GRAVITOMAGNETISM SUCCESSES IN EXPLAINING THE COSMOS

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Silvester McLaughlin
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1 GRAVITOMAGNETISM SUCCESSES IN EXPLAINING THE COSMOS

2 The purposeof thispresentation PART ONE - To explain what Gravitomagnetism exactly is and how the magnetic part can be interpreted. -To show thatmanycosmicissues canbeexplainedby calculating it strictly, without other assumptions, just by using common sense. -To show thatthe bending of lightand the Mercuryissue canbe purelydeducedand don tneedto begaugesfora theory. PART TWO -Explainmycurrentresearch, consistingof a newtheoryof forces: the Coriolis Gravity and Dynamics Theory.

3 Whatis Gravitomagnetism? Coulomb s Electrostatic Law Newton s Gravity Law q1q2 FC = ke r = q E 3 r F F q m G k e 1 2 m1m2 FN = G r = m g 3 r 1 2

4 Lorentz force F ( ) L2 = q2 E1 + v2 B1 Oliver Heaviside Equivalent Lorentz force for gravity F F F v v q m E g B?...Ω = m g + v Ω ( ) H m m 1 N = kg + 2 s s s Ω= gyrotation

F c Heaviside Maxwell equations m g + v Ω ( ) H2 2 1 2 1 2 g 4πG ρ Ω 4π Gj + g t Ω = 0 g Ω t (Minus sign inverses vector orientation) Gravitomagnetic force= gravity force + gyrotational force The

5 F c Heaviside Maxwell equations m g + v Ω ( ) H g 4πG ρ Ω 4π Gj + g t Ω = 0 g Ω t (Minus sign inverses vector orientation) Gravitomagnetic force= gravity force + gyrotational force The gravity field is radial(diverges) and its amplitude is directly proportional to its mass The gyrotation field samplitude is directly proportional to a mass flow oranincreasinggravityfield and is perpendicular to it(encircles it) There are no gyrotational monopoles The inducedgravitationfield s amplitude is directlyproportionalto anincreasinggyrotation field and perpendicular to it(encircles it)

6 The meaningof Gyrotation Ω A linear mass flux is encircled by a gyrotation field according c 2 2 π R Ω or or 4πGj Ωdl 4πGmɺ c Ω = 2Gmɺ Rc An external gravity field defines the zero velocity 2 2 The localabsolute velocity of the massis defined by an external gravity field In otherwords: the aether velocityof a massis alwayszero

7 Electromagnetismand Gravity are totallysimilar Maxwell equationsand Lorentzforce are applicableto both (besides the fact that masses always attract) No furtherassumptions! No furthertheories! Just simplemathsand commonsense!

A circular mass flow induces a dipole-like gyrotation Gyrotation of a ring is analogue to the magnetic field of an electrical dipole (steady system) Ring Sphere GI

8 A circular mass flow induces a dipole-like gyrotation Gyrotation of a ring is analogue to the magnetic field of an electrical dipole (steady system) Ring Sphere GI Ω ( r ) = ω 2r c ext The own gravity field defines the zero velocity 3r r ( ω ) r The local absolute velocity of the mass is defined by the own gravity field

9 First effect of Gyrotation Whathappens to aninclinedorbitof a planet? sun Lorentz- Heaviside acceleration: a = g + v Ω p sun p sun Every planet s orbit swivels to the Sun s equator plane. Same occurs for: Saturn rings, disk galaxies. Gyrotation transmits angular momentum at a distance by gravity.

10 Examples: Swiveling to prograde orbits Inclined retrograde orbit equatorial prograde orbit prograde prograde retrograde retrograde retrograde a = g + v Ω p sun p sun sun

11 Consequence: Star svelocityin disc galaxies

withconcentricalshells, eachwitha massm 0 : v GM 2 0 sphere = (Kepler) R

12 Simplified explanation without dark matter Spherical galaxy with a spinning center Considernucleus withmassm 0 and a mass distribution withconcentricalshells, eachwitha massm 0 : v GM 2 0 sphere = (Kepler) R Swiveled galaxy The nucleus mass has totally changed: m v GnM 2 0 disc kr0 = = constant MilkyWay: v= 235 km/s

pressure upon orbits Swivelling time High density of

13 Further consequence: Spiraldisc galaxies Total life time side view Swivelling of the orbits Gyrotational pressure upon orbits Swivelling time High density of disc Local grouping Local voids Winding time top view

