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<title>THE ETERONIC THEORY</title>
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<div class=3DSection1>

<p class=3DMsoTitle><span style=3D'font-size:16.0pt;color:windowtext;font-s=
tyle:
normal'><o:p>&nbsp;</o:p></span></p>

<p class=3DMsoTitle><span style=3D'font-size:16.0pt;color:windowtext;font-s=
tyle:
normal'><o:p>&nbsp;</o:p></span></p>

<p class=3DMsoTitle><span style=3D'font-size:16.0pt;color:windowtext;font-s=
tyle:
normal'><o:p>&nbsp;</o:p></span></p>

<p class=3DMsoTitle><span lang=3DEN-US style=3D'font-size:16.0pt;color:wind=
owtext;
mso-ansi-language:EN-US;font-style:normal'>THE ETERONIC THEORY</span><span
lang=3DEN-US style=3D'font-size:16.0pt;mso-ansi-language:EN-US;font-weight:=
normal'><o:p></o:p></span></p>

<p class=3DMsoNormal align=3Dcenter style=3D'text-align:center'><b><i><span
lang=3DEN-US style=3D'font-size:16.0pt;font-family:Arial;color:red;mso-ansi=
-language:
EN-US'><o:p>&nbsp;</o:p></span></i></b></p>

<p class=3DMsoNormal><span lang=3DEN-US style=3D'mso-ansi-language:EN-US'><=
o:p>&nbsp;</o:p></span></p>

<p class=3DMsoNormal><span lang=3DEN-US style=3D'mso-ansi-language:EN-US'><=
o:p>&nbsp;</o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>This chapt=
er
deals with the basic building blocks of space.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>I mentioned it fleetingly in the
previous chapter as an advance and I am further describing it here adding y=
et
more detail.<o:p></o:p></span></p>

<p class=3DMsoBodyText><span lang=3DEN-US style=3D'font-size:12.0pt;mso-bid=
i-font-size:
10.0pt;mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>The Eteron=
 is a subatomic
particle having complex structure and possessing the following functional
properties: <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:0cm'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>1. Eterons=
 fill
space very compactly touching each other on surfaces created by electrical
repulsions.<span style=3D'mso-spacerun:yes'>&nbsp; </span>The length in spa=
ce is
measured by juxtaposed Eterons.<span style=3D'mso-spacerun:yes'>&nbsp; </sp=
an>The
diameter of identical Eterons acts as a measurement unit in space and there=
fore
the size of physical objects. Eterons are made of sub-Eterons (sub-particles
much smaller than the mentioned Eteron). They have a special surface-struct=
ure
made up of sub-Eterons able to generate small dipole-fields with a short ra=
nge.
<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>2. The Ete=
ron
can be compressed or expanded (decompressed). Its diameter can vary. To
compress an Eteron requires energy supplied to it, and correspondingly, whe=
n it
expands, it returns that energy. The internal energy of the Eteron is the
inverse function of its radius:<span style=3D'mso-spacerun:yes'>&nbsp;
</span>E=3Dk/(r&sup3;) where k is a constant and r is its radius. The Etero=
n also
can be compressed in only one dimension, that is, flattened like a pancake
rather than a reduction in radius in all directions. This way, the internal
energy is an inverse function of its volume. <span style=3D'color:blue'><sp=
an
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;</span><o:p></o:p></span></span></p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:36.0pt'><span
lang=3DEN-US style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>3. The Ete=
ron
has an internal clock. When an Eteron is compressed, the radius reduces in =
an
elastic form. When the compression force ceases, the Eteron returns to its
previous size. The clock has the function of determining an interval of tim=
e t.
Compression occurs such that, when applying force to an Eteron, the Eteron
compresses without transmitting this compression to any of its neighbours.<=
span
style=3D'mso-spacerun:yes'>&nbsp; </span>This action is confined to a singl=
e time
interval (t), as initially, this is the smallest useful period for observat=
ion.
It absorbs the entire energy of the compression during this single interval.
After the interval concludes, the Eteron then begins to compress the adjace=
nt
Eteron in the direction of the force. Basically a single Eteron is compress=
ed
for a single interval of t.<span style=3D'mso-spacerun:yes'>&nbsp; </span>F=
or a
series of t&#8217;s the Eterons along the plane of the applied force-vector
will each experience compression. Only during a single interval t will a si=
ngle
Eteron be compressed.<span style=3D'mso-spacerun:yes'>&nbsp; </span>This
compression will only occur providing the Eteron about to be compressed has=
 a
radius bigger than the Eteron about to compress it.<o:p></o:p></span></p>

