strangerep said:
Er,... was that a typo? Did you mean "..
.there are no preferred inertial reference frames..." ?
BTW, I'm glad that someone mentioned this approach -- i.e., that the light principle is not essential as an axiom. I was going to mention it, but I suspect others are sick of hearing me say that.
Perhaps, "preferred" is a somewhat unfortunate word for what I wanted to express, but off course, the notion of inertial frames separates out these frames from any "accelerated" frame of reference.
What I like about this approach is that it shows that SRT makes very strong assumptions on the symmetry properties of the space-time structure and thus you have a very limited choice of space-times, namely only the Galilei-Newton and the Einstein-Minkowski spacetime. At the same time, it takes out this mentioned postulate about the speed of light being the universal "limiting speed". At the present state of our understanding this is rather an empirical question than a fundamental principle of nature, i.e., whether the photon is massless or not is to be decided by experiment (and as I said before, there's nothing yet indicating that the photon might have a tiny mass). From a didactic point of view the advantage of this more general approach is that it shows that the possible existence of a limiting speed is a general property of the space-time description and not limited to electromagnetic phenomena. To the dismay of the HEP community, who'd like to find some physics beyond the Standard Model, we know pretty well today that the SRT space-time structure is the basis for the entire Standard Model of elementary particles, which is much more comprehensive than just electromagnetic interactions.
However, the principle of the special status of inertial frames is inherited also by GRT, where you just loosen the demand of the existence of a global inertial frame and make it to a local concept, which is the concrete mathematical formulation of the (weak) equivalence principle: The space-time is described as a pseudo-Riemannian manifold with a pseudo-metric (fundamental form) of signature (1,3) (or (3,1) if you prefer the east-coast convention), which implies that you have a torsion free affine connection compatible with the pseudo-metric and local inertial frames (i.e., the tangent space at each space-time point is Minkowskian, modulo possible singularities).
Of course, you can then also specify additional symmetry properties for given physical situations, like admitting a spherical symmetry for a radially symmetric body/point particle (Schwarzschild, Reissner-Nordström) or a maximally symmetric space (FLRW solutions for the large-scale coarse-grained description of the universe in the standard model of cosmology).