Erasmus00 said:
Sure, especially if it helps me understand just what an anti-particle is in your theory.
The Einstein Field Equations for a spherically symmetric charged body are derived like this:
Substituting the Stress Tensor values for a charged body yields the Reissner-Nordstrom metric:
This is a very interesting geometry. The first thing to notice is that the center of the geometry is influenced by the +Q²/r²
and not the -2M/r term, no matter what the values of Q and M are! And notice that they are of
opposite signs. It turns out that that this geometry has a gravitationally
repulsive charged singularity at the center of the geometry.
If one plots light geodesics near the center of this charged geometry one obtains plots like this:
The gravity is actually repulsive in this region near the charge center. Any charged geometry like this
must come apart.
For an uncharged body, the Schwarzchild metric applies:
This geometry has an attractive singularity at its center. If one plots light geodesics near the center, they look like this:
Light is pulled into the center, exactly opposite of a charged geometry.
So, to set the stage for our pulsations, consider an uncharged geometry according to Schwarzchild. An event horizon masks the center. Create several charges and drop them into the geometry like this:
1) It is amazing to see that the repulsive forces of the charges heading inward cannot span the geometry to "repel each other". The charges can crash into the center without any energy of assembly.
2) Once this happens, a repulsive charged geometry must form, according to Reissner-Nordstrom.
3) The center must then come apart as the charges head towards a Reissner-Nordstrom geometry with a repulsive center.
4) The charge is both electrically repulsive and feels the repulsive gravity. The charge must therefore get out first, leaving the uncharged matter behind.
5) The original Schwarzchild matter is again by itself in the center, setting up another hole. The charge will be caught again and will be drawn into the center.
6) ... back to step 1.
We see that
it is more natural for charge and matter to pulsate than for it to be in equilibrium. And notice that the electrical forces to the outside world are periodically cut off by the horizon that temporarily forms around them.
Additionally, if one writes down a "mass function" for this dynamic geometry, the mass function oscillates between positive and negative. While the charge is "exposed" to the outside world and it "feels its own self-repulsion", the mass function is positive. While the charge is "cloaked" behind a horizon and cannot feel its own self repulsion, the mass function is negative.
This means that the mass of the electron m
e is simply the time-averaged mass of the electron. The "amplitude" of the electron mass may be enormous. That is, gravity may be playing a part in the electron's structure in an enormous way, but its "time average" is small.
Finally, notice that the structure of a positron or an electron would essentially be the same, as the sign of the charge is irrelevant.
Erasmus00 said:
What are the large neutrino detectors (like snow) seeing then? Do you have an alternative
explanation for their data?
These huge detectors typically detect about 1 positron or 1 muon event per day.
Definite evidence for neutrinos? No. Not even close.
Alternate explanation? Yes, the normal production of a positron or muon.
Erasmus00 said:
I am having a great deal of trouble writing down equations that let the charge blink but don't
allow for spherically symmetric radiation (similar to the pressure wave from a spherical explosion).
I understand the dilema. The new Microscopic Maxwell's equations will have to be different, but one tends to use
Maxwell's equations to try to change Maxwell's Equations. This is a circular trap. This new electromagnetic theory
will have to be bootstapped from scratch, probably starting from a New Coulomb's Law. So how are you defining
radiation? Are you defining radiation in the usual sense using a Poynting Vector with crossed E and B fields? If so, then there can be no radiation.
Or, are you defining energy flux simply as the motion of "electrical influence" moving away from the charge at
c? If so, then what about in the normal static electron's case. It has electrical influence that is constantly moving away from the charge at
c.
Andrew A. Gray