Prof. Dr.-Ing. Konstantin Meyl: Vortex Physics Laws in physics have to be accepted 19th NPA Conference, Albuquerque Friday July 27, 2012, 2:15 PM, 1h Vortex Physics and its consequences like: * basic forces, * derivation of the gravitational force, * extended field theory, * big bang nonsense, * calculation of all particles and atomic cores Prof. Dr.-Ing. Konstantin Meyl: about vortex physics Spherical Symmetry The law of “inverse square“ of distance field source (E or H): projection screen = x L² L = distance to the source Prof. Dr.-Ing. Konstantin Meyl: about vortex physics Spherical Symmetry The law of “inverse square“ of distance field source (E or H): projection screen = x L² L = distance to the source E 1/r² H 1/r² surface of a sphere = 4r² r = radius of the sphere Prof. Dr.-Ing. Konstantin Meyl: unified theory conclusion: about the speed of light from E, H 1/r2 and rc follows: • the field determines the length measures (what is 1 m) • the field determines the velocities v (in m/s) • the field determines the speed of light c [m/s] • Measurement of the speed of light is made with itself • measured is a constant of measurement c = 300.000 km/s the speed of light c is not a constant of nature! Prof. Dr.-Ing. Konstantin Meyl: vortex physics about the Big Bang Theory problem solving the Doppler-effect is based on the addition theorem of velocities v c - v: c c+ v Prof. Dr.-Ing. Konstantin Meyl: vortex physics Big Bang contradicting laws of physics fixed stars are without any blue shift? because the galaxies are contracting slowly other galaxies outside our galaxy have to show a red shift? even if they don’t move the red shift increases with an accelerated contraction (Nobelprize 2012 Perlmutter, Schmidt und Riess) problem solving Prof. Dr.-Ing. Konstantin Meyl: vortex physics About the light carrying aether If electromagnetic waves would be bonded to a stationary aether, we should measure the proper motion of earth and sun as a wind of the aether What determines the speed of light? wind of the aether earth sun Prof. Dr.-Ing. Konstantin Meyl: Potsdam 1881 Michelson Interferometer Wirbelphysik Prof. Dr.-Ing. Konstantin Meyl: vortex physics field-dependent length contraction statement of the law in physics E 1/L² H 1/L² field source scale of length L Prof. Dr.-Ing. Konstantin Meyl: unified theory Observation of an action of force one body is in the field of another from E, H 1/L2 follows: the distance is getting smaller the bodies are attracting each other Prof. Dr.-Ing. Konstantin Meyl: unified theory curvature of space the earth in the gravitational field of the sun E, H 1/r2 Orbital curvature depending on the field R.J. Boscovich: the earth is respiring unobservable! De spatio et tempore, ut a nobis cognoscuntur, 1755. Ruder Boscovich 1755 E, H 1/r2 R.J. Boscovich: the earth is respiring unobservable. De spatio et tempore, ut a nobis cognoscuntur. Prof. Dr.-Ing. Konstantin Meyl: unified theory interactions, forces Auxiliary terms = formalization of our imagination Examples for auxiliary terms: (Mass or charge) Gravitational law (central force + centrifugal force) m1 m2 1 F = G· ——— ~ —— r² r² (gravitational mass or inertial mass) Coulomb‘s law (force in the electric field) 1 Q1 Q2 1 F = ——— · ——— ~ —— 4or r² r² Prof. Dr.-Ing. Konstantin Meyl: unified theory Speed reduction in a field field dependent speed of light experimental examples about: E, H 1/c2 field-or gravitational lenses Deflection of light (Einstein, at the eclipse 1919) observer x gravitational field star Prof. Dr.-Ing. Konstantin Meyl: unified theory curvature of space in the gravitational field of a heavenly body An experimental example: L[m] 1/E,H with c [m/s] Prof. Dr.-Ing. Konstantin Meyl: unified theory Length contraction in a field cause: only electric or magnetic field More experimental examples: E, H 1/L2 field- or gravitational lenses deflection of light Space curvature electrostriction (piezo speaker) magnetostriction Question: is it always the electromagnetic field? Prof. Dr.-Ing. Konstantin Meyl: unified theory electromagnetic interaction caused by open field lines E, H 1/L2 Example charged mass points (e¯, e+, Ions,...): As a consequence of open field lines: strong attraction or repulsion Prof. Dr.