According to SR (but not GR) it is everywhere the same constant relative to all points in space as defined with a Newtonian reference system ("inertial frame"). Thus, probably I did not understand what you meant (and I still don't!).
I don't know what you mean with that; Lorentz did not really work with "postulates" but developed theories based on physical models and the results of experiments.
However, as Lorentz came to prefer Einstein's derivation over his own (which indeed was much more complicated), perhaps it's useful to highlight how they they fit together, although Lorentz might phrase a few sentences a little different from Einstein. For the subtlety of the difference is, if I see it correctly, what you are missing.
So, please take Einstein's 1905 derivation and I'll show you how easy it is to switch between Lorentz and Einstein. The following translation is quite OK:
http://www.fourmilab.ch/etexts/einstein/specrel/www/
To make his derivation perfectly "Lorentz compatible", only a few sentences need slight modification (
in italics) as follows:
Examples of this sort, together with the unsuccessful attempts to discover any motion of the Earth relatively to the “light medium,” suggest that the phenomena of electrodynamics as well as of mechanics possesses no properties
that permit the detection of absolute velocity. They suggest rather that, as has already been shown to the first order of small quantities, the same laws of electrodynamics and optics will be valid for all frames of reference for which the equations of mechanics hold good. We will raise this conjecture (the purport of which will hereafter be called the “Principle of Relativity”) to the status of a postulate, and also introduce another postulate, which is only apparently irreconcilable with the former, namely, that light is always propagated in empty space with a definite velocity c which is independent of the state of motion of the emitting body. These two postulates suffice for the attainment of a simple and consistent theory of the electrodynamics of moving bodies based on Maxwell's theory for stationary bodies. The
concept of a “luminiferous ether”
will be helpful to explain the second postulate; however the theory will not provide a “preferred stationary space” with special properties, nor assign a velocity-vector to a point of the empty space in which electromagnetic processes take place.
That's about it; if I see it correctly, there isn't much else that really needs to be modified although Lorentz would add here and there some more qualifiers as "true", "apparent", "local" etc.
However, Einstein makes a subtle switch from "empty space" to "reference system" without a clear motivation. To make the logic as well as the derivation easier to follow for the readers, Lorentz could instead stick with the original, physical meaning of the second postulate as formulated in the introduction - let's call it Maxwell's light postulate.
Next, Lorentz could explain that if we combine Maxwell's light postulate with the PoR, it follows that this postulate should also appear to hold in an inertial reference system that is in motion with respect to the ether, so that it could appear to be a "stationary" system just as in Newton's mechanics. He could refer to his 1895 and 1899 papers that explain how this works.
If we next operationally define all terms such as "speed", "time" etc. as described in section 1 (free from metaphysical meaning), then we obtain the following result:
Any ray of light moves in the “stationary” system of co-ordinates with the determined velocity c, whether the ray be emitted by a stationary or by a moving body.
I hope that this sufficiently clarifies the perceptual differences as well as the complete lack of difference in practice.
Harald
ADDENDUM: I forgot to point out that from Lorentz perspective one may proceed the derivation directly based on Maxwell's version of the light postulate, it is not necessary to make the intermediate step from "empty space" to an arbitrary Newtonian reference system.
Einstein wouldn't like that but it's much more straightforward (and of course, Newton would like that).
The Lorentz transformations that then result describe primarily a transformation between a system that is at rest in the ether and one in inertial motion. Thanks to the form of those transformation equations (they form a group), the same transformation equations are valid between inertial reference systems - just as is the case with the Galilean transformations.