relative.txt   [~217K]

relative.htm [~621K]

 

 

INTERFACE RELATIVITY

 

 

 

Interface between special and general relativity

 

A helpful sonic stereo experiment reports contains possible
insights casting more light on Interface Relativity, see the
reports here:
http://www.cosmicastronomy.com/appendix.txt

 

ABSTRACT:


A step toward unifying the forces. The gravitational force, and electro-magnetic forces (strong, electro-weak, and charge) are unified through Interface Relativity equations which join general and special relativitist effects into a fundamental equality. The interface specifies the principles and properties by which the general (gravity) and special relativity (radiation) modes are unified into a single set of of coherent balanced equations.

 

 

 

 

 

INTRODUCTION TO MASS INCREASES BY

 GRAVITATIONAL RELATIVITY

 

 

 

 

The following proposes that steady state relativistic effects can be understood to occur pursuent to gravitational fields.

The wider range of distortions in space embraced by the GENERAL
THEORY OF RELATIVITY are put aside and certain specific effects
are studied in detail. These specific effects are understood to
come under the heading of GRAVITATIONAL RELATIVISTIC EFFECTS.

Greydon Moore
Ottawa, Canada, June, 1990.

 

 

 

 

 

GRAVITATIONAL RELATIVITY THEORY

CONNECTS CERTAIN SOLAR PLANET MASSES

 

 

 

 

 

ALSO, GRAVITATIONAL AND SPECIAL RELATIVITY THEORIES ARE INTRINSICALLY RELATED

 

 

 

 

By assuming a mass and spacial effect in general relativity, a
proposed gravitation relativity is evident, in which there is a
direct tie-