+ All Categories
Home > Documents > "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

"Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

Date post: 10-Apr-2018
Category:
Upload: sipora1
View: 212 times
Download: 0 times
Share this document with a friend

of 41

Transcript
  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    1/41

    GRAVITOMAGNETISMSUCCESSES IN EXPLAINING THE COSMOS

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    2/41

    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

    PART ONE

    common sense.

    - To show that the bending of light and the Mercury issue can be

    purely deduced and dont 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

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    3/41

    What is Gravitomagnetism?

    Coulombs

    ElectrostaticLaw

    1 21 23C e

    q q

    F k r q Er= =

    F F

    NewtonsGravity Law

    1 21 23N

    m mF G r m gr

    = =

    q mke G

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    4/41

    Lorentz force ( )L2 2 1 2 1F q E v B= +

    F F

    v vq m

    Equivalent

    Lorentz force

    for gravity ( )H2 2 1 2 1F m g v= +

    B ?...

    2

    1m mN kg

    s ss

    = +

    Oliver Heaviside

    = gyrotation

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    5/41

    Heaviside Maxwell equations

    ( )H2 2 1 2 1F m g v +

    4 G

    Gravitomagnetic force =

    gravity force + gyrotational force

    The gravity field is radial (diverges) and its

    amplitude is directly proportional to its mass

    2 4c G j g t +

    directly proportional to a mass flow

    or an increasing gravity field and is

    perpendicular to it (encircles it)

    0 =

    There are no gyrotational monopoles

    g t The induced gravitation fields

    amplitude is directly proportional to

    an increasing gyrotation field andperpendicular to it (encircles it)(Minus sign inverses vector orientation)

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    6/41

    The meaning of Gyrotation A linear mass flux is encircled by a gyrotation field according

    or

    2 4c G j

    2d 4l G m c

    The local absolute velocity of the mass is

    defined by an external gravity field

    An external gravity field defines the zero velocity

    22 G m R c =

    In other words : the aether velocity of a mass is always zero

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    7/41

    Electromagnetism and Gravity

    are totally similar

    Maxwell equations and Lorentz forceare applicable to both

    No further assumptions !

    No further theories !

    Just simple maths and common sense !

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    8/41

    A circular mass flow induces a dipole-like gyrotation

    Ring SphereGyrotation

    of a ring is

    analogue

    to themagnetic

    field of an

    electrical

    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 Ir

    r c r

    =

    dipole(steady

    system)

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    9/41

    First effect of Gyrotation

    sun

    What happens to an inclined orbit of a planet ?

    p sun p suna g v= + Lorentz- Heaviside

    acceleration:

    Every planets orbit swivels to the Suns equator plane.

    Same occurs for : Saturn rings, disk galaxies.

    Gyrotation transmits angular momentum at a distance by gravity.

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    10/41

    Examples: Swiveling to prograde orbits

    Inclined retrograde orbit equatorial prograde orbit

    retro rade

    retrograde

    re rogra eprogra e

    prograde

    sun

    p sun p suna g v= +

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    11/41

    Stars velocity in disc galaxies

    Consequence:

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    12/41

    Spherical galaxy with a spinning center

    2 0sphere

    G Mv = (Kepler)

    Simplified explanation without dark matter

    Consider nucleus with mass M0

    and a mass

    distribution with concentrical shells,

    each with a massM0 :

    Swiveled galaxy

    2 0disc

    0

    G n Mv

    k R= = constant

    Milky Way : v= 235 km/s

    The nucleus mass has totally changed :

    m

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    13/41

    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

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    14/41

    Second effect of Gyrotation

    p pa g v= +

    Lorentz-Heaviside acceleration :

    Like-spinning planets with Sun

    = unstable momentum

    Opposite spinning planets

    than Sun = stable momentum

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    15/41

    Third effect of Gyrotation

    Gyrotational

    Internal

    gyrotation

    Rotation

    Gyrotation surface-compression forces

    p pa g v= +

    compressionforces

    Centrifugal

    force

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    16/41

    0 < surface compression < 3516

    ( )22x,tot 2 2

    1 3 sin coscos 1

    5

    G m G ma R

    R c R

    =

    2 23 cos sin sinG m G m

    centrifugal gyrotation gravitation

    35 16

    F > Fc

    y,tot 2 2a c R = +

    gravitationgyrotation

    y

    x

    Gyrotationalcompression forces

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    17/41

    R 21 5 CR Rr R

    +

    F

    < Fc

    For a fast spinning sphere (the equationis then almost spin-independent) :

    Internal gyrotation and centripetal forces

    for given values of

    r

    0

    C

    ( )2

    5CR G m c=

    wherein

    = critical compression radius

    For large masses, small radii : ( )2

    5 6 3 sinr R

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    18/41

    Supernovae examples

    Caterinae SN 1987 - a

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    19/41

    hourglass

    nebulahs-1999-32-a

    More supernovae examples

    hs-1997-38-a

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    20/41

    Prediction attempt : the shape of supernova stars

    After the explosion of the sphere:

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    21/41

    Fourth effect of Gyrotation

    Attraction and repelling between molecules

    Ha g v= +

    Horizontal reciprocity

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    22/41

    Like spins attractOpposite spins repel

    Vertical reciprocity

    Va g v= +

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    23/41

    Application: the expanding Earth

    Natural preferential

    ordering inside the

    Earth:

    - aligns with

    - vertical attraction

    - horizontal repel

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    24/41

    Stars life cycle

    E

    X

    PA

    N

    C

    O

    LL

    A

    Sun

    I

    O

    N

    P

    S

    E

    Red Giant

    White

    Dwarf

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    25/41

    Probable process to a white dwarf

    The star expands and becomes a red giant

    - Spin speed decreases dramatically

    - Stars 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

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    26/41

    Other succesful applications

    of Gyrotation

    - The Mercury perihelion advance

    22 21 12 2 2 3 2

    cos cosm M m M m M R

    F G G v G v

    = + +

    v2v1

    With v1 the Suns velocity in the Milky Way, v2 Mercurys velocity and

    is Mercurys angle to the Milky Ways centre.