<p class=3DMsoBodyTextIndent2 style=3D'margin-left:0cm;text-align:justify'>=
<span
lang=3DEN-US style=3D'font-size:12.0pt;mso-bidi-font-size:10.0pt;mso-ansi-l=
anguage:
EN-US'><span style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </sp=
an>4.
The final radius of an Eteron is a function of a force f such that:<o:p></o=
:p></span></p>

<p class=3DMsoNormal style=3D'margin-left:36.0pt;text-align:justify'><span
lang=3DEN-US style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;</span>f =3D k/(r<sup>4</sup>) where k is a
constant and r is its radius.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>A chain of
compressed Eterons can exist such that the previous Eteron compresses the
following Eteron and the chain is supported by the initially compressed
element.<o:p></o:p></span></p>

<p class=3DMsoBodyTextIndent2 style=3D'margin-left:0cm;text-align:justify'>=
<span
lang=3DEN-US style=3D'font-size:12.0pt;mso-bidi-font-size:10.0pt;mso-ansi-l=
anguage:
EN-US'><span style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </sp=
an>The
speed of propagation of this compression wave is given by the diameter of t=
he
Eteron divided by the interval t or:<span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp; </span>(2r)/t<o:p></o:p></spa=
n></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>As the for=
ce
persists during interval t, the Eteron becomes compressed, however after t =
only
a force much smaller in magnitude is required to maintain that Eteron&#8217=
;s
compressed state.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>In another=
 way,
the compression force is proportional to the radius raised to the power of =
4.
This would be applied during a time interval t such that, when ceasing the
force, the Eteron remains compressed. To maintain this compression state a
force much smaller in magnitude needs to be applied constantly. The
relationship between the two forces is constant.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>If a maint=
enance
force is constantly applied, then for the duration of this applied force, t=
he Eteron
remains compressed. If the maintenance force ceases, the Eteron does not
decompress immediately; but rather an interval (t) will lapse during which =
it
decompresses. It is the same t interval for which it was initially compress=
ed.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>There is a=
nother
part to this process. When the force ceases to be applied to the Eteron the
Eteron will subsequently decompress and it will do it in a time t.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>However when it does decompress it
actually returns all the energy that was initially applied to it. The decom=
pression
behaves like an explosion.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>A
&#8216;compression-element&#8217; is a force that is or can be applied to an
Eteron.<span style=3D'mso-spacerun:yes'>&nbsp; </span>It is a moving elemen=
t that
compresses Eterons along or in it&#8217;s path. When compressing an Eteron,=
 the
radius will reduce. Corresponding to this decreasing radius, the resistance
force increases by a factor of 1/(r<sup>4</sup>). When the compression force
equals the resistance force the compression stops.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>The
compression-element will only compress one Eteron on the straight line of i=
ts
action in any one time-interval. All its energy concentrates on a single Et=
eron
at a single time interval. Instead of compressing every Eteron in the array=
 a
little in a single time interval, it will concentrate its entire energy at
compressing a single Eteron (the next one in line) to a smaller radius. The
compression-element is also an Eteron and another phenomenon exists here.<s=
pan
style=3D'mso-spacerun:yes'>&nbsp; </span>If an Eteron pushes against anothe=
r,
this Eteron will respond with the same force but of contrary sense. The rea=
sons
for this behaviour reside in the electric structure of the Eteron (dipole
confrontation on the surface, will be discussed later on).<span
style=3D'mso-spacerun:yes'>&nbsp; </span>Suffice to say the Eterons have two
dipole structures - one within the Eteron and the other existing on the sur=
face
of the Eteron.<span style=3D'mso-spacerun:yes'>&nbsp; </span>The dipoles on=
 the
surface of the Eteron have a smaller energy state than those inside but do =
have
the effect of causing an attraction based on the speed of the collision or
colliding force between two Eterons.<span style=3D'mso-spacerun:yes'>&nbsp;
</span>The opposite poles (plus to minus) on the surface of each Eteron
actually attract causing the overall attraction force.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>We tend to imagine that two collid=
ing
solid objects bounce however because of this Eteron &#8216;feature&#8217; t=
hey
don&#8217;t. As an advance, I shall introduce the concept of the
&#8216;barrier&#8217;. The Eteron has over its entire surface a barrier mad=
e up
of small dipoles. When two Eterons move close to one another, at first ther=
e is
a repulsion force generated by each Eteron&#8217;s small dipole barrier. If=
 the
force causing the two Eterons to move closer increases at a determined value
this barrier is broken and the small dipoles of each Eteron&#8217;s surface
instead start to attract. The barrier-effect is due to the behaviour of each
Eteron&#8217;s small dipoles. (Explanation in chapter on TIME)<o:p></o:p></=
span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'color:blue;mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span></span><sp=
an
lang=3DEN-US style=3D'mso-ansi-language:EN-US'>The state of compression of =
the
Eterons determines the intensity of the torsion of space. The speed of ligh=
t is
given by d/t, where d is the diameter of the Eterons and t (considered cons=
tant
at the moment) is the same interval that was mentioned before. The distance=
 in
space is measured using the diameter of the Eterons. This diameter varies
depending on location hence where there is gravity, the diameters are small=
er
because within this space there are many compressed Eterons &#8211; Eterons=
 in
this locale have collectively a smaller diameter.<o:p></o:p></span></p>

