Overunity Secrets: Charge Blocking, Collection, Shuttling, and Two Isolated Circuits

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 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.