Bearden Fact Sheet Overunity EM power systems


Permissible NESS COP > 1.0 Electrical Power Systems Taking Energy from the Vacuum

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© T. E. Bearden, Sept. 19, 2003

Problem: Develop the concepts for COP > 1.0 electrical power systems that receive and utilize EM energy from their active vacuum environment.

"First a negative entropy interaction occurs to produce some controlled order (available controlled energy). Then that initial available controlled order will either remain the same or be progressively disordered and decontrolled by subsequent entropic interactions over time, unless additional negative entropy interactions occur and intervene."

"A century [Author ID1: at Sat Feb 22 21:39:00 2003 ]or so [Author ID1: at Sat Feb 22 21:47:00 2003 ]ago[Author ID1: at Sat Feb 22 21:39:00 2003 ],[Author ID1: at Sat Feb 22 21:47:00 2003 ] Ludwig Boltzmann and other[Author ID1: at Sat Feb 22 21:39:00 2003 ] physicists [Author ID1: at Sat Feb 22 21:48:00 2003 ]attempted to explain the temporal asymmetry of the second law of thermodynamics. [Author ID1: at Sat Feb 22 21:39:00 2003 ]…t[Author ID1: at Sat Feb 22 21:49:00 2003 ]he hard-won lesson of that endeavor—a lesson still commonly misunderstood—was that the real puzzle of thermodynamics is not why entropy increases with time, but why it was ever so low in the first place."[Author ID1: at Sat Feb 22 21:39:00 2003 ]

"…{The] major task of an account of thermodynamic asymmetry is to explain why the universe as we find it is so far from thermodynamic equilibrium, and was even more so in the past."

Focusing on the COP > 1.0 System Problem:

Approach:

Peculiar Fact: Every electrical power system is a COP >> 1.0 system when its Heaviside energy flow component is included.

Proof of Heaviside's Energy Flow Component.

"...the Poynting vector is arbitrary to the extent that the curl of any vector field can be added to it. Such an added term can, however, have no physical consequences."

Known COP > 1.0 Vacuum-Powered EM System.

Known COP = " Vacuum-Powered EM System.

“The connection between the field and its source has always been and still is the most difficult problem in classical and quantum electrodynamics.”

“A generally acceptable, rigorous definition of radiation has not as yet been formulated. … “The recurring question has been: Why is it that an electric charge radiates but does not absorb light waves despite the fact that the Maxwell equations are invariant under time reversal?”

Some Background Definitions and Their Ramifications.

Unusual Phenomenology of COP > 1.0 Vacuum-Powered Systems.

Additional Definitions and Discussion.

Recapitulating:

Extracting Energy from the Vacuum:

"What might appear to be empty space is, therefore, a seething ferment of virtual particles. A vacuum is not inert and featureless, but alive with throbbing energy and vitality. A 'real' particle such as an electron must always be viewed against this background of frenetic activity. When an electron moves through space, it is actually swimming in a sea of ghost particles of all varieties—virtual leptons, quarks, and messengers, entangled in a complex mêlée. The presence of the electron will distort this irreducible vacuum activity, and the distortion in turn reacts back on the electron. Even at rest, an electron is not at rest: it is being continually assaulted by all manner of other particles from the vacuum.”

The “Magic” Universal Negative Entropy Process:

Operation of a home heat pump .

Electrical Power Situation in Science and Engineering:

How the External Circuit Is Powered:

“…one of the most remarkable and inexplicable aberrations of the scientific mind which has ever been recorded in history."

Ramifications:

An Implacable Old Foe: The Seriously Flawed Second Law of Thermodynamics that Prohibits COP>1.0 VP EM Systems.

"The law that entropy always increases—the second law of thermodynamics—holds, I think, the supreme position among the laws of nature. If someone points out that your pet theory of the universe is in disagreement with Maxwell's equations—then so much the worse for Maxwell's equations. If it is found to be contradicted by experiments—well, these experimentalists do bungle things sometimes. But if your theory is found to be against the second law of thermodynamics I can give you no hope; there is nothing for it but to collapse in deepest humiliation."

