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  • Beyond Einstein’s problems

  • Newton(1687)

    Maxwell(1864)

    Einstein(1915)

    Einstein’sFirst Problem

    Shipov( 1972)

    Einstein’sSecond ProblemShipov (1976)

    Inertia FieldEquations

    Shipov (1979)

    Universal Relativityand PV

    Shipov (1988)

    Schrödinger(1926)

    Dirac (1926)

    Mandelstam(1958)

    Gell-Mann(1964)

    Venetziano(1969)

    Glashow, others.(1974)

    Fermi(1934)

    Feynman(1957)

    Weinberg -Salam(1967)

    Gell-Mann(1953)

    StandardModel

    Nambu, others(1970)

    ElectroweakInteractions

    Green& Schwarz(1984-86)

    Witten,others(1995)

    A Theoryof Everything

    Universal Relativity and a Theory of Physical VacuumUniversal Relativity and a Theory of Physical VacuumBeyond Einstein’s problems

    Hawking(1990)

    Carmeli(1972)

    Penrose(1962)

    Cartan(1922)

    SuperUnification

    Equationsof Physical Vacuum

    Shipov (1984)

    Frenet(1849)

    Ricci(1895)

    Cartan(1927)

    Einstein(1928)

    Weinberg-Glashow- Hawking--Witten Program

    Clifford- Einstein’ Program

    Clifford(1870)

    Weitzenbock(1924)

    DescartesianParadigm

    NewtonianParadigm

    I

    II

    Super StringTheory

    String Theory

    PointOrientable Point

  • Riemanncurvature

    Ricci curvaturecreated by torsion

    )1.(,

    sA

    ,1,0...,,1,0...,

    )2.(,

    sA

    )1.(,2

    sDBCADCABDCAB BT

    1,0...,,1,0...,

    )2.(,

    DBBA

    BJTTTTTT

    TTTTTTC

    sDBCADCBAFC

    F

    DABDF

    F

    CBA

    FA

    F

    BCDBF

    F

    ADCDCBABADCDCBA

    ,,

    ss BA

    ssss BABA ,,,

    dS2>0

    dS2>0

    dS2

  • Spinor structure ofSpinor structure of AA ((6)6) spacespace

    4 holonomic4 holonomiccoordinates ofcoordinates of basebase :: ct, x,ct, x, y,y, zz

    ((local spinor grouplocal spinor group ТТ(4) )(4) )

    66 anholonomicanholonomic

    coordinates ofcoordinates of fiber:fiber: ((local spinor grouplocal spinor group SL(2.C)SL(2.C)))

    44

    AB

    TranslationalTranslationalmetricmetric

    RotationalRotationalmetricmetric

    .01

    10

    ,1,0...,

    ,1,0...,

    ,3,2,1,0...,

    ,

    ,2

    DC

    DCAB

    AB

    DC

    k

    BA

    iDBAC

    ik

    kiik

    DC

    BA

    ki

    g

    dxdxgds

    kkDC

    BADC

    BA

    DC

    BADCBA

    kBADC

    iDCBA

    ik

    kiik

    dxTd

    ddd

    DB

    CA

    ki

    TTG

    dxdxGd

    ,

    1,0...,

    ,1,0...,

    ,3,2,1,0...,

    ,

    ,

    2

    2

  • PRIMARY TORSION FIELDPRIMARY TORSION FIELD(SUPERCONSCIOUSNESS)(SUPERCONSCIOUSNESS)

    PHYSICAL VACUUMPHYSICAL VACUUM

    ELEMENTARY PARTICLESELEMENTARY PARTICLES

    LIQUIDLIQUID

    GASGAS

    SOLIDSOLID

    PotentialState of Matter

    State of Matter

    ABSOLUTEABSOLUTE ““NOTHINGNOTHING”” 00≡≡00II

    IIII

    IIIIII

    IVIV

    VV

    VIVI

    VIIVII

  • Theories in Physics Strategical Tactical Operational

    I. Fundamental(Mechanics, Gravity,Electrodynamics,Theory of Physical Vacuum)

    0Newton, Maxwell, Einstein,Newton, Maxwell, Einstein,Shipov.Shipov.

    1Euler, Coulomb, Ampere,Euler, Coulomb, Ampere,Faraday, Lorentz,Faraday, Lorentz,Einstein, Shipov.Einstein, Shipov.

    2Lagrange , Hamilton,Lagrange , Hamilton,Abraham, Einstein,Abraham, Einstein,Poynting, LenardPoynting, LenardGubarev, SidorovGubarev, Sidorov……

    II. Semi fundamental(Quantum Mechanics,Quantum Electrodynamics)

    3Schrödinger, Heisenberg,Dirac.

