The Teaching of Djwhal Khul - Ethereal Mechanics

8/12/2019 The Teaching of Djwhal Khul - Ethereal Mechanics

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THE TEACHING OF DJWHAL KHUL

Book 2

ETHEREAL MECHANICS

* * * * *

THE SERIES

ESOTERIC NATURAL SCIENCE


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* * * * *

The Teaching of the Master of the Trans-Himalayan Esoteric School,

Djhal !h"l# The contin"ation of $ooks of H% Bla&atsky an' (( Bailey#Synthesis of Science an' Religion

* * * * *

TATIANA DANINA

* * * * *

The Teaching of Djhal !h"l - Ethereal Mechanics

)oyright + 2. $y Tatiana Danina

Translation from R"ssian $y Tatiana Danina

(nother $ook of the series /The Teaching of Djwha Kh! "E#o$e%ic Na$!%a Science0 & 'The (ain occ!$ aw# an) conce*$#+ &

htt1#ama3on#comMain-4cc"lt-5as-)oncets-

e$ook'B6788R92

( fragment from the $ook /New E#o$e%ic A#$%oog,0 yo" can rea'

here : htt1r"#scri$'#com'oc29;


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;# %articles Ain an' Aang# Mass an' antimass# %ositi&e an' negati&e

charges# Matter an' anti-matter.# Ether filling elementary articles : is their mo&ing factor

C# ?hat is a orce@ )lassification of orces# ?hy 'o elementary articles o$ey to the action of forces@

9# orce an' ress"re

=# The R"le of %arallelogram for elementary articles an' for'ifferent tyes of forces


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./0 1REFACE

HOW DOES A CONTACT WITH THE TEACHER OCCUR2

(ll $ooks of the series JThe Teaching of Djhal !h"l - Esoteric

nat"ral scienceJ are create' '"ring a me'itati&e contact of the 'iscileFa"thorG ith the conscio"sness of the Teacher Fthe (scen'e' Master Djhal

!h"lG#

IKll try to 'escri$e this rocess#I F'iscileG t"ne# I ent into a state of me'itation, mo&e aay from

earthly concerns an' start to concentrate on the theme that I ant to

"n'erstan' an' roerly interret for myself# 4r j"st I go into a me'itati&estate an' in this state fin' in my min' Ja$o&eJ something like a mental

arcel : some theme, a "estion that re"ires a arsing an' concentrate'consi'eration# Either this toic is knon to me or may $e entirely ne# I illnot kno "ntil look at this# ( &ieing is almost instantaneo"s# (n' no ILm

in the nee'e' state for ork# ItKs 'esira$le that $oth the hysical ell-$eing

is consistent to the high le&el of a mental-emotional acti&ity# Therefore, sloalks are the most 'esira$le time for s"ch me'itati&e contacts#

If a le&el of my moti&ation is high, i#e# itKs great the 'esire to"n'erstan' the iss"e : a comm"nication is m"ch easier, an' any noise 'i'

not interfere#

S"ch sessions are like teleathic lessons#The Messages from the Teacher are the tho"ght-ackages# They

'escen' to the $rain an' $ecome a JtriggerJ to the start of thinking on this

theme#In arallel, I am rearing for them - rea' $ooks, atch the st"'ie'

rocesses an' henomena, &is"ali3e, me'itate on gi&en toics# Ho"rs an'

'ays, ho"rs an' 'ays# E&en eeks an' months ere nee'e' sometimes forconsi'eration of a single, artic"larly 'iffic"lt iss"e# I can say that

a$sortion of 'etaile', $asic information on the occ"lt an' the &ario"s fiel's

of science took me a$o"t .-C years# There ere times, esecially in the

$eginning hen I co"l' not "n'erstan' many things# I highly straine' an's"ffere' hen it t"rne' $a'#

irst #C years there as a kin' of a"tomatic riting# I as immerse'

into the trance state an' j"st fie' on the aer that aeare' in the $rain# I

reali3e' all that I rote 'on# Hoe&er, I reali3e' that it as not comletelymy tho"ghts# This erio' as in some ay, a rearatory training# (n' the

most imortant an' interesting $egan then# D"ring this time F#C yearsG, I


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st"'ie' the metho' of ercetion of imressions sent teleathically#

Tho"ghts of the Master ere &ery clear, energetic an' highly 'eman'ing ofimme'iate fiation Fotherise they ill $e misse', an' they ill ha&e to $e

retransmitte'G# So I ent e&eryhere ith ens an' note$ooks, an'constantly rote hat ca"ses s"rrising an' c"rio"s glances of ro&incial

resi'ents that $y the ay 'i' not care me# 5et get "se' to the image of a

riter, I tho"ght to myself#(s the assimilation of transferre' material, an' rea'ing of more an'

more n"m$er of scientific an' esoteric literat"re Fmore - scientificG, I

gra'"ally $ecame a f"ll mem$er of the creati&e rocess of riting of articlesfor the $ooks# Together e orke' o"t the lang"age in hich it as ossi$le

to ass a ne terminology necessary to 'escri$e nat"ral henomena an'

rocesses eactly from o"r oint of &ie# I say Jo"rJ - in fact, I ha&e longago $ecome JtheirJ, teachers, orker# Therefore, I say Jo"rJ#

By the en' of -9- year arenticeshi I am so im$"e' ith the siritof the ne transmitte' teachings that co"l' no itho"t a constant controlof the Teacher elain most of things haening in the orl'# (ny scientific

$ook $ecame for me tr"ly oen, "nsol&a$le iss"es an' ro$lems

'isaeare'# E&erything has $ecome a$sol"tely clear# The 5as of(ttraction an' Re"lsion, Transformation an' I'entification tr"ly r"n the

sho in the "ni&erse# (t least in this "ni&erse# If to recogni3e the nat"re ofthese las then yo" ill "n'erstan' the meaning of science#

.30 WHAT IS ETHEREAL MECHANICS2

In this $ook, ethereal mechanics ser&es as an alternati&e to thequantum mechanics# (n' "ant"m mechanics as is knon, aims to

"n'erstan' the nat"re an' the las of the $eha&ior of elementary articles#

That ethereal mechanics seek to the same goal# (n alternati&e title : isMechanics of elementary articles FSo"lsG

"ant"m mechanics is really has fo"n' its footing in the early NN

cent"ry in connection ith the 'isco&ery of ra'ioacti&ity# The henomenon

of ra'ioacti&ity as a roof that s"$stances Fchemical elementsG arecomose' of smaller constit"ent arts : elementary articles# ?ith some ofthe rinciles of "ant"m mechanics e agree, ith others : 'oes not# In the

f"t"re, e ill talk a$o"t this in more 'etail#

In a''ition, e 'o not share the roositions of relati&istic mechanicsFith some ecetionsG# ?e remin' yo" that as the $asis of relati&istic

mechanics the secial theory of relati&ity, of (l$ert Einstein as lai' 'on#


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In relati&istic mechanics, there is eresse' the &ie that o$jects of

microcosm in its mo&ement an' $eha&ior in general are s"$ject to theentirely 'ifferent las of mechanics, rather than macroscoic o$jects, i#e#

allege'ly the las of classical mechanics canKt $e alie' to micro-o$jects,s"ch as elementary articles#

?e 'o not agree ith these theses#

It may seem s"rrising, $"t classical mechanics is the key to sol&ingof all ro$lems in hysics, chemistry, astronomy an' $iology# The las of

this mechanics "n'erlie of a$sol"tely each nat"ral henomenon, $"t not

eactly in the form in hich they c"rrently eist#?hen e talk a$o"t $o'ies : 'ense, li"i' or e&en gaseo"s, e think

that e&erything that haens to them is &ery nat"ral# Bo'ies mo&e : $y

inertia, "n'er an infl"ence of gra&ity, or $y contin"o"s eos"re Fress"reGto them $y other $o'ies# (lso, they are 'eforme' or 'estroye'# (nyone is

free to atch it all, 'escri$e, an' elore# That is hat scientists aro"n' theorl' are 'oing#

Hoe&er, these metho's are comletely inaroriate for the st"'y of

micro-orl' : chemical elements an' elementary articles : sta$le an'

"nsta$le# Their si3es are too small, so e canKt 'irectly o$ser&e &is"allythem an' ho they $eha&e# Hence, all the ro$lems an' challenges of

"ant"m hysics an' the lethora of theories seeking to 'isco&er the nat"reof the microcosm an' the las $y hich it eists#

In this ork, the (geless ?is'om Teachers in the face of one of them

: Master Djhal !h"l : 'efen' the osition accor'ing to hich a str"ct"reof any $o'y e&ent"ally re'"ce' to only one elementary articles# (ll is

constr"cte' of them# In'i&isi$le elementary articles : are sta$le articles#

7nsta$le articles : are conglomerates collecte' from sta$le articles# Int"rn, the smallest conglomerates $"il' the $igger ones, an' so on : as long

as e see the $o'ies arecia$le of &ie#

(n' if yo" accet, at least temorarily the claim that e&erything is$"ilt from the sta$le elementary articles Fso"lsG, then it o"l' $e logical to

ass"me that the las that go&ern the mechanical $eha&ior of $o'ies, are

s"ita$le an' for that from hich these $o'ies are $"ilt, that is, for articles#

Moreo&er, yo" ha&e to reali3e that mechanics of a $o'y consists ofmechanics of each smallest comonent in its comosition# (n' if the

articles o$ey to any other 5as of $eha&ior, then, of co"rse, an' the $o'ies

are o&en from the articles o"l' $e g"i'e' $y the same 5as#

5et "s recall the ell-knon occ"lt eression : JAs above, sobelowJ# Bo'ies are attracte' $eca"se the articles ha&e the a$ility to attract

in their comosition# (n' the re"lsion of $o'ies takes lace only '"e to the


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fact that a certain tye of articles is reelle' in their comosition# (n'

inertial motion of a $o'y : is the res"lt of inertia of the articles#?e "rge yo" not to in&ent something ne here not f"lly "n'erstoo'

an' "se' the ol' one# 5etLs take a chance to re&ie the las of classicalmechanics, gi&en the fact that the sace is fille' ith so"ls FarticlesG# (s

ell as letKs form"late ne las# Relying on the ol' re&ise' an' the ne

las letKs try to lay the fo"n'ations of mechanics of So"ls FelementaryarticlesG : of Ethereal Mechanics# ?e are confi'ent that the las of

classical mechanics can $e s"ccessf"lly "se' to elain all the henomena of

the microcosm# (n' e ill try to sho that in this $ook#

.40 1ARTICLES 5IN AND 5ANG0 MASS AND ANTIMASS0

1OSITI6E AND NEGATI6E CHARGES0 MATTER AND ANTI&MATTER

1) PARTICLES YIN AN YAN!A) Pa"ticles Yin # abso"bin$ Ethe": form in the ethereal fiel' of the