Recommendations: It is recommended that:

Observations:

Closing Thoughts:

"...the scientist makes use of a whole arsenal of concepts which he imbibed practically with his mother's milk; and seldom if ever is he aware of the eternally problematic character of his concepts. He uses this conceptual material, or, speaking more exactly, these conceptual tools of thought, as something obviously, immutably given; something having an objective value of truth which is hardly even, and in any case not seriously, to be doubted. ...in the interests of science it is necessary over and over again to engage in the critique of these fundamental concepts, in order that we may not unconsciously be ruled by them."

"[Hypotheses made without realizing that they are being made] …are what Poincaré has called "unconscious" or "natural" hypotheses—a type which one hardly ever challenges, for it seems too unlikely that we could make progress without them. Nevertheless it should be the endeavor of the physicist always to drag them out into the light of day, so that it may be perfectly clear what we are actually doing."

"An important scientific innovation rarely makes its way by gradually winning over and converting its opponents: it rarely happens that Saul becomes Paul. What does happen is that its opponents gradually die out, and that the growing generation is familiarized with the ideas from the beginning."

References:

NESS is an acronym for nonequilibrium steady state. Thermodynamically, NESS systems far from equilibrium in their energetic exchange with their active environment are permitted to exhibit COP > 1.0 (more energy or work output than the energy that the operator inputs) and even COP = " (“self-powering”, where all the input energy is freely furnished by the active environment). For general background, the reader is referred to
D. Kondepudi and I. Prigogine, "Thermodynamics, Nonequilibrium," Encyclopedia of Applied Physics, Vol. 21, 1997, p. 311-337.

We accent that, in a general relativistic case, thermodynamics is a local description only. Indeed, due to the relativity of simultaneity, during a given period energy may be conserved for one observer and not conserved for another, since something can have happened already for the first observer and not yet have happened for the second observer in a different frame.

Imagine a “standard size rock” fixed on the bottom of a rushing stream. A certain divergence of the stream around the rock will be accomplished. Now imagine the same rock not fixed, but being surged back and forth at right angles to the water flow, very violently. Obviously much more water flow will be diverged by the churning rock. Both cases are simply approximations of the intensity of the water's flow at that point, determined in differing ways.

The definition of the field (point intensity) as the “force per unit static point charge” should be amended to “force per unit point charge and its dynamic condition”. The potential's definition should be changed similarly.

The terms “self-powered” or “self-powering” are corrupted terms meaning that the system is completely powered by energy received from its active environment. They are synonymous with “COP = "”.

The sooner classical electrodynamics incorporates the more fundamental Whittaker longitudinal EM wave internal structuring inside the present “envelope” EM fields, potentials, and waves, the better. The phrase “static field” should be replaced in every textbook and paper by the phrase “steady state field”.

The present statement of the second law is thus an oxymoron that implicitly assumes its own contradiction has first occurred. Its correction also solves the temporal asymmetry problem of thermodynamics stated by Price {1}. The second law has always been grossly incomplete, and it has been wrong in excluding negative entropy processes. However, to model negative entropy EM processes and solve the temporal asymmetry problem, one must transcend Klein geometry and methods {7}, and go to Leyton geometry and methods {8}.

Fact Sheet 2003-06

27

. Huy Price, Time's Arrow [Author ID1: at Sat Feb 22 21:39:00 2003 ]and Archimedes' Point[Author ID1: at Sat Feb 22 21:48:00 2003 ], [Author ID1: at Sat Feb 22 21:39:00 2003 ]Oxford[Author ID1: at Sat Feb 22 21:48:00 2003 ] University Press, 199[Author ID1: at Sat Feb 22 21:39:00 2003 ]6[Author ID1: at Sat Feb 22 21:48:00 2003 ], [Author ID1: at Sat Feb 22 21:39:00 2003 ]paperback 1997[Author ID1: at Sat Feb 22 21:56:00 2003 ], p. 78.

. Price, ibid., p. 36.

. T. E. Bearden, Energy from the Vacuum: Concepts and Principles, Cheniere Press, Santa Barbara, CA, 2002, Chapters 3, 8, and 9.

. E.g., see (a) Dilip Kondepudi and Ilya Prigogine, Modern Thermodynamics: From Heat Engines to Dissipative Structures, Wiley, New York, 1998, reprinted with corrections 1999; (b) G. Nicolis and I. Prigogine, Self-Organization in Non-Equilibrium Systems: From Dissipative Structures to Order through Fluctuations, Wiley, New York, 1977; (c) — Exploring Complexity, Piper, Munich, 1987.

