic theory, including the treatment of wave speed, frequency, and wavenumber. There is also a recognition of the limitations of Galilean transformations in accurately describing electromagnetic phenomena.

Pushoam
Messages
961
Reaction score
53
Two very similar threads were merged. Some posts may seem redundant
Dale said:
Why don't you try it out yourself. Write down a simple plane wave. Confirm that it satisfies all of Maxwell's equations in vacuum. Use the Galilean transformation. Check if it still satisfies Maxwell's equations in vacuum.
For using Galilean transformation, I have to assume that speed of light w.r.t. ether frame is c.
W.r.t. ether frame,
E = E0 eik(x-ct)

W.r.t. S' frame which is moving with speed v along the direction of propagation of light,
E' = E0 eik(x'-c't')
Under Galilean transformation,
x' = x-vt,
t' = t,
c' = c -v
So, (x'-c't') = x -ct
thus, E' = E
i.e. under the Galilean transformation, em wave equation is invariant.

Is this correct?
I am asking it here instead of creating a new thread, because I think the topic is similar.
If it is not allowed, sorry for it.
 
Physics news on Phys.org
Pushoam said:
under the Galilean transformation, em wave equation is invariant

No, it isn't, because the speed of the wave changes. You go from a wave moving at speed ##c## to a wave moving at speed ##c - v##.

(You are also assuming that the wavenumber ##k## does not change. I'm not sure that assumption is justified.)
 
PeterDonis said:
You go from a wave moving at speed cc to a wave moving at speed c−vc - v.
Then, x also changes from x to x - vt. And the two changes get canceled in the wave equation.
PeterDonis said:
You are also assuming that the wavenumber kk does not change. I'm not sure that assumption is justified.)
Assuming that the frequency of an em wave depends on the source generating em wave.
So, the frequency will remain same w.r.t. both reference frames.
Then, ω=ω',
k ≠k'.
k = ω/c,
k' = ω/(c -v)
E = E0ei(kx-ωt) = E0eiω(x/c - t)
E' = E'0eiω((x-vt)/(c -v) - t)
E' ≠ E
Is this correct?
,
 
Any em wave could be written as a combination of plane waves.
So, if I show the plane wave solution of em wave equation to be variant under Galilean transformation and then using superposition principle, I can say that any solution of em wave equation is variant under Galilean transformation.
Will this be a proof of variance of em wave equation under Galilean transformation?For using Galilean transformation, I have to assume that speed of light w.r.t. ether frame is c.
W.r.t. ether frame,
E = E0 eik(x-ct)

W.r.t. S' frame which is moving with speed v along the direction of propagation of light,
E' = E0 eik'(x'-c't')

Under Galilean transformation,
x' = x-vt,
t' = t,
c' = c -v
So, (x'-c't') = x -ct

Assuming that the frequency of an em wave depends on the source generating em wave.
So, the frequency will remain same w.r.t. both reference frames.
Then, ω=ω',
k ≠k'.
k = ω/c,
k' = ω/(c -v)
E = E0 eiω(x/c - t)
E' = E'0 eiω((x-vt)/(c -v) - t)
E' ≠ E
Is this correct?
 
The question isn't if E' is different from E. The question is if it satisfies Maxwell's equations in both frames.
 
Dale said:
The question is if it satisfies Maxwell's equations in both frames.
Do you mean that I have to check whether E satisfies Maxwell's equations(or Maxwell's wave equations ?) in ether frame and E' satisfies Maxwell's equations in S' frame?
They have to (as I have taken them as solutions of Maxwell's wave equations in their respective frames).
 
Dale said:
The question is whether or not it still satisfies Maxwell's equations.
When you say Maxwell's equations, you mean Maxwell's equations of electrodynamics or Maxwell's wave equation?
 
Pushoam said:
Maxwell's equations of electrodynamics
This one. When I say "Maxwell's equations" that is always what I mean.
 
Last edited:
  • #10
Pushoam said:
When you say Maxwell's equations, you mean Maxwell's equations of electrodynamics or Maxwell's wave equation?
Both. The wave equation is derived from the electrodynamic ones. That's why we say that a plane wave moving with speed c is a solution of Maxwell's equations and a plane wave moving at any other speed is not.

The wave equation, from Maxwell's equations, is ##(c^2\frac{\partial^2}{\partial{x}^2}-\frac{\partial^2}{\partial{t}^2})E=0##.

##E=E_0e^{ik(x-ct)}## is a solution to that equation. ##E=E_0e^{ik(x-c't)}## where ##c'=c-v## is not.
 
  • Like
Likes   Reactions: Pushoam
  • #11
The problem is to define (!) Galileo transformations on the quantities in Maxwell's equations such that these equations stay form-invariant. That turns out to be impossible, and that's how Einstein found the modern interpretation of Lorentz transformations, i.e., that observations clearly show that the Galilei-Newton spacetime is inaccurate and Einstein-Minkoski spacetime is a much better approximation, which is only invalidated by gravity, which needs General Relativity with its completely changed view of spacetime as a dynamical entity.
 

Similar threads

  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 18 ·
Replies
18
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 146 ·
5
Replies
146
Views
12K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
3
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K