- #386
clj4
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Ah, now the "gregory" personality re-emerges (and the same prose, with no math).NotForYou said:Again. What do you feel I have said that is incorrect regarding the field tensor? What do you feel I have misunderstood?
Are you denying that the form of Maxwell's equations and the Lorentz force law change form in GGT depending on whether you choose the contravarient or the covarient field tensor to define the electromagnetic fields in the GGT frame? The form of maxwell's equations requires this. And also, you'd be contradicting Gagnon's ref 9.Sure I have. I'll post it again. Follow through the proof yourself:
I found the form of physics in GGT frames not worth the effort. So instead I chose to do the calculations in a "lorentz frame", transform to some arbitrary "special frame" (where GGT and SR are defined to agree), then transform back to the "lab GGT frame". Because GGT and SR have identical metrics in the special frame, and have identical definitions of proper time (invarient interval [tex]ds^2=c^2 dt^2[/tex] is always true in the clock's rest/"proper" frame according to both SR and GGT), the frequency measured in a GGT frame agrees with the SR value (independent of the choice of "special frame").
Which statement do you deny?
Which reminds me , how did you convince "gregory" that he was wrong about the boundary conditions? You never produced the mathematical proof. Knowing "gregory", this wasn't such an easy task. Can you show us?