<p class=3DMsoBodyText><span lang=3DEN-US style=3D'font-size:12.0pt;mso-bid=
i-font-size:
10.0pt;mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>5. The int=
ernal
components of the Eteron (called sub-Eterons) have electric polarity and th=
ey
confer to the Eteron electric properties. The Eteron can have three special
electric states:<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:0cm'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp; </span>a.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>Neutral state, a state without a s=
trong dipole-field.
Internal electric charges are not separated. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:0cm'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>b. Strong-=
dipole
state, with strong dipole-field that has a longer range than the dipole fie=
ld
of the surface dipoles. The internal electric charges are separated so as to
generate a dipole field extending out further past the surface. The separat=
ion
has many levels of digital variation, specifically; there is a minimum
(determined) difference between two consecutive levels. Each level belongs =
to a
determined dipole-field-intensity of digital variation.<o:p></o:p></span></=
p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:0cm'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>c. Eter-ion
state, the separation of an Eteron into two ions, one being positive and the
other negative. Actually it&#8217;s not so much a splitting of the Eteron b=
ut
the &#8216;polarization&#8217; of two Eterons. Each of the two separate Ete=
ron
halves now containing opposite charges. Starting from two neutral Eterons, =
it
is the total exchanging of opposed electric charges. These charges are ioni=
zed
sub-Eterons.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:0cm'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>The first =
two
states preserve their characteristics of internal energy. They preserve the=
ir
state in relation to the Eteron&#8217;s size and internal clock.<o:p></o:p>=
</span></p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:0cm'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>The
&#8216;a&#8217; state with a weak dipole is the state normal space is in. W=
eak
dipole fields mean that the Eteron has many small dipoles scattered through=
out
the Eteron &#8211; each dipole being a little positive and negative charge.
(See diagram 5.2) Overall the combined group of dipoles have a weak dipole
effect. <o:p></o:p></span></p>