. Kondepudi and Prigogine, Modern Thermodynamics, 1999, ibid., p. 459. Later in this paper we will discuss some of the negative energy and negative entropy phenomena associated with sharp gradients in COP > 1.0 EM circuits taking their energy from the vacuum.

. D. J. Evans and Lamberto Rondoni, "Comments on the Entropy of Nonequilibrium Steady States," J. Stat. Phys., 109(3-4), Nov. 2002, p. 895-920.

. See (a) Felix Klein, "Vergleichende Betrachtungen über neuere geometrische Forschungen," 1872. Klein's Erlanger program was initiated in 1872 to describe geometric structures in terms of their automorphism groups. It has driven much of the physics development in the twentieth century. See also (b) I. M. Yaglom, Felix Klein and Sophus Lie: Evolution of the Idea of Symmetry in the Nineteenth Century, Birkhäuser, Boston, MA, 1988.

. Michael Leyton, A Generative Theory of Shape, Springer-Verlag, Berlin, 2001.

. T. E. Bearden, Fact Sheet 2003-03, “Leyton's Hierarchies of Symmetry: Solution to the Major Asymmetry Problem of Thermodynamics,” 2003.

. See (a) Oliver Heaviside, "Electromagnetic Induction and Its Propagation," The Electrician, 1885, 1886, 1887, and later. A series of 47 sections, published section by section in numerous issues of The Electrician during 1885, 1886, and 1887. See also (b) — "On the Forces, Stresses, and Fluxes of Energy in the Electromagnetic Field," Phil. Trans. Roy. Soc. Lond., 183A, 1893, p. 423-480.

. J. H. Poynting, “On the transfer of energy in the electromagnetic field,” Phil. Trans. Roy. Soc. Lond., Vol. 175, Part I, 1884, p. 343-361; — "On the Connection Between Electric Current and the Electric and Magnetic Inductions in the Surrounding Field," Phil. Trans. Roy. Soc. Lond., Vol. 176, Part II, 1885, p. 277-306.

. See H. A. Lorentz, Vorlesungen über Theoretische Physik an der Universität Leiden, Vol. V, Die Maxwellsche Theorie (1900-1902), Akademische Verlagsgesellschaft M.B.H., Leipzig, 1931, "Die Energie im elektromagnetischen Feld," p. 179-186. Figure 25 on p. 185 shows the Lorentz concept of integrating the Poynting vector around a closed cylindrical surface surrounding a volumetric element. This procedure arbitrarily selects only a small component of the energy flow associated with a circuit—specifically, the small Poynting component being diverged into the circuit to power it—and then treats that tiny component as the "entire" energy flow. Thereby Lorentz arbitrarily discarded the huge Heaviside circuital energy transport component that is usually not diverged into the circuit conductors at all, does not interact with anything locally, and is just wasted.

. J. D. Jackson, Classical Electrodynamics, 2nd Edn., Wiley, New York, 1975, p. 237.

. See H. J. Josephs, “The Heaviside papers found at Paignton in 1957,” IEE Monograph No. 319, Jan. 1959, p. 70-76.

. See E. R. Laithwaite, “Oliver Heaviside—establishment shaker,” Electrical Review, 211(16), Nov. 12, 1982, p. 44-45.

. Kondepudi and Prigogine, Modern Thermodynamics, 1999, ibid., p. 61.

. Cf (a) V. S. Letokhov, “Generation of light by a scattering medium with negative resonance absorption,” Zh. Eksp. Teor. Fiz., Vol. 53, 1967, p. 1442; (b) — “Generation of light by a scattering medium with negative resonance absorption,” Sov. Phys. JETP, 26(4), Apr. 1968, p. 835-839; (c) — “Stimulated emission of an ensemble of scattering particles with negative absorption,” ZhETF Plasma, 5(8), Apr. 15, 1967, p. 262-265; (d) — “Stimulated emission of an ensemble of scattering particles with negative absorption,” ZhETF Plasma, 5(8), Apr. 15, 1967, p. 262-265.

. (a) Craig F. Bohren, “How can a particle absorb more than the light incident on it?” Am. J. Phys., 51(4), Apr. 1983, p. 323-327. Metallic particles at ultraviolet frequencies are one class of such particles and insulating particles at infrared frequencies are another. For independent confirmation, see (b) H. Paul and R. Fischer, “{Comment on “How can a particle absorb more than the light incident on it?'},” Am J. Phys., 51(4), Apr. 1983, p. 328.

