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Konstantin MeylScalar wavesFrom an e x te n d e d v o rte x a nd field th e o ryto a te chn ica l, b io lo g ica l a nd h isto rica l useof longitudinal w a v e s .Edition b e lo n g in g to th e le c tu re a nd s e m in a r„E le ctro m a gn e tic E n v iro n m e n ta l C o m p a tib ility ”

E dition b e lo n g in g to th e s e m in a r (p a rt 1 - 3 )„ E le c tro m a g n e tic E n v iro n m e n ta l C o m p a tib ility ”by Prof. Dr. Konstantin MeylFrom Maxwell's field equations only the well-known (transverse) Hertzian waves canbe derived, whereas the calculation of longitudinal scalar waves gives zero as a result.This is a flaw of the field theory, since scalar waves exist for all particle waves, like e.g.as plasma wave, as photon- or neutrino radiation. Starting from Faraday's discovery,instead of the formulation of the law of induction according to Maxwell, an extendedfield theory is derived, which goes beyond the Maxwell theory with the description ofpotential vortices (noise vortices) and their propagation as a scalar wave, but containsthe Maxwell theory as a special case. With that the extension is allowed and doesn'tcontradict textbook physics.Besides the mathematical calculation of scalar waves this book contains a voluminousmaterial collection concerning the information technical use of scalar waves, if theuseful signal and the usually interfering noise signal change their places, if a separatemodulation of frequency and wavelength makes a parallel image transmissionpossible, if it concerns questions of the environmental compatibility for the sake ofhumanity (bio resonance, among others) orto harm humanity (electro smog).From an e x te n d e d v o rte x and field th e o ryto a te chn ica l, b iolo g ica l and histo rica l useo f long itud in al w a v e s .IN D EL G m b H , V e rla g s a b te ilu n gISBN 3-9802542-4-0

480Neutrino radiationV » Chard neutrino radiation(small ring-like vortex)w eak neutrino radiation(large ring-like vortex)photon radiation (light individual ring-like vortex oras an oscillating pair).plasma waves,noise,earth radiation(vortex balls,consisting ofa multitude ofring-like vortices).Fig. 22.5:The ring-like vortex model o f scalar waves.

Noise, a scalar wave phenomenon478A.5Fig. 22.4: The wave rolling up to a vortex.wavelength o f the wave:wavelength o f the vortex:fs ft i? f2 flA,i c/fiA,n (n 1,2,3,4,5) A.iX,5 .4 .3 A.2 A,1

62pair creationFig. 4.6:The photon as oscillating electron-positron pairThe decay o f the y - quanta (photon) j ( pair creation Bethe-Heitler-process 1934 ):y ------ - e e i (4.2)Nachtmann, Otto: Phänomene und Konzepte der Elementarteilchenphysik,Vieweg, Braunschweig 1986, S. 135, ISBN 3-528-08926-1

56electron as an elem entary vortex "A,fthe positron e s !-—/- !sthe elektron eFig. 4.3:Elem entary particles as configurations o f potentialvortices

Overlap effecta) standing waveb)localized vortex noisec) broadband antenna for EMC-measurements“ X2Fig. 1.4: M easurem ent o f localized waves and vortices

Millions o f voluntary test subjects at 11.8.1999412Fig. 19.12:Experimentalconstructions forthe „neutrinolyse“ .earthFig. 20.1: Course o f the neutrino radiation focussed by the moonon the occasion o f the eclipse o f the sunat the 11th August 1999. i concerning the calculation o f the position o f the sun at 11.8.99:at 21.6. after 0 days is23.4 cos 0 23.4 at 21.9. after 92 days is 23.4 cos 90 0 northern latitude equatorat 11.8. after 51 days is 23.4 cos 51 daYS.9 0c 23.4 0.64492 days 15.1 n. lat.A t 11.8.1999 the sun at noon stands above latitude 15.1. i :Konstantin Meyl: Zur Brennglaswirkung des Mondes bei einer Sonnen finsternis, NET-Journal, Jg. 4, Heft Juli/August 1999, Seite 13-17

M odel o f calculation for the cosmic experiment414focussed neutrinoFig. 20.2: The course o f the focussed neutrino radiation at11.08.1999 for 48.4 northern latitude.(this corresponds to the line Ulm -Augsburg-Freising)calculation o f the critical latitude:sin a 3500 km 0.5488 resulting in the angle a 33.3 6378 km The neutrino rays touch the earth’s core at: 48.4 n.lat.minimum distance to the moon:radius o f the moon:radius o f the earth:length o f the Tangente:rm* 358000 kmR m 1738 kmR 6378 km (at the equator)X 3500 km/tan 33 5332 kmscattering radius: rx X- — — 25.5 km around the centre line.Tm XFocussing w ithout scattering on earth’s surface increase toRm / rx 68 times ,resp. with scattering to68 0.5 0.8 27 timesthe natural neutrino radiation!

4163200%Physical technical consequencesdistribution percentageof the neutrino radiationrelated to the natural'1600%800%400%200%distancefrom centreof circle100%-150-100100150 [km]50 %Fig. 20.3: The spatial distribution in the case o f focussing ofthe neutrino radiation by means o f the burningglass effect o f the moon on earth’s surface.