<p class=3DMsoBodyTextIndent3 style=3D'margin-left:0cm;text-align:justify;
tab-stops:0cm'><span lang=3DEN-US style=3D'font-size:12.0pt;mso-bidi-font-s=
ize:
10.0pt;mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>The
&#8216;b&#8217; state refers to charges (positive) separated from their
opposite charge (negative). A small separation for low dipole intensities u=
p to
a significant separation at opposite ends of the Eteron for the strong inte=
rnal
dipole charges.<span style=3D'mso-spacerun:yes'>&nbsp; </span>In the
&#8216;b&#8217; state, the fields of strong dipoles connect to each adjacent
Eteron in the structure creating a chain, linked by the ends of the opposed=
 poles
(polar threads; see diagram 5.1). The strong dipole chargers also work as a
static linking force. The weak (superficial) barrier dipoles work only as a
dynamic interaction for Eteron-compression. <o:p></o:p></span></p>

<p class=3DMsoBodyTextIndent3 align=3Dcenter style=3D'margin-left:0cm;text-=
align:
center;tab-stops:0cm'><span lang=3DEN-US style=3D'mso-ansi-language:EN-US'>=
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</v:shapetype><v:shape id=3D"_x0000_i1025" type=3D"#_x0000_t75" style=3D'wi=
dth:181.5pt;
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 <v:imagedata src=3D"5ettheo_archivos/image001.wmz" o:title=3D""/>
</v:shape><![endif]--><![if !vml]><img width=3D242 height=3D138
src=3D"5ettheo_archivos/image002.gif" v:shapes=3D"_x0000_i1025"><![endif]><=
o:p></o:p></span></p>

<p class=3DMsoBodyTextIndent3 align=3Dcenter style=3D'margin-left:0cm;text-=
align:
center;tab-stops:0cm'><span lang=3DEN-US style=3D'mso-ansi-language:EN-US'>=
DIAGRAM
5.1</span><span lang=3DEN-US style=3D'font-size:12.0pt;mso-bidi-font-size:1=
0.0pt;
mso-ansi-language:EN-US'><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:0cm'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>In the
&#8216;c&#8217; state the Eteron separates into two Eter-ions of opposed po=
les.
This provides a new kind of current, a<o:p></o:p></span></p>

<p class=3DMsoNormal align=3Dcenter style=3D'text-align:center;tab-stops:0c=
m'><i><span
lang=3DEN-US style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;</span></span></i><b><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'>sub-electric current</span></b><span
lang=3DEN-US style=3D'mso-ansi-language:EN-US'>. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:0cm'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>The speed =
of
flow of this sub&#8211;electric current is significantly higher than the
compression transfer - described earlier. It is significantly higher than t=
he
speed of light. It is because the Eter-ions move inside conceptually new ki=
nd
of conducting medium. This idea will be expounded upon in the chapters TIME=
 and
SUBELECTRICITY.<o:p></o:p></span></p>

<p class=3DMsoNormal align=3Dcenter style=3D'text-align:center;tab-stops:0c=
m'><span
lang=3DEN-US style=3D'mso-ansi-language:EN-US'><!--[if gte vml 1]><v:shape =
id=3D"_x0000_i1026"
 type=3D"#_x0000_t75" style=3D'width:270pt;height:270pt'>
 <v:imagedata src=3D"5ettheo_archivos/image003.gif" o:title=3D"dcol5_2"/>
</v:shape><![endif]--><![if !vml]><img width=3D360 height=3D360
src=3D"5ettheo_archivos/image004.jpg" v:shapes=3D"_x0000_i1026"><![endif]><=
o:p></o:p></span></p>

<p class=3DMsoNormal align=3Dcenter style=3D'text-align:center;tab-stops:0c=
m'><span
lang=3DEN-US style=3D'mso-ansi-language:EN-US'>DIAGRAM 5.2<o:p></o:p></span=
></p>

