Extracting and Using Electromagnetic Energy from the Active Vacuum
Thomas E. Bearden
Summary and citation · read the original at the source
In one page
Thomas Bearden’s chapter makes one argument and then follows it as far as it goes. Ordinary field theory already says that the electromagnetic energy flowing around a working circuit fills the space around the wires, and that only a small part of it — the part Poynting accounted for — is actually turned into the conductors to do the work. Oliver Heaviside noticed the much larger remainder in the 1880s and could not say where it came from; Lorentz later set it aside as physically insignificant on the grounds that it never enters the circuit. Bearden proposes that the remainder is neither insignificant nor mysterious. A battery or a generator, on his account, spends its chemical or shaft energy only to separate charges and form a source dipole, and it is that dipole, asymmetric with respect to the vacuum, which pours out the energy the circuit actually runs on. He then asks the engineer’s question: what would a circuit have to look like to catch the part that is currently missed?
Why it matters hereChapter 6 collects the routes by which people have proposed to draw usable energy out of the vacuum, and this is the most fully argued electrical-engineering version of that case — it names a specific quantity that standard practice discards and asks what it would take to intercept it. Chapter 10 gets the other half: the potential treated as a structured object with its own internal wave content, which is where the vector-potential thread of this site begins.
What it claims
01The starting fact is ordinary field theory. The energy flow around a current-carrying circuit fills the surrounding space, and only the small component that strikes the surface charges is diverted into the conductors to power the circuit; the far larger remainder passes by and is not intercepted. Bearden calls the intercepted part the Poynting component, after Poynting’s 1884 paper, and the non-intercepted remainder the Heaviside component, after Heaviside’s 1885 work on electromagnetic induction and its propagation.Posted paper, section 1 Introduction, and section 6 on how the external circuit is powered
Settled physics02His central proposal is about where a circuit’s power comes from. The shaft energy put into a generator, or the chemical energy in a battery, is not what powers the external circuit — it is spent separating internal charges to form a source dipole. Once formed, that dipole is a broken symmetry in the vacuum flux, and it is the dipole that receives energy from the vacuum and pours it out along the circuit. Bearden grounds the symmetry-breaking language in particle physics, citing Wu and colleagues in 1957 and T. D. Lee’s statement that discoveries of asymmetry must imply observables.Posted paper, section 6, and the argument from broken symmetry in section 3
What to watch03The structure he assigns to the potential comes from a published decomposition. Extending earlier work by Stoney, Whittaker showed in 1903 that a scalar potential can be decomposed into a harmonic set of bidirectional longitudinal wave pairs, each consisting of a wave and its phase-conjugate replica. Bearden takes the convergent half of that set as an inflow toward the dipole and the divergent half as the outflow we measure, with a one-to-one correlation between them — his reading of the Whittaker decomposition as a real energy-flow mechanism rather than a mathematical identity is the proposal, and it is the part that would have to be tested.Posted paper, section 3, on the Whittaker decomposition of the potential between the end charges
What to watch04The one experimental result he leans on is settled physics used for a new purpose. A resonant particle can absorb and re-emit substantially more light than falls on its geometric cross-section — Craig Bohren’s much-cited demonstration, confirmed by Paul and Fischer, gives a factor of up to about eighteen. Bearden accepts the standard explanation, that the resonant particle sweeps a larger reaction cross-section than the static-particle calculation assumes, and argues that this is exactly what interception of the non-diverted flow would look like.Posted paper, section 10, Bohren’s experiment and the explanation that follows it
Settled physics05The chapter is explicit that its central number is an estimate awaiting a proper calculation. A back-of-the-envelope comparison for a nominal simple direct-current circuit puts the non-diverted component at the order of ten to the thirteenth times the magnitude of the diverted one, and the author writes that a more exact calculation and a functional theoretical model would be welcomed but could not be found in the literature. That missing calculation is the first thing an interested reader could actually supply.Posted paper, section 7 and section 10, the magnitude estimate and the request for a model
What to watch06The design requirements are stated as a list, which is what makes the chapter usable rather than only argumentative. A system aiming at a coefficient of performance greater than one must, during its excitation discharge, be an open system far from equilibrium in its exchange with the vacuum; its loads must not sit in the same closed current loop as the source dipole, since forcing spent charge back through the dipole destroys it; and it must iteratively collect from the non-diverted flow. Four candidate routes are named — retroreflecting the flow back across the surface charges on each pass, Kron’s open path as the dual of the closed path, Tesla’s energy shuttling as developed by Barrett, and self-excitation in intensely scattering optically active media.Posted paper, section 8 on the closed current loop, and section 9, requirements 1 through 3
Designed, not yet built
The way in
https://doi.org/10.1002/0471231487.ch11WHAT THIS PAGE IS WRITTEN FROM. The registered work is chapter 11 of Modern Nonlinear Optics, Part 2, second edition, edited by Myron W. Evans, volume 119 of Advances in Chemical Physics, John Wiley and Sons, 2001 and 2003. The Wiley chapter is closed access and could not be opened on 2026-09-08, so none of its text is reproduced here. The summary and claims were written from the author’s own paper of the same title, which Bearden posted on his site cheniere.org as bearden4.pdf and which was read in full for this sheet through the Internet Archive capture of 9 March 2016 — ten pages of text plus notes, signed T. E. Bearden, CEO of CTEC Inc. and director of the Association of Distinguished American Scientists. That posted paper carries the chapter’s title and argument, but it is shorter than a book chapter and may be a condensed version rather than the chapter itself; every locator below cites a numbered section of the posted paper and says so. When the Wiley chapter can be read, this sheet should be checked against it. The site’s five maturity phrases are used to separate the established physics the chapter builds on from the proposals it makes.
How to cite it
Thomas E. Bearden (2003) Extracting and Using Electromagnetic Energy from the Active Vacuum. doi:10.1002/0471231487.ch11
Where it sits in the curriculum
Scalar waves and the field behind the fieldsEnergy from the vacuum