7ni&erse iel's of (ttraction#

Ether ten's to mo&e to s"ch article in accor'ance ith the firstrincile of the $eha&ior of Ether : JIn the ethereal fiel' &oi's 'o not

aearJ# This mo&ing in the 'irection of the article ethereal flo is a %iel&

o' Att"action#E&ery article Ain a$sor$s er "nit of time a fie' amo"nt of Ether#

Beca"se an ethereal fiel' is "niform e&eryhere, has no comression or

sarseness, e can talk a$o"t a see' of a$sortion of Ether# ( see' ofa$sortion ill j"st in'icate an amo"nt of Ether, a$sor$e' $y a article er

"nit of time#

() Pa"ticles Yan$ # emittin$ Ethe": form in the ethereal fiel' of the7ni&erse iel's of Re"lsion#

Ether ten's to mo&e aay from s"ch article in accor'ance ith the

secon' rincile of $eha&ior of Ether : JIn the ethereal fiel' the areas ith

ecess 'ensity 'o not aearJ# This ethereal flo mo&ing aay from thearticle : is a %iel& o' Reulsion#

Each article emitting Ether emits er "nit of time a fie' amo"nt ofEther# Emission see' in'icates the amo"nt of Ether emitte' $y article er

"nit of time#-------------------------------------------------------------------------------------

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*) +ASS # ANTI+ASS

>o letLs 'ra a arallel $eteen the hysical term that eists inscience : mass an' the concets fre"ently "se' in this $ook : iel's of

(ttraction an' Re"lsion#%articles ith iel's of (ttraction FAinG are resonsi$le for the rocess

of gra&itation - that is, for attraction to them of other articles# ( iel' of

(ttraction : this is mass#%articles ith iel's of Re"lsion FAangG are resonsi$le for the

rocess of anti-gra&itation Fstill "nrecogni3e' $y official scienceG : i#e# for

the rocess of re"lsion from them other articles# In science, there is notcomliance ith the concet of Re"lsion iel' therefore, e ill ha&e to

create it# Th"s, a iel' of Re"lsion : is antimass#

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) ELECTRIC C-AR!E # P.SITI/E AN NE!ATI/EI 'o not think that only I ant to com$ine a form"la 'escri$ing the

gra&itational interaction of $o'ies Fthe Law o' $"avit0G an' the form"la

'e&ote' to the interaction of electric charges Fthe Coulombs lawG# So letLs

'o itO>ee' to "t an e"al sign $eteen the concets of massan'ositive

cha"$e, as ell as $eteen the concets of antimassan' ne$ative cha"$e#( ositi&e charge For massG characteri3es the articles Ain Fith iel's

of (ttractionG : i#e# a$sor$ing Ether from am$ient ethereal fiel'#

( negati&e charge For antimassG characteri3es the articles Aan Fithiel's of Re"lsionG : i#e# emitting Ether into s"rro"n'ing ethereal fiel'#

In fact, mass For ositi&e chargeG an' antimass For negati&e chargeG

oints "s to the fact that the article a$sor$s For emitsG Ether#Regar'ing the rincile of electro'ynamics that there is a re"lsion of

e"al sign charges F$oth negati&e an' ositi&eG, an' an attraction to each

other of oosite sign charges, it is not entirely acc"rate# (n' the reason forthis : is the not "ite tr"e interretation of eeriments on

electromagnetism#

%articles ith the iel's of (ttraction Fositi&ely charge'G ne&er reel

each other# They only attract an' are attracte'# B"t articles ith the iel'sof Re"lsion Fnegati&ely charge'G, in'ee', alays reel from each otherFincl"'ing from the negati&e ole of a magnetG#

%articles ith the iel's of (ttraction Fositi&ely charge'G attract to

themsel&es any articles1 negati&ely charge' Fith the iel's of Re"lsionGan' ositi&ely charge' Fith the iel's of (ttractionG# Hoe&er, if $oth

articles ha&e iel's of (ttraction, then those of them hose 6ra&ity iel' is


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more, increasingly shift to its other article than it 'oes a article ith a

smaller iel' of (ttraction#-------------------------------------------------------------------------------------

--------------2) +ATTER # ANTI+ATTER3

In hysics a matter is $o'ies, as ell as chemical elements from hich

these $o'ies are $"ilt an' yet elementary articles# In general it can $econsi'ere' aroimately tr"e the "se of the term in this ay#+atte"in fact,

from the esoteric oint of &ie, is orce centers, i#e# elementary articles#

)hemical elements are $"ilt " of elementary articles, an' $o'ies : ofchemical elements# B"t e&ent"ally t"rns o"t that all consist of elementary

articles# B"t to $e acc"rate, then e see aro"n' "s not the Matter, an' So"ls

: that is, elementary articles# (n elementary article in contrast to the &oi'sace Fi#e#, in contrast of So"l to MatterG is en'oe' ith the "ality : in it

Ether aears an' 'isaears#The concet of substancecan $e consi'ere' as synonym ith the "se'

$y hysics concet of matter# S"$stance : is, "ite literally, hat constit"tes

things s"rro"n'ing a erson : that is, chemical elements an' their

como"n's# )hemical elements, as alrea'y mentione', consist of elementaryarticles#

or the s"$stance in science there are concets-antonyms : anti4substancean' antimatte", hich are synonyms to each other#

Scientists recogni3e an eistence of antimatter# Hoe&er, hat they

take to $e anti-matter, in reality is not that# In fact, antimatter alays is onhan' of science an' as in'irectly 'isco&ere' a long time ago, since then

eeriments on electromagnetism are $egan to con'"ct# ( manifestation of

its eistence e can constantly feel in the orl' aro"n' "s# (ntimatter in the"ni&erse came together ith matter at the &ery moment hen elementary

articles FSo"lsG aear# Substance: itKs articles Ain Fi#e# articles ith

iel's of (ttractionG# Anti4substance: itKs articles Aang Farticles ithiel's of Re"lsionG#

%roerties of articles Ain an' Aang are 'irectly oosite, in

connection ith hich they are ell s"ite' to the role of the re"ire' matter

an' antimatter#

.70 ETHER FILLING ELEMENTAR5 1ARTICLES IS THEIR

MO6ING FACTOR


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An elementa"0 a"ticle alwa0s ten&s to move to$ethe" with Ethe",which cu""entl0 'ills it in the same &i"ection an& with the same see&3

Ether : is a mo&ing factor of elementary articles# If Ether that fills the

article is motionless, an' the article is immo$ile too# (n' if Ether, fillingthe article, is mo&ing, the article is mo&ing too#

Th"s, $eca"se there is no essential 'ifference $eteen Ether of the

ethereal fiel' of 7ni&erse an' Ether of articles, all %rinciles of Ether$eha&ior are alica$le to elementary articles# If Ether, hich c"rrently

$elongs to a article, mo&ing toar' a 'eficiency of Ether Faccor'ing to the

first rincile of $eha&ior Ether : JIn ethe"eal 'iel& voi&s &o not occu"JG ormo&es aay from an ecess Fin accor'ance ith the secon' rincile

$eha&ior Ether - JIn ethe"eal 'iel& a"eas with e5cessive &ensit0 &o not

occu"JG, the article is mo&ing ith it in the same 'irection an' ith thesame see'#

.80 WHAT IS A FORCE2 CLASSIFICATION OF FORCES

%o"ce: is one of the f"n'amental concets in hysics in general, an'

esecially in one of its s"$-sections : in mechanics# B"t hat is it, ho tocharacteri3e it an' to s"ort $y something eisting in reality@

To $egin, letKs oen any %hysical )ollegiate Dictionary an' rea' the

'efinition#Jorce in mechanics : is a meas"re of the mechanical action on this material

$o'y of other $o'iesJ F%ED, JorceJ, e'# (M %rokhoro&G#

(s yo" can see, orce in mo'ern hysics 'oes not carry informationa$o"t something secific, real# B"t at the same time the manifestations of

orce are more than concrete# To reme'y the sit"ation, e nee' to look on

orce from the osition of the occ"ltism#rom the esoteric oint of &ie a %o"ce: it is nothing like Sirit,

Ether Energy# (n' a So"l, as yo" recall, this is also Sirit, only it is Jfol'e'

like a ringJ# Th"s, $oth the free Sirit : is the orce an' So"l Flocke' SiritG

: is the orce# This information ill greatly hel "s in the f"t"re#Desite some &ag"eness of the 'efinition of orce, it has "ite real

imlications# This is not an a$stract concet, as it aears in hysics to'ay#%o"ce : is the reason that comels Ether to mo&e toar' its

'eficiency or go aay from its ecess# ?e are intereste' in Ether enclose' inelementary articles FSo"lsG, so for "s a orce : is, first of all, the reason that


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'ri&es articles to mo&e# (ny elementary article : is the orce, as it 'irectly

or in'irectly affects on other articles#%o"ce can be measu"e& b0 the see& ith hich Ether filling the

article Fin other or's, the article itselfG mo&e "n'er the infl"ence of theorce if on it o"l' act other forces# That is, the see& o' ethe"eal 'low

coe"cin$ a"ticles to move, this is the ma$nitu&e o' this %o"ce#

5et "s classify all tyes of forces arising in articles, 'een'ing on areason, hich ca"ses them#

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--------------1) %.RCE .% ATTRACTI.N 6TENENCY .% ATTRACTI.N)3

The ca"se of this orce is any 'eficiency of Ether, aearing

anyhere in the ethereal fiel' of the 7ni&erse#That is, the cause o' a"isin$ in a a"ticle a %o"ce o' Att"action is an0

othe" a"ticle that abso"bs Ethe" # i3e3 'o"min$ a %iel& o' Att"action3-------------------------------------------------------------------------------------

--------------

*) %.RCE .% REP7LSI.N 6TENENCY .% REP7LSI.N)3

The ca"se of this orce is any ecess of Ether, aearing anyhere inthe ethereal fiel' of the 7ni&erse#

That is, the cause o' a"isin$ in a a"ticle a %o"ce o' Reulsion is an0othe" a"ticle emittin$ the Ethe" # i3e3 'o"min$ a %iel& o' Reulsion3

-------------------------------------------------------------------------------------

--------------) %.RCE .% INERTIA 6INERTIAL %.RCE)3

The ca"se of this orce is emission of all ro'"ce' $y a article Ether

not $y its entire s"rface, an' only the rear hemishere Fin the 'irection of itsmo&ementG#

Inertial orce arises in a article only '"e to the fact that there eists a

iel' of Re"lsion - an' an Inertial orce can $e consi'ere' as a secial caseof Re"lsion orce#

The 'ifference $eteen these forces is that a Re"lsion orce is a

ten'ency of a article to mo&e aay from the eternal for it the so"rce of

Ether, $"t an Inertial orce : is a ten'ency of a article to mo&e aay fromEther, hich emits $y itself#

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--------------

2) %.RCE .% PRESS7RE .% PARTICLE S7R%ACE3(ny mo&ing article itself is not an ethereal flo Fas oose' to real

ethereal streams create' $y the lack or ecess of Ether in the ethereal fiel'G#


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B"t, ne&ertheless, '"e to the fact that articles are fille' ith Ether, an effect

of the action of a mo&ing article on the article along the ay, m"ch like anaction of the iel' of Re"lsion#

