This document discusses gravitomagnetism and how it can explain various cosmic phenomena without relying on other assumptions or theories like general relativity. It defines gravitomagnetism and shows how it is analogous to electromagnetism. It then explains how gravitomagnetism can account for: 1) the bending of light near massive objects and Mercury's orbit, 2) the swiveling of inclined orbits toward the equatorial plane of massive objects, and 3) the orbital velocities of objects around spinning stars. It proposes gravitomagnetism can explain other phenomena like supernova shapes, galaxy formation, and the fly-by anomaly. Finally, it discusses an emerging theory of "Coriolis gravity" which links gravit

1. GRAVITOMAGNETISM
SUCCESSES IN EXPLAINING THE COSMOS

2. The purpose of this presentation
- To explain what Gravitomagnetism exactly is and how the magnetic
part can be interpreted.
- To show that many cosmic issues can be explained by
calculating it strictly, without other assumptions, just by using
common sense.
PART ONE
common sense.
- To show that the bending of light and the Mercury issue can be
purely deduced and don’t need to be gauges for a theory.
- Explain my current research, consisting of a new theory of forces:
the Coriolis Gravity and Dynamics Theory.
PART TWO

3. What is Gravitomagnetism?
Coulomb’s
Electrostatic
Law
1 2
1 23C e
q q
F k r q E
r
= =
F F
Newton’s
Gravity Law
1 2
1 23N
m m
F G r m g
r
= =
F F
q m
ke G

4. Lorentz force ( )L2 2 1 2 1F q E v B= + ×
F F
v v
q m
E g
Equivalent
Lorentz force
for gravity
( )H2 2 1 2 1F m g v= + × Ω
E g
B ?...Ω
2
1m m
N kg
s ss
  
= + ⋅  
  Oliver Heaviside
Ω = ‘gyrotation’

5. Heaviside – Maxwell equations
( )H2 2 1 2 1F m g v⇐ + × Ω
4g G∇ ⋅ ⇐ π ρ
Gravitomagnetic force =
gravity force + “gyrotational” force
The gravity field is radial (diverges) and its
amplitude is directly proportional to its mass
The gyrotation field’s amplitude is
2
4c G j g t∇ × Ω ⇐ π + ∂ ∂
The gyrotation field’s amplitude is
directly proportional to a mass flow
or an increasing gravity field and is
perpendicular to it (encircles it)
0∇ ⋅ Ω = There are no gyrotational monopoles
g t∇ × ⇐ − ∂ Ω ∂
The induced gravitation field’s
amplitude is directly proportional to
an increasing gyrotation field and
perpendicular to it (encircles it)
(Minus sign inverses vector orientation)

6. The meaning of Gyrotation ΩΩΩΩ
A linear mass flux is encircled by a gyrotation field according
or
or
2
4c G j∇ × Ω ⇐ π
2
2
d 4
R
l Gm c
π
Ω ⇐ π
∫ ɺ
The “local absolute velocity” of the mass is
defined by an external gravity field
An external gravity field defines the zero velocity
or2 Rπ
2
2Gm RcΩ = ɺ
In other words : the aether velocity of a mass is always zero

7. Electromagnetism and Gravity
are totally similar
Maxwell equations and Lorentz force
are applicable to both
(besides the fact that masses always attract)(besides the fact that masses always attract)
No further assumptions !
No further theories !
Just simple maths and common sense !

8. A circular mass flow induces a dipole-like gyrotation
Ring Sphere
Gyrotation
of a ring is
analogue
to the
magnetic
field of an
electrical
dipole
The own gravity field defines the zero velocity
The “local absolute velocity” of the mass is defined by
the own gravity field
( )
( )
ext 3 2 2
3
2
r rG I
r
r c r
 ω⋅
Ω = ω −  
 
dipole
(steady
system)

9. First effect of Gyrotation
sun
What happens to an inclined orbit of a planet ?
p sun p suna g v= + × Ω
Lorentz- Heaviside
acceleration:
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
retrograde
retrograde
prograde
retrograde
retrograde
retrograde
prograde
prograde
sun
p sun p suna g v= + × Ω