<p class=3DMsoBodyTextIndent3 style=3D'margin-left:0cm;text-align:justify'>=
<span
lang=3DEN-US style=3D'font-size:12.0pt;mso-bidi-font-size:10.0pt;mso-ansi-l=
anguage:
EN-US'><span style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </sp=
an>If
it were possible to measure inside an Eteron, different positive and negati=
ve
values would be observed depending on the particular point the measurement =
was
made. Different electric values would correspond to different positions wit=
hin
the structure.<span style=3D'mso-spacerun:yes'>&nbsp; </span>(diagram 5.2) =
In
fact the position of the positive and negative loads is responsible for all
three states mentioned above. When the positive and negative loads are very
close together it would be described as being in the &#8216;a&#8217;
state.<span style=3D'mso-spacerun:yes'>&nbsp; </span>If however an external
electric field moves them away from each other, the Eteron absorbs energy a=
nd
it passes to the &#8216;b&#8217; state in</span><span lang=3DEN-US
style=3D'font-size:12.0pt;mso-ansi-language:EN-US'> a stable </span><span
lang=3DEN-US style=3D'font-size:12.0pt;mso-bidi-font-size:10.0pt;mso-ansi-l=
anguage:
EN-US'>form.<span style=3D'mso-spacerun:yes'>&nbsp; </span>In the structure=
 of
the Eteron, there is &#8216;support&#8217; that, once in the &#8216;b&#8217;
state, it doesn't allow the two electrically opposed loads to move closer
again.<span style=3D'mso-spacerun:yes'>&nbsp; </span>It exists in a new sta=
ble state.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>This &#8216;support&#8217; is like=
 an
obstacle that over-rides the natural attraction of both loads. If it were
contrary to this the stable &#8216;b&#8217; state simply would not exist. <=
o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;
</span>Sub&#8211;electricity, introduced just above, really forms a major p=
art
of the overall theory.<span style=3D'mso-spacerun:yes'>&nbsp; </span>It wou=
ld be
too much for a detailed in depth discussion on this subject at this point
however given its importance to the theory an overview for clarity must be
presented. Certainly the reader must have a basic appreciation for this con=
cept
if the rest of the theory is to be understood. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'color:red;mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span></span><sp=
an
lang=3DEN-US style=3D'mso-ansi-language:EN-US'>The electrical field is gene=
rated by
other dipoles. As shown in the chapter POLAR SHEAVES<span style=3D'color:ol=
ive'> </span>a
polar sheaf is two parallel threads flowing in opposite directions. This op=
posing
flowing creates (in the sub-Eteronic medium) an electric field, like that of
the interaction of weak dipoles mentioned above. The electric force is what
links polar threads and when this sub-electric force reaches an appropriate
value it can generate a change in a dipole forcing it to the b state or
further, can actually ionize the Eteron (the c state). This electric field =
is
generated near to the moving dipole. These electric fields also have two
polarities and have a special characteristic; a moving charge moves the same
pole in the same direction, while the opposite pole is moved in the opposite
direction. Among electrons, this happens due to the generation the EDF
(electro-dynamic-field). These forces are added to the static interactions.
(See chapter ELECTRON) However, the creation of a &#8216;b&#8217; dipole is=
 a
dynamic phenomenon, coexisting with the static forces. <o:p></o:p></span></=
p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>Returning =
back
to the discussion at hand, when an Eteron is being compressed the loading
(charge) of the strong dipoles never move closer to each other. The compres=
sion
and the creation of the &#8216;b&#8217; state are two different and indepen=
dent
phenomena. The act of compressing an Eteron has no bearing on its
&#8216;dipole-generating device&#8217;, which is not affected, so charge-di=
stances
of the dipole do not vary. This causes the effect of the dipole-field (E) on
the adjacent Eterons to increase according to the inverse of the cube of the
radius of the Eteron, while the simple cohesion-forces of the polar sheaf v=
ary
with the inverse of the square of distance. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;=
&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nb=
sp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;=
&nbsp;&nbsp;&nbsp;
</span>E =3D k/(r&sup3;)<span style=3D'mso-spacerun:yes'>&nbsp; </span><o:p=
></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'>where k is a constant and r is its radius=
 as
mentioned earlier in this chapter.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>By increas=
ing
this field intensity to such a point a phenomenon occurs that the Eteron
becomes ionized. The sum of the (E) fields of several Eterons acting on one
Eteron will cause it to ionize and create two Eter-ions.<o:p></o:p></span><=
/p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>It is the =
same
phenomenon that creates the &#8216;b&#8217; state mentioned before but in t=
his
case it&#8217;s strong enough to ionize an Eteron. For this to occur a dense
polar-sheaf is required to exist causing the creation of more polar sheaves
when at a particular point a value is reached where the dipole-creating for=
ce
is too high for the Eteron. The dipole field increases with the cube of the
inverse of the radius of the Eteron (1/r<sup>3</sup>) while the lateral
cohesion of the threads only increases with the square. Increasing the ener=
gy
the ionizing force increases by an extra factor and upon reaching a determi=
ned
value, the Eteron being affected splits in two.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>The voltage
threshold for this to occur is in the order of 1022 Kilovolts.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>The act of ionizing will cause the
Eteron being polarized to take the energy for the ionization from the
decompression of the surrounding Eterons that generated the field. Observe =
that
there is an interaction between dipoles and compression, but it is indirect.
Compression causes the dipoles to move nearer to each other and that proces=
s of
moving closer causes an increase of the field intensity that finally causes
ionization to occur.<span style=3D'mso-spacerun:yes'>&nbsp; </span><o:p></o=
:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>The charge
loading that generates the dipole-field are attractive to each other &#8211=
; as
in a North Pole of a magnet being attracted to a South Pole. The &#8216;b s=
tate
support mechanism&#8217; or obstacle causing the loads to remain apart is a=
 special
internal structure. The &#8216;releaser key&#8217; of this structure works =
with
perpendicular forces to the axis of the dipole. The pressure of another Ete=
ron
on one with a strong dipole can rotate this key in such a way that the loads
become closer to each other again and pass to the &#8216;a&#8217; state. The
energy, in this way is released and passes to the other Eteron that moves f=
rom
the &#8216;a&#8217; state and passes to the &#8216;b&#8217; state. The stro=
ng
dipoles are transferred in this way and are called a dipole wave. It transf=
ers
energy perpendicular to the axis of the dipole. </span>(See diagram 5.3)</p>