14 Secondeffect of Gyrotation Lorentz-Heaviside acceleration: Like-spinningplanets withsun = unstable momentum a = g + v Ω p Opposite spinning planets than Sun = stable momentum p

15 p Gyrotational compression forces Thirdeffect of Gyrotation Gyrotation surface-compressionforces a = g + v Ω p Internal gyrotation Rotation Centrifugal force

16 0 < surfacecompression< a Gm ( 2 ) 1 3 sin α Gm cos α 5Rc R 2 x,tot = R ω cos α centrifugal gyrotation gravitation ω 2 2 3Gm ω cos α sin α Gm sin α a y,tot = c R gyrotation gravitation y Gyrotational compression forces F Ω > F c x

17 Internal gyrotation and centripetal forces For a fast spinning sphere(the equation is then almostspin-independent) : R F Ω < F c r R forgivenvaluesof α 1 + 5R R C ( 2 6 3sin α ) 6 3sin RC R r 0 α C wherein ( 2 5 ) R = Gm c = critical compression radius For large masses, small radii : ( 2 r R 5 6 3sin α)

18 Supernovae examples η Caterinae SN a

19 More supernovae examples hourglass nebula hs a hs a

20 Prediction attempt: the shape of supernova stars After the explosion of the sphere:

21 Fourtheffect of Gyrotation Attraction and repelling between molecules a = g + v Ω H Horizontal reciprocity Opposite spins attract Like spins repel

22 Opposite spins repel Vertical reciprocity a = g + v Ω V Like spins attract

23 Application: the expandingearth Natural preferential ordering insidethe Earth: Ω - ωalignswith Ω - vertical attraction - horizontal repel

24 Star slifecycle Sun E X P A N S I O N C O L L A P S E White Dwarf Red Giant

25 Probableprocessto a white dwarf The star expandsand becomesa red giant - Photosphere-matter gets continuously lost - Star s nuclear activity decreases dramatically - Spin speed decreases dramatically Expansion stops Molecules spin vector becomes less oriented Again compression Spin accelerates again Collapse with matter release

26 Othersuccesfulapplications of Gyrotation - The Mercury perihelion advance α v 1 v ω cos mm mm mmr Fα = G + G v α + G v cos α r 2 r c 5 r c Gravity Sun s motion in Milky Way Sun s rotation (negligible) ( 2 cos ) v π 2 1 av 0 α = = 24v2 δ = 6v2 c (excentricity neglected) Withv 1 the Sun svelocityin the MilkyWay, v 2 Mercury svelocityand αis Mercury sangleto the MilkyWay scentre.

27 -The bending of lightgrazingthe Sun ω ϕ 2mM mm 2 2 mmr ωϕ F ϕ, α = G + G v cos α + G cos ϕ 2 r 2r c 5r c v 1 Gravity and gyrotation Sun s motion in Milky Way (neglectible) Sun s rotation Withv 1 the Sun svelocityin the MilkyWay, αthe anglebetweenthe rayand the Sun sorbitand ϕthe Sun slatitudewherethe raypasses.

28 Other application: The formationof a set of tinyringsaboutsaturn Ring section Motion, collisions Pressure without motion Turbulence, separation

29 - The fly-by anomaly onto equa ator onto poles a Poles E E S t, Ω 2 2 The acceleration is : (0 is the equator) -Stronglyontothe equator when flying near the poles -Weak onto the poles when flying under inclination of 25 -Absent near0 and near45 GI ω ω ( 2 ) 3 = sin α cos 2α 1 3 sin α sin 4α cos α 2r c 4 E for Earth, S for satellite, α is the satellite s inclination to the Earth s equator.

30 -The halo of disc galaxies Stars are vacillating in the halo of disc galaxies Poles - The motions of asteroids Preferentialorbit-and spin orientationsand theirinstabilities.