The similarity lies in the fact that in each of these cases the articleten's to mo&e aay from ressing on it Ether : from Ether filling the

article, or from Ether of iel's of Re"lsion# The 'ifference lies in the fact

that is, if the article is fie' $y some iel' of (ttraction Ffor eamle, $yiel' of (ttraction of a chemical elementG an' canKt freely mo&e ith

ressing on it Ether, in the case of the action of Re"lsion iel' the Ether of

this iel' ass thro"gh it# Ether enters into the article an' transforms it# B"tEther filling a article canKt lea&e it an' enter in another article, hich

resses an', accor'ingly, its transformation 'oesnKt occ"r#

The most common eamle hen in articles the %ress"re orce onthe art of the other article is forme' : is collision of articles#

( ress"re on a article &ery often lea's to arising the orce of Inertiaan' the $eginning of its inertial motion#

A)A a"ticle, uttin$ "essu"e on the othe" a"ticle is '"ee 6not a"t

o' an0 con$lome"ate a"ticles) an& moves on thei" own # b0 ine"tia3

(ccor'ingly, at the time of collision it has a iel' of Re"lsion an' anInertial orce acts in it# Hoe&er, '"e to the fact that the ethereal fiel',

relati&e to hich it mo&es, offers resistance an' 'islaces emitte' $y thearticle Ether to the $ack, the article ressing not ith Ether of the iel' of

Re"lsion, an' ith the filling it Ether#

()A a"ticle uttin$ "essu"e is a a"t o' the con$lome"ate o'a"ticles, such as a chemical element3

( chemical element, in t"rn, is a art of the $o'y hich is j"st mo&ing

$y inertia#(s a res"lt, the articles in the elements on the s"rface of the $o'y "t

a ress"re#

>ot all articles of elements of the $o'y mo&ing $y inertia form aRe"lsi&e iel' at the moment of inertial motion# Therefore, the ress"re of

the analy3e' article may "t as a article ith a iel' of Re"lsion an' a

article ith a iel' of (ttraction# Hoe&er, in any case, the Ether filling the

article "ts the ress"re on the st"'ying article# E&en if it is a article itha iel' of Re"lsion, as emitte' $y it Ether is 'islace' '"ring the inertialmotion $ack "n'er the ress"re of s"rro"n'ing ethereal fiel'#

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--------------So, letLs s"mmari3e an' gi&e 'efinition to all .th tyes of orce#


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%o"ce o' Att"action: is a reason that ca"ses a article to mo&e in the

'irection of aearing anyhere in the ethereal fiel' of the "ni&erse a lack ofEther#

%o"ce o' Reulsion: is a reason ca"ses a article to mo&e aay fromaearing anyhere in the ethereal fiel' of the "ni&erse an ecess of Ether#

%o"ce o' Ine"tia: is a ten'ency of a article to mo&e aay from its

on Ether emitte' $y its rear Fon the 'irection of mo&ingG hemishere#%o"ce o' P"essu"e o' the a"ticle su"'ace : is a ten'ency of a article

to mo&e in the same 'irection that an' ressing on it other article#

.90 WH5 DO ELEMENTAR5 1ARTICLES O:E5 TO THE

ACTION OF FORCES2

5et "s ask o"rsel&es the folloing "estion : hy orces are caa$leto infl"ence on elementary articles@ 4r yo" can say otherise : hy 'o

articles o$ey to orces@

In the $ooks, films an' TP rograms on hysics e can hear or rea'the folloing statements1 JThe force ith hich the $o'y is eose' toQJ,

JThe force that as alie' to the $o'yQJ, etc# Ho to interret the 'eeermeaning of these hrases@

?e m"st start ith a remin'er that orce : this is a reason that ca"ses

articles FSo"lsG to mo&e in the Sace# Each of the fo"r eisting tyes oforces affects on the So"ls FarticlesG : i#e# 'ri&es them : in a manner

somehat 'ifferent from the rest# The orce of (ttraction makes articles to

aroach# The orce of Re"lsion an' the orce of %ress"re of the %articleS"rface reel articles# The orce of Inertia "shes forar' the emitting this

orce Fthis EtherG article# B"t 'esite this 'ifference, the reasons for hich

articles o$ey to the orces, f"lly fit into the frameork of to rinciles of$eha&ior of Ether, hich e 'escri$e' in the $ook /The main occ"lt las

an' concets0# Beca"se articles are nothing more than Ether# 5et "s recall

the main oints a$o"t these to reg"larities#

To rinciles manage $y 'istri$"tion of Ether in the "ni&erse# Ao"can call them J>at"re a$hors a &ac""mJ an' J >at"re a$hors a s"rl"sJ# Inother or's :JIn the ethe"eal 'iel& voi&s &o not occu"J an' /In the ethe"eal

'iel& a"eas with e5cessive &ensit0 &o not occu"J#

(ll eisting in the "ni&erse Ether ten's to e&enly fill e&ery oint ofSace# Hence, the first rincile of $eha&ior of Ether - JIn natu"e the"e is

no voi&J# The eression JNatu"e abho"s a vacuumJ in this case means that,


14/89

if at any oint of Sace Ether 'isaears, am$ient ethereal fiel' JflosJ in

this 'irection, creating an ethereal flo#Ho is it going a mo&ement of Ether in the 'irection of 'eficiency of

it@ Ether, a'jacent to the lace here some Ether 'isaears r"shes there# (sa res"lt, the lace here it has j"st $een is release'# In its lace, Ether

r"shes, hich coeiste' ith it, an' is f"rther from the lace here Ether

'isaears# (n' in its lace Ether r"shes, locate' f"rther aay from thelace of 'eficiency of Ether# (n' so on to infinity#

(s a res"lt to the lace of 'eficiency of Ether from the am$ient

ethereal fiel' an ethereal stream mo&es#Th"s, Sirit FEtherG 'oes not allo the Sace $eing emty, i#e# 'e&oi'

of Ether#

This rincile of Ether $eha&ior is the $asis of the mechanism ofgra&ity : an attraction to each other of o$jects ranging from s"ch as

elementary articles#The secon' rincile of $eha&ior of Ether - JIn natu"e the"e is no

e5cessJ - meaning that if at any oint of the Sace, there is an ecess of

Ether, that Ether s"rro"n'ing this oint $egins to mo&e aay from this oint#

4therise yo" can say that arising Ether "shes s"rro"n'ing Ether#This rincile, like the re&io"s one, also alies to Ether in

elementary articles#This rincile is the $asis of the mechanism of anti-gra&ity - that is, a

re"lsion of o$jects#

If areas ith 'eficiency or ecess of Ether 'i' not arise in the etherealfiel' of the "ni&erse, then all eisting Ether o"l' $e a$sol"tely motionless#

B"t an eistence of elementary articles in Sace is the reason that Sirit of

the "ni&erse is constantly in motion, stri&ing in any 'irection# It either ten'sto 'istance itself from a emerging near$y re'"n'ancy Fforming $y articles

ith iel's of Re"lsionG, or ten's to aroach to the fail"re occ"rring

near$y Fforming $y articles ith iel's of (ttractionG# (ll Ether, mo&ing toa artic"lar lace here there is a 'eficiency of it, or mo&ing aay from the

lace here there is an ecess, forms an ethe"eal 'low# (n eistence of

ethereal flos is a conse"ence of the first an' secon' rinciles of $eha&ior

of Ether#(ny "nit of Ether &ol"me at each moment of time is a art of any

ethereal stream : i#e# seeks to 'istance itself from the ecess of Ether or

aroach to 'eficiency# Elementary articles may lay the role of J"nits of

the Ether &ol"meJ# Esecially that it is in fact - each elementary article is ashere that has a certain &ol"me Fthe same for all articlesG#


15/89

Ether, hich $elongs each moment of time the elementary articles is

not 'ifferent from the free Ether# Therefore Ether of any elementary articleat each moment of time incl"'e' in the comosition of any ethereal stream -

i#e# ten's to mo&e aay from an ecess of Ether or aroach to a 'eficiency#Elementary articles ten' to mo&e together ith filling them ethereal a&es#

(ny ten'ency that arises in an elementary article - to mo&e aay from an

ecess of Ether or aroach to a 'eficiency, this is the Jsubo"&ination to the%o"ceJ#

4nly one of fo"r orces : orce of (ttraction : is $ase' on the

rincile of aroimation to a 'eficiency of Ether# (ll other orces :Re"lsion orce, orce of %ress"re an' orce of Inertia : are $ase' on the

secon' rincile : searation from the ecess of Ether#

So e ha&e tol' a$o"t the reasons that make the articles to o$ey#An0elementa"0 a"ticle is a cause o' eme"$ence o' the %o"ce 6Att"action o"

Reulsion # this is a "e"equisite) in all othe" a"ticles o' the unive"se3An& at the same time, an0 a"ticle is the oint o' alication o' %o"ce

%iel&s o' all othe" a"ticles o' the unive"se3 .tional 6but not necessa"il0)

a"ticles ma0 become a sou"ce o' %o"ce o' +ovin$ Pa"ticle o" oint o'thei" alication o' othe" a"ticles3 An& in a movin$ a"ticle a %o"ce o'

Ine"tia can a"ises3

.;0 FORCE AND 1RESSURE

orce is closely linke' ith the concet of"essu"e#

orce is Ether, Energy# ree Ether emitte' $y articles, is a orce#

This Ether Fi#e#, this orceG is a$le to "t ress"re on $o'ies, i#e# to imactmechanically : an' to mo&e them, 'eform an' 'estroy# (t the same time

Ether filling articles : it is also a orce# That is, each elementary article :

its s"rface : is a orce# (n' hen any article mo&es an' colli'es ith otherarticles, it "t ress"re on them#

The first of these orces : free, emitte' Ether : is associate' ith

articles Aang, since eactly they emit Ether# %articles Aang : are %o"ces o'

Reulsion#The secon' orce : is %o"ce o' "essu"e o' the a"ticle su"'ace # (ny

mo&ing article : hether Ain or Aang : reresents a orce of Mo&ement#

That is, a mo&ing article acts as a orce : it can eert ress"re#

The thir' orce is %o"ce o' Att"action# %articles Ain a$sor$ing Etherhen they are motionless ne&ertheless also are orces# B"t this orce is

secial, "nlike the re&io"s to# Beca"se that the 6ra&ity iel' create' $y


16/89

s"ch article 'oes not lea' to ress"re of the article on another F"nlike the

a$o&e to casesG# Hoe&er, the 6ra&ity iel' of a article Ain is the ca"se,first, of the ress"re on this article $y other articles Ain that are attracte'

to it, an' secon'ly, of the ress"re eerte' $y the articles Ain each other intheir asiration to $e attracte' to o"r article# This latter case of ress"re e

can o$ser&e in the orl' aro"n' "s hen e are in the hea&enly $o'y : in

the lanet# Soli' an' li"i' $o'ies, aiming toar's the center of Earth, resson each other# Each of "s can feel this ress"re $y its on $o'y, if, for

eamle, "t on the alm any o$ject, e&en a $ook# Elementary articles of

chemical elements of the $ook are gra&itate' $y articles Ain of chemicalelements of the Earth# Beca"se of this, the articles of the $ook "t ress"re

on each other, an' on the articles of the han'#

The last of the orces : is %o"ce o' Ine"tia# Ether emitte' $y rearhemishere of a mo&ing article resses only on the article itself#

