„Emission & Regeneration“ Unified Field Theory
Osvaldo 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
Postulated
2
Particle representation
transversal
longitudinal

p

p
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Introduction
Distribution in space of the relativistic energy of a BSP with v  c
Ee = Eo2  E p2  Es  En
Es =
d =
Eo2
E E
2
o
2
p
where
En =
E p2
Eo2  E p2
1 ro
d
dr
sin

d

2 r2
2
dEe = Ee d =  J e
dEs = Es d =  J s
dEn = En d =  J n
dV=r 2 dr sin d

p
d
2
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Introduction
Linear momentum out of opposed angular momentum


dE n  ν J n

Jn

dp

 Jn
 
1
dE p 
dE n dl

2R
 1

dp  dE p s p
c
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Introduction
Moving particles with their angular momenta

p
   

p

6
Introduction
Definition of field magnitudes dH
dH e = H e d  s e
with
H e = Ee
Longitudinal emitted field
dH s=H s dκ s
with
H s = Es
Longitudinal regenerating field
dH n=H n dκ n
with
H n= E n
Transversal regenerating field
Relation between the angular momentum J and the dH Field
dH e se= ν J e dκ se
dH s s = ν J s dκ s
dH n n = ν J n dκ n
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Characteristics of the introduced fundamental particles (FPs)
• Fundamental Particles are postulated.
• FPs move with light speed relative to the focal point.
• FPs store energy as rotations in moving and transversal directions
• FPs interact through their angular momenta or dH fields.
• Pairs of FPs with opposed transversal angular momenta generate
linear momenta on subatomic particles.
Classification of Subatomic Particles
• Basic Subatomic Particles (BSPs) are the positrons, the electrons
and the neutrinos
• Complex Subatomic Particles (CSPs) are composed of BSPs and are
the proton, the neutron, nuclei of atoms and the photons.
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Index
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)
These three interactions between BSPs correspond to the three following
interactions between the longitudinal and transversal dH fields of the
Interacting BSPs.


1) dE p  dH s1 s1  dH s2 s2


2) dE p  dH n1 n1  dH n2 n2
3) dE p  dH n  dH s
p
Longitudinal X longitudinal (Coulomb)
Transversal X transversal
(Ampere)
Transversal X longitudinal (Induction)
The three following slides show each interaction in detail.
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Coulomb law
1) Interaction law between two static BSPs (Coulomb)
dH s = ν J dκ s

dE p =


dH e1 s1   dH s2 s2
re
rs
dp 
dpstat
1
dE p
c


1 
 d l  ( se1  ss2 ) 

sR =  
H
d

H
d

r1 e1 r1 r2 s2 r2  sR
c R
2R


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Ampere law
2) Interaction law between two moving BSPs (Ampere, Lorentz and Bragg)
dE1( n ) = dH n n1  dH n n2
1
2
with
dH n ni =  n J n d i ni
i
dpdyn
i
i




1  dl  (n1  n2 ) 
sR =  
H n d r  H n d r  s R

1
1 r
2
2
R
r
c 
2R
1
2

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Induction law
3) Interaction law between a moving and a static BSP (Maxwell, Gravitation)
„Induction law“
( n)
dpind
sR =
1  dl  n

c R  2R


rr

H
d

sp
r p  sR
r r
p

H n d r

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Quantification
Time quantification
dp dE p
1
F


dH 1 s1  dH 2 s2
dt c dt c dt
Fstat=
1 Q1 Q2
4π o d 2
t = K ro ro
1
2
Coulomb
Fdyn=
Proposed approach
μo I 1 I 2
2π d
 s 
K = 5.427110 4  2 
m 
Ampere
Standard theory
roi  radius of focal point
The radius of focal points of BSPs.
ro =
c
E
with
E = Eo2  E p2
for v  c
and
E = 
for v = c
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Coulomb
Linear momentum pstat as a function of the distance between static BSPs
0    0.1
pstat = 0
0.1    1.8
pstat  d 2
1.8    2.1
pstat  constant
2.1    518
pstat 
518    
pstat
1
d
1
 2
d
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Ampere law
Diffraction of BSPs at a Crystal due to reitegration of BSPs
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Induction gravitation law
Gravitation between two neutrons due to aligned reintegration of BSPs
FG = G
M 1M 2
d2
At stable nuclei migrated BSPs that interact with
BSPs of same charge do not get the necessary
energy to cross the potential barrier.
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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Ampere gravitation law
Gravitation between two neutrons due to parallel reintegration of BSPs
FR =
R
M 1M 2
d
R = 6.05 10  27 Nm/kg 2
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Induction +Ampere gravitation laws
Total gravitation force due to the reintegration of BSPs
 G R
FT  FG  FR= 2   M 1 M 2
d
d
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Quantification of momenta and forces
 o  1.2373 10 20 s 1
Fi  N i  o pelem   i pelem
pelem  2.0309  10 23 kgms 1
-----------------------------------------------------------------------------------------------------
C
a ro2
 o
4 k d2


Coulomb
b ro2
I m1 I m2
 A  o
64 k m 2 c 2 d

 2.0887
Coulomb
Ampere
 G  o
1 2 2 M 1M 2
γG r0
4
d2
 R  o
h
M M
γR2 1 2
2kmc
d

Δl
Induction

 5.8731
Ampere

Induction
 2.4662
h  Planck constant
----------------------------------------------------------------------------------------------------a  8.774  10 2
k  7.4315  10 2
b  0.25
-----------------------------------------------------------------------------------------------------
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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
- The inertia of particles with rest mass is explained
- No strong force is required to explain coexistence of charged particles
- No weak force is required to explain radioactivity
- No dark matter is required to explain flattening of galaxie‘s speed curve.
- No dark energy is required to explain accelerated expansion
- etc.
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The complete work is available at
www.odomann.com
Thank you for your attention,
Osvaldo Domann
[email protected]
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