The postulates of Special Relativity

Debdutta
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According to the first postulate of Special Relativity, all the laws of physics are symmetrical in all inertial frames. So that also means that Maxwell's equations are true in any such frame (experimentally verified). Now we can easily uncouple the four first-order differential equations in free space and that leads to two second order differential equations (in fact six) for the electric and magnetic fields, the wave equations, with the speed of such waves being that of light, which is precisely a constant, depending only on the permitivity and permeability of free-space. So my question is, what is the need of the second postulate if it is easily derivable from the first? It is a radical conclusion, but not an independent assumption, or is it?
 
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Einstein did not want to assume Maxwell's equations. What if they were superseded? In fact, the were superseded by QED, while special relativity survives unchanged. Another way to look at it is the axiomatic framework chosen by Einstein acts to constrain any possible future theories of physics - they must be Lorentz invariant.
 
Another reason to not assume Maxwell's equations is that this would make SR a theory of electromagnetism. It's much prettier to define it as a model of space and time that serves as a framework in which we can define theories of particles, fields and interactions, like for example classical electrodynamics (Maxwell's equations).
 
I see. Thank you PAllen and Fredrik. I got my answer.
 
OK, so this has bugged me for a while about the equivalence principle and the black hole information paradox. If black holes "evaporate" via Hawking radiation, then they cannot exist forever. So, from my external perspective, watching the person fall in, they slow down, freeze, and redshift to "nothing," but never cross the event horizon. Does the equivalence principle say my perspective is valid? If it does, is it possible that that person really never crossed the event horizon? The...
ASSUMPTIONS 1. Two identical clocks A and B in the same inertial frame are stationary relative to each other a fixed distance L apart. Time passes at the same rate for both. 2. Both clocks are able to send/receive light signals and to write/read the send/receive times into signals. 3. The speed of light is anisotropic. METHOD 1. At time t[A1] and time t[B1], clock A sends a light signal to clock B. The clock B time is unknown to A. 2. Clock B receives the signal from A at time t[B2] and...
From $$0 = \delta(g^{\alpha\mu}g_{\mu\nu}) = g^{\alpha\mu} \delta g_{\mu\nu} + g_{\mu\nu} \delta g^{\alpha\mu}$$ we have $$g^{\alpha\mu} \delta g_{\mu\nu} = -g_{\mu\nu} \delta g^{\alpha\mu} \,\, . $$ Multiply both sides by ##g_{\alpha\beta}## to get $$\delta g_{\beta\nu} = -g_{\alpha\beta} g_{\mu\nu} \delta g^{\alpha\mu} \qquad(*)$$ (This is Dirac's eq. (26.9) in "GTR".) On the other hand, the variation ##\delta g^{\alpha\mu} = \bar{g}^{\alpha\mu} - g^{\alpha\mu}## should be a tensor...
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