<p class=3DMsoNormal align=3Dcenter style=3D'text-align:center'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><!--[if gte vml 1]><v:shape id=3D"_x0000_=
i1027"
 type=3D"#_x0000_t75" style=3D'width:129.75pt;height:135.75pt'>
 <v:imagedata src=3D"5ettheo_archivos/image005.gif" o:title=3D"dcol5_3"/>
</v:shape><![endif]--><![if !vml]><img width=3D173 height=3D181
src=3D"5ettheo_archivos/image006.jpg" v:shapes=3D"_x0000_i1027"><![endif]><=
o:p></o:p></span></p>

<p class=3DMsoNormal align=3Dcenter style=3D'text-align:center'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'>DIAGRAM 5.3<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp; </span>A dipole-wave in space=
 will
move with the speed of light because the Eteron in the &#8216;b&#8217; state
transfers as much its strong-dipole (&#8216;b&#8217; state) as its
compression-state. An Eteron in a &#8216;b&#8217; state, which transfers en=
ergy
to an adjacent Eteron along the dipole axis, doesn't lose its strong dipole.
Instead it transfers a bit of its energy to the following Eteron in the
&#8216;a&#8217; state causing this Eteron to take some of the energy of the=
 first
and move to the &#8216;b&#8217; state.<span style=3D'mso-spacerun:yes'>&nbs=
p;
</span>(See diagram 5.4) The first Eteron loses some of its compression ene=
rgy
becoming slightly decompressed. In another way it loses some of the energy =
of
its compression however because the energy was directed along the axis it d=
oesn't
lose its strong dipole. <o:p></o:p></span></p>

<p class=3DMsoNormal align=3Dcenter style=3D'text-align:center'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><!--[if gte vml 1]><v:shape id=3D"_x0000_=
i1028"
 type=3D"#_x0000_t75" style=3D'width:162pt;height:120pt'>
 <v:imagedata src=3D"5ettheo_archivos/image007.gif" o:title=3D"dcol5_4"/>
</v:shape><![endif]--><![if !vml]><img width=3D216 height=3D160
src=3D"5ettheo_archivos/image008.jpg" v:shapes=3D"_x0000_i1028"><![endif]><=
o:p></o:p></span></p>

