Moore, Stockton & Bearden - ic Energy from the Vacuum - System Efficiency and Coefficient of Performance of Symmetric and Asymmetric Maxwellian Systems.pdf

ic Energy from the Vacuum:
System Efficiency (ε) and Coefficient of Performance (COP) of
Symmetric and Asymmetric Maxwellian Systems

© K. Moore,1 M. Stockton, and T. Bearden
April 25, 2006

Abstract
Asymmetric regauging, deliberately induced in an ic (EM) system, increases the
magnitude of EM energy collected, without doing work. The energy can then be used to freely do work.
This paper clarifies the theoretical basis for such free energy systems, which harvest EM energy directly
from the virtual-state vacuum.
We clarify thermodynamic efficiency (ε) and coefficient of performance (COP) for all Maxwellian
systems — both the standard symmetric ones and the asymmetric ones not modeled by Lorentz’s
simplification of the Heaviside-Maxwell equations. We also clarify entropy and negative entropy, and
formally correct the flawed second law of thermodynamics.
Rigorously, work is only a change in energy’s form, not its magnitude. Energy collection — that is,
potentialization — is always a negative entropy operation. Evans and Rondoni {11} showed that negative
entropy operations are theoretically possible.
Every charge, in polarizing its surrounding vacuum, is a dipolar ensemble exhibiting the proven broken
symmetry of opposite charges. Without any observable EM energy input, the charge emits a continual
stream of real, observable photons spreading radially outward at light speed. Cranking a generator’s shaft is
not the source of the EM energy flowing in the circuit; cranking only creates a dipole by separating
opposite charges within the generator. But it is the negative entropy operation produced by that dipole’s
broken symmetry that gates the emergence of observable energy from the seething virtual-state vacuum’s
ever-present energy repository. We focus on this subtle distinction because of its extremely useful practical
implications. This is consistent with Whittaker’s model {1} characterizing every EM field and