    Gravity Suns motion in Milky Way Suns rotation

    (negligible)

    2 226 v c =

    2 21 224v v= (excentricity neglected)

    ( )2

    2

    av0

    1cos

    2

    =

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    27/41

    - The bending of light grazing the Sun

    v1

    2 21, 2 2 2 2

    2 cos cos2 5

    m M Rm M m M F G G v G

    r r c r c

    = + +

    With v1 the Suns velocity in the Milky Way, the angle between the

    ray and the Suns orbit and the Suns latitude where the ray passes.

    Gravity and

    gyrotation

    Suns rotationSuns motion in Milky Way

    (neglectible)

    O h li i

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    28/41

    The formation of a set of tiny rings about Saturn

    Ring section

    Other application:

    Motion,

    collisionsPressure

    without

    motionTurbulence,

    separation

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    29/41

    - The fly-by anomaly

    -Strongly onto the equator

    The acceleration is :

    25

    45

    tor

    onto

    poles

    (0 is the equator)

    -Weak onto the poles when

    flying under inclination of 25

    -Absent near 0 and near 45

    Poles

    onto

    equ

    ( )2E E St, 2 23

    sin cos 2 1 3 sin sin 4 cos42

    G Ia

    r c

    =

    E for Earth, S for satellite , is the satellites inclination to the Earths equator.

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    30/41

    Stars are vacillating in the halo of disc galaxies

    - The halo of disc galaxies

    25

    4590

    0

    25

    45

    - The motions of asteroids

    Preferential orbit- and spin orientations and their instabilities.

    Poles

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    31/41

    - The orbital velocity about fast spinning stars

    2

    3 2 22

    G I G M vv

    r r c r

    = +

    The velocity v can be found out of :

    v

    Gyrotationof the star

    Gravityof the star

    Orbitmotion (if

    circular)

    Causes velocity-dependent orbit

    precession

    I is the stars inertia moment

    is its angular velocity

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    32/41

    Explosion-free fast spinning stars and black holes

    Tight compression by gyrotation forces a v =

    Prediction attempt :

    ( )2 2a G mr Rc

    R

    r

    At the surface:

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    33/41

    Prediction attempt : bursts of binaries

    Matter from

    companion

    a v =

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    34/41

    - Mass- and light horizons of (toroidal) black holes

    The graphic for the black holes horizons

    at its equator level is mass-independent !

    Hsradius Light horizon : limit surrounding

    the black hole, where light remains

    trapped by the black hole.

    Schwarzschild radius Orbiting incoming massesdesintegrate but behind the light

    horizon.

    BHs spin rate

    Mass horizon : limit surrounding

    the black hole, where the orbits

    reach the speed of light, and

    matter disintegrate.

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    35/41

    -Self-compression of fast moving particles

    by gyrotation

    Gravity field deformation due to the gravitys speed retardation effect

    Oleg Jefimenko

    Prediction attempt : the high-speed meson lifetime increase

    is caused by the gyrotation compression.

    ( )

    ( )

    ( )( )

    2 2 2

    3 22 2 2 2

    3 1

    ,4 1 sin

    G m v v c

    p rr c v c

    =

    Pressure :

    Between brackets

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    36/41

    But say : I use the Linear Weak Field

    How to be accepted by Mainstream as a dissident?

    Dont say : GRT is wrong;

    I use Gravitomagnetism!

    Between brackets

    Approximation of theGeneral 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:

    C l i

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    37/41

    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 relativitytheory. 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 dont

    need any correction for the retardation of gravity.

    - Only the calculation of the position of orbiting objects ortranslating objects at high speed can be improved by including the

    retardation of gravity.

    Current research

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    38/41

    Discovery : Relationship between

    the suns spin and its geometry:

    I found :

    Frequency:

    Current research

    Coriolis Gravity and Dynamics Theory

    Suneq 2

    eq2c R =

    The possible meaning is : the rotational speed of a body is

    determined by its enclosed mass

    graviton

    Suneq

    eq

    G mvc R

    =

    Velocity:

    Wh ld b h h i l h i ?

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    39/41

    2 22c a =

    What could be the physical mechanism?

    12Coriolis : let

    1) A tangential graviton from particle 1 hits particle 2 directly

    Let us consider particles as trapped light, that release gravitons:

    Analysis

    22 12a G m R=

    12 22

    G m

    c R =12 2

    G m

    c R

    =

    In the case of outgoing gravitons that are tangential to the trapped light,

    we get the case of the Suns spin rate explained.

    a

    and let:

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    40/41

    4 42c a =

    3

    4

    a

    2) A tangential graviton from particle 1 hits particle 2 indirectly

    Coriolis :

    From 1 :

    ( )2 2a=

    22a G m R=

    24 1a G m R=

    In the case of outgoing gravitons that are spirally hitting the trapped light

    we get Newtons gravity law !

    Hence :

  • 8/8/2019 "Gravity Beyond Einstein"-Series : Gravitomagnetism - Successes in Explaining the Cosmos

    41/41

    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 =

    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 Suns spin

    fits with the Newton gravity.

    of part two


Recommended