Th"s, articles Ain an' Aang may either themsel&es act as orcesFtheir s"rfaceG, or $ecome an in'irect ca"se of a orce : articles ith iel'sof Re"lsion generate orces of Re"lsion an' articles ith iel's of

(ttraction gi&e rise to orces of (ttraction#

?e remin' yo" once again that a %o"ce: it is nothing like EtherFEnergyG : either free Femitte'G, or enclose' in a article# (n' there are only

fo"r tyes of forces : Reulsion, Att"action, P"essu"e o' Su"'ace o' thea"ticlean'Ine"tial#

(ll fo"r of these tyes of orces are the ca"se of the ress"re on

articles : either on free, or on ones that in conglomerates of articles#%ress"re ca"se' $y any of three orces, is not 'ifferent from ress"re of

other tyes of orces# %ress"re of emitte' Ether is eactly the same as

ress"re of a mo&ing article# (n' it is comletely i'entical to ress"re theca"se of hich : is a orce of (ttraction# That is, free Ether resses as ell

as Ether, enclose' in an elementary article# The only 'ifference $eteen

ress"re of free Ether an' ress"re of articles - is that free Ether, eertingress"re on a article, at the same time is a$le to ass thro"gh it, $reak 'on

in it, an' heat it in a s"ch ay Ftransform itG# By the ay, atmosheric

ress"re is eactly this tye of ress"re# It is caa$le to heat $o'ies on the

s"rface of the lanet, assing thro"gh them# B"t hen a article s"rfaceresses on a article, Ether of the article canKt enter into the article, an'conse"ently, canKt transform FheatG it#


17/89

.


18/89

meaning of hat is haening ith the article hen more than one orce

affects on it# or eamle, it says nothing a$o"t the fact that there are'ifferent tyes of orces#

The Dominant orce : is the orce hich is greater in magnit"'e# (se sai' earlier, a magnit"'e of a orce - is the rate of ethereal flo

entraining the article# Moreo&er, Ether j"st fills a article can act as an

ethereal flo Fas in the case of the orce of %ress"re of the article s"rfaceG#The Rule o' Subo"&ination to the ominant %o"ce Fthe R"le of

%arallelogramG reresents that the article, on hich act more than one

orce, to the greatest etent ill $e s"$ject to the higher of them# ?hat 'oesthis mean@ This means that the &ector of res"ltant forces at each moment

ill $e more $iase' toar's the &ector of orce ith the highest magnit"'e#

That is, the $iggest orce re&ails, $"t other orces also ha&e an effect onthe osition of the res"ltant force &ector# Ao" can f"rther secify the name of

the r"le - Subo"&ination to the ominant %o"ce ith an acco"nting ofactions of the remaining forces#

The Dominant orce shifts the &ector of res"ltant orce in its on

'irection more than others# (n' other, smaller forces 'o not gi&e this &ector

to f"lly s"$mit to this $iggest orce# They "ll the &ector in their 'irection inroortion to their magnit"'e#

---------------------------------------------------------------------------------------------------

In general, in the analysis of any sit"ation in hich an elementary

article is infl"ence' $y more than one force it is necessary to consi'er an"m$er of factors# irst,0ou nee& to 8now how man0 'o"ces actin$ on the

a"ticle an& the value o' each o' them# Secon'ly,0ou nee& to 8now at what

an$le the vecto"s o' %o"ces a"e lace& one a$ainst the othe"# (n' thir',0ou must consi&e" the t0e each o' 'o"ces# 4nly e&al"ating all these factors,

e can try to calc"late the 'irection an' &elocity of a article at e&ery

moment of time# 5etLs take a little closer look at these factors#1) A value an& total quantit0 o' 'o"ces actin$ on a a"ticle m"st $e

assesse' in each artic"lar case#

In that case, if a n"m$er of forces acting on the article is greater than

to, e sho"l' 'o the same as in the case of $o'ies# ?e nee' to $"il' thearallelogram for to forces# Then e ill make the net arallelogram,"sing the res"lting &ector an' the net of forces# (n' so on, "ntil it ill $e

acco"nt all of orces#

*) An an$le between the vecto"s o' 'o"ces actin$ on a a"ticle is ve"0imo"tant in cla"i'0in$ the ma$nitu&e an& &i"ection o' the "esultant 'o"ce3

A) An an$le between vecto"s o' %o"ces is '"om 9: to ;9:3


19/89

In this case there is some kin' of s"mmation of the orces acting on

the article# 4f co"rse, the res"ltant orce ill not $e eactly e"al to thes"m of to orces acting on the article# B"t in any case it ill $e more than

either of to forces, on hose &ectors e $"il' the arallelogram# Ao" cansee this in the &al"e of the 'iagonal of a arallelogram# (n' the sharer an

angle is, the $igger the &al"e of the res"ltant orce is#

An e5t"eme case o' an acute an$le is 9:, i3e3 absence o' co"ne"# orce&ectors are on one line, an' their 'irection is the same# In this case, it is

imossi$le to constr"ct the arallelogram# Instea' of it - straight, e "t on

it to segments, each of hich is e"al to one of the oerating orces# (t is the total s"mming of orce &ectors#

() An an$le between vecto"s o' %o"ces is mo"e than ;9:3

In this case yo" can see from the ict"re, there is a kin' of s"$tractionorces# The res"ltant orce is alays more than the smaller of to orces

an' less of the $iggest one# )onfirmation of this is a &al"e of the 'iagonal#(n' the greater an angle is, the smaller the res"ltant force is#

An e5t"eme case o' an obtuse an$le is an an$le o' 1


20/89

he has 'one in relation to the orces, ith hich some $o'ies "t ress"re

on others or 'rag them, making to mo&e# This tye of orce is calle' in this$ook the orce of %ress"re of the %article S"rface# ?e ha&e hear' a little

a$o"t that the R"le of %arallelogram is "se' for 6ra&ity orce# Esecially,this limit alies to Re"lsi&e orce an' orce of Inertia, the first of hich

is almost not recogni3e' $y science, an' the secon' is not knon at all#

B"t anyay, this r"le is "ni&ersal an' can $e "se' for any of fo"rtyes of forces - %ress"re of the %article S"rface, (ttraction, Re"lsion an'

Inertia# Hoe&er "nchange' it can $e alie' only to orce of %ress"re of

the %article S"rface, i#e# for the same e&ent, hich is 'escri$e' $y 6alileofor $o'ies#

To $o'ies affect on the $o'y from $oth si'es - or "t ress"re on it

or 'rag# In o"r case, to articles ress on the article Fthey canKtmechanically 'rag the articleG#

Taken searately a free article ill ne&er ca"se long-term ress"re onother article, if only the orce of (ttraction 'oesnKt act on it from another

article# (lternati&ely, if articles are incl"'e' into $o'ies an' they s"ee3e

each other an' any article $eteen them# Therefore, in o"r case it is one-

stage ress"re on the article of to articles as a res"lt of the collision ithit# ?hen to articles colli'e ith a article, it starts to mo&e $y inertia,

eactly in accor'ance ith the R"le of %arallelogram# The 'iagonalFres"ltant orce &ectorG shos the 'irection in hich the article ill mo&e#

Ho long inertial motion ill, 'een's on the rate at hich the articles

ere mo&ing at the time of the collision ith it, on the angle $eteen the&ectors of orces an' more on the "ality of the article itself#

C) The onl0 &i''icult0 that we 'ace in the const"uction o'

Pa"allelo$"am o' %o"ces is "elate& to Att"action an& Reulsion %o"ces3Here it is soken e&en more likely not a$o"t the 'iffic"lty $"t a$o"t of

strangeness# So"rces of forces of attraction or re"lsion are locate' from the

article on one or another 'istance# Hoe&er, the article feels effect ofthese forces 'irectly# This is not s"rrising, $eca"se a gra&itational

interaction or anti-gra&itational roagates instantaneo"sly# This

instantaneo"s 'issemination is elaine' $y the fact that an ethereal JclothJ

: it is a kin' of monolith that fills homogeneo"sly the entire "ni&erse# (n'the aearance in this cloth of any ecess or 'eficiency of Ether isimme'iately felt at any 'istance#

In this case, hen tyes of orces acting on a article, are 'ifferent,

the &ector of orces m"st in'icate the 'irection in hich the orce stri&es to'islace the article# or eamle, if a orce of (ttraction acts on a article,

so the &ector ill $e 'irecte' to an o$ject, the so"rce of this force, an' not of


21/89

it# B"t in the case of Re"lsion orce all is the oosite# The &ector ill $e

'irecte' from the so"rce of the orce#(s the orce of %ress"re of the %article S"rface, e&erything is the

same as in mechanics of $o'ies# In this case, the so"rce of orce is in 'irectcontact ith the article - colli'es ith it# (n' &ector of this orce is

'irecte' in the same 'irection as the motion &ector of a article hose

s"rface eerts ress"re#(n' finally, there is last of orces : orce of Inertia# The resence of

this force can $e 'isc"sse' only in the case if a article is mo&ing $y inertia#

If the article is not mo&ing $y inertia, there is no orce of Inertia# ( &ectorof Inertia orce alays coinci'es ith the &ector of motion of article at this

moment# ( &ector of Inertia orce is Ether emitte' $y the rear Hemishere

of article#) Neve" haens that two 'o"ces actin$ on a a"ticle we"e ine"tial,

as a a"ticle can move b0 ine"tia at each moment o' time onl0 in one&i"ection3

E)If one or $oth of orces acting on a article relate to the tye or of

(ttraction or Re"lsion, the a"ticle will move in a"abola, gra'"ally

'islacing $y the action of the larger orce#If one of orces acting on a article refers to the tye of (ttraction or

Re"lsion, an' the secon' - is orce of Inertia, hile the trajectory of thearticle is also ara$olic#

%)It is neve" at the same time %o"ces o' Att"action an& Reulsion

act on a a"ticle, an& thei" vecto"s woul& on the same line an& woul& beoosite &i"ections# The reason is that orce of (ttraction an' orce of

