llection, 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 faster, while the remaining half is distributed among all external loads and losses. Since there are always some external losses besides the load, then the ratio of load power to source dissipation power is always less than unity in a conventional closed-loop circuit containing both load and source. Hence the necessity for utilizing two isolated circuits: one where energy is collected freely from the source, and one where energy is dissipated as work in the load without dissipative work in the source, and energy shuttling between them.
A Simple Open-Loop Overunity Device
Figure 1 shows a very simple but very powerfully amplified
overunity device, using an AC charge blocking semiconductor
(CBS) (such as a Fogal semiconductor). The gist of the circuit
is that an AC source furnishes AC current dq/dt to the CBS,
which uses some of the power to power itself, but then blocks the
dm/dt portion of the dq/dt input current, passing only the
massless displacement current component (dØ/dt) into its
output circuit. The (dØ/dt) output of the CBS is fed
through the primary winding of a transformer, in this case a
step-up transformer. The "current gain" of the CBS will depend
upon (1) the load connected to it, and (2) the ability of the CBS
to continue to block the increasing E-field on its trapped
charges, as more free energy flow (dØ/dt) is drawn through
it by the load. Thus the load and the CBS must be matched within
the operational ability of the CBS, so that the CBS does not fail
In the primary winding of the transformer, the (dØ/dt) displacement current produces a magnetic field H, storing the excess flowing energy in that field. This is a normal magnetic field; all magnetic fields are produced by the (dØ/dt) component of the current anyway. This magnetic field, as it changes, couples to the secondary winding, producing a normal magnetic field H therein by normal means. In the secondary circuit, electrons are not restrained by a CBS. Hence the (dØ/dt) induced in the circuit on the secondary side couples to the unrestrained e