    4Plank, Einstein,Einstein, Bohr, deBroglie, Pauli, Born,

    5Schwinger, Lamb,Feynman, Glauber…

    III. Phenomenological(Strong, Weak, Form Factors,Quarks, Superconductivity)

    6.Van der Waals, Fermi,Hofstadter, Gell-Mann,Weinberg, Salam, Glashow,Lee,Yang

    7.Yukawa, Hoft, Veltmann,Regge, Veneziano,Mandelshtam, Goldberg…

    8.London, Bardeen, Cooper,Schrieffer, Landau, Perl,Wilson,Abricosov, Leggett …

    IV. UnifiedPhenomenological(Electroweak, Electro-Strong,SM, Cosmology)

    9.Alfen, ChandrasekharWeinberg, Salam,Glashow, Higgs …

    10.Nambu, Kobayashi,Maskawa, Wheeler,Hawking, Oaks…

    11.Hawking, Wheeler,Ivanenko, Zeldovich,Linde…

    V. SemiPhenomenological(Gauge, Supersymmetries,Multidimentional)

    12.Yang, Mills, Utiyama,Kibble, Kaluza, Klein,Carmeli…

    13.Lord, Rubakov, Vladimirov,Frolov, Krechet…

    14.Majority oftheoreticians

    VI. Academic(Superstring, Twistors)

    15.E. Whitten, M. Green,B. Green, G. Schwartz…Penrose…

    16.About 1000 names

    17.Several thousands of names

    The

    imp

    ort

    an

    ce

    ,de

    gre

    eof

    risk

    and

    refle

    ctio

    ns

    0

    Generalization of theoretical basis of physics

  • • A Theory of Physical Vacuum is a newA Theory of Physical Vacuum is a newParadigm based on the orientable pointParadigm based on the orientable pointmanifold.manifold.

    ••Any object created from Vacuum is describedAny object created from Vacuum is describedby the system of nonlinear spinorby the system of nonlinear spinorHeisenbergHeisenberg--EinsteinEinstein--YangYang--MillsMills--like equations.like equations.

    ••TheThe Physical VacuumPhysical Vacuum equations describeequations describeseven levels of the Reality including Potentialseven levels of the Reality including PotentialState of a MatterState of a Matter..

  • AA

    AB

    AC

    AB-BA≠0

    100

    0cossin

    0sincos

    A

    cossin0

    sincos0

    001

    B

    100

    0cossin

    0sincos

    C

    Euler angles are anchonomic coordinates

    D=CBA Total rotation

    Unit basis vectors

    .20,0,20

    0,1)()( )1()3()3()2()2()1(2)3(2)2(2)1( eeeeeeeee

    )1(e

    )2(e

    )3(e

    ')1(e

    ')2(e

    )1(e

    )2(e

    ')1(e

    )3(e

    ')2(e

    ')3(e

    )1(e '

    )1(e

    )2(e

    ')2(e)3(e

    ')3(e

    )3(,' ODeDe ABBAB

    A

  • 90

    90

    o

    o

    9090

    o

    o

    Turn to 180 clockwiseTurn to 180 clockwise

    a) around of axis b) around of axis

    c) around of axis d) around of axis

    oo

    The resultThe resultdependsdepends uponupona pathwaya pathway

    )1(e

    )2(e

    )3(e

    )1(e

    )3(e

    )2(e

    )1(e

    )3(e

    )2(e

    )3(e )1(e

    )1(e )3(e

    )1(e )1(e

    )1(e

    )2(e )2(e

    )2(e

    )3(e )3(e

    )3(e

  • ,,

    ,,,

    )3()2(

    )2()1(

    321

    ds

    dxT

    ds

    dxT

    beneds

    dxte

    n

    t

    b

    m

    x

    y

    z X(t)

    0,1)()(,1, 222 tbbnntbntds

    xdt

    Inds

    td,

    IIbtds

    nd,

    IIInds

    bd,

    ,2222 dzdydxds

    ,

    B

    BA

    A

    eds

    dxT

    ds

    de

    Ricci rotationalRicci rotationalcoefficientscoefficients

    .3,2,1...,,3,2,1..., BA

    Ricci C.Ricci C.