-Ing. Konstantin Meyl: unified theory Derivation of Gravitation caused by closed loop field lines E, H 1/L2 Example: uncharged Mass points (n°, atoms,...) As a consequence of closed loop field lines: weak attraction, no repulsion Prof. Dr.-Ing. Konstantin Meyl: unified theory From Subjectivity to Objectivity physical standpoints the following physical standpoints can be distinguished: Subjectivity Relativity Objectivity observal laboratory physics mediator role transformation not observal. exemplary theories and their representatives: Newton Maxwell Poincaré Einstein Boscovich Meyl with the associated transformation: Galilei-transf. for c Lorentz-transf. c constant new transf. c variable Prof. Dr.-Ing. Konstantin Meyl: unified theory Derivation of the standpoints two approaches are possible: example: a signal in a distance (r) from the source approach: r c t (determine distance by signal prop. time) dr cdt + tdc change: case 1: c = constant (total differential) case 2: t = constant dr cdt dr tdc r ct r tc theory of relativity r t theory of objectivity r c Prof. Dr.-Ing. Konstantin Meyl: unified theory Relativity versus Objectivity a comparison of the physical standpoints case 1: c constant r ct theory of relativity r t case 2: t constant r tc theory of objectivity r c from: length contraction variable speed of light follows: time dilatation dependence of meter measure with absolute speed of light Observation domain with absolute time model domain (measurable) many paradoxons x(r) (can only be calculated) without paradoxon M{ x (r)} Prof. Dr.-Ing. Konstantin Meyl: unified theory Relativity - Objectivity model transformation Observation domain model domain (measurable) (only calculable) x(r) M{ x (r)} I. approach II. transform III. calculate VI. compare IV. transform back V. result Prof. Dr.-Ing. Konstantin Meyl: the unified field theory New Transformation I transformation of the length dependency dependency: SRT (observation) AOT (model domain) S.of L. c [m/s] = 1/c²: [Vs/Am] [As/Vm] c = co = constant oo = 1/co² o = constant o = constant c r H [A/m] E [V/m] H 1/r² E 1/r² H 1/r E 1/r B=H [Vs/m²] D=E [As/m²] B 1/r² D 1/r² B 1/r² D 1/r² 1/r 1/r Prof. Dr.-Ing. Konstantin Meyl: the unified field theory New Transformation II transformation examples SRT (observation) capacity: charge: energy: AOT (model domain) C [As/V] = 4r Q [As] = CU W [VAs] = Q²/C C = constant Q = constant W = constant derivation of the law of energy conservation: W = const. relaxation time: sp. conductivity 1 [s] = / [A/Vm] elementary vortices are indestructible: 1 = constant 1/r 1/r Prof. Dr.-Ing. Konstantin Meyl: physical particles derivations with the theory of objectivity 4500 Comparison of the measured with the calculated particle mass. 4000 3500 3000 particle mass related to the electron mass measured gemessen calculated berechnet 2500 2000 1500 1000 500 0 Elementary particle: – 0 – K0 K¯ 0 – n0 0 + ¯ 0 0 ¯ ¯ – F+ Prof. Dr.-Ing. Konstantin Meyl: vortex physics Principle of causality Vortex as a primary form of causality Quantum Physical Approach: Field theoretical Approach: cause effect cause effect quanta fields fields quanta Principle of causality requires a vortex physics The vortex term in the science of Demokrit (460-370 BC) was identical with “natural law“ - the first attempt to formulate a unified physics. Prof. Dr.-Ing. Konstantin Meyl: vortex physics Vortex in Nature Ein physikalisches Grundprinzip •Innen: expandierender Wirbel •Außen: kontrahierender Wirbel •Bedingung für Wirbelablösung: gleich mächtige Wirbel •Kriterium: Viskosität •Folge: röhrenförmige Struktur •Beispiele in d. Strömungslehre: Tornado, Windhose, Wasser-, Abflusswirbel •Beispiel E-Technik: Blitz Prof. Dr.-Ing. Konstantin Meyl: vortex physics another Vortex in Nature Ein physikalisches Grundprinzip •Innen: expandierender Wirbel •Außen: kontrahierender Wirbel •Bedingung für Wirbelablösung: gleich mächtige Wirbel •Kriterium: Viskosität •Folge: röhrenförmige Struktur •Beispiele in d. Strömungslehre: Tornado, Windhose, Wasser-, Abflusswirbel •Beispiel E-Technik: Blitz Prof. Dr.-Ing. Konstantin Meyl: vortex physics vortex and anti-vortex a physical basic principle •Inside: expanding vortex •Outside: contracting anti-vortex •Condition for coming off: equally powerful vortices •Criterion: viscosity •Result: tubular structure •Examples in hydrodynamics: tornado, waterspout, whirlwind, drain vortex •Example in electrical engineering: lightning Prof. Dr.