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Hmm. Well, I see that you are very invested in promoting "your" model, I was thinking more of having an exchange here. No issue.
Then, ok I see that you are describing the magnetic scalar potential, we are back at "quantities". But we are still not defining anything, just theorizing things we could "count". As I understand it, a vector and scalar potentials are not physical things (or things at all whatsoever) but again, they are conceptualized quantities, units of measure, functions.
Don't you think that assuming these conceptualization as actual physical things is working against your model?
Telling you fully respectfully, even though I see that you are able to describe the functions, I don't think you have still defined the actual variables.
Don't worry, no one in mainstream physics, particularly those working in quantum, have done it yet. I was just curious if you had. I'm always on the look for that. I do congratulate you to bring the luminiferous aether to the equation though, that is brave of you, and I think that it makes you closer to the truth than anyone else working from the quantum perspective. Although, I wouldn't go the way you are going. Just to show you what I meant regarding the lack of definition, this is Richard Feynman, "trying" to answer/define, what I asked you about magnetism. Very funny
My entire work hinges on a postulate of an aether that is made of two materials, at least one of which may not be prevalent outside of the aether itself.
The mass of the attached-aether quanta could be anything. I was hoping the theory would determine it, but the theory still has a few free parameters and the mass is not yet known. As an example I don't think is correct, let's say it is 100 times greater than the proton mass.
So what happens when attached aether is kicked out and becomes detached is that some other stuff is added or subtracted to become the prevalent particles we see. I hope this helps to clarify the situation, although I understand it is a bit tricky.
I am up to page 110. The one thing that stuck out was how tension is one variable / dimension that does not cross this attached / detached place you are looking for.
As for one proposition to define this separation between the attached / detached place. Maybe sub atomic and greater atomic?
The substances themselves are the same.
Maxwell’s Equations and the Lorentz Force Equation are invariant in form under a Lorentz Transformation. In frames moving with respect to the aether, meter sticks shrink, clocks slow down, and the electromagnetic fields transform in just the right way so that the equations retain their form.
The first test might be to see if we can observe time dilation of an atomic clock immersed in high power RF radiation. Such radiation should move the aether back and forth over the clock and we might be able to see something, although the effect might be quite small
For the general math, what is it that you done with Maxwell, Lorenz and Newton that is different?
Maxwell's equations, or Maxwell–Heaviside equations, are a set of coupled partial differential equations that, together with the Lorentz force law, form the foundation of classical electromagnetism, classical optics, and electric circuits.