Force, Coupled Gradients, and Electron Translation

Force, Coupled Gradients, and Electron Translation
Electrons Coupled to a Potential Gradient Move Themselves. The point is, when activated
by a "coupled potential gradient," the activated electron moves itself until it loses its activation
(its coupled potential gradient).
Let me say that again, in a little more detail. Forget the standard notion that a force field such as
the E-field causes electrons to move. Also forget the notion that the E-field is given by E = -∇φ.
In foundations of physics, those equations are known to be incorrect for the vacuum. EM force
fields are known (in QM foundations theory) to be effects, existing only in and on the charged
particles, and not existing separately at all,14 or in the vacuum at all.15 Instead of E = -∇φ, in the
vacuum the correct equation would be something like this: PE = -∇φ. In this case, we have
correctly stated that the potential gradient PE provides the potential for producing an antiparallel
E-field in and on a coupling/collecting charged mass, and the magnitude and direction of that
potential gradient will be given by -∇φ, if and only if a charged mass particle is first introduced
so that it couples to PE.
At any rate, the activated/potentialized electron moves itself. The reason is that it constitutes a
force. Force ≡ (mass x acceleration) (non relativistic case). So the potentialized/activated
electron is continuously accelerating. However, it is prevented from easily moving down the wire
directly. To begin to do that, it essentially has to first move to the outer skin of the copper
conductor.
The Collector: We now consider a circuit element that we called a collector . (It could be a
special coil made of special material, a capacitor with doped plates rather than simple
conducting plates, or any one of a number of things). The objective is for the collector to be
made of special material so that it has a free electron gas whose electrons are momentarily not
free to move as current (they continue to move violently around microscopically, but essentially
with zero net macroscopic translation) for a finite delay (relaxation) time, while they are settling
themselves upon the surface and preparing to move as current. Let's call the electrons NNTE
(no net translation electrons) during that finite delay (relaxation time). During that "no-current"
delay time, the NNTE electrons become potentialized/activated by the potential gradient
impressed across the collector. So at the end of the NNT time, the NNTE electrons are
potentialized, and each is of the form [∇φ•me].