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Re: Space-Time Curviture
Ok what I was getting at was this.
Concider the idea that Space-Time was interelated with Mass-Energy. they are but I mean on a more definite and intimate relationship.
Imagine it like this. A sphere within a sphere within a sphere. Our three spheres would be representing Space-Time as the outer most. Mass-Energy as the next. and Charge as the Center Sphere.
Though I did consider the possibility of charge being the middle sphere.
What becomes crusial in this idea is these main questions:
Does everything have charge. Not net charge but charge period. I believe photons do. because of the equation c = (u0)(e0) which has to do with the magnetic and electric fields.
Also I need more information about Einstiens Field Equation on Space-Time.
So back to the concept. now imagine if these three spheres interacted in ways. When Space-Time expands then Mass-Energy contracts. and vise versa. I need to know if charge is constant to comment on it's interaction in this Concept. Now one knows that Mass-Energy is strictly conserved. Also we know that there is a speed limit for the universe, c. As such from this I draw the conclusion that Mass-Energy can grow no larger than it's Space-Time sphere Shrinks. That their boundries may meet but may never cross. So that Mass-Energy is bound by Space-Time. Mass-Energy may be found anywhere within it's S-T Sphere but never outside.
This to me would be in agreement with Einstien's SR and GR theories. would explain to me Length contraction and the Theory of the expanding/collapsing universe.
If my concept is correct then it would mean to me that:
1) Time is Quantasized.
2) Space is Quantasized.
3) Mass is Quantasized.
4) indirectly Gravitational Force is Quantasized.
and the golden egg:
*) The waveform equation for mass. The schrodinger equations. Would fit into this model. The Probability density is as shows:
ψ(x, y, z, t)
ψ'(x', y', z', t')
i also would like to go one step further and postulate that:
t(x, y, z)
t'(x', y', z')
P.S. I so eagerly await my books on QT and Classical Mechanics.
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