31 - The orbital velocity about fast spinning stars The velocity vcanbefoundout of : v 2 v GI ω GM = v + r r c r ω Orbit motion (if circular) Gyrotation of the star Gravity of the star Causes velocitydependent orbit precession I is the star s inertia moment ω is its angular velocity

32 Prediction attempt: Explosion-free fast spinning stars and black holes Tight compression by gyrotation forces R ω Ω a v Ω Ω = r At the surface: ( Rc ) 2 2 aω Gmr ω π

33 Prediction attempt: bursts of binaries ω a v Ω Ω = Ω Matter from companion

34 -Mass-and lighthorizonsof (toroidal) black holes The graphic for the black hole s horizons at its equator level is mass-independent! BH s radius Light horizon : limit surrounding the black hole, where light remains trapped by the black hole. Mass horizon : limit surrounding the black hole, where the orbits reachthe speed of light, and matter disintegrate. Schwarzschild radius BH s spin rate Orbiting incoming masses desintegrate but behind the light horizon.

-Self-compression of fast moving particles by gyrotation Gravity field deformation due to the gravity s speed retardation effect Oleg Jefimenko Pressure: (, ) p

35 -Self-compression of fast moving particles by gyrotation Gravity field deformation due to the gravity s speed retardation effect Oleg Jefimenko Pressure: (, ) p r θ = 3Gmv 1 ( v c ) ( ( ) ) v c θ rc 1 sin 3 2 Prediction attempt: the high-speed meson lifetime increase is causedbythe gyrotation compression.

36 Between brackets Howto beacceptedbymainstreamas a dissident? Don tsay: GRT is wrong; I use Gravitomagnetism! Butsay: I usethe Linear Weak Field And referto: Approximation of the General Relativity Theory M. Agop, C. Gh. Buzea, C. Buzea, B. Ciobanuand C. Ciubotariu of the PhysicsDepartmentof the TechnicalUniversity, Iasi, Romania. Theywrote many papers this way, accepted by mainstream, and could boost their studies on superconductivity.

37 Conclusions of part one - All these phenomena are explained in detail without any need of relativity, spites the high speeds used. -No gaugesare used, the theoryis notsemi-empiricas the relativity theory. Even the bending of the lightand the Mercuryissue are purely deduced. - Most of the explained phenomena are steady systems and don t need any correction for the retardation of gravity. - Only the calculation of the position of orbiting objects or translatingobjectsat high speed canbeimprovedbyincludingthe retardation of gravity.

38 ω Currentresearch Coriolis Gravityand Dynamics Theory Discovery: Relationship between the sun s spin and its geometry: graviton I found: Frequency: GmSun υ eq = 2 2cReq Velocity: Sun The possiblemeaningis : the rotational speed of a body is determined by its enclosed mass v eq = πgm cr eq

39 Analysis What could be the physical mechanism? Let us consider particles as trapped light, that release gravitons : 1) A tangential graviton from particle 1 hits particle 2 directly 2 1 Coriolis : let 2c ω = a 2 2 a ω = and let: πgm cr a = 2 πgm R 2 1 Gm υ = 2cR 2 In the case of outgoing gravitons that are tangential to the trapped light, we getthe case of the Sun sspin rateexplained.

40 2) A tangential graviton from particle 1 hits particle 2 indirectly 4 a Coriolis : 3 From1) : 2c ω = a a 4 4 = a 2 2π = 2 πgm R 2 1 ( ) 2 Hence : a = Gm R In the case of outgoing gravitons that are spirally hitting the trapped light we getnewton sgravitylaw!

41 3) A tangential graviton from particle 1 hits particle 1 indirectly F a a Coriolis : let Newton : 2c ω = a F = m a Are forces between particles just a Coriolis effect? Conclusions of part two -The relationshipbetweenthe Suns spin and the Suns gravityis not a coincidence. -The Coriolis effect ontrappedlight, and testedbythe Sun sspin fits with the Newton gravity.

On the geometry of rotary stars and black holes

2005 Thierry De Mees On the geometry of rotary stars and black holes T. De Mees - thierrydemees@pandora.be Abstract Encouraged by the great number of explained cosmic phenomena by using the Maxwell Analogy