. (a) E. T. Whittaker, “On the Partial Differential Equations of Mathematical Physics,” Math. Ann., Vol. 57, 1903, p. 333-355; (b) — “On an Expression of the Electromagnetic Field Due to Electrons by Means of Two Scalar Potential Functions,” Proc. Lond. Math. Soc., Series 2, Vol. 1, 1904, p. 367-372.

. (a) Myron W. Evans, “A Generally Covariant Field Equation for Gravitation and Electromagnetism,” Found. Phys. Lett., Vol. 16, 2003, p. 367-377; (b) — A Generally Covariant Field Equation for Grand Unified Field Theory,” Found. Phys. Lett, 16(6), Dec. 2003, p. 507-541; (c) — “The Equations of Grand Unified Field Theory in Terms of the Maurer Cartan Structure Relations of Differential Geometry,” Found. Phys. Lett. (in press); (d) — “Generally Covariant Field and Wave Equations for Gravitation and Quantized Gravitation in Terms of the Metric Four Vector,” Found. Phys. Lett. (in review); (e) — “Derivation of the Dirac Equation from the Evans Wave Equation,” Found. Phys. Lett. (in review).

. D. K. Sen, Fields and/or Particles, Academic Press, London and New York, 1968, p. viii.

. B. P. Kosyakov, "Radiation in electrodynamics and in Yang-Mills theory," Sov. Phys. Usp. 35(2), Feb. 1992, p. 135, 141.

. (a) T. E. Bearden, "Giant Negentropy from the Common Dipole," Proc. Congr. 2000, St. Petersburg, Russia, Vol. 1, July 2000, p. 86-98; also published in J. New Energy, 5(1), Summer 2000, p. 11-23. See also (b) M. W. Evans, T. E. Bearden, and A. Labounsky, "The Most General Form of the Vector Potential in Electrodynamics," Found. Phys. Lett., 15(3), June 2002, p. 245-261.

. (a) Bearden, Energy from the Vacuum: Concepts and Principles, ibid., 2002, Chap. 3; (b) — "Extracting and Using Electromagnetic Energy from the Active Vacuum," in M. W. Evans (ed.), Modern Nonlinear Optics, Second Edition, 3 vols., Wiley, 2001, Vol. 2, p. 639-698. The 3 vols. comprise a Special Topic issue as vol. 119, I. Prigogine and S. A. Rice (series eds.), Advances in Chemical Physics, Wiley, ongoing.

. T. E. Bearden, Fact Sheet 2003-01, “The Source Charge Problem: Its Solution and Implications,” Aug. 18, 2003.

. Tom Van Flandern, Phys. Lett. A, Vol. 250, Dec. 21, 1998, p. 8-9.

. E.g., see Jackson, Classical Electrodynamics, 2nd Edn., ibid., p. 222-223.

. R. Feynman, QED: The Strange Theory of Light and Matter, Princeton University Press, 1988 discusses Feynman's excellent interpretation of the conventional negative energy hole in the Dirac Sea. The reader is alerted that there are different interpretations for negative energy entities, and there is still much disagreement on the subject among scientists.
Our own use of the term “Dirac hole” is actually a little different from the standard use of Dirac's equation. His equation prescribes
a continuum of energy levels above E = m, and a continuum of energy levels below E = "m, while in between there is a gap with no energy eigenstates. We strongly believe (and COP > 1.0 VP EM systems seem to substantiate) that the region from E = 0 to
E =
"m is also a region that can be a special kind of Dirac sea in the form of a nonquantized negative energy scalar potential, filled with the equivalent of negative energy electrons (so to speak), but with the equivalent Dirac negative energy electrons “nonseparated” because of the absence of quantization.
Another way of seeing this is to view this region as a region where the quantized particles (holes) can in fact use the duality principle to exist in continuous nonquantized form, as far as their interactions are concerned. This “nonquantized” negative energy potentialization can interact with the normal positive energy overpotentialization of electrons in a normal electron current, partially or totally depotentializing them of their positive energy or some of it. This
depotentialization or fractional depotentialization occurs without pair annihilation radiation, because of the absence of quantized pairs (of real electron and positron). What happens is that the normal spacetime curvature for the positive energy potentialization merely relaxes.
It is a method of directly engineering the associated spacetime curvature, and thus of “directly regauging” the potentialized electrons in a power current being furnished to the system's input section from an outside power source. We believe the phenomenon happens in the Coulomb gauge, or self-evokes the Coulomb gauge, so that only the magnetic vector potential A is quantized and the scalar potential
 is not quantized.