Re"lsion are orces-antio'es# ( &ector of orce of (ttraction is 'irecte' to

the so"rce of orce# (n' a &ector of Re"lsion orce is 'irecte' from it#Therefore, if so"rces of (ttraction an' Re"lsion orces are locate' on

oosite si'es of a article, the &ectors of their forces ill $e s"mme'#

If so"rces of orces are on one si'e of a article, the article ill feelonly any one of orces - either of (ttraction or Re"lsion# (n' all $eca"se

the iel's of (ttraction an' Re"lsion screen an' affect on the &al"e of each

other#

B"t in any case, the Rule o' Pa"allelo$"am can be use& to an0a"ticle, to &ete"mine with its hel a &i"ection an& ma$nitu&e o' "esultant%o"ce3 In acco"&ance with the ma$nitu&e an& &i"ection o' the vecto" a

a"ticle will be &islace& in a $iven moment o' time3

(ll that e ha&e j"st $een sai' of the R"le of %arallelogram forarticles can $e f"lly "se' for $o'ies#


22/89

.=0 MECHANICAL 1ROCESSES AND 1HENOMENA RE6EAL

MACHANICAL 1RO1ERTIES OF ELEMENTAR5 1ARTICLES

( mechanical rocess an' a mechanical henomenon - are secialcases of hysical rocess an' hysical henomenon#

("ocess- is an e&ent, occ"rring in time#

( henomenoncan $e &iee' either as an e&ent selecte' at someoint of time of a rocess, either as a generali3e' name of a rocess#

(ccor'ingly, e "n'erstan' "n'er a mechanical "ocess any

mechanical e&ent ha&ing time frames# ?e ill call as a mechanicalhenomenon the same mechanical rocess, $"t in a more general form,

itho"t secifying that it has any time limits#-------------------------------------------------------------------------------------

--------------

There are fo"r $asic mechanical rocesses# They correson' to the

fo"r $asic mechanical henomena, each of hich s"mmari3es themechanical rocess ith the same name# In this section e talk a$o"t

mechanics of elementary articles, so e form"late concets relate' toelementary articles# Here are fo"r $asic mechanical rocesses an'

henomena1

G (ttraction of elementary articles2G Re"lsion of elementary articles

;G Inertial motion of elementary articles

.G )ollision of articles#+echanical "oe"ties o' elementa"0 a"ticles - are their

characteristics that manifests Fare 'isclose'G in those rocesses an'

mechanical henomena, in hich articles in&ol&e'#--------------------------------------------------

------------------------------------------------

5etLs 'ra a arallel $eteen the main mechanical rocesses Fan'

henomenaG an' mechanical roerties of elementary articles, hich in thiscase are re&eale'#

1) The henomenon of JAtt"action o' a"ticlesJ re&eals their

folloing mechanical roerty - an a$ility to aroach ith other articles

an' kee them near, i#e# an abilit0 to 'o"m an& maintain a connection withothe" a"ticles# This mechanical roerty Fi#e# this a$ilityG $elongs only to

articles ith iel's of (ttraction#


23/89

*)The henomenon of JReulsion o' a"ticlesJ re&eals the folloing

mechanical roerty of articles - an a$ility to mo&e aay from otherarticles, i#e# an abilit0 to 8ee a &istance between itsel' an& othe" a"ticles#

In artic"lar, the a$ility to eaken or $reak eisting connections Fe#g#, anincrease in the total n"m$er of articles ith iel's of Re"lsion in elements

linke' chemically, can lea' to r"t"re of the connectionG#

) The henomenon of JInertia of articlesJ re&eals an abilit0 o'a"ticles to maintain a state o' ine"tial motion# (n' as a 'isting"ishing

feat"re of articles of 'ifferent "ality it re&eals an abilit0 o' a"ticles to

8ee the initial see& &u"in$ the motion#2) The henomenon of JCollisions o' a"ticlesJ re&eals to

mechanical roerties of elementary articles1

a) An abilit0 o' a"ticles to be b"ou$ht into the state o' ine"tialmotion>

b) An abilit0 o' a"ticles to lea& othe" a"ticles into the state o'ine"tial motion3

/.0 THE MECHANISM OF GRA6ITATION >ATTRACTION?

The mechanism o' att"action$ases on the first rincile of $eha&ior

of Ether - JIn the ethe"eal 'iel& voi&s &o not occu"J# Ether filling a articlemo&es in the 'irection of lack of Ether, aearing in the lace of ethereal

fiel' here an o$ject ith a iel' of (ttraction is locate'# It 'oes not matter

hat "ality the gra&itating article has - it can has as an (ttracti&e iel'an' a Re"lsi&e iel', an' a magnit"'e of these fiel's can $e any# In any

case, filling it Ether ill mo&e in the 'irection of lack : i#e# comrising an

ethereal flo of (ttraction iel' of the o$ject that attracts the article#(n ethereal flo of iel' of (ttraction, enthralling the attracting

article, this is the %o"ce o' Att"action#

Imme'iately e sho"l' clarify a &ery imortant oint# If $oth

interacting articles ha&e iel's of (ttraction ith 'ifferent magnit"'es,then an attracting article is the one ith a $igger fiel', an' an attracte'

article is the one ith a smaller iel'# I#e# a a"ticle with a smalle" %iel&

o' Att"action will a"oach to the a"ticle with a bi$$e" 'iel&, an& not vice

ve"sa# Ao" can call it the Rule o' Submission to the ominant %o"ce o'!"avit0# Hoe&er, $oth articles fell an eistence an' action of iel's of

(ttraction of each other : as it a iel' of greater magnit"'e an' smaller#


24/89

B"t to feel a iel' : it 'oesnKt mean to o$ey him# 5etKs reeat : the article

ith a smaller iel' o$eys to the article ith a $igger one mo&es toar' it#I' both a"ticles have %iel&s o' Att"action an& thei" value is the

same, then the0 a"e both simultaneousl0 att"actin$ an& att"acte&3 An& bothwill move towa"&s each othe" 4 conve"$e3

In the event that onl0 one o' the a"ticles has an Att"active %iel&,

an& the secon& is cha"acte"i?e& b0 the %iel& o' Reulsion, while onl0 aa"ticle Yin can be an att"actin$ one3 A Yan$ a"ticle alwa0s is att"acte&3

?hen a article mo&ing in 6ra&ity iel' of other article, an' then

comes closer, it stos - a connectionarise $eteen the articles# Ao" can callit the$"avitational, i#e# '"e to the action of (ttraction iel'# There is no

chemical, n"clear or any other kin's of connection#An0 t0e o' this one is

$"avitational, i3e3 e5istin$ &ue to the action o' the Att"action %iel&3 (nemergence of connection $eteen articles e can call as a fiing of the

articles each to other#Hoe&er, as eKll say in the f"t"re in an article a$o"t the

transformation $y gra&ity, attracte' articles 'o not to"ch each other# The

ga $eteen them remains# (n' henomenon of transformation of the

"ality elains $y the reser&ation of 'istance#The rocess of gra&itation e can comare ith the in'ing " of

threa'# If $oth articles ha&e iel's of (ttraction, then the JtanglesJ arelocate' 'irectly at $oth en's of Jthrea'J, an' they $oth in' the Jthrea'J at

the same time, each ith their on si'e# The Jthrea'J in this case - is Ether

an' the JtanglesJ : are articles# ( tangle-article, Jin'ingJ Ether ith ahigher see' $ring closer to itself a JtangleJ in'ing Ether ith a sloer

see'# ?hen the JtanglesJ comletely reel " free Jthrea'J among

themsel&es, they are in contact ith each other an' sto# In this case, $othJtanglesJ reel " the /threa'0, that is, $oth ha&e the iel' of (ttraction#

B"t it may $e that only one of the JtanglesJ is in'ing a Jthrea'J,

hile another is "nin'ing it : i#e# only one of the articles has a iel' of(ttraction, hile other has a Re"lsi&e iel'# >at"rally, tangles-articles

ith iel's of (ttraction can in' the threa' onto itself in'efinitely itho"t

changing their si3es, as ell as articles ith iel's of Re"lsion are

infinitely caa$le to "nin' it off Falso not changing a si3e of the ra'i"sG# Sothis is the rocess of attraction of articles#

Th"s, e&en after the articles are attracte' to the contact they contin"e

to stri&e toar's each other so as Ether, filling e&ery article at each oint in

time contin"es to stri&e toar's an a'jacent article, here a lack of Etheris# )onstantly create' $y attracte' articles ith iel's of (ttraction an

Jethereal emtinessJ is recisely the ca"se of the JconnectionJ of articles#


25/89

?hen attracting an' attracte' articles close together an' to"ch, they

contin"e to a$sor$ Ether $eteen them at the oint of contact# Do not forgetthat the articles a$sor$ not the Ether, hich is in contact ith the s"rface of

the articles, an' the one in hich the s"rface is s"$merge'# %articles are thesheres an' the area of their contact ith each other is only one oint# Ether

still contin"es to recei&e from the am$ient fiel' to the article s"rfaces

contacting each other# Therefore, in the area of contact of the articles itheach other the lack of receit of Ether from the s"rro"n'ing fiel' 'oes not

arise#

//0 THE FORCE OF ATTRACTION

(s alrea'y mentione', an ethereal flo, ca"sing the article to mo&ealong ith filling it Ether is a orce Fin this case, a orce of (ttractionG#

orce of (ttraction can occ"r in articles of any "ality# 5etLs look at

the 'etails of the mechanism of gra&ity on eamle of articles of 'ifferent

"ality# A thou$ht e5e"iment that we a"e con&uctin$ occu"s in i&eal

con&itions # i3e3 in a totall0 emt0 sace3 4ne of the interacting articles

necessarily has a iel' of (ttraction#1) (oth inte"actin$ a"ticles have %iel&s o' Att"action3

A) The value o' Att"action %iel&s o' both a"ticles is the same3 In

this case, each of the articles is $oth attracti&e an' attracte'# In each of thearticles an (ttracti&e orce occ"rs an' it ca"ses the article to come closer

to the secon' article#

In this case, each of the articles is in the comosition of the etherealcloth# (n' this ethereal fa$ric is contracte' from $oth si'es, an' $oth

articles mo&e in its comosition# (n' each of them is s"$ject to the first

rincile of $eha&ior of Ether - JIn the ethe"eal 'iel& voi&s &o not occu"J# Inaccor'ance ith this rincile, in each of si'es there an ethereal flo is,

'irecte' to the secon' article# I#e# each of these articles creates toar'

itself an ethereal flo : a iel' of (ttraction# (n' other article reson's to

this ethereal flo, as it is fille' ith Ether too# Therefore it mo&es in thecomosition of this ethereal flo in the 'irection of a secon' article hichis its ca"se#

The orce of (ttraction of each of to gra&itating articles - is an

ethereal flo, carrying it to another, attracting it article# The orce of(ttraction of each of to attracte' articles e can meas"re $y the see'

ith hich the attracte' article comes near to the attracting one#


26/89

?hat factors 'etermines the see' of aroaching of an attracte'

article to attracting@?ell, firstly, a ma$nitu&e o' the %iel& o' Att"action o' att"actin$

a"ticle3 This is the 'i"st 'acto"3(n ethereal flo, hich is comose' ofattracte' article, aroaches to this article# ( magnit"'e of iel' of

