gure 2 shows the close-looping of the device shown in Figure 1, in such manner that, once stable operation is underway and the load and input stabilized, the ordinary power supply for the CBS can be switched out of the circuit. In this case, the circuit operates as a self-powered overunity device; i.e., as a negative resistor.
A normal resistor receives an ordered energy flow from its external circuit and scatters this energy as work out to the vacuum. I.e., it receives i = (Ø+Ø)/dt(dm/dt) (scatters the excess (Ø)/dt component (i.e., of the dq/dt passing into it from the high potential side) by radiating it away to the surrounding vacuum as scattered photons (heat)), and outputs inert (no excess (Ø) component) electron current dq/dt into the ground side.
A negative resistor does exactly the opposite: it accepts inert incoming electrons from its "ground" side, also accepts incoming (converging) dØ/dt energy from the vacuum as virtual photons being absorbed upon these inert electrons so that a Ø is added to the electron current, creating an excited, excess energy-carrying i = (Ø+Ø)/dt(dm/dt), and passes this excited current out of its high side and out into the external circuit to power the circuit. In other words, the negative resistor becomes a self-contained free power source, once brought up to stable operation.
In Figure 1, all that needs to be done is simply to extract some of the secondary power and feed it back to create the power input consumed by the CBS and the other normal components of the primary circuit side of the transformer.
Multitaps can be added to the secondary side, to provide varying voltage power supplies for loads requiring different voltages.
Energy is conserved in the device, because it always functions as an open circuit, receiving excess energy from an external source (the surrounding vacuum, in its virtual photon exchange with the charges in the system). It is far from thermodynamic equilibrium, and classical thermodynamics (including the second law) does not apply.
It is simply a continuous free power supply: it is a negative resistor.
Far more complicated units can be designed and produced. The basic point is that this type of overunity power supply is continuous and self-powered, driven by the violent exchange of energy from the vacuum, and simply collecting and gating some of that energy to the load to power the load.
With this third paper, we complete the triad of papers we set out to write a little over a year ago. With the availability of charge barrier devices such as the Fogal semiconductor, together with the collection, shuttling, and use of free dØ/dt flowing energy, the Age of Free, Clean, Electrical Energy has finally dawned.
Let us use it wisely, and for the betterment of humankind, not for its destruction.
[Support of portions of this research by A.D.A.S. is gratefully acknowledged.]
References and Notes
1. Bearden, T.E., Feb. 9, 1993, "The Final Secret of Free Energy," ADAS, distributed over Internet. The paper was also published in Magnets, 7(5), May 1993, p.4-26, in Explore!, 4(3/4), 1993, p.112-126, and in several other media. See also Bearden, T.E., "Additional Information on the Final Secret of Free Energy," Feb. 15, 1994, distributed on Internet.
2. For proof that an ordinary capacitor can be charged almost without entropy, see Fundaun, I., C. Reese, and H.H. Soonpaa, "Charging a Capacitor," American Journal of Physics, 60(11),Nov. 1992, p.1047-1048. See also Calkin, M.G. and D. Kiang, "Entropy change and reversibility," American Journal of Physics, 51(1), Jan. 1983, p.78-79. See also Heinrich, F., "Entropy change when charging a capacitor: A demonstration experiment," American Journal of Physics, 54(8), Aug. 1986, p.742-744. See also Gupta, V.K., Gauri Shanker, and N.K. Sharma, "Reversibility and step processes: An experiment for the undergraduate laboratory," American Journal of Physics, 52(10), Oct. 1984, p.945-947.
3. In most texts, the treatment of displacement current is far from adequate. A better treatment than most is given by Krauss, John D., Electromagnetics, F