lugita15 said:
ghwellsjr said:
What definition of PoR are you using that let's you identify a preferred frame by experiment?
I'm just using the traditional definition "The laws of physics are the same in all inertial reference frames."
That is a good definition but it has consequences as Richard Feynman points out in his chapter on Special Relativity from Lectures on Physics:
The principle of relativity was first stated by Newton, in one of his corollaries to the laws of motion: "The motions of bodies included in a given space are the same among themselves, whether that space is at rest or moves uniformly forward in a straight line." This means, for example, that if a spaceship is drifting along at a uniform speed, all experiments performed in the spaceship and all the phenomena in the spaceship will appear the same as if the ship were not moving, provided, of course, that one does not look outside. That is the meaning of the principle of relativity.
lugita15 said:
Maxwell believed that space and time are absolute, so in his mind the principle of relativity implied the Galilean transformations.
That's an understatement. At that time, all scientists believed the principle of relativity was embodied in the Galilean transformation.
lugita15 said:
So the fact that his equations predicted that the speed of light is c led Maxwell to conclude that his equations violated Galilean invariance and thus could only be exactly true in one preferred frame. So he wanted to conduct an experiment to determine that frame.
But violating Galilean invariance is the same as violating the principle of relativity. Here's how Feynman expresses it:
However, the Maxwell equations did not seem to obey the principle of relativity. That is, if we transform Maxwell's equations by the substitution of equations [of the Galilean transformation], their form does not remain the same; therefore, in a moving spaceship the electrical and optical phenomena should be different from those in a stationary ship. Thus one could use these optical phenomena to determine the speed of the ship; in particular, one could determine the absolute speed of the ship by making suitable optical or electrical measurements.
lugita15 said:
If he was successful, that would not violate the principle of relativity, it would just mean that his equations would have to be modified in order to become Galilean invariant, so that measurements of the speed of light in other frames would be c+v or c-v, where v is the speed of the aether with respect to you.
No, if he was
unsuccessful, it would mean his equations would have to be modified, or so they thought. Here's how Feynman expresses it:
A number of experiments...were performed to determine the velocity of the earth, but they all failed--they gave no velocity at all...something was wrong with the equations of physics. What could it be?...the first thought that occurred was the trouble must lie in the new Maxwell equations of electrodynamics, which were only 20 years old at the time. It seemed obvious that these equations must be wrong, so the thing to do was to change them in such a way that under the Galilean transformation the principle of relativity would be satisfied. When this was tried, the new terms that had to be put into the equations led to predictions that of new electrical phenomena that did not exist at all when tested experimentally, so this attempt had to be abandoned. Then it gradually became apparent that Maxwell's laws of electrodynamics were correct, and the trouble must be sought elsewhere.
So if an experiment did determine the velocity of the earth, it would mean that the principle of relativity was not valid. But since the experiments were unsuccessful, the principle of relativity survived intact but since Maxwell's equations also survived, it meant that the Galilean transformation must be in error and that's what eventually was discovered to be the case and it was replaced by the Lorentz transformation but this was all done in the context of an absolute ether rest frame.