(ttraction, as e recall, is the &al"e of the rate of a$sortion of Ether $y the

o$ject forming this fiel'# The see' ith hich Ether mo&es to the o$jectforming this fiel' 'een's on the 'istance to the o$ject# The greater is a

'istance, the sloer a flo of Ether is an' the loer, resecti&ely, the orce

of (ttraction to the o$ject that arises at this oint# Th"s, a &istance toatt"actin$ a"ticles 4 this is the secon& 'acto" in'luencin$ a ma$nitu&e o'

%o"ce o' Att"action#

(n' finally, the thi"& 'acto" 4 is a qualit0 o' an att"acte& a"ticle #"ality of articles can $e anything# This is either an (ttracti&e iel' or a

Re"lsion iel'# (n' the &al"e of the fiel' can $e any# In this case e aretalking a$o"t an attracte' article ith a iel' of (ttraction# So hy 'oes a"ality of a article affect a magnit"'e of orce of (ttraction@

(ll the matter is that any article ith a iel' of (ttraction, a$sor$ing

Ether, there$y constantly creates aro"n' a so-calle' Jethe"eal itJ Fethereal&oi'G# It t"rns o"t that a article ill fall into an Jethereal itJ hich it

constantly creates itself on the other si'e, here the attracting article is#(n' a see' of creation of Jethereal itJ correson's to the rate of

a$sortion of Ether $y itself : i#e# to its &al"e of the iel' of (ttraction#

Th"s, e no take an' slightly mo'ify the form"la of Isaac >eton,'escri$ing the la of gra&itation# 4f co"rse, the scientist alies his la

only to macro-o$jects - in artic"lar, to the hea&enly $o'ies# B"t any $o'y is

constr"cte' of chemical elements, hich in t"rn are $"ilt from elementaryarticles# (n' so gra&ity in the first t"rn is inherent to elementary articles#

(t >eton an (ttraction orce e"als the ro'"ct of to masses 'i&i'e' $y

the s"are of the 'istance $eteen the $o'ies1% @ m1 m* B " Fcoefficient 6 left asi'e here, $eca"se e ant to

'ra yo"r attention to the $asic hysical "antitiesG#

(men'ments to this form"la ill $e as follos# irst, instea& o' the

multilication, we use the sum3In or'er to kno at some oint of time thesee' at hich an in&estigate' attracte' article comes near to an attractingo$ject, e nee' not to m"ltily their iel's of (ttraction FmassesG, namely to

s"m# ( iel' (ttraction - is see' of mo&ing of Ether to an o$ject hich

a$sor$s Ether# In or'er to kno the see' of articles is necessary to s"m thesee' of ethereal flo generate' $y an attracting article Fthe &al"e of its


27/89

iel' of (ttraction at this ointG, as ell as the see' ith hich an attracte'

article falls into the create' $y itself an Jethereal itJ#So e j"st ha&e to take mass of an attracte' article an' to a'' to it an

(ttracti&e iel' of an attracting article, calc"late' at a gi&en oint, i#e#gi&en a 'istance# To 'o this, e 'o not take an original &al"e of the mass of

the attracting o$ject, an' the mass 'i&i'e' $y the 'istance# I#e#'o"mula 'o"

calculatin$ %o"ce o' Att"action must have the 'o"m1% @ 6m1 B ") D m*, here m1 B "- is the mass of an attracting o$ject,

calc"late' for a gi&en oint, i#e# gi&en the 'istance, an' m*- is the mass of

an attracte' article# This form"la can $e alie' not only in relation to onein'i&i'"al elementary article, $"t also to attraction of chemical elements, as

ell as $o'ies#

%ay attentionO This 'o"mula is suitable onl0 'o" those cases whe"e anobect itsel' has a %iel& o' Att"action # i3e3 mass3 If an attracte' article has

antimass Fi#e# generates a Re"lsi&e iel'G, the form"la ill changesomehat# Ho it ill change, e ill see $elo#

(n (ttraction iel' increases as e come near to the so"rce of this

fiel'# This means that the closer to a so"rce of gra&ity, the higher the see'

of an ethereal flo is# or this reason, conve"$ence o' an att"acte& a"ticle

to an att"actin$ a"ticle occu"s at not a constant see&, an& at

accele"ation# >ote, shoul& not con'use this accele"ation with anaccele"ation o' bo&ies, which is obse"ve& &u"in$ thei" '"ee 'all in the

atmoshe"e o' a celestial bo&03

In this case, iel's of (ttraction of $oth articles are e"al# Thismeans that $oth ill come near each other ith the same acceleration#

Hoe&er, as eKll see in the folloing eamle, all ill $e somehat

'ifferent in the case of (ttraction iel's of articles are not the same# (n'e&en the most 'ifference ill $e hen an attracte' article has not the iel'

of (ttraction an' the iel' of Re"lsion#

-------------------------------------------------------------------------------------------------

() The value o' Att"action %iel& o' one o' the a"ticles is la"$e" than%iel& o' Att"action o' othe" a"ticle3

E&en 'esite the fact that in this case the &al"e of iel's of (ttractionof the articles is 'ifferent, the mechanism of their attraction to each other inmany resects similar to that 'escri$e' a$o&e# In this case, only one of the

articles is an attracte' to each other - the one that has greater (ttraction

iel' &al"e Fattracts Ether ith a higher see'G# It is this article $ecomes aca"se of orce of (ttraction in the secon' article - ith less iel' of

(ttraction# The magnit"'e of this orce of (ttraction can $e fo"n' from the


28/89

form"la that e 'eri&e' in the re&io"s eamle1 % @ 6m1 B ") D m*, herem1 B "- is the mass of an attracting o$ject, calc"late' for a gi&en oint, i#e#gi&en the 'istance an' m*- is the mass of an attracte' article# Here m1- is

the mass of the article ith a larger iel' of (ttraction an' m*: is the massof a article ith the iel' of lesser magnit"'e#

*) An att"acte& a"ticle has %iel& o' Reulsion3

In this case, a orce of (ttraction also occ"rs in only one article - onethat has a iel' of Re"lsion# The article ith a iel' of (ttraction calls the

orce#

In this case, the attracte' article is also mo&ing toar's the attractingarticle comrising an ethereal flo, hich it creates# Hoe&er, an attracte'

article ith a iel' of Re"lsion constantly emits in all 'irections Ether -

incl"'ing in the 'irection of an attracting article# Th"s, this article isconstantly increasing a n"m$er of Ether, that shares it an' the gra&itating

article : i#e# constantly forms a kin' of Jethe"eal cushionJ that re&ents acon&ergence of the article ith attracting one or j"st slos it#

( Re"lsion iel' - is also an ethereal flo, $"t not coming ear to the

article, an' mo&ing aay from it# (n' all the articles that fall into a 3one

of action of this ethereal flo also mo&e ith it an' mo&e aay from theso"rce of this Re"lsion iel'# I#e# $eca"se an attracte' article ossess $y a

iel' of Re"lsion, it ca"ses a resonse orce in attracting article - a %o"ceo' Reulsion#

%articles ill aroach still closer or there ill $e their 'istancing or

the 'istance $eteen them remains constant, it 'een's of the iel's of(ttraction of an attracting article at a gi&en 'istance an' of the iel' of

Re"lsion of an attracte' article# If $oth fiel's at a gi&en oint are e"al in

magnit"'e, the 'istance $eteen the articles ill remain "nchange'# If themagnit"'e of the iel' of (ttraction at a gi&en oint of (ttraction is more in

mo'"l"s, the articles ill aroach closer# (n' if more the &al"e of

Re"lsion iel' of a article, the 'istance $eteen the articles illincrease#

(n' here is the romise' form"la for calc"lating an initial orce of

(ttraction of a article, hich itself has a iel' of Re"lsion#

% @ 6m1 B ") 4 am*, here m1 B "- is the mass of an attracting o$ject,calc"late' for a gi&en oint, i#e# gi&en the 'istance an' am*- is the antimassof an attracte' article# >ote here e make no s"mming of the iel's of

(ttraction an' Re"lsion, an' their s"$traction# S"$traction e ro'"ce for

the reason that a Re"lsi&e iel' of an attracte' article re'"ces the see' athich in each moment of time this article ten's to mo&e in the 'irection of

the attracting article#


29/89

5et "s ill"strate the a$o&e form"la $y means of small com"ting#

(ss"me the mass of an attracte' article e"als < ar$itrary "nits# Theantimass of an attracte' article is ; stan'ar' "nits, an' the 'istance $eteen

the articles is 2 stan'ar' "nits# Then, accor'ing to the form"la a rimaryorce of (ttraction in the attracting article is1 % @ 6;B*) 4 @ 13F#

Since the %o"ce o' Att"action he"e has the GDG si$n, the att"acte&

a"ticle with the %iel& o' Reulsion will a"oach close" with theatt"actin$ a"ticle3

There is another eamle# The mass of an attracting article e"als

stan'ar' "nits# The antimass of an attracte' article is ; stan'ar' "nits, an'the 'istance $eteen the articles is 2 stan'ar' "nits# Then, accor'ing to the

form"la a rimary orce of (ttraction in the attracte' article is1 % @ 6HB*) 4

@ 9#Since the %o"ce o' Att"action in this case is ?e"o, the"e will no be an

a"oachin$ o' the a"ticles o" &istancin$ them#There is a thir' eamle# The mass of an attracte' article e"als .

stan'ar' "nits# The antimass of an attracte' article is ; stan'ar' "nits# The

'istance $eteen the articles is 2 stan'ar' "nits# Then, accor'ing to the

form"la a rimary orce of (ttraction in the attracte' article is1 % @ 62B*) 4

@ 41#

In this case, the orce of (ttraction has a J-J sign# This means thatthe a"ticles will &"i't aa"t '"om each othe"3

/30 THE TRUTH A:OUT FORCE OF ATTRACTION

5etLs re&isit again all &al"es in the form"la % @ !m1 m* B ", hich'escri$es the 5a of 6ra&itation, form"late' $y Isaac >eton#

1) An elementa"0 a"ticle is the main a"ticiant o' $"avit03

Isaac >eton 'e'"ce' the 5a of 7ni&ersal 6ra&itation, $ase' ono$ser&ations of motion of celestial $o'ies#

He lai' great gro"n'ork in or'er to f"lly "n'erstan' hat a

henomenon of attraction is# He lai' a fo"n'ation, $"t this is not eno"gh#

>eton talke' a$o"t attraction of o$jects of macrocosm an' has not srea'this henomenon to microcosm# This is "n'erstan'a$le# (fter all, at his life,h"manity has not yet oene' a microcosm - not chemical elements, not

elementary articles#

The task of mo'ern hysics is recisely to gras $y its las all that isin the "ni&erse, in artic"lar, to eten' the henomenon of attraction

Fgra&itationG to o$jects of microcosm# (s long as this is not 'one, there ill


30/89

$e searate from each other $"avitational inte"action, st"on$ inte"actionan& ma$netism#