11. Star’s velocity in disc galaxies
Consequence:

12. Spherical galaxy with a spinning center
2 0
sphere
G M
v
R
= (Kepler)
Simplified explanation without dark matter
Consider nucleus with mass M0 and a mass
distribution with concentrical shells,
each with a mass M0 :
R
Swiveled galaxy
2 0
disc
0
G n M
v
k R
= = constant
Milky Way : v = 235 km/s
The nucleus’ mass has totally changed :
m

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

14. Second effect of Gyrotation
p pa g v= + × ΩLorentz-Heaviside acceleration :
Like-spinning planets with Sun
= unstable momentum
Opposite spinning planets
than Sun = stable momentum

15. Third effect of Gyrotation
Gyrotational
Internal
gyrotation
Rotation
Gyrotation surface-compression forces
p pa g v= + × Ω
compression
forces
‘Centrifugal
force’

16. 0° < surface compression < 35°16°
( )2
2
x,tot 2 2
1 3sin cos
cos 1
5
G m G m
a R
R c R
 − α α = ω α − − 
 
 
2 2
3 cos sin sinG m G m
a
ω α α α
− = +
‘centrifugal’ gyrotation gravitation
ω
35° 16’
FΩ > Fc
y,tot 2 2
3 cos sin sinG m G m
a
c R
ω α α α
− = +
gravitationgyrotation
y
x
ω
Gyrotational
compression forces

17. R
( )2
1 5
6 3sin
C
C
R R
r R
R R
+
≤
− α
FΩ < Fc
For a fast spinning sphere (the equation
is then almost spin-independent) :
Internal gyrotation and centripetal forces
for given values of α
α
r
0°
( )2
6 3sin CR R− α
( )2
5CR Gm c=
wherein
= “critical compression radius”
For large masses, small radii : ( )2
5 6 3sinr R≤ − α

18. Supernovae examples
η − Caterinae SN 1987 - a

19. ‘hourglass’
nebula
hs-1999-32-a
More supernovae examples
hs-1997-38-a

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

21. Fourth effect of Gyrotation
Attraction and repelling between molecules
Ha g v= + × Ω
Like spins repelOpposite spins attract
Horizontal reciprocity
Like spins repelOpposite spins attract

22. Like spins attractOpposite spins repel
Vertical reciprocity
Va g v= + × Ω

23. Application: the expanding Earth
ΩΩΩΩ
Natural preferential
ordering inside the
Earth:
- ω aligns with Ω- ω aligns with Ω
- vertical attraction
- horizontal repel

24. Star’s life cycle
E
X
P
A
N
S
C
O
L
L
A
P
Sun
S
I
O
N
P
S
E
Red Giant
White
Dwarf

25. Probable process to a white dwarf
The star expands and becomes a red giant
- Spin speed decreases dramatically
- Star’s nuclear activity decreases dramatically
- Photosphere-matter gets continuously lost
Spin accelerates again
Collapse with matter release
Molecules’ spin vector becomes less oriented
Again compression
Expansion stops

26. Other succesful applications
of Gyrotation
- The Mercury perihelion advance
2
2 2
1 12 2 2 3 2
cos cos
2 5
m M m M m M R
F G G v G v
r r c r c
α
ω
− = + α + α
α
v2v1
2 5r r c r c
With v1 the Sun’s velocity in the Milky Way, v2 Mercury’s velocity and
α is Mercury’s angle to the Milky Way’s centre.
Gravity Sun’s motion in Milky Way Sun’s rotation
(negligible)
2 2
26 v cδ =2 2
1 224v v= (excentricity neglected)
( )
2
2
av 0
1
cos
2
π
α =

27. - The bending of light grazing the Sun
ω
v1
ωϕ
2 2
1, 2 2 2 2
2
cos cos
2 5
m M Rm M m M
F G G v G
r r c r c
ϕ
ϕ α
ω
− = + α + ϕ
With v1 the Sun’s velocity in the Milky Way, α the angle between the
ray and the Sun’s orbit and ϕ the Sun’s latitude where the ray passes.
Gravity and
gyrotation
Sun’s rotationSun’s motion in Milky Way
(neglectible)

28. The formation of a set of tiny rings about Saturn
Ring section
Other application:
Motion,
collisions
Pressure
without
motion
Turbulence,
separation

29. - The fly-by anomaly
-Strongly onto the equator
when flying near the poles
The acceleration is :
25°
45°
equatorontopoles
(0° is the equator)
when flying near the poles
-Weak onto the poles when
flying under inclination of 25°
-Absent near 0° and near 45°
Poles
ontoequator
( )2E E S
t, 2 2
3
sin cos 2 1 3sin sin 4 cos
42
G I
a
r c
Ω
ω ω  
= − α α − α − α α 
 
‘E’ for Earth, ‘S’ for satellite , α is the satellite’s inclination to the Earth’s equator.