Also, in the Coulomb gauge the scalar potential  has “instantaneous velocity”, so such a potential formed at the output section of the system would instantly also appear in the input section—a multiply connected spacetime phenomenon also exhibited by Bohm's quantum potential. One might refer to this region between E = 0 and E = "m , when some of the holes are unfilled (so to speak), as the Dirac “subsea” or “fractional Dirac sea” or some such. Its significance is that quantization functions and limitations are transcended by continuous functions in the Coulomb gauge.
At any rate, it appears that in a COP > 1.0 VP EM system, electrons can be lifted from this peculiar region to leave a special kind of nonquantized “holes” in the presence of curved spacetime. Or, one may view this as simply the spacetime curving to change the “energy density of that spacetime region's nonquantized scalar potential
” in the Coulomb gauge. In that case, the potential's existence in the Coulomb gauge (or pseudo-Coulomb gauge) means that it functions in a multiply connected spacetime (or a pseudo-multiply connected spacetime).
In susceptible COP > 1.0 VP EM systems with sharp gradients, this functioning does appear and the phenomenology does occur. For all intents and purposes, this odd negative energy potential just “directly appears” in the input section, where it can and will “eat” or absorb some of the
positive energy potentialization of the incoming powered electron currents from the external power source. This “eating” of the incoming potentialization (and Poynting energy flow) avoids pair annihilation and the emitting of the usual pair annihilation radiation photons. It just “relaxes” the incoming potential energy of the incoming current to less potential energy and less curved spacetime.
Our use of the term “Dirac hole” with respect to COP > 1.0 VP EM systems in this fact sheet is thus in a special sense where (i) quantization is avoided as well as pair annihilation, and (ii) unquantized Coulomb gauge negative energy potential appears in the input section of the system to reduce or “eat” positive energy potentialization transported on the incoming electron currents. This is an hypothesis empirically formulated from observing such phenomena in COP > 1.0 VP EM systems with and without sharp gradients. It is also a correction to and updating of appropriate sections of my book,
Energy from the Vacuum, 2002, ibid.
Obviously much additional scientific work still needs to be done on this unusual phenomenon.

T. E. Bearden, Energy from the Vacuum: Concepts and Principles, 2002, ibid., Chapter 9: “The Supersystem and Remarks on Gravity, Antigravity, and Testing.”

. To see how Maxwell's equations are conventionally regauged symmetrically, see J. D. Jackson, Classical Electrodynamics, Wylie, New York, Third Edition, 1999, p. 240-246.

. For a discussion of asymmetrical regauging, see M. W. Evans, P. K. Anastasovski, T. E. Bearden et al., “Some Notes on `Asymmetric Regauging',” J. New Energy 4(3), Winter 1999, p. 325-326.

. Hence our wry comment that one pays the electrical power company to use a closed current loop circuit, engage in a giant wrestling match inside its generators, and deliberately lose.

. The first law of thermodynamics thus requires a minor correction. Presently, any change in an external parameter—such as the potential V—of a system is defined as work a priori. That is a non sequitur that, if true, would exclude gauge freedom from physics. Hence gauge field theory and much of physics would be wrong. Change of magnitude of the energy of a parameter is only work if the energy to make the change of parameter is input in a different form than the energy of the parameter being changed, and then work has to be done to change its form before regauging occurs.

. Robert Bruce Lindsay and Henry Margenau, Foundations of Physics, Dover, New York, 1963, p. 217. Quoting: “…the condition of equilibrium is the condition of maximum entropy."