    FrenetFrenet’’s equationss equations

    dxdxTTd ABBA2

    ShipovShipov’’s rotational metric (1997)s rotational metric (1997)

    Translational metricTranslational metric

    Frenet’s triad

    ,BaA

    BA eeT

  • .20,0,20

    3D orientable point describes by 6 coordinates:3 – translational x,y,z and 3 rotational

    Infinitesimal displacement of an orientable pointfrom a point M to a point M’ describes by 6 equations

    ).(),(),(),(),(),( sssszzsyysxx

    Only one solution

    ,,,,,, 0000000 ssforzzyyxx

    Entry conditions

    define position of an original point M .0

    ',',' )3()2()1( ebenet

    )3()1()3(

    )2()1()2(

    )1()1()1(

    )()1()(

    )1( ' eDeDeDeDet BB

    ).sin(/

    ,cos/,sin

    sin/

    ,sinsin/

    ),cossincoscos(sin/

    ,)cossinsincos(cos/

    )1()3(

    )1()2(

    )1()1(

    ctgdsd

    dsddsd

    Ddsdz

    Ddsdy

    Ddsdx

    Rene DescartesRene Descartes

    Every motionEvery motionis rotation.is rotation.

  • o

    o’l

    y’

    x’

    x

    y

    R

    y

    x

    C

    r’к

    ),sinsinsin( Rxm

    ),sinsincos( Rym

    ,0

    ,0mx , Rym

    ,0mdx ,Rddym

    ,0mm xx

    ),( 00 Ryy mm

    Equations of motion of center of mass

    Plane-parallel motion

    S’

    ,0' kmk rvv

    S

    anholonomic coordinates

    Skidless motion became holonomic

    Rvm

  • ,22

    2

    nvtadt

    xd

    ,3 32323

    3

    bvndt

    dvatv

    dt

    da

    dt

    xd

    dt

    dsv - absolute velocity,

    dt

    dva - tangent acceleration

    dt

    ds

    ds

    xd

    dt

    xdt

    dt

    dsts

    ),(),( - Transition to time parameter t

    - Newton-like equations

    - have no analogues in the Newtonmechanics

    In electrodynamics for reaction force of radiation we haveIn electrodynamics for reaction force of radiation we have

    ,33

    2

    3

    2 33323

    2

    3

    3

    3

    2

    bvn

    dt

    dvatv

    dt

    da

    c

    e

    dt

    xd

    c

    eFrad

    Electro-torsion radiation created by ownrotation of an electron (by spin). This radiation wasobserved experimentally and torsion generatorswere created in Russia by A.Akimov, I.Shachparonov and others

    A.AkimovA.Akimov I.ShachparonovI.Shachparonov

  • M.CarmeliM.Carmeli

    phs spin of photonspin of photon

    2/elsspin of electronspin of electron

    CarmeliCarmeli’’s idea (1986)s idea (1986)

    Two constants are connected withTwo constants are connected withlight:light:

    •• cc –– speed of light, generatingspeed of light, generating

    Translational RelativityTranslational Relativity;;

    •• ħħ –– spin of light, generatingspin of light, generating

    Rotational Relativity.Rotational Relativity.

    0

    vdiv

    t

    /),(),(),( txiSetxtx

    0),(2

    2

    txV

    mti

    ),,,(2

    12

    0

    2

    0

    2

    00 tzyxVz

    S

    y

    S

    x

    S

    mt

    S

    ...)()( 2

    210 SiSiSS

    1.

    2.

    0

    Classical mechanics = mechanics ofnonorientable point

    Quantum mechanics == orientable point mechanics

    Classicallimit

    Nonlocality

    Schrödinger- de Brogliematter field = field ofinertia (Shipov 1979)

    N.RosenN.Rosen

    Pupil of RosenPupil of Rosen

    Those mathematicalThose mathematicalexpressions which willexpressions which willbe covariant concerningbe covariant concerningrotation can haverotation can havereal sense only (1928)real sense only (1928)

    Own rotationOwn rotation of electronof electron(spin) in the classical(spin) in the classicaldescriptiondescription isis ananorientableorientable point (1985)point (1985)

    Pupil of EinsteinPupil of Einstein

  • ••The Universal Relativity based on the 10The Universal Relativity based on the 10dimensional orientable point manifold with 4dimensional orientable point manifold with 4translational and 6 rotational coordinates.translational and 6 rotational coordinates.

    ••The Universal Relativity leads usThe Universal Relativity leads us toto a Mechanicsa Mechanicsof an orientable point (point with spin)of an orientable point (point with spin)..

    ••Quantum MechanicsQuantum Mechanics describes the dynamics ofdescribes the dynamics ofthe field of inertia and represents a part of athe field of inertia and represents a part of aMechanics of an Orientable PointMechanics of an Orientable Point..

    ••Mechanics of an Orientable PointMechanics of an Orientable Point predicted thepredicted theelectroelectro--torsion radiation that was observedtorsion radiation that was observedexperimentallyexperimentally..

