„emission & regeneration“ unified field theory osvaldo domann -methodology -main...
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„Emission & Regeneration“ Unified Field TheoryOsvaldo Domann
- Methodology- Main characteristics of Fundamental Particles (FPs)- Unified field for all forces- Coulomb law- Ampere law- Induction law- Time quantification - Gravitation laws- Momentum and force Quantification
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Methodology
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Postulated
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Particle representation
p p
ltransversaallongitudin
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nnn
sss
eee
JdEdE
JdEdE
JdEdE
==
==
==
22
2
22
2
22
==
=
po
pn
po
os
nspoe
EE
EE
EE
EE
whereEEEEE
Distribution in space of the relativistic energy of a BSP with v c
Introduction
4
2sin
2
1=
2
dddr
r
rd o
2
d ddr sindV=r 2
p
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Linear momentum out of opposed angular momentum
Introduction
nn Jν Ed
ldEdR
dE np
2
1
pp s dEc
1pd
pd
nJ
nJ
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Moving particles with their angular momenta
Introduction
p
p
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eeeee EHwithsdHHd ==
Definition of field magnitudes dH
Longitudinal emitted field
Transversal regenerating field
Longitudinal regenerating field
eeee sdκJν=sdH
ndκJν=ndH nn
Relation between the angular momentum J and the dH Field
Introduction
7
ssss E= H with sdκ=HHd
nnnn E= H with ndκ=HHd
sdκJν=sdH ss
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Characteristics of the introduced fundamental particles (FPs)
• Fundamental Particles are postulated.
• Basic Subatomic Particles (BSPs) are the positrons, the electrons and the neutrinos
• FPs store energy as rotations in moving and transversal directions
• FPs move with light speed relative to the focal point.
• Complex Subatomic Particles (CSPs) are composed of BSPs and are the proton, the neutron, nuclei of atoms and the photons.
• Pairs of FPs with opposed transversal angular momenta generate linear momenta on subatomic particles.
• FPs interact through their angular momenta or dH fields.
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Classification of Subatomic Particles
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Interaction laws between two BSPs (electrons and positrons)
1) Interaction between two static BSPs (Coulomb)
2) Interaction between two moving BSPs (Ampere, Lorentz, Bragg)
3) Interaction between a moving and a static BSP ( Maxwell, Gravitation)
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Index
These three interactions between BSPs correspond to the three following interactions between the longitudinal and transversal dH fields of the Interacting BSPs.
21 21ndHndHdE nnp
psnp dHdHdE
21 21sdHsdHdE ssp
Longitudinal X longitudinal (Coulomb)
Transversal X transversal (Ampere)
Transversal X longitudinal (Induction)
1)
2)
3)
The three following slides show each interaction in detail.
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1) Interaction law between two static BSPs (Coulomb)
Rrsrrer
se
RRstat sdHdHR
ssld
csdp
222111
21
2
)(1=
21 21sdHsdH=dE s
r
e
r
p
se
pdEc
dp1
sdκJν=s dH
Coulomb law
10
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2) Interaction law between two moving BSPs (Ampere, Lorentz and Bragg)
iiininiin
nnn
ndJndH
withndHndHdE
=
= 2211
)(1
RrnrrnrRRdyn sdHdHR
nnld
csdp
222111
21
2
)(1=
Ampere law
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3) Interaction law between a moving and a static BSP (Maxwell, Gravitation)
Rprpsprrrn
rrRRn
ind sdHdHR
nld
csdp
2
1=)(
„Induction law“
Induction law
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Time quantification
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21105.4271= =
m
sKrrKt oo
Ampered
II
2π
μ=FCoulomb
d
4π
1=F 21o
dyn221
ostat
cvforEEEwithE
cr poo 22==
cvforE ==
The radius of focal points of BSPs.
Quantification
13
and
Proposed approach
Standard theory
tfocal poinradius of rio
21p sdHsdH
c dt
1
c dt
dE
dt
dpF
21
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0.10 0=statp
1.80.1 2dpstat
2.11.8 constantpstat
5182.1 d
pstat
1
518 2
1
dpstat
Linear momentum as a function of the distance between static BSPsstatp
Coulomb
14
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Diffraction of BSPs at a Crystal due to reitegration of BSPs
Ampere law
15
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Gravitation between two neutrons due to aligned reintegration of BSPs
At stable nuclei migrated BSPs that interact with BSPs of same charge do not get the necessary energy to cross the potential barrier.
221=
d
MMGFG
Induction gravitation law
16
At unstable nuclei some of the migrated BSPs that interact with BSPs of same charge get the necessary energy to cross the potential barrier.
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Gravitation between two neutrons due to parallel reintegration of BSPs
21= MMd
RFR
Ampere gravitation law
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227 /106.05= kgNmR
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212RGT MMd
R
d
G=FFF
Total gravitation force due to the reintegration of BSPs
Induction +Ampere gravitation laws
18
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Quantification of momenta and forces
2.0887Coulomb
5.8731Ampere
2.4662Induction
Coulomb2
2o
oC 4 k d
a r
elemielemoii pp NF 13 kgms102.0309p 2elem
2107.4315k
d
MMγ
2 k m c
h 212RoR stantPlanck conh
Induction2212
02GoG d
MM r γ
4
1
Δ l d
II
c64 k m
b rAmpere
m2m122
2o
oA
0.25b 2108.774a -----------------------------------------------------------------------------------------------------
-----------------------------------------------------------------------------------------------------
-----------------------------------------------------------------------------------------------------
120102373.1 so
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Findings of the proposed approach
- Probability and quantification are inherent to the model
- All forces are generated by only one field
- The generation mechanism of forces out of the dH field is defined
- The origin of the charge of a particle is defined
- No weak force is required to explain radioactivity
- No strong force is required to explain coexistence of charged particles
- No dark matter is required to explain flattening of galaxie‘s speed curve.
- No dark energy is required to explain accelerated expansion
- etc.
- The inertia of particles with rest mass is explained
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Thank you for your attention,
The complete work is available at
www.odomann.com
Osvaldo Domann