30. Stars are vacillating in the halo of disc galaxies
- The halo of disc galaxies
25°
45°90°
0°
25°
45°
- The motions of asteroids
Preferential orbit- and spin orientations and their instabilities.
Poles

31. - The orbital velocity about fast spinning stars
2
3 2 2
2
G I G Mv
v
r r c r
ω
= +
The velocity v can be found out of :
ω
v
Gyrotation
of the star
Gravity
of the star
Orbit
motion (if
circular)
Causes velocity-
dependent orbit
precession
‘I’ is the star’s inertia moment
ω is its angular velocity

32. Explosion-free fast spinning stars and black holes
Tight compression by gyrotation forces a vΩ = × Ω
Prediction attempt :
ΩΩΩΩωωωω
( )2 2
a Gmr RcΩ ≈ ω π
R
r
At the surface:

33. Prediction attempt : bursts of binaries
ΩΩΩΩωωωω
Matter from
companion
a vΩ = × Ω

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

35. -Self-compression of fast moving particles
by gyrotation
Gravity field deformation due to the gravity’s speed retardation effect
Oleg Jefimenko
Prediction attempt : the high-speed meson lifetime increase
is caused by the gyrotation compression.
( )
( )
( )( )
2 2 2
3 2
2 2 2 2
3 1
,
4 1 sin
G m v v c
p r
r c v c
−
θ =
− θ
Pressure :

36. But say : I use the Linear Weak Field
Approximation of the
How to be accepted by Mainstream as a dissident?
Don’t say : GRT is wrong;
I use Gravitomagnetism!
Between brackets
Approximation of the
General Relativity Theory
M. Agop, C. Gh. Buzea, C. Buzea, B. Ciobanu and C. Ciubotariu of
the Physics Department of the Technical University, Iasi,
Romania. They wrote many papers this way, accepted by
mainstream, and could boost their studies on superconductivity.
And refer to:

37. Conclusions
- All these phenomena are explained in detail without any need
of relativity, spites the high speeds used.
- No gauges are used, the theory is not semi-empiric as the relativity
theory. Even the bending of the light and the Mercury issue are
purely deduced.
of part one
- 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
translating objects at high speed can be improved by including the
retardation of gravity.

38. SunGm
υ =
Discovery : Relationship between
the sun’s spin and its geometry:
graviton
ω
I found :
Frequency:
Current research
Coriolis Gravity and Dynamics Theory
Sun
eq 2
eq2
Gm
c R
υ =
The possible meaning is : the rotational speed of a body is
determined by its enclosed mass
graviton
Sun
eq
eq
Gm
v
c R
π
=
Velocity:

39. 2 22c a× ω = −
What could be the physical mechanism?
12
Coriolis : let
1) A tangential graviton from particle 1 hits particle 2 directly
Let us consider particles as trapped ‘light’, that release ‘gravitons’:
Analysis
2
2 12a Gm R= − π
1
2 2
2
Gm
c R
υ =1
2 2
Gm
c R
π
ω =
In the case of outgoing gravitons that are tangential to the trapped light,
we get the case of the Sun’s spin rate explained.
a
and let:

40. 4 42c a× ω = −
3
4
a
2) A tangential graviton from particle 1 hits particle 2 indirectly
Coriolis :
From 1) :
( )2 2a= − π
2
2 12a Gm R= − π
2
4 1a Gm R= −
In the case of outgoing gravitons that are spirally hitting the trapped light…
From 1) :
… we get Newton’s gravity law !
2 12a Gm R= − π
Hence :

41. 3) A tangential graviton from particle 1 hits particle 1 indirectly
Are forces between particles just a Coriolis effect?
a a
5 55
F
5 52c a× ω = −Coriolis : let
5 5F m a=Newton :
Conclusions
- The relationship between the Suns’ spin and the Suns’ gravity is
not a coincidence.
- The Coriolis effect on trapped light, and tested by the Sun’s spin
fits with the Newton gravity.
of part two