Dale said:
I will ask the same thing of you that I asked of the OP. Do you have a reference that supports this claim (that this set of premises is self consistent)? I do not think this is a self consistent premise.
Nugatory said:
Which is to say that Einstein's second postulate is necessary. We've had a number of threads on this question over the years. However...
How are the laws the same in both frames? Maxwell's laws of electrodynamics cannot hold in both frames, because they they have no solution in which a flash of light in vacuum is moving at any speed except ##c##. To maintain consistency with the principle of relativity you would have to propose some other laws of electromagnetism, ones that are consistent with a frame-dependent speed of light.
From Einstein's paper "The Foundation of the General Theory of Relativity" 1916
http://hermes.ffn.ub.es/luisnavarro/nuevo_maletin/Einstein_GRelativity_1916.pdf
"If a system of co-ordinates K is chosen so that, in relation to it, physical laws hold good in their simplest form, the same laws also hold good in relation to any other system of co-oordinates K’ moving in uniform translation relatively to K. This postulate we call the “special principle of relativity”"
The principle of relativity, as stated above by Einstein, is silent on optics. You cannot derive from the principle of relativity anything about optics, electricity and magnetism, or clocks other than if you have a theory of them valid in one frame then it must be valid in other frames.
Orodruin wrote: "I created this thread to *rigorously* examine the claim, such as in Brian Greene's book, that principle of relativity prohibits different clock mechanisms from having different time dilation. I emphasize "rigorously."" [Mentor's note: Orodruin didn't write that, the original poster did]
The principle of relativity as quoted above does not prohibit different clock mechanisms from having different time dilation:
Consider two clock mechanisms C1 and C2 and assume that relative to a system of co-ordinates K there is some law that says that the time dilation of clocks of type C1 is some function f() and the the time dilation of clocks of type C2 is some function g() such that f() is not equal to g(). Suppose further that both f'() and g'() are the functions that govern the dilation in some frame K'. Further suppose f()=f'() and g()=g'(). Then these laws are consistent with the special principle of relativity and they predict that time dilation be different for different clock mechanisms. As a concrete example let f()=2*g() and let delta t'=v * delta t.
In theoretical work it is important to trace logically to the assumptions involved. Orodruin wanted a "rigorous" examination of a certain claim that the principle of relativity prohibits different clock mechanisms from having different time dilation. As long as you propose a theory that says that if different clock mechanisms do have different time dilation in one frame, and that same situation is present relative to all frames moving with constant velocity relative to the first, then the principle of relativity holds.
So the principle of relativity as stated by Einstein does not prohibit different clock mechanisms from having different time dilation.
A more interesting question is whether the meaning of time itself prohibits it. Certainly if all mechanisms had different dilation then the notion of time itself would not be very useful. One might say of such a world, that clocks don't exist. However, setting optics aside, if all mechanisms operated according to Newtonian mechanics except one then the concept of time would be useful and a theory could be constructed that was consistent with the principle of relativity.
That this world is counterfactual is not a problem as it is only being cited to illustrate the absence of logical dependence of conclusions about clocks (or optics, or electromagnetism) on the principle of relativity as stated by Einstein. Counterfactual arguments are routinely used to illustrate lack of logical dependence.
As a historical note, the principle of relativity in Einstein's 1903 paper was restricted to electricity and magnetism. So in a sense he generalized the principle in 1917 not only by making laws invariant relative to more general coordinate transformations, but technically he also expanded the principle to apply to physical laws in general.