4nce hysics ill make an elementary article as the main arty of

the 5a of "ni&ersal gra&itation, this ro$lem ill 'isaear $y itself, an'all three of these interactions in the min's of scientists merge into one#

(n' hile carriers of gra&itational interaction are only celestial $o'ies

: i#e# itKs a >etonLs legacy# B"t celestial $o'ies are not $"ilt of chemicalelements an' chemical elements are not $"ilt of elementary articles@

Hoe&er, mo'ern science is still afrai' to let go of the fatherly han'

of >eton an' mo&e on its on# >ee', e nee' to 'o itO >ecessary totransform an elementary article of a Jassi&e o$ser&erJ of the rocess of

gra&itation of celestial $o'ies into the sole ca"se of this rocess#

--------------------------------------------------------------------------------------------------

*) You &o not consi&e" accele"ation o' $"avit0 as a cause o'&een&in$ o' 'o"ce o' att"action on the &istance3

I' an0one believes that inc"easin$ o' see& o' a 'allin$ soli& o"

liqui& bo&0 as sho"tenin$ the &istance between it an& the cente" o' thelanet can be seen as evi&ence that %o"ce o' Att"action inc"eases with

&ec"easin$ a &istance between obects, it is a w"on$ conclusion3

The "eason 'o" accele"ation o' the bo&0 &u"in$ its '"ee 'all 4 not"e&ucin$ the &istance to the cente" o' the lanet, an& ine"tia o' the 'allin$

bo&0J?e consi'er in 'etail the reasons for acceleration of freely falling

$o'ies in the $ook /+echanics o' bo&ies0#There is a roof of o"r arg"ments# ( $o'y can achie&e the same see'

at 'ifferent heights of fall# It 'een's on the magnit"'e of ath tra&ele' $y it

in the atmoshere# The longer it is, the greater the see' is# ( $o'y mayreach a certain &elocity an' near the s"rface an' somehere at high altit"'e#

(s yo" can see, this fact contra'icts the concl"sions of mo'ern hysics# It

claims that at a certain height the rate of fall m"st ha&e a certain &al"e,hich m"st $e a constant# So it follos from >etonKs la of gra&ity# B"t in

ractice it is not# )onse"ently, it is not orce of 6ra&ity is the reason for

the groth of &elocity of the $o'y '"ring its free fall#

The tr"e ca"se of acceleration : is inertia of $o'y motion, i#e# self-s"staining mo&ement# ItKs an im"lse#

-------------------------------------------------------------------------------------

---------

) The &istance between $"avitationall0 inte"actin$ bo&ies3Does the 'istance $eteen gra&itationally interacting o$jects affect the

magnit"'e of orce of (ttraction@


31/89

The anser : /yes0# Distance to the o$ject ith iel' of (ttraction

affects the &al"e of orce of (ttraction, ca"se' $y this o$ject in the st"'ie'article#

(s alrea'y mentione', a article is a shere an' if mo&ing aay fromit, the &ol"me of sace s"rro"n'ing the article ill increase concentrically#

(ccor'ingly, the farther aay from the article, the $igger is an amo"nt of

Ether s"rro"n'ing the article# Each article ith orce of (ttractiona$sor$s Ether from the am$ient ethereal fiel' at a certain see'# The see'

of a$sortion of Ether $y the article - this is originally inherent to this

article a &al"e of the iel' of (ttraction# Hoe&er, the farther aay from aarticle, the greater is an amo"nt of Ether ill s"rro"n' it# (ccor'ingly, the

farther aay from a article, the smaller ill $e the rate at hich Ether is

closer to a gi&en article Fi#e#, the smaller the see' of an ethereal floG - i#e#the smaller is the &al"e of the iel' of (ttraction# Th"s, e say, first, a$o"t

the &al"e of the iel' of (ttraction originally inherent to this article, an'secon', a$o"t the &al"e of the iel' of (ttraction at a certain 'istance fromthe article#

(ccor'ingly, the farther aay an in&estigate' article is from the

article ith the iel' of (ttraction, ca"sing in it the orce of 6ra&ity, theless is the &al"e of this orce#

or eamle, letKs consi'er s"ch a case# Some article interacts ithto articles forming iel's of (ttraction# Hoe&er, the 6ra&ity iel' of

one of these articles is greater than the iel' of (ttraction of the secon'

article# >e&ertheless, all "ltimately 'etermine the 'istance at hich thesearticles ill $e sit"ate' from the in&estigate' article# (n' it may haen

that a article ith a larger iel' of (ttraction ca"ses a smaller orce of

(ttraction - if it ill $e m"ch farther than a article ith smaller iel' of(ttraction#

/40 MASS IS FIELD OF ATTRACTION@ WEIGHT " IS FORCE

OF ATTRACTION

( little earlier, e ha&e alrea'y "t an e"al sign $eteen theconcets of massan' %iel& o' Att"action# >o letLs fin' o"t hat is wei$ht#

Referring to the Encycloe'ic Dictionary - hat is 'efinition of

eight gi&en there@

J?eight is a force ith hich a $o'y acts on a reliance For hangerG, itre&ents free fallJ FSo&iet Encycloe'ic Dictionary, e'# %rokhoro&G#


32/89

J?eight is a n"merical &al"e of the orce of 6ra&ity acting on a $o'y

locate' near the earthLs s"rfaceJ F%hysical Encycloe'ic Dictionary, e'#%rokhoro&G#

In this case, the concet eo"n'e' in this $ook, is consonant ith thetheory of mo'ern hysics# =ei$ht- is orce of (ttraction F6ra&ityG#

In encycloe'ic 'ictionaries no$o'y says a$o"t eight of elementary

articles, this term e&ery$o'y refers only to $o'ies# Hoe&er, $o'ies areconstr"cte' of chemical elements, hich, in its t"rn, consist of elementary

articles# Therefore, $efore e talk a$o"t eight Force of (ttractionG of

$o'ies, e sho"l' aly this concet to elementary articles#( so"rce of iel' of (ttraction is a article ith iel' of (ttraction or

a chemical element, hich f"lly or artially manifests o"tar'ly the Total

iel' of (ttraction, or a $o'y of "s"al si3es, containing elements ith iel'sof (ttraction, or a celestial $o'y# If e take at ran'om any elementary

article, then any of these so"rces ill ca"se in it the correson'ing orce of6ra&ity# (ny of these orces reresents j"st the eight of article ithresect to the so"rce of the iel' of (ttraction, ca"sing this orce#

/70 THE MECHANISM OF ANTIGRA6ITATION

>RE1ULSION?

%articles ith iel's of (ttraction are the ca"se of orces of (ttraction

in the s"rro"n'ing articles# (n' hat is a$o"t the articles forming in theethereal fiel' iel's of Re"lsion@ They 'o not ca"se the orce of

(ttraction# >o, any article ith the iel' of Re"lsion is the ca"se of the

orce of Re"lsion in s"rro"n'ing articles#%o"ce o' Reulsion, arising in any article - is an ethereal flo,

ca"sing Ether of the article to mo&e aay from ecess of Ether arising in

the ethereal fiel'# Ecess of Ether is alays forme' $y the article ith theiel' of Re"lsion#

In the section of hysics 'e'icate' to electromagnetism orces of

Re"lsion eist on a ar ith orces of (ttraction# Hoe&er, in

electromagnetism not the $o'ies an' charge' articles are attracte' an'reelle', i#e# there is no relationshi ith gra&itation# B"t if anti-gra&itationFre"lsionG o"l' ha&e $een recogni3e' $y scientists, an' not j"st

recogni3e', an' as the antio'e of gra&itation ill $ecome, e&erything

o"l' fall into lace# Elect"oma$netism woul& aea" in the min&s o'scientists not mo"e than the $"avitational4anti$"avitational inte"action3

%ositi&e an' negati&e charges o"l' $e con&erte' into mass an' antimass#


33/89

ThatLs all# This o"l' $e the first ste in the 'irection of G!"an&7ni'icationG o' 'ou" inte"actions#

In reality, the so"rce of Re"lsion iel' Farticle, chemical element or

cl"ster of chemical elementsG can $e shiel'e' $y free articles or chemicalelements Fsoli's, fl"i'sG# iel's of (ttraction an' iel's of Re"lsion of the

shiel'ing o$jects change the magnit"'e of the Re"lsion orce in the

in&estigate' o$ject#Shiel'ing articles ith iel's of Re"lsion themsel&es are the ca"ses

of Re"lsion orces# (n' these orces of Re"lsion e sho"l' a'' to the

orce of Re"lsion of the o$ject, infl"ence of hich e eamine#Shiel'ing articles ith iel's of (ttraction are the ca"ses of orces

of (ttraction# These orces of (ttraction e m"st s"$tract from the orces

of Re"lsion, hich e elore#>o there are fe or's a$o"t the feat"res of re"lsion of the

articles ith 'ifferent &al"es of iel's of Re"lsion#If $oth interacting articles ha&e iel's of Re"lsion ith 'ifferent

&al"es, then a re"lsi&e article is the article ith the larger iel', an' a

reelle' one is the article ith the smaller iel'# I#e# the a"ticle with thesmalle" %iel& o' Reulsion will move awa0 '"om the a"ticle with the

la"$e" %iel&, an& not vice ve"sa# 5et "s call it theRule o' Submission to the

ominant %o"ce o' Reulsion3I' both a"ticles have %iel&s o' Reulsion an& thei" values a"e the

same, then the0 both will be simultaneousl0 "eelle& an& "eulsive3 An&

both a"e est"an$e& '"om one anothe" with the same see&3In that case, i' onl0 one o' the a"ticles has %iel& o' Reulsion, the

secon& is cha"acte"i?e& b0 the %iel& o' Att"action, an& then the "eulsive

one is the a"ticle Yan$3 Yin is alwa0s ust "eelle&3(s yo" can see, all is $y analogy ith the orce of (ttraction, j"st the

oosite#

-------------------------------------------------------------------------------------The mechanism of anti-gra&itation Fre"lsionG is comletely oosite

to the mechanism of gra&itation FattractionG#

4ne of to articles in&ol&e' in the interaction of antigra&ity, m"st

necessarily ha&e a Re"lsi&e iel'# 4therise, e can not kee talkinga$o"t antigra&ity interaction#

?e comare' the rocess of gra&itation ith the in'ing " of a

JtangleJ# If to 'ra an analogy ith the mechanism of gra&itation, then the

rocess of re"lsion - is the "nin'ing of the JtangleJ# ( article ith aiel' of Re"lsion is a JtangleJ# Emission $y it of Ether is "nin'ing of

Jthrea'J FEtherG# ( article ith a iel' of Re"lsion "nin'ing the Jthrea'J


34/89

Femitting EtherG increases the 'istance $eteen it an' s"rro"n'ing articles,

i#e# reels, an' alienates them from itself# Ether in articles ith the iel'sof Re"lsion 'oes not 'ry o"t# %articles 'o not sto to emit it#

