clj4 said:
The proponents of this idea "Aether" and "gregory=NotForYou" ...
Um, hello? How many times do I need to tell you that I am not gregory. Seriously, stick to the physics.
I must admit that I'm getting more curious about this topic. I worked out some of the math and disagree with gregory on where Gagnon's error is. When I worked it out, of course the Lorentz force law changes. And if I define the electromagnetic fields from the contravarient field tensor (to conserve the form of the 2 "source" Maxwell equations), the boundary conditions do
not stay the same. However, if I define the electromagnetic fields from the covarient field tensor (to conserve the form of the 2 "non source" Maxwell equations), the boundary conditions
do stay the same. Interestingly enough, the "wave equations" obtained from the standard method of evaluating\nabla \times (\nabla \times E) and \nabla \times (\nabla \times B), are the same regardless of whether you choose the contravarient or covarient field tensor to define the fields (should that be obvious for some reason?).
In case there is any confusion, clj4, in his
https://www.physicsforums.com/showpost.php?p=950704&postcount=324" he attached ... he used the contravarient field tensor to define the electromagnetic fields (this is forced by his choice in his eq 3.6). Therefore the boundary conditions do
not stay the same with that definition, ruining his arguement. However, Gagnon's paper uses the covarient field tensor to define the electromagntic fields, so if my calculations are correct (I think I see gregory's error, but I'll discuss this with him tomorrow), then the boundary conditions do stay the same using that particular definition (and therefore, clj4's error is moot since gregory is wrong as well).
Anyway, I read over the paper today and my calculation agrees with equation 5 (the wave equation in B is also of the same form). Equation 8 however is wrong, and unfortunately, they do not explain their calculation explicitly enough ... so while unsatisfying, we can not see the details of their mistake.
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 ds^2=c^2 dt^2 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"). They will however disagree on the value of k since that depends on the simultaneity convention.
To help this discussion along, I was wondering if anyone knew what the full form of E(x,y,z) is in equation 6. (ie. what is the result that they obtain for E(x,y) after applying their boundary conditions and the remaining maxwell's equations?). If they had included this in their paper, we could double check their intermediate results easier. So if you somehow figured out what they claim the full form of E(x,y,z) is in eq. 6, let us know.