<p class=3DMsoNormal align=3Dcenter style=3D'text-align:center'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'>DIAGRAM 5.4<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify'><span lang=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>In summary=
 then:
<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:0cm'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>I. If the =
Eteron
transfers energy in a perpendicular direction to the axis of the dipole, it
transfers its compression state as well as its strong dipole, becoming neut=
ral
or dropping back to the &#8216;a&#8217; state. (Refer diagram 5.3)<o:p></o:=
p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:0cm'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>II. If how=
ever
the Eteron transfers energy parallel to the direction of the axis of the st=
rong
dipole, it doesn't lose its strong dipole, but a bit of its energy is used =
by
the other Eteron to pass it from the &#8216;a&#8217; state to the
&#8216;b&#8217; state.<span style=3D'mso-spacerun:yes'>&nbsp; </span>This c=
an
generate a long polar thread that can be projected for a great distance, if=
 the
energy supply exists from the base of the thread. (Refer diagram 5.4)<span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp; </span><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'text-align:justify;tab-stops:0cm'><span lang=
=3DEN-US
style=3D'mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>In the cas=
e of
an electron, the projection of its field is like the quills of a sea
urchin.<span style=3D'mso-spacerun:yes'>&nbsp; </span>These quills are actu=
ally
polar threads with negative poles pointing in an opposite direction to the
particle. The Eterons here are in a minimum compression state, but still ex=
ist
in the &#8216;b&#8217; state. The sum of the energy of these Eterons is par=
t of
the internal energy of the electron. Be aware that while there appears to b=
e a
conflict with that explained in chapter on ELECTRON after reading the chapt=
er
PARTICLES there will be no conflict.<o:p></o:p></span></p>

<p class=3DMsoBodyText><span lang=3DEN-US style=3D'font-size:12.0pt;mso-bid=
i-font-size:
10.0pt;mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>Having dis=
cussed
the basics of Eterons it is now possible to provide an initial insight into=
 the
internal structure and dipole formations within an Eteron.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>Strong dipole formation is due to a
couple of charges around the centre of the Eteron.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>Diagram 5.2 (lower side) represent=
s an
Eteron in the &#8216;b&#8217; stage having a dipole axis. <o:p></o:p></span=
></p>

<p class=3DMsoBodyText2><span lang=3DEN-US><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>In the
perpendicular direction to the axis of the dipoles, the transfer of the dip=
ole
is total and this allows the formation of &#8216;dipole-waves&#8217; (the
photon).</span></p>

<p class=3DMsoBodyText><span lang=3DEN-US style=3D'font-size:12.0pt;mso-bid=
i-font-size:
10.0pt;mso-ansi-language:EN-US'><span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>5) The
compression of the Eteron has at its heart a digital mechanism. Compressing=
 an
Eteron and changing its radius doesn't produce any infinitesimal values of
variation. There is a minimum but digital difference that is a constant that
multiplies from the previous value of the Eteron. The difference of value
between the two consecutive radii must be the product of the initial radius=
 by
a constant. The value is (n.s), where s is the variation constant and n is =
an
integer. <o:p></o:p></span></p>

<p class=3DMsoNormal><span lang=3DEN-US style=3D'mso-ansi-language:EN-US'><=
span
style=3D'mso-spacerun:yes'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </span>Infinite a=
nd
infinitesimal are incomprehensible concepts and cannot be used for practical
entities. Between two given values, there is a very large but finite number=
 of
possible energy levels for the Eteron. Each radius of the Eteron is due to =
an
accommodation of its structure to the external force that presses against it
and is governed by electrical forces generated by a finite amount of intern=
al
elements.<o:p></o:p></span></p>

<p class=3DMsoNormal><span lang=3DEN-US style=3D'mso-ansi-language:EN-US'><=
o:p>&nbsp;</o:p></span></p>

<p class=3DMsoNormal><span lang=3DEN-US style=3D'mso-ansi-language:EN-US'><=
span
style=3D'mso-spacerun:yes'>&nbsp;</span><o:p></o:p></span></p>

</div>

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