4f to articles in&ol&e' in the anti-gra&itational rocess, one thathas a iel' of Re"lsion is re"lsi&e# ( secon' article, resecti&ely, is

reelle'# ( article of any "ality can $e reelle' - as ith the iel' of

Re"lsion an' ith the iel' of (ttraction# In that case, if $oth articlesha&e iel's of Re"lsion, each of them is lay a role as re"lsi&e an'

reelle'#

( re"lsion mechanism $ase' on the secon' rincile of $eha&io"r ofEther - JIn the ethe"eal 'iel& a"eas with e5cessive &ensit0 &onKt occu"J#

Ether, filling a article, an' ith it the article itself mo&ing aay from

ecess of Ether arising in that lace of ethereal fiel' here an o$ject ith aiel' of Re"lsion is locate'#

/80 THE FORCE OF RE1ULSION

(n ethereal flo, ca"sing Ether of the reelle' article mo&e aayfrom ecess of Ether, i#e# from the o$ject ith iel' of Re"lsion e call as

the J%o"ce o' Reulsion0#

>at"rally, in contrast to the rocess of gra&ity a connection $eteenreelling articles 'oes not form# There can $e no "estion a$o"t connection

$eteen the articles# S"ose to articles are gra&itationally $o"n'# B"t

as a res"lt of transformation one of them or $oth at once change' the6ra&itational iel' on the Re"lsi&e iel'# The mechanism of

antigra&itation comes into action imme'iately, an' the articles reel each

other, i#e# a connection is $roken off#Magnit"'e of Re"lsion orce 'een's on the same three factors as

magnit"'e of the orce of (ttraction1

G Magnit"'e of Re"lsion iel' of the article Fthe chemical element

or $o'yG ser&ing the ca"se of Re"lsion orce2G The 'istance $eteen a so"rce of Re"lsion iel' an' an

in&estigate' article

;G ( "ality of reelle' article#

5etLs consi'er an effect of all these factors#1) +a$nitu&e o' Reulsion %iel& o' an obect is the cause o'

Reulsion %o"ce3


35/89

Magnit"'e of Re"lsion iel' of the article - is the see' of

a$sortion of Ether $y its s"rface# (ccor'ingly, the hi$he" is the see& o'

abso"tion o' Ethe", the $"eate" is ma$nitu&e o' Reulsive %o"ce cause&

b0 this a"ticle in an investi$ate& a"ticle#*) The &istance between the sou"ce o' Reulsion %iel& an& an

investi$ate& a"ticle3

Elanation of 'een'ence of magnit"'e of Re"lsion orce on the'istance similar to the 'escrition the reason for hich the orce of

(ttraction 'een's on the 'istance#

(n elementary article is a shere, an' if to mo&e aay from it, anamo"nt of sace s"rro"n'ing the article ill gro concentrically#

(ccor'ingly, the farther aay from the article, the greater is the &ol"me of

Ether, s"rro"n'ing the article# Each article ith the iel' of Re"lsionemits Ether into s"rro"n'ing ethereal fiel' at a certain rate# The "ate o'

emission o' Ethe" b0 the a"ticle 4 that is o"i$inall0 inhe"ent to thisa"ticle the value o' Reulsion %iel&3Hoe&er, the farther aay from thearticle, the greater an amo"nt of Ether ill s"rro"n' it# (ccor'ingly, the

'a"the" awa0 '"om the a"ticle, the smalle" will be the "ate at which Ethe"is movin$ awa0 '"om a $iven a"ticle Fi#e#, the smaller the &elocity of anethereal flo isG - i#e# the smalle" is the value o' Reulsion %iel Th"s, e

say, first, a$o"t an originally inherent to the article magnit"'e of Re"lsioniel', an' secon', a$o"t the magnit"'e of Re"lsion iel' at a certain

'istance from the article#

The 'u"the" an investi$ate& a"ticle is '"om the a"ticle with the%iel& Reulsion, that causin$ in it a Reulsive %o"ce, the smalle" is the

ma$nitu&e o' this %o"ce3

) The qualit0 o' "eulsive a"ticles34f co"rse, the "ality can $e any# This may $e as a article ith the

iel' of (ttraction an' ith the iel' of Re"lsion#

(n' the &al"e of the iel' can $e any# If e are talking a$o"t reelle'article ith the iel' of Re"lsion, then hy 'oes on the &al"e of

Re"lsion orce of the articles affects the "ality of its on@ (ll the matter

is that any article ith the iel' of Re"lsion emitting Ether, there$y

constantly creates aro"n' a so-calle' Jethe" illowJ# It t"rns o"t that aarticle ill $e a''itionally reelle' $y the Jethereal illoJ, hich itconstantly creates from the other si'e, here the reelling article is

sit"ate'# (n' the rate of creation $y the article of the Jethereal illoJ

correson's to the rate of emission of Ether $y itself, i#e# of its &al"e ofRe"lsion iel'#


36/89

In mo'ern hysics, there is no the Law o' 7nive"sal Reulsion

similar to the 5a of 7ni&ersal (ttraction, oene' $y >eton# (n' in &ain#?e 'o not "n'erstan' hy s"ch la has not $een form"late' still, $eca"se

its manifestations are not less e&i'ent than the 'emonstration of the 5a of6ra&itation# Take at least the knon fact, as the rise of heate' air "#

If there is no the la, there is no form"la that 'escri$es the interaction

of o$jects, at least one of hich is the ca"se of Re"lsion orce# B"t e illcorrect this mis"n'erstan'ing#

By analogy ith the form"la for the 5a of 6ra&itation, $"t not of

Isaac >eton, an' ith that 'eri&e' $y "s in the article a$o"t gra&itation, eill make the folloing form"la for the 5a of (ntigra&itation1

% @ 6am1B ") D am*here am1B ": itKs antimass of a reelling o$ject

com"te' for a gi&en oint, i#e# gi&en the 'istance an' am*: itKs antimass ofthe reelle' article#

(s yo" can see, in this case e also "se not a m"ltilication ofantimasses an' their a''ition# In or'er to kno at some oint in time the rateat hich in&estigate' reelle' article mo&es aay from its re"lsi&e o$ject,

e nee' not to m"ltily their Re"lsion iel's FantimassesG, an' namely to

s"m# Re"lsion iel' : is a rate of emitting of Ether $y the o$ject# In or'erto kno the &elocity of the articles it is necessary to s"m the rate of

ethereal flo generate' $y the re"lsi&e article, i#e# the &al"e of itsRe"lsion iel' at a gi&en oint, as ell as the &elocity ith hich the

reelle' article is reelle' $y the create' it on Jethereal illoJ#

?e take the antimass of the re"lsi&e article an' a'' to it theRe"lsi&e iel' of the re"lsi&e article, calc"late' at the gi&en oint, i#e#

gi&en the 'istance# To 'o this, e take no initial &al"e of antimass of the

re"lsi&e o$ject an' the antimass, 'i&i'e' $y the 'istance#This form"la is only s"ita$le for those occasions hen the reelle'

o$ject itself has the iel' of Re"lsion, i#e# antimass# If reelle' article is

characteri3e' $y mass Fi#e#, generates an (ttracti&e iel'G, the form"la illchange somehat# ?e ill gi&e the form"la $elo#

-------------------------------------------------------------------------------------

5etLs look at 'etails of the mechanism of anti-gra&itation on the

eamle of articles of 'ifferent "ality#A thou$ht e5e"iment con&ucte& b0 us will occu" in i&eal con&itions

# i3e3 in the totall0 emt0 sace34ne of interacting articles necessarily has

the iel' of Re"lsion#

1) (oth inte"actin$ a"ticles have Reulsion %iel&s3A) The value o' Reulsion %iel&s o' both a"ticles equals3


37/89

In this case, each of the articles is $oth re"lsi&e an' reelle'# (

orce of Re"lsion ca"se' $y the action of the secon' re"lsion fiel' ofinteracting articles ca"se' $y the action of the Re"lsion iel' of the

secon' of interacting articles arises in e&ery article#5et to articles initially are searate' $y some 'istance# Beca"se

e"ality of iel's of Re"lsion $oth articles 'rift aart at a constant see'#

The see' of 'istancing is constant $eca"se the constant is the rate ofemission of Ether in the articles#

() The value o' Reulsion %iel& o' one o' the a"ticles is $"eate"

then Reulsion %iel& o' anothe" a"ticle3E&en tho"gh in this case the &al"e of iel's of Re"lsion &aries, the

mechanism of their re"lsion from each other is similar to the a$o&e# 4nly

in one of the articles a orce of Re"lsion arises - in the reelle' one, i#e# inthat here the iel' of Re"lsion is less# ( re"lsi&e article is one in hich

a Re"lsi&e iel' is more# It generates a Re"lsi&e orce#( reelle' article ill mo&e aay from the re"lsi&e one ith e"al

'eceleration# Deceleration is relate' to a concentric increase of the &ol"me

of the sace ith 'istance from the article emitting Ether# Distancing see'

of the article at each time oint is roortional to the &al"e of aearing init the Re"lsion orce# The more is the Re"lsi&e orce occ"rring in the

article, the greater is the see' of alienation of the article at the gi&enmoment#

*) An att"acte& a"ticle has %iel& o' Reulsion3

In this case, the Re"lsion orce arises only in one article - one thathas a iel' of (ttraction# ( article ith iel' of Re"lsion ca"ses this

orce#

Since the reelle' article has a iel' of (ttraction, it ca"ses in are"lsi&e article a resonse orce - the orce of (ttraction#

There ill $e 'istancing or aroach of the articles, or the 'istance

$eteen them remains constant, in'een'ent of the &al"e of Re"lsionorce in the reelle' article an' (ttracti&e orces in reelling one# If to

forces are e"al in magnit"'e, the 'istance $eteen articles ill remain

"nchange'# If the &al"e of Re"lsion orce is more in mo'"l"s, the articles

ill $e 'istancing# (n' if the &al"e of the orce of (ttraction is more, thenthe 'istance $eteen the articles ill $e re'"ce'#

(n' here is the form"la for calc"lating the initial Re"lsion orce in a

reelle' article, hich itself has a iel' of (ttraction#

% @ 6 AmB") 4 m, here amB" is antimass of the reelling o$jectcom"te' for the gi&en oint, i#e# gi&en the 'istance an' m- is the mass of

reelle' article# >ote here e make no a''ition of the iel's of Re"lsion


38/89

an' (ttraction, an' their s"$traction# S"$traction is for the reason that the

iel' of (ttraction of reelle' article re'"ces the rate at hich in each timeoint the article ten's to mo&e aay from the re"lsi&e article# (s yo" can

see, the rocess is a mirror oosite of hat e ha&e 'escri$e' for theattraction of article ith the iel' of Re"lsion#

/90 WH5 HA6E ATIGRA6ITATION STILL NOT

RECOGNIED :5 SCIENCE2

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The Teaching of Djwhal Khul - Ethereal Mechanics