lectrons, producing normal electron current dq/dt, and driving it through the load to power it. Note that energy is conserved across the primary and the secondary; however, dissipative power and work (energy loss rate and energy loss) are not conserved, because a free flow of lossless excess energy in the form of displacement current is flowing from the vacuum through the source antenna, thence to the CBS, through it to the primary of the transformer and into the primary magnetic field, through it to the secondary magnetic field, through it into the (dØ/dt) induced in the secondary circuit and coupled to the electrons, through the resulting dq/dt into the load, where the scattering of photons as heat dissipates the free flowing energy in the displacement current dØ/dt component flowing through the load as a component of dq/dt = (dØ/dt)( dm/dt) = (dØ/dt)(dm/dt).
Free "Power" Amplification
If one places an ammeter in the output from the CBS, between it and the primary winding of the step-up transformer, one will read the (dØ/dt) as normal dq/dt in the ammeter itself. If one calculates the "free power" (i.e., the rate of energy dissipation) that is going into the transformer primary using this as the "current," one will show that energy and "power" are conserved between primary and secondary of the transformer. However, the actual dissipative power going into the primary side is zero or, in real circuits, vanishingly small. Consequently, the device has a very high variable power gain that depends upon the rate of energy draw and dissipation of the load on the secondary side. If one adds more load, one draws more dq/dt current on the secondary side, hence more excess dØ/dt displacement current on the primary side. The overall "power amplification" is limited by the ability of the transformer to handle the power in the secondary and the ability of the CBS to withstand the pressure of the internal charge barrier. This device can be easily "close-looped."
The Negative Resistor: A Close-Looped "CBS and Shuttle" System
Figure 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 cont