  • )6(4

    A44 translational coordinatestranslational coordinates ct, x, y, zct, x, y, z ,,form external space (base) on which the local groupform external space (base) on which the local group T(4)T(4) operates.operates.

    66 rotationalrotational coordinatescoordinates ,,formform inner space (fiber) on which local groupinner space (fiber) on which local group O(3.1)O(3.1) operates.operates.

    kik

    bi

    aab

    kiik dxdxeedxdxgds

    2Translational metricTranslational metric

    kiak

    bbi

    aa

    bb

    a dxdxTTddd 2 Rotational metricRotational metric

    bj

    ja

    kbka eeT

    Ricci rotationalRicci rotationalcoefficientscoefficients

  • ,0 amb

    b

    k

    a

    mkTee

    ][[ ]

    ,022 c mba

    kca

    mbkabkm TTTR ][][

    .,,,a,b,c...,,,i,j,k... 3210,3210

    (A)

    (B)

    Structural Cartan equations of local translational group T(4) == first Structural Cartan equations of A (6) space

    Structural Cartan equations of local rotational group O(3.1) == second Structural Cartan equations of A (6) space

    Coordinate (external)indexes

    Matrix (inner) indexes

    4

    4

    Springer New York , Russian Physic Journal,Springer New York , Russian Physic Journal,Volume 3, pages 238Volume 3, pages 238--241 / March 1985241 / March 1985,, ISSN 1064ISSN 1064--88878887

  • ee -- e Te T = 0, (= 0, (АА) (2.11 NP)) (2.11 NP)

    RR + 2+ 2 TT + 2+ 2TT TT = 0, (B) (2.7 NP)= 0, (B) (2.7 NP)abkm

    a a[k |b|m] c [k

    c|b|m]

    [kam]

    b[k

    a|b|m]

    Equations of Physical Vacuum (Shipov 1984)Equations of Physical Vacuum (Shipov 1984)or Equations of Newmanor Equations of Newman--Penrose formalism (1962)Penrose formalism (1962)or Structural Cartan equations of A (6) geometry (1926)or Structural Cartan equations of A (6) geometry (1926)

    i, j, k... =0,1,2,3, a, b, c... =0,1,2,3., j, k... =0,1,2,3, a, b, c... =0,1,2,3.

    TTa

    bk-- RicciRicci torsion fieldtorsion field (1895)(1895)

    ( or field of inertia)( or field of inertia)

    eea

    k- anholonomic tetradanholonomic tetrad –– FrenetFrenet orientable pointorientable point (1847)(1847)

    RRabkm - RiemannRiemann curvaturecurvature (1854)(1854)

    44

  • ,0j][][ ai

    ik

    ajk eTe

    ,jmTR

    jmg

    jmR

    2

    1

    ,22][ ]

    ijkm

    smj

    iks

    imj

    ijkm JTTTC k [

    (A)

    (B.1)

    (B.2)

    s

    npTi

    iTi

    npT

    ipn

    jmsmi

    Tij

    Timj

    Tijm

    T][][2

    1

    ]s[][

    2

    sgg

    .gg jkmimjikijkm TTJ ][])([3

    12g

    Einstein’s generalized vacuum equations

    Geometrized energy- momentum tensor

    Generalized Yang-Mills equations

    Geometrized tensor current

    i,j,k…=0,1,2,3 a,b,c…=0,1,2,3

    Torsion field equations

  • ••Torsion field is a Matter field which describesTorsion field is a Matter field which describes aastructure of sources of all other fieldsstructure of sources of all other fields..

    ••In the Universal Relativity all physical laws haveIn the Universal Relativity all physical laws haveancholonomic nature connected with the rotationalancholonomic nature connected with the rotationalcoordinatescoordinates..

  • ,02 )(2

    2

    ds

    dx

    ds

    dxg

    ds

    dx

    ds

    dx

    ds

    xd kj

    jkmim

    kj

    jki

    i

    4D Frenet equations

    ,02 )( ds

    dxeg

    ds

    dxe

    ds

    de ka

    jjkm

    imk

    aj

    jkia

    i

    where )(2

    1,,, mjkjkmkim

    imjk

    i gggg - Christoffel symbols and

    )(2

    1,,],[

    ..kjjk

    aa

    ijk

    aa

    ijk

    i eeeee - anholonomity object

    6 equations

    Let’sds

    dxe

    ii 0 and we have from 4D Frenet equations

    4 equations

    Hereds

    dx

    ds

    dxm

    kj

    jki - gravitational force and

    ds

    dx

    ds

    dxmg

    kj

    jkmim

    )(2 - force of inertia

    Upon the absence of external gravitational force the center of mass of an isolatedsystem moves under the action of controllable force of inertia

    ,02 )(2

    2

    ds

    dx

    ds

    dxmg

    ds

    xdm

    kj

    jkmim

    i

  • The Small massesThe Small massesm rotate around ofm rotate around ofan axis Oan axis O1

    The big massThe big mass MM

    The rodsThe rods

    The 4D gyroscope =The 4D gyroscope =ooscillatorscillator + rotator+ rotator

    Using Newton mechanicswe will receive:1. Translational equation

    0)sin( dt

    dBvvc

    2. Rotational equation

    0sin r

    v

    Solution:

    1.