. One method that we previously published is to switch to an external circuit a source of static potential as a momentary input section that potentializes the external circuit, with the circuit's electrons momentarily pinned so that the current is zero during the potentializing process. In short, the external circuit is simply regauged by energy transfer, and none of the regauging energy is dissipated as work during the regauging part of the cycle. Then the source is switched back out of the circuit and the external potentialized circuit is simultaneously completed (e.g., by a diode and resistor) so that the current can only flow in one direction when the circuit excitation (potentialization) decays and pushes current through the resistor load, producing power. In short, pin the circuit's current while potentializing the circuit in a static mode with a static potential V. Disconnect the static potential source, simultaneously completing the remaining circuit with a one-way current valve and load, and discharge the regauged potential energy in a normal dynamic circuit fashion with current flowing. If enough charges q are pinned during potentialization, the energy Vq discharged in the load during circuit decay can exceed the energy one must expend for efficient switching.

. For a method of extracting free energy from a stress potential's composite Whittaker internal bidirectional energy flows, see Bedini's battery-charging method in (a) John C. Bedini, “Device and Method for Pulse Charging a Battery and for Driving other Devices with a Pulse,” U. S. Patent #2003/0117111 A1, June 26, 2003. A simplified description of the process is given in (b) T. E. Bearden, "Bedini's Method For Forming Negative Resistors In Batteries," J. New Energy, 5(1), Summer 2000, p. 24-38. Simply put, a battery powered circuit is not really a true closed current loop, since mostly ion currents move between the plates inside the battery but not in the external circuit, and the electron currents move mostly in the external circuit half-loop between one plate and the other, outside the battery rather than inside between the plates. By sharply “back-popping” the battery for recharging while the battery is in powering mode, these two “half-loop” currents can be dephased and made antiphased. With such a “back-pop”, the heavy internal ion currents keep bearing down in powering mode momentarily because of their large inertia, but are now overpotentialized and thus deliver more energy for powering. The electrons in the “back-pop” pile up on the plate attempting to repel the incoming ions back into charging mode. This dramatically increases the charge density on the plate, resulting in overpotentialization (typically 100 volts or so in a 12 volt lead-acid battery) and creation of a significant local curvature of spacetime. The electrons that “pile-up” on the plate—in attempting to reverse the oncoming ion flow direction—produce this overpotential (regauged voltage) which reaches in both directions: onto the oncoming but slowing ions in powering mode and back out into the circuit in powering mode, overpotentializing the circuit as well and thereby resulting in collection of excess energy in that external circuit, for additional powering. We point out that the free regauging energy collected is a function of (V)q, and is limited only by q for a given overpotential (say, for 100 volts). Then as the ions reverse and move backwards in charging mode, the applied pulse is abruptly terminated, which evokes Lenz's law and causes a further sharp jump in overpotentialization. In a 12-volt battery, this second overpotential may be some 400 volts or even more. Again, this further overpotentializes the ions now moving in recharging direction, so much more recharging energy is delivered inside the battery. At the same time, the overpotential also flows in the other direction back out into the external circuit, again overpotentializing its Drude electrons for delivery of additional powering (voltage x amps). The net result is that with very adroit and meticulously timed switching, the battery can be recharged in great overpotential spurts while the external circuit continues to be powered to include substantial additional captured regauging energy from the overpotentialization in powering mode. The simplest way of applying the Bedini method is to use the free overpotentialization on a second battery not engaged in powering the system, just to recharge it, while powering normally from a primary battery. Then as the primary battery heads toward significant normal discharge, simply switch the batteries, and then continue the periodic switching of primary and secondary batteries as appropriate. In this manner, a legitimate continuous self-powering VP COP = " system can be and has been demonstrated by Bedini that obeys the laws of physics and NESS system thermodynamics. He has also discovered a further quite marvelous improvement to the process by several orders of magnitude, and is preparing a formidable patent on that new process as well. With proper development funding, Bedini will be able to recharge quite large batteries with extraordinary swiftness, using a matchbox-sized little switcher-charger and taking the excess potential energy directly from the vacuum via highly amplified self-regauging, as a direct application of the gauge freedom principle. Again, gauge freedom already implies that one can freely change the potential energy of an EM system at will. Bedini has simply found practical though unusual ways to directly apply that proven principle.

. Paul Davies, Superforce: The Search for a Grand Unified Theory of Nature, Simon and Schuster, New York, 1984, p. 105.

. An exchange between vacuum flux and the charge or mass creates a change in the energy density of the vacuum, which is a change in the energy density of space, which is a curvature of spacetime. Any force is a massless curvature of spacetime acting on a mass. Mass is a component of force, as can be seen by F " "p/"t = m"v/"t + v"m/"t. Both expansion expressions contain a mass term.