M istakes o f the HF technology458ionospherespatial wave Hertzian waveWMWWWMMWhground wave scalar wavetransmitterearthFig. 21.6: i :Ground waves, which follow the curvature o f theearth and radio waves reflected at the ionosphere. i: Meinke, Gundlach: Hochfrequenztechnik, 4.Aufl. Springer-Verlag Berlin1986, Seite R 18: „Lang-, Mittel- and Kurzwelle breiten sich einerseitsentlang der Erdoberfläche als Bodenwellen, andererseits unter Mitwirkungder Ionosphäre als Raumwellen aus.“

464Fig. 21.9 A:Transition to the far-fieldThe com ing off o f the electric field lines from a dipoleThe form ing vortex structures found a longitudinalelectric wave cariying impulse.electromagnetic wave (transverse)Fig. 21.9 B:The planar electromagnetic wave in the far zone

466Scalar wave modelCircularly polarized wave (transverse)Fig. 21.10 A:Left-circular polarized wave(as explanation for the transition to a vortex andto a scalar wave)electric wave (longitudinal)v, EFig. 21.10 B: Magnetic ring-vortices form an electric scalar wave.vortex and wave two stable field configurationselectromagnetic wave transverse wave propagating in a straightlinering-like vortex transverse wave running in circlesvortex velocity speed o f light cchange o f structure if the field is disturbed without expenseo f energy

468Double-frequent oscillation o f sizemagnetic wave (longitudinal)Fig. 21.11 A:The magnetic scalar waveFigure 21.11 B: Wave propagation in a coaxial cable.(Example for waveguide, horn radiator. etc.) j Cross-section o f coaxial conductor and fielddistribution in the direction o f propagation. i :H. Armbrüster, G. Grünberger: Elektromagnetische Wellen im Hochfrequenz bereich, Hüthig und Pflaum Verlag.

Electric and magnetic scalar wave4701. H. Hertz:electromagnetic wave (transverse)2. Nikola Tesla: electric wave (longitudinal)V,EV,H3. (Konstantin Meyl): magnetic wave (longitudinal)Fig. 21.12:The three basic types according to the wave equation(21.1). (electric, magnetic and electromagnetic wave).

Derivation o f the gravitation584The length measure (the distance L between the spheres)**’is determ ined by the field strength:----------------( law oft the inverse square o f a distance)E, H 1/L2( 28 . 18)A. Charged mass points (electrons, positrons, ions,.):Fig. 28.7: i :Observation o f a mutual force o f attraction becauseo f the effect o f the fields on the distance measure.Repetition of part 1, chapters 6.7 - 6.9 and part 2, chapters 10.4 and 15.2

The pentacle602Graphical construction at a right-angled triangle (Pythagoras):Golden Proportion o f length a x y :X CD 0.618aa(29.9)andx1 1 1.618 (29.10)tf The pentacleFig. 29.7: Constructions for the Golden Proportion

136elem entary vorticesW ith the classical radius o f the electron re 2,82 ' 10 15 m:Ce UeSo ’ 47tre e/C e3,135 10 25 F 5 1 lk V(6.4*)(6.31*)(constant independent o f re)F o r m a tio n fo r m s (vortex properties):I. A m a s s in g (formation o f vortex balls):II. O v e r la p p in g (phenomenon o f transport)Fig. 7.1: The am assing and overlapping o f elem entary vortices

226Four fundam ental interactionsThe effect of open field lines i: chargeconstant charge:oscillating onThe effect of closed field lines*** mass\------- constant mass:oscillating mass:gravitationlevitationFig. 10.4, b: i :Explanation o f the fundamental interactionsKonstantin Meyl: Potentialwirbel, Band 2, INDEL-Verlag (1992)see also in Part 1, chapters 6.8 and 6.9

228Example:resonant interactioncentral star Sz with 3 planets P 1 -P 3and with 4 neighbouring stars S 1 -S 4milky way-radius: 15000pc-3-109 45-1016kmsun system-radius: 50a-15-107 7 ,5 1 0 9 km45-10167,5-1091.27-10 the resonant interaction is more than eightdecimal powers bigger than the gravitation.

Unipolar field configuration320A:electric dipole (e.g. electrostatics, see also fig. 6.8)B:electric monopole (e.g. electron e , see also fig. 4.3) C:Mixed form in the case of cylindrical symmetryFig. 15.8: Dipole fields with unipolar parts

W indow o f the sensuous perception514Frequency spectrum o f the human organism:intensitysignal power o f10-' 10 101 102 103 104 105 106 107 10s 109 101010u 1012 1013 1014 1015 1016 10 710 8ULFELF VLF LW MW VHFSchumann waves radio/TV. j¡microwavesIFig. 25.1: i :! and theIRlight UV X-rays.---------------IIIcell communicationrange ofioperation o f!the bioresonancefrequency [Hz]¡UHF i ---------------------------------- 1The measured frequency spectrum o f m an.*1*Dr. P. Bembenek: Akupunktur und (Bio-) Resonanz, CO'med 6/98, S. 50-58

focussed neutrino Fig. 20.2:_The course of the focussed neutrino radiation at 11.08.1999 for 48.4 northern latitude. (this corresponds to the line Ulm-Augsburg-Freising) calculation of the critical latitude: sin a 3500