Originally posted by Spokane1
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First of all, watch this video:
MIT Physics Demo -- Dissectible Capacitor - YouTube
Steinmetz comment on this:
Eric Dollard and Tesla
"Unfortunately, to a large extent in dealing with the dielectric fields the prehistoric conception of the electrostatic charge on the conductor still exists, and by its use destroys the analogy between the two components of the electric field, the magnetic and the dielectric, and makes the consideration ot dielectric fields unnecessarily complicated. There obviously is no more sense in thinking of the capacity current as current which charges the conductor with a quantity of electricity, than there is of speaking of the inductance voltage as charging the conductor with a quantity of magnetism. But while the latter conception, together with the notion of a quantity of magnetism, etc., has vanished since Faraday's representation of the magnetic field by the lines of magnetic force, the terminology of electrostatics of many textbooks still speaks of electrostatic charges on the conductor, and the energy stored by them, without considering that the dielectric energy is not on the surface of the conductor, but in the space outside of the conductor, just as the magnetic energy."
As I stated before, electrostatic energy is a "D.C." steady state flow of the aether itself. In my Pes article, I use the concept of a "fandoor" to explain the interactions of an electron (the fandoor) with the aether (wind, airflow).
The forces that we measure, are not static forces, just like the airflow generated by a fan is not a static force.
In other words: in actual fact, no energy is actually stored in a capacitor. What you have is a certain configuration of fandoors, ether pumps, electrons and atom nuclei, which pump the aether around along a certain path. It is that flowing aether which pushes against your electrons, which makes them move around, which is what we call a current.
You can create the same kind of aether flow with a polarized dielectric, which leads to an effect that has been observed with Bedini-charged capacitors as well as lead-acid batteries, which we called "the electret effect". I have posted some on this quite some time ago, which posts I linked from my pes article in the electret effect section:
Article:Free Electric Energy in Theory and Practice - PESWiki
There is a video wherein Bedini explains what happens within his batteries:
BatteryForming_2008_04_25_16_16_47.wmv - YouTube
And someone did some laboratory work on lead-acid batteries charged with Bedini pulses, too:
Directory contents of /pdf/Reference_Material/Rogers/
Also see this post by Cody:
The polarization of a dielectric is a very interesting effect:
Dielectric - Wikipedia, the free encyclopedia
A dielectric is an electrical insulator that can be polarized by an applied electric field. When a dielectric is placed in an electric field, electric charges do not flow through the material as they do in a conductor, but only slightly shift from their average equilibrium positions causing dielectric polarization.
[...]
When the electric field is removed the atom returns to its original state. The time required to do so is the so-called relaxation time; an exponential decay.
[...]
The relationship between the electric field E and the dipole moment M gives rise to the behavior of the dielectric, which, for a given material, can be characterized by the function F defined by the equation:
M = F(E).
[...]
Dielectric relaxation is the momentary delay (or lag) in the dielectric constant of a material. This is usually caused by the delay in molecular polarization[disambiguation needed] with respect to a changing electric field in a dielectric medium (e.g. inside capacitors or between two large conducting surfaces). Dielectric relaxation in changing electric fields could be considered analogous to hysteresis in changing magnetic fields (for inductors or transformers).
[...]
When the electric field is removed the atom returns to its original state. The time required to do so is the so-called relaxation time; an exponential decay.
[...]
The relationship between the electric field E and the dipole moment M gives rise to the behavior of the dielectric, which, for a given material, can be characterized by the function F defined by the equation:
M = F(E).
[...]
Dielectric relaxation is the momentary delay (or lag) in the dielectric constant of a material. This is usually caused by the delay in molecular polarization[disambiguation needed] with respect to a changing electric field in a dielectric medium (e.g. inside capacitors or between two large conducting surfaces). Dielectric relaxation in changing electric fields could be considered analogous to hysteresis in changing magnetic fields (for inductors or transformers).
To sum this up:
What you can do with a londitudinal shock wave in the shape of a sharp rising edge (large dE/dt) and a soft dropping falling edge is to super-polarize a dielectric, such that it keeps it's polarization for a considerable time, depending on the applied voltage, etc.
When you put such a polarized dielectric in between capacitor plates, you can get an effect whereby capacitors spontaneously recharge after having been shortcutted. This has been observed with electrolytic capacitors, whereby you have a very thin layer of aluminum oxide as your dielectric on one of the capacitor plates. This is a very similar construction as with a lead-acid battery, especially in the old days.
In other words: you can super-polarize a dielectric layer within both an electrolytic capacitor as well as a lead-acid battery, which would result as the cap/battery being observed as having been charged.
Just as the MIT dissectible Leyden jar, whereby the energy is "stored" in the dielectric...

; when it revolved towards the left, they appeared thus,
. In no case did I see them thus,
, or thus,
, as required in the hypothesis of the actual transfer of a single fluid.


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