-Ing. Konstantin Meyl: Maxwell approximation Failure of the Maxwell theory problem of continuity in the case of the coming off of vortices In conductive materials vortex fields occur, in the insulator however the fields are irrotational. i.e.hightension cable That is not possible, since at the transition from the conductor to the insulator the laws of refraction are valid and these require continuity! Hence a failure of the Maxwell theory will occur in the dielectric! Prof. Dr.-Ing. Konstantin Meyl: vortex physics Vortices in Microcosm and Macrocosm spherical structures as a result of contracting potential vortices examples: expanding vortex contracting vortex • quantum physics collision processes (several quarks) Gluons (postulate!) • nuclear physics repulsion of like charged particles strong interaction (postulate!) • atomic physics centrifugal force of the electrical attraction enveloping electrons Schrödinger-equation • Newton‘s centrifugal force physics (inertia) gravitation (can not be derived?!) • astro phys. centrifugal f.(galaxy) dark matter, strings, ... Vortex physics seminar Prof. Dr. Konstantin Meyl Albuquerque 2012 Thank you for your attention! • Books available including the presentation: Prof. Dr. Konstantin MEYL, www.meyl.eu K. Meyl: Scalar Waves (all we know about) Furtwangen University, Germany and 1st K. Meyl: Self consistent Electrodynamics Transfer Centre of Scalar wave technology: www.etzs.de ) (in the shop of www.meyl.eu Prof. Dr.-Ing. Konstantin Meyl: Discovery the extended 3rd Maxwell-equation self-consistent electrodynamics solution 2 With the consequences: (field vortices are forming a scalar wave): - prooved by experiments, -reproducible -international accepted 1) div B ╪ 0 (offence against the 3rd Maxwell-eq.) 2) Maxwell-equations are only describing a special case (loosing universality). 3) The existence of magnetic monopoles calls for field vortices and scalar waves 4) Vector potential A is obsolete (→ 1) 5) The new vector of potential density b replaces the vector potential A Prof. Dr.-Ing. Konstantin Meyl: Discovery electric monopoles (charge carriers) consitent with the Maxwell-theory curl H = j + D/t) (Ampère‘s law) div curl H = 0 (acc. to the rules of vector analysis) and: 0 = div j + /t (div D) (eq. of continuity) • relation: j = – vel = D/1 with 1 time constant of eddy currents (relaxation time) div D = el (electric charge density, resp. electric monopoles) Prof. Dr.-Ing. Konstantin Meyl: discovery magnetic monopoles ? extension of the Maxwell-theory – curl E = b + B/t) (law of induction) extended by the potential density b [V/m²], Meyl 1990) – div curl E = 0 and: 0 = div b + /t (div B) (eq. of continuity) • relation: b = – vmagn = B/2 with 2 time constant of the new developed potential vortex div B = magn (magnetic monopoles?! conflicting the 3rd Maxwell-eq.) Prof. Dr.-Ing. Konstantin Meyl: discovery self-consistent calculation extended Poynting vektor S – div S = – div (E x H) = E·rot H – H·rot E – div S = E·( j + D/t ) + H·( b + B/t ) – div S = ½·/t E·D + ½·/t H·B + E·j + H·b input power = stored power (electric + magnetic) + ohmic + dielectric losses losses d d 1 1 U² – — divS dV = —(—·C·U² + —·L·I²) + I²·R1 + — dt dt 2 2 Self-consistent electrodynamics, if b replaces A: R2 New! Prof. Dr.-Ing. Konstantin Meyl: Summer Semester 2010 Supervisor at the University of Konstanz Experimental proof of calculated losses (qualitative comparison) with a MKT capacitor (SiemensMatsushita) Prof. Dr.-Ing. Konstantin Meyl: potential vortex vortex structure in HV-capacitor visible proof for the existence of potential vortives Measurement set up (a) and photo of vortex structure in a metallized polypropylen layer capacitor (at 450 V/ 60 Hz/ 100OC), A. Yializis, S. W. Cichanowski, D. G. Shaw: Electrode Corrosion in Metallized Polypropylene Capacitors, Proceedings of IEEE, International Symposium on Electrical Insulation, Bosten, Mass., June 1980; Prof. Dr.-Ing. K. Meyl: potential vortex Vortex and anti-vortex Energy of losses The power density shown against frequency for noise (a) according to Küpfmüller, as well as for dielectric losses of a capacitor (also a) and for eddy current losses (b) according to Meyl (b in visible duality to a)