„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

1

Methodology

2

Postulated

3

Particle representation

p p

ltransversaallongitudin

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

5

Linear momentum out of opposed angular momentum

Introduction

nn Jν Ed

ldEdR

dE np

2

1

pp s dEc

1pd

pd

nJ

nJ

6

Moving particles with their angular momenta

Introduction

p

p

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

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.

8

Classification of Subatomic Particles

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)

9

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.

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

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

11

3) Interaction law between a moving and a static BSP (Maxwell, Gravitation)

Rprpsprrrn

rrRRn

ind sdHdHR

nld

csdp

2

1=)(

„Induction law“

Induction law

12

Time quantification

24

21105.4271= =

m

sKrrKt oo

Ampered

II

2π

μ=FCoulomb

d

QQ

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

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

Diffraction of BSPs at a Crystal due to reitegration of BSPs

Ampere law

15

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.

Gravitation between two neutrons due to parallel reintegration of BSPs

21= MMd

RFR

Ampere gravitation law

17

227 /106.05= kgNmR

212RGT MMd

R

d

G=FFF

Total gravitation force due to the reintegration of BSPs

Induction +Ampere gravitation laws

18

19

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

21

Thank you for your attention,

The complete work is available at

www.odomann.com

Osvaldo Domann

odomann@yahoo.com