    2.

    constvc

    )(sin1

    sin1

    22

    022

    0

    tk

    k

    2rkB

    mM

    mk

    2

    22

    cv - center mass velocity

    v - cart velocity - angular velocity

  • 2,1...,,,02 )(2

    2

    kjids

    dx

    ds

    dxg

    ds

    dx

    ds

    dx

    ds

    xd kj

    jkmim

    kj

    jki

    i

    cv - center mass velocity

    v - cart velocity - angular velocity

    )2/(22 mMmrrkB

    constg

    k

    '

    0Solution for gives

    '

    /)sin1()cos(

    '

    4))sin(1(

    00222

    00

    0

    00

    gr

    kvkkrtkk

    grk

    v

    gyroDfreeofprecessiontimespacetkkvvc

    0v - initial velocity of center of mass

    Newton solution appears when 00 k

    ds

    dggt

    ds

    dxVt cc

    )(sin,)(cos

    dt

    d

    k

    g 2

    where

    ))(sin1()( 222 tkktg

    Andrei SidorovAndrei Sidorov

    c

    c

    vvr

    Bv

    sin

    ,

    dtdvv /

    xx tncdt

    dxv

  • Predictionof NewtonMechanics

    Prediction of an orientablepoint mechanics ))sin(1( 00 tkkvvc

    0v

    0vvc

    0vvc

    00 k

    cartcart

    Prediction of an orientablepoint mechanics

    ))sin(1( 00 tkkvvc

  • 4D gyroscope4D gyroscopewith selfwith self--actionaction

    The small massesm rotate aroundan axis O1 in opposite

    directions

    Spring is a sourceof the internal energy

    Weels are free

    O1

    m

    m

  • Lc ak

    vrkLmr

    B

    v

    22

    2

    2

    sin1

    )sin(2

    sin

    LN

    k

    vBrmr

    L

    k

    k

    22

    2

    22

    22

    sin1

    sin2

    sin1

    sincos

    ,2 )( ai

    k

    aj

    jkmim

    k

    aj

    jkia

    i

    Lds

    dxeg

    ds

    dxe

    ds

    de

    Here aimL - external and internal forces

    For 4D gyro we have

    If 0/,0 21 LL we will have

    where LL 2 -internal angularmomentum changesvelocity of the centerof mass

    1.

    2.

    When 0)( jkm then 0 and self-action disappears !

    2,1...,,,2 0)(2

    2

    kjiLds

    dx

    ds

    dxg

    ds

    dx

    ds

    dx

    ds

    xd ikj

    jkmim

    kj

    jki

    i

  • 4D gyro on a table4D gyro suspendedon the string

    22

    2

    2

    sin1

    )sin(2

    sin

    k

    vrkmr

    LB

    dt

    dvc

    Predictionof NewtonMechanics

    constvc constvc

    L(t)L(t)

    L(t)L(t)

    constvc constvc

    Predictionof an orientablepoint mechanics

  • ω

    bv

    cv

    Energy

  • Velocity of CM Cart velocity

    Look films on a site www.shipov.comLook films on a site www.shipov.com

    Predictionof NewtonMechanics

    constvc constLvv cc )(

  • ••Mechanics of an Orientable PointMechanics of an Orientable Point predicts newpredicts newancholonomic effects:ancholonomic effects:1. space1. space--time precession of 4D gyroscope;time precession of 4D gyroscope;2. controllable precession of 4D gyroscope,2. controllable precession of 4D gyroscope,

    that were confirmed experimentally.that were confirmed experimentally.

    ••Results of experiments with 4D gyroscope confirm existenceResults of experiments with 4D gyroscope confirm existenceof 6 additional angular coordinates as elements of 10of 6 additional angular coordinates as elements of 10dimensional space of the Universal Theory of Relativitydimensional space of the Universal Theory of Relativity..

    ••The discovered properties of space allow to create theThe discovered properties of space allow to create thepropulsion system of a new kind that can move in spacepropulsion system of a new kind that can move in spacewithout rejection of mass.without rejection of mass.

  • UFO