DrGreg said:
Yes, they do. But who said Maxwell's equations were one of the postulates of relativity?
Let me guess you might answer this by saying that Maxwell's equations are one of the "laws of physics" covered by the 1st postulate. To my way of thinking, that doesn't really cover it. The 1st postulate doesn't actually explicitly identify which laws of physics it applies to. Just "all of them", whatever they turn out to be.
no, just the valid ones. what relativity does is orthogonal to the other physical law. it just says that the expressions of that other physical law must apply identically to every inertial frame of reference. no qualitative
or quantitative difference. since one of these "other physics" is EM, then two different observers observing the identical beam of light, will both observe the very same changing
E field causing this other changing
B field which itself is causing this other changing
E field, etc. both observers of the same phenomena using the same Maxwell's equations to describe it, will both see the same wave advance at the same speed, having identical \epsilon_0 and \mu_0 in those Maxwell's equations.
But the 2nd postulate is explicitly necessary for relativity to work, an intrinsic part of the theory itself, and therefore ought to be explicitly identified, albeit in the watered-down version I suggested.
it's follows from the first and the other laws of physics. there is nothing about relativity that isn't conformed to the
Correspondence principle. Newton's 2
nd law works both ways if it's expressed as dp/dt.
it turns out that the magnetic action, expressed as a fundamental law in classical physics, can be expressed as a consequence of the sole electrostatic action, but with the effects of special relativity accounted for. the inverse-square law of gravitation (in fact an entire set of corresponding Maxwell-like GEM equations) can be derived from the GR equation. SR can do away with the necessity of the equations of magnetism (essentially leaving just one action) and GR gets rid of Newton's law of gravitation.
relativity doesn't eliminate all other laws of physics. but it does help us understand that some of the old Laws are approximations to the new Laws for speeds much less that
c and for reasonably flat space-time (i don't know how to quantitatively express it).
I've never thought about this much, but I imagine it might be possible to invent some fictitious laws of physics for a hypothetical universe that are incompatible with Maxwell's equations but still fully compatible with the postulates of relativity, and with each other.
it doesn't matter. if some other expression of what happens to charged particles ends up obsoleting Maxwell's equations, it would be those laws of physics that would be subject to the postulates of physics.
By the way, there was a heated exchange on this very subject on the talk page of Wikipedia's article on special relativity. See
here[/color].

no one is saying that Maxwell's equations are the specific physics that fall under the postulates of relativity but that Maxwell's equations are
in the set of what is covered under the postulates of relativity. i guess some of them become unnecessary. but if they didn't become unnecessary, they're still physical law that is expressed within the context of relativity.