Variance of the EM wave equation under Galilean transformation

AI Thread Summary
The discussion centers on the invariance of the electromagnetic (EM) wave equation under Galilean transformation. It begins with an attempt to demonstrate that a plane wave solution remains invariant when transforming between different reference frames. However, it is pointed out that the speed of the wave changes from c to c - v, indicating that the wave equation does not satisfy Maxwell's equations in both frames. The conversation highlights the necessity of checking whether the solutions derived from Maxwell's equations maintain their form under transformation, ultimately leading to the conclusion that Galilean transformations are inadequate for electrodynamics. The discussion underscores the transition to Lorentz transformations as a more accurate framework for understanding the behavior of light and electromagnetic waves.
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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.
 
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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.
 
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  • #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.
 
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  • #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.
 
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