. (a) T. D. Lee, "Question of Parity Conservation in Weak Interactions," Phys. Rev., 104(1), Oct. 1, 1956, p. 254-259; (errata in Phys. Rev. 106(6), June 15, 1957, p. 1371); (b) T. D. Lee, Reinhard Oehme, and C. N. Yang, "Remarks on Possible Noninvariance under Time Reversal and Charge Conjugation," Phys. Rev., 106(2), 1957, p. 340-345.

. C. S. Wu et al., "Experimental Test of Parity Conservation in Beta Decay," Phys. Rev., Vol. 105, 1957, p. 1413.

. T. D. Lee, Symmetries, Asymmetries, and the World of Particles, U. Wash. Press, Seattle, 1988, p. 11.

. As an example, (a) William C. Reynolds, Thermodynamics, 2nd Edn., McGraw-Hill, New York, 1968, p. 250-252 gives an analysis of the Carnot heat pump. A nice section on heat pumps and refrigerator Carnot cycles is given in (b) David Halliday and Robert Resnick, Fundamentals of Physics, Third edition extended, Wiley, NY, 1988, Chapter 22.

. E.g., see Halliday and Resnick, Fundamentals of Physics, 1988, ibid., p. 518, Sample Problem 5.

. Any two points in the circuit (or in the universe, for that matter) that are at differing potential in one's frame, constitute at least a weak source dipolarity. This dipolarity is a broken symmetry in the vacuum flux, and so it is continuously pouring out at least some real EM energy extracted from the virtual photon flux of the vacuum, unaccounted by present science. More of interest, any two points in a circuit or EM device that are at different potentials in one's frame, constitute a source dipolarity extracting energy from the vacuum. This is Gabriel Kron's open path, which he discovered decades ago in a General Electric project for the U.S. Navy at Stanford University, with the Network Analyzer simulator. He was never permitted to totally reveal the secret of his “open path”. In the Network Analyzer project in the 1930s, Kron also built a true negative resistor that could power itself and its connected Network Analyzer simulator with the generator disconnected. See (a) Gabriel Kron, “Electric circuit models of the Schrödinger equation,” Phys. Rev. 67(1-2), Jan. 1 and 15, 1945, p. 39. Quoting: "Although negative resistances are available for use with a network analyzer, in practice it is more convenient to use a second type of circuit, in which the positive and negative resistances are replaced by inductors and capacitors and the dc currents and voltages are replaced by ac currents and voltages of fixed frequency. The use of the second type of interpretation is equivalent to multiplying the wave equation by i = ""1." The first clause states very plainly that true negative resistors were indeed available—this was one that Kron slipped through his censors. See also (b) Gabriel Kron, “Electric circuit models of the Schrödinger equation,” Phys. Rev. 67(1-2), Jan. 1 and 15, 1945, p. 41. Quoting: “Now a value E of the negative resistances, at which the generator current becomes zero, represents a state at which the circuit is self-supporting and has a continuous existence of its own without the presence of the generator, as the negative resistances just supply the energy consumed by the positive resistances. (If the circuit contains inductors and capacitors, the circuit is a resonant circuit and it oscillates at its basic frequency.) … When the generator current is positive the circuit draws energy from the source, and when the current is negative the circuit pumps back energy into the source. At zero generator current the circuit neither gives nor takes energy, and theoretically the generator may be removed.” In that quotation, Kron was required to insert the word “theoretically”, to prevent the blunt statement that such had actually been done.

. For a complete story and appropriate references, see (a) T. E. Bearden, Energy from the Vacuum, ibid., 2002, entries under Kron condition, Kron negative resistor, and Kron, Gabriel. It is indeed true that some known scientists have developed COP>1.0 and COP = " EM vacuum-powered systems in the past, and their work has been suppressed. See also (b) .W. Lynn and R.A. Russell, "Kron's Wave Automaton," Physical Structures in System Theory, J. J. Dixhoorn and F. J. Evans (Eds.), Academic Press, London, 1974, p. 131. Quoting: "Kron has never published details of his method of making the polyhedron self-organizing, although his published results show that in this state it has some remarkable properties, associated with harmonic integrals on multiply connected spaces." We also point out that multiply connected spaces may well involve Bohm's quantum potential; see (c) David J. Bohm, "A Suggested Interpretation of the Quantum Theory in Terms of 'Hidden' Variables, I and II." Phys. Rev., 85(2), Jan. 15, 1952, p. 166-179 (Part I); 180-193 (Part II).

. Phrase used by Tesla (who also used the more fundamental longitudinal EM waves) to describe his view of the transverse EM wave model, in Nikola Tesla, "The True Wireless,” Electrical Experimenter, May 1919.

. Kenneth S. Deffeyes, Hubbert's Peak: The Impending World Oil Shortage, Princeton University Press, Princeton, NJ, 2001.

. On an upbeat note, the Foundations of Physics series of journals is scientifically interested in extraction of EM energy from the vacuum and in the broken symmetry of opposite charges. Accordingly a series of important scientific papers dealing with energy from the vacuum have been published, with a few here and there in some other journals as well. For example, see (a) M. W. Evans, T. E. Bearden, and A. Labounsky, "The Most General Form of the Vector Potential in Electrodynamics," Found. Phys. Lett., 15(3), June 2002, p. 245-261. This paper contains the giant negentropy of the common dipole, proposes a solution to the dark energy problem of astrophysics, and clearly shows vacuum energy currents; (b) M. W. Evans, P. K. Anastasovski, T. E. Bearden et al., "Runaway Solutions of the Lehnert Equations: The Possibility of Extracting Energy from the Vacuum," Optik, 111(9), 2000, p. 407-409; (c) — "Classical Electrodynamics without the Lorentz Condition: Extracting Energy from the Vacuum," Physica Scripta, 61(5), May 2000, p. 513-517; (d) — “The Aharonov-Bohm Effect as the Basis of Electromagnetic Energy Inherent in the Vacuum,” Found. Phys. Lett. 15(6), Dec. 2002, p.561-568; (e) — “Effect of Vacuum Energy on the Atomic Spectra,” Found. Phys. Lett., 13(3), June 2000, p. 289-296; (f) — “Operator Derivation of the Gauge Invariant Proca and Lehnert Equations: Elimination of the Lorenz Condition,” Found. Phys., 30(7), July 2000, p. 1123-1129; (g) — “Explanation of the Motionless Electromagnetic Generator with O(3) Electrodynamics,” Found. Phys. Lett., 14(1), Feb. 2001, p. 87-94; (h) — “Explanation of the Motionless Electromagnetic Generator by Sachs's Theory of Electrodynamics,” Found. Phys. Lett., 14(4), Aug. 2001, p. 387-393; (i) T. E. Bearden, “Extracting and Using Electromagnetic Energy from the Active Vacuum,” Modern Nonlinear Optics, M. W. Evans (Ed.), 2nd Edn., Vol. 2, p. 639-698.

. A. S. Eddington, The Nature of the Physical World, Macmillan, New York, 1929, p. 74.

. G. M. Wang, E. M. Sevick, Emil Mittag, Debra J. Searles, and Denis J. Evans, "Experimental Demonstration of Violations of the Second Law of Thermodynamics for Small Systems and Short Time Scales," Phys. Rev. Lett., 89(5), 29 July 2002, 050601.

. However, we strongly point out that, if the national labs seek out private inventors who are known to hold patents and/or have working overunity prototypes, the government must be directed to sign noncircumvention agreements as well as nondisclosure agreements. Otherwise, the labs all seek and obtain patents, and circumvention is a strong threat to any legitimate inventor attempting to work with them. The DARPA contractual practice of inserting an insidious “March In Rights” clause in the contract, giving the government (i.e., a single bureaucrat) the authority to seize the inventor's patent and run with it, is intolerable to any sane inventor and borders on being unethical piracy.

. T. E. Bearden, Energy from the Vacuum: Concepts and Principles, Cheniere Press, Santa Barbara, CA, 2002.

. Albert Einstein, "Foreword," in Max Jammer, Concepts of Space: The History of Theories of Space in Physics, Harvard University Press, Cambridge, Massachusetts, 1969, p. xi-xii..

. Lindsay and Margenau, Foundations of Physics, 1963, ibid., p. 25.

. Max Planck, in G. Holton, Thematic Origins of Scientific Thought, Harvard University Press, Cambridge, MA, 1973.



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