quantumdude
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Tom Mattson said:Neither one of you understands how light propagates[/color].
And this is what I mean by that:
In any course in classical EM, we obtain the following equation that describes the propagaition of light:
From Maxwell's Equations to the EM Wave Equation:
Using the boldface ∂ for the "del" operator, Maxwell's equations in vacuo are:
∂xE+(1/c)∂E/∂t...(1)
∂xB-(1/c)∂E/∂t...(2)
∂.E=0...(3)
∂.B=0...(4)
Making use of the vector identity:
∂x∂xA=∂(∂.A)-∂2A,
We can take the curl of equation (1) to obtain:
∂x∂xE+(1/c)(∂/∂t)∂xB=0
∂(∂.E[/color])-∂2E+(1/c)(∂/∂t)∂xB[/color]=0
The part in blue[/color] vanishes by virtue of equation (3), and the part in red[/color] can be rewritten as -(1/c)∂E/∂t, by virtue of equation (2).
This gives us:
∂2E-(1/c2)∂2E/∂t2=0,
which is a wave equation. Taking the curl of equation (2) and following a similar path will show you that B satisfies the exact same wave equation.
We know this is a wave equation because, when we solve it, we get...
Solutions of the EM Wave Equation:
The components of the plane wave solutions of the wave equation are of the form:
Ai(x,t)=Ai0sin(k.x-wt+f)
where w/|k|=c. Since the solutions have constant phase, we can derive the speed of the waves to be c.
Now, if we assume that Galilean relativity is right, and all those effects predicted by SR don't really exist (despite the fact that they've been confirmed experimentally many, many times), we get:
Why Galileo and Maxwell Can't Both Be Right:
If electrodynamics is to be reformulated so that it is Galilean invariant, then the resulting equations will not be Maxwell's equations.
Here's what the reference from Jackson has to say about it. First, assume Galilean relativity. For a moving frame S' and a stationary frame S, we have:
x'=x-vt
t'=t
Let the wave equation hold in frame S. What does it look like in S'? We can derive that as follows:
∂/∂x=(∂x'/∂x)∂/∂x'=∂/∂x'
∂/∂y=(∂y'/∂y)∂/∂y'=∂/∂y'
∂/∂z=(∂z'/∂z)∂/∂z'=∂/∂z'
∂/∂t=(∂x'/∂/t)(∂/∂x')+(∂y'/∂t)(∂/∂y')+(∂z'/∂t)(∂/∂z')+(∂t'/∂t)(∂/∂t')
∂/∂t=v.∂'-(1/c)∂/∂t'
Squaring each operator and writing the equation in the coordinates of S' yields:
(∂'2-(1/c2)(∂2/∂t'2-(2/c2)v.∂'(∂/∂t')-(1/c2)(v.∂)2)Ai=0
where Ai is any component of either the E or B field.
Notice that the above equation is not a wave equation[/color]. That means that, if Galilean relativity is correct, then radio waves emitted from towers should become non-waves when you are driving in your car.
If Galilean relativity is correct, then you should not be able to listen to the radio in your car.[/color]
Why the Correctness of Maxwell Implies the Correctness of Einstein:
The Lorentz transformation, on the other hand, does preserve the form of the EM wave equation.
SR predicts the everyday observation that EM waves are EM waves in every frame. Galilean relativity, on the other hand, fails miserably here.
And to Wrap Up:
This is what none of the preachers of the Anti Relativity Religion understand. Einstein did not pull length contraction and time dilation out of thin air. They are logically derived consequences of the requirement that the EM wave equation and the speed of light be the same in every frame. The original paper was not even called, "Intro to Special Relativity", it was called, "On the Electrodynamics of Moving Bodies".
Like it or not folks, relativity is correct. If any of you wants to convince thinking persons otherwise, then you will have to argue on these terms, because these are the terms in which relativity was formulated.
Now, who can argue with that post on its merits?