n. A specific differential of energy flow may exist on a specific finite collector. However, it only represents a certain constant differential amount of energy flow compared to the universal vacuum energy flow or some other flow reference point. It is like a whirlpool in the river. Energy is like the flowing water, and an "amount" of energy is like the amount of water in the collecting whirlpool form (between its input flow and its output flow) at any time. Obviously, energy (ordering) forms can come and go; the water flow itself remains. Any "magnitude of energy" is always a "trapped" amount of energy in a "collector" (form).
Decoupling Current Components and Utilizing dØ/dt
The two components of electron current dq/dt can be decoupled, by blocking the dm/dt component while allowing the dØ/dt displacement current to continue to flow. In our first paper, we pointed out one way: utilizing a special degenerate semiconductor material whose electron gas relaxation time is extended, providing a finite time during which the material serves as a charge (i.e., a charged particle) blocking device, while passing the flow of potential (the dØ/dt massless displacement current component) and restraining the mass displacement current component dm/dt. With the advent of Fogal's semiconductor, the process becomes much easier to obtain and utilize in practical machines and circuits.
In our second paper, we pointed out a second way: utilize an ordinary capacitor and ramp-up step-charging. We found, however, that in most ordinary capacitors, the capacitive aspect is defeated by the sloppy movement of the plates and dielectric, converting dØ/dt into dq/dt. Only a few very carefully selected capacitors are sufficiently rigid and can provide overunity. One must use rigidized calibration standard capacitors for the ramp-charging by series steps method to be successful. With ordinary capacitors, however, one can readily demonstrate that the efficiency can approach 1.0 rather than 0.50 as expected.
Overunity Secrets: Charge Blocking, Collection, Shuttling, and
Two Isolated Circuits
The charge (actually charged mass) blocking approach provides a massless, free flow of vacuum EM energy that can be directed to a collector (capacitive or inductive) where it can be stored in either an E-field or a B-field. This stored energy can then be transferred to an isolated load circuit whose electrons (and hence their dm/dt mass displacement current) are free to flow as dq/dt. In the isolated load circuit, then, the two components [(dØ/dt)(dm/dt)] again couple to form i = dq/dt = [(dØ/dt)(dm/dt)], powering the load. All work in an electrical circuit is due to the mass displacement current dm/dt component; the massless displacement current (dØ/dt) is a flow of pure energy transport without loss, as is well-known. (For example, see Reference 4.)
Therefore, the first major free energy secret is simply to block the "working" component dm/dt of the current dq/dt while allowing the excess "lossless energy flow" component dØ/dt to flow to collectors to produce either free E-field or free B-field thereupon.
The second major secret is to transfer the collected excess free energy (via energy shuttling) to a second, isolated, load circuit, where the energy is discharged through the load in the conventional fashion (i.e., such that the two current components are coupled, and electron current i = dq/dt occurs through the load). The second circuit must be isolated from the original collection circuit, so that none of the load electron current dq/dt passes back through the original source, against its back EMF.
Should the grounds be the same between the load circuit and the collection circuit so that load electron current is returned through the back EMF of the primary source, then exactly as much excess work will be done inside the source to dissipate its separation of charges as was done in the external load to furnish useful work and in the external losses. In that case, overunity is destroyed, because one is using one-half the excess free energy to destroy the source fa