Bearden Fact Sheet Leyton Hierarchies of Symmetry updated 04 07 2004


Leyton's Hierarchies of Symmetry: Solution to the Major Asymmetry Problem of Thermodynamics

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© T. E. Bearden

August 22, 2003; updated July 4, 2004.

The Problem: Thermodynamics Has a Temporal Asymmetry Problem, Recognized for a Century, Because the Second Law Excludes Negative Entropy processes and Nature does not.

"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."

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

Kosyakov {} states the problem bluntly:

"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?”

Facts Bearing on the Problem: Characteristics of the Second Law and Its Experimental Falsification.

“…the problem persists for situations arbitrarily close to equilibrium, and for all deterministic dissipative dynamics."

More Facts: Leyton's New Object-Oriented Geometry and Hierarchies of Symmetry vs. the older Klein Geometry.

The Resulting Solution: Adopt Leyton's More Advanced Object-Oriented Geometry, Apply Leyton's Hierarchies of Symmetry, and Rewrite the Second Law of Thermodynamics.

“Given some available controlled order (available controlled energy) in a system, this initial controlled order will either remain the same or be progressively disordered and decontrolled over time by subsequent entropic interactions.”

Or, simply put, dS/dt " 0. The system is assumed close to equilibrium but still out of it, and is merely decaying back to equilibrium, thus increasing its entropy. If the system is far from equilibrium and is not decaying back to equilibrium, its entropy can even be increasing. Hence this Second Law statement does not apply to that system. An example is any nonequilibrium steady-state (NESS) system. Another example is any system while departing—statistically or deterministically—from equilibrium, thereby reducing its entropy by such departure.

"First a negative entropy interaction occurs in the system to produce some controlled order (available controlled energy). Then that initial available controlled order will either remain the same (not be dissipated) or be progressively disordered and decontrolled (dissipated) by subsequent entropic interactions over time, unless additional negative entropy interactions also occur and intervene."

Or, simply put, " " < dS/dt < + " if negative entropy interactions also occur as well as positive entropy interactions.

Implications: We argue that:

"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:

An earlier version of this Fact Sheet is published in Explore, 12(6), 2003, p. 59-61.

Fact Sheet 2003-03

14

. 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.

. Boltzmann's suggestion was that the world is simply a product of a chance fluctuation into a state of very low entropy[Author ID1: at Sat Feb 22 21:50:00 2003 ]. Little or no real progress has been made on the problem since then.

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

. Energy density estimates vary, but an acceptable estimate is given by R. Podolny, Something Called Nothing: Physical Vacuum: What Is It?, Mir Publishers, Moscow, 1986, p. 181. In mass units, the energy density of the virtual particle flux of vacuum is on the order of 1080 grams per cubic centimeter.

. Price, ibid., p. 36.

. See (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. (b) — Fact Sheet, “The Source Charge Problem: Its Solution and Implications,” Aug. 18, 2003. In this fact sheet, we give the exact physical mechanism that coherently integrates absorbed totally disordered virtual photon energy into real observable photons. The energy of each absorbed virtual photon is changed to a differential change of the mass m of the absorbing charge(s). Iterative changes thus algebraically sum since mass is unitary. When the mass differential reaches sufficient magnitude to constitute the energy for an observable photon, the zitterbewegung of the vacuum causes expulsion of an observable photon, decaying the mass back down to base level to start the process again. We have nominated the source charge (using this mechanism) as the first known physical system that continuously produces negative entropy, along the lines theoretically predicted by Evans and Rondoni {15}. We have also nominated the coherent summation by the mass of the charge as the first known physical mechanism continuously producing negative entropy and thus falsifying the present form of the Second Law. See also (c) 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.

. 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.

. See Robert Bruce Lindsay and Henry Margenau, Foundations of Physics, Dover, NY, 1963, p. 213. Quoting: "Equilibrium states are the only ones that are capable of explicit analysis in thermodynamics…" Quoting, p. 217. "Non-equilibrium conditions cannot be specified by variables of state, and their entropy cannot be computed. …the condition of equilibrium is the condition of maximum entropy."

. For a statistical fluctuation to occur, the system initially in equilibrium must depart from equilibrium, thereby reducing system entropy since equilibrium is the maximum entropy condition. The departure thus constitutes a negative entropy operation, contradicting the Second Law. By “fluctuation” one also implies that the initial departure from equilibrium is accompanied by a return back to equilibrium, and the “return portion” of the excursion is a positive entropy-producing operation.

. A most useful and rigorous transient fluctuation theorem is given by D. J. Evans and D. J. Searles, "Equilibrium microstates which generate second law violating steady states," Phys. Rev. E, Vol. 50, 1994, p. 1645-1648.

. Gavin E. Crooks, "Entropy production fluctuation theorem and the nonequilibrium work relation for free energy differences," Phys. Rev. E, Vol. 60, 1999, p. 2721-2726

. 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.

. Under proper conditions, the normally entropic reactions in a significant region of a solution can therefore “run in reverse” negentropically because of the departure phase of a transient fluctuation, lasting up to two seconds. In such a “reversed reactions” situation, it is possible for two like charges to attract rather than repel. Hence two H+ ions (two protons) can sometimes attract together sufficiently for each to enter the strong force region of the other, thereby forming a quasi-nucleus. As the “driving fluctuation excursion” peaks and then reverses, this quasi-nucleus can remain bound by the strong force as the law of attraction and repulsion of charges reverts back to normal. In the increasingly excited state of the quasi-nucleus, the quasi-nucleus “tightens” due to its more rapid change in strong force than in the Coulomb force. Hence one of the protons “decays” to a lower state by flipping the orientation of one of its quarks, thereby turning into a neutron. The result is the anomalous formation of a normal deuterium ion. The formation of excess deuterium is one of the direct indicators of “cold fusion” experimentally shown in hundreds of cold fusion experiments. We have nominated the “fluctuation reversal of reactions” effect of transient fluctuations as a primary mechanism for legitimate cold fusion reactions. Other ion combinations would result in the emergence of other anomalous quasi-nuclei decaying into real cold transformation nuclei. We give some of these additional anomalous cold fusion reactions in T. E. Bearden, Energy from the Vacuum: Concepts and Principles, Cheniere Press, Santa Barbara, CA, 2002, Chapter 10. Cold Fusion: Low Spatial-Energy Nuclear Reactions at High Time-Energy.

. 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 Steven Weinberg, Dreams of a Final Theory, Vintage Books, Random House, 1993, p. 109-110 for a very clear statement of vacuum polarization by the “isolated” charge.

. For definitions of gauge and gauge freedom, see the definitions guide and explanations at http://explanation-guide.info/meaning/Gauge-theory.html.

. E.g., for the symmetrical regauging of the classical electrodynamic equations, see J. D. Jackson, Classical Electrodynamics, Second Edition, Wiley, New York, 1975, p. 219-221; 811-812. In symmetrically regauging the Heaviside-Maxwell equations, electrodynamicists assume that the potential energy of a system can be freely changed at will (i.e., that the system can be asymmetrically regauged). This is also included under one of the major principles of quantum field theory, known as gauge freedom. But electrodynamicists arbitrarily do two asymmetrical regaugings of the Maxwell-Heaviside equations in succession, thereby carefully and very specially selecting the regauging so that the two new free force fields that emerge in the system are equal and opposite. This effectively “locks up” any received excess symmetrical regauging energy as physical stress in the system. There is thus no net resultant free force field to dissipate the free excess system energy from regauging, and thereby to perform free work in a load.

. Dilip Kondepudi and Ilya Prigogine, Modern Thermodynamics: From Heat Engines to Dissipative Structures, Wiley, Chichester, 1998, reprinted 1999 with corrections, p. 459. Present thermodynamics is violated in rarefied media where local equilibrium fails, in strong gradients (about which little is known, either theoretically or experimentally), and in long-lasting memory effects occurring in materials and in many nonequilibrium processes. Other violations due to fluctuations are shown by Wang et al. (cited above).

. The “precursor” referred to is the force-free field (as a set of energy flows) as it actually exists in space and vacuum in the absence of mass. Once one pays to form a source of “static” potential or “static” field, one has actually formed a source of steady EM energy flows extracted directly from the vacuum (particle physics view) or from the curvature of spacetime (relativistic view). Indeed, the virtual particle flux of vacuum becomes identically “energy”, as does spacetime itself—thereby resolving Feynman's lament that “It is important to realize that in physics today, we have no knowledge of what energy is." [Richard P. Feynman, Robert B. Leighton, and Matthew Sands, The Feynman Lectures on Physics, Addison-Wesley, Reading, MA, Vol. 1, 1964, p. 4-2]. We also resolve his lament that "One of the most important characteristics of force is that it has a material origin, and this is not just a definition. … If you insist upon a precise definition of force, you will never get it!" [Feynman et al., ibid., p. 12-2]. A preliminary draft paper has been prepared as T. E. Bearden, “Precursor Engineering: Directly Altering Physical Reality,” draft, 2004. In the future we hope to finish the paper and publish it in final form.

. 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.

. Also see I. M. Yaglom, Felix Klein and Sophus Lie: Evolution of the Idea of Symmetry in the Nineteenth Century, Birkhäuser, Boston, MA, 1988.

. (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.

. (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. See also (b) H. Paul and R. Fischer, “{Comment on “How can a particle absorb more than the light incident on it?'},” Am J. Phys., ibid. Scientists in the area just use a change of reaction cross section. EM field and potential intensities are defined in terms of a “static unit point charge's” scattering. If the same charge is resonant, it scatters more energy, much as a strongly churning rock on the bottom of a river displaces more water than does the same rock fixed on the bottom. Thermodynamically, that gives
COP > 1.0—in fact, it provides COP = 18.

. Scientists in the area do not speak of the thermodynamic coefficient of performance of their experiments. Instead, they speak of the change in reaction cross section. EM field and potential intensities are defined in terms of a “static unit point charge's” reaction cross section and resulting diverting of energy from the energy flows comprising the field or potential. If the same charge is resonant at the input light energy frequencies, its reaction cross section appreciably increases and it “collects” or diverts or “intercepts” more energy—from the field or potential as a set of energy flows—than when the same charge is static. The situation is roughly analogous to the diverting of a river's flow around a rock that is being churned violently back and forth at right angles to the flow, as compared to the diversion of water flow around the same rock when the rock is fixed stationary. Thermodynamically, the free 18-fold increase in reaction cross section gives COP > 1.0—in fact, in that case the thermodynamic COP = 18.

. A close colleague and I have filed a rather formidable patent application for possibly the first practical negative entropy engineering application of electromagnetic circuits. The circuitry is employed in an entirely different manner from that prescribed in the textbooks. The invention converts seemingly ordinary impedance components and sections into true negative resistors freely receiving excess EM energy from their active external vacuum environment. This results in the output of much more EM energy than the operator himself inputs—by repeatedly evoking free asymmetrical regauging which increases the potential energy circulating in the circuit and then dissipated in the loads to power them. Conservation of energy is obeyed at all times, since the excess energy is freely input from the active environment, much like a common home heat pump process. Negative entropy processes are quite real in nature, and they can also be evoked and utilized in otherwise somewhat ordinary electrical circuits. In short, Leyton's epochal work has very practical application, and we expect to see it vigorously applied to electrical power systems in the future.

. E. T. Whittaker, “On the Partial Differential Equations of Mathematical Physics,” Mathematische Annalen, Vol. 57, 1903, p. 333-355. In this paper, Whittaker demonstrated that any scalar potential decomposes mathematically into a set of longitudinal EM wave energy flows.

. E. T. Whittaker, “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. The paper was published in 1904 and orally delivered in 1903. This paper initiated what today is known as “superpotential theory”. Here Whittaker showed that any EM field (or wave, etc.) mathematically decomposes into a set of differential functions imposed upon two scalar potentials. By applying Whittaker's 1903 paper to each of the two base scalar potentials, it follows that further decomposition into interfering sets of longitudinal EM wavepairs occurs. Hence all EM potentials and fields decompose into bidirectional sets of longitudinal EM wave energy flows, with differential functions applied to those sets. It follows from these considerations that there exists a far more fundamental electrodynamics that is comprised of sets of longitudinal EM wave energy flows, with shaping and controlling differential functions applied. This leads directly to negentropic engineering, where one “pays” a little to shape, direct, and control large sets of such Whittaker energy flows, then interacts the resulting large energy dynamics with matter to produce large force system dynamics acting in the matter to change it as one wishes. This is a form of negentropic engineering, since one only “pays a little work” to shape and control “a lot of energy” that then interacts with matter to form force dynamics in the interacting mass system.

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

. Dr. M. King Hubbert, in response to remarks by Exxon's David Nissen. See the web article http://www.hubbertpeak.com/hubbert/to_nissen.htm.

. For excellent, professional briefings on the situation with oil, natural gas, and other aspects of the energy crisis, not considering the terrorist threat scenarios added to it, the reader is encouraged to, see speeches and briefings by Matthew R. Simmons, President, Simmons & Company International, accessible on http://www.simmonsco-intl.com/research.aspx?Type=msspeeches.

. To get a “feel” for the vulnerability of the power grid to terrorist use of cyber attack, see the PBS interview with Joseph Weiss, control systems engineer with KEMA Consulting and a leading expert in control system security, and technical manager for 15 years at the Electric Power Research Institute (EPRI) and its Enterprise Infrastructure Security Initiative (EIS). The interview is carried at http://www.pbs.org/wgbh/pages/frontline/shows/cyberwar/interviews/weiss.html. Weiss stated, “My very, very, very strong feeling is, if and when we get hit, we will never know why we were hit. All we will know is breakers are opening, valves are closing, certain things are happening. But we won't have a clue as to why.” In answer to the question, “What's the worst-case power scenario, power we're talking here—power lines, power grid?” Weiss replied: “Absolute worst? I won't even say absolute, but a very worst case could be loss of power for six months or more.” He also confirmed the loss of power could be over as big an area in the U.S. as one wanted. If one then allows for the terrorist assets already inserted into the United States and simply waiting for the “go” signal, and factors in some additional key physical strikes—on refineries, pipelines, and major power plants themselves including major nuclear power plants— to the cyber warfare strikes being confirmed by Weiss, one begins to grasp the full economic implications of the critical vulnerability of our centralized power system. It can indeed be largely laid in the dirt or terribly crippled for long periods of time. The nation is simply not prepared to withstand and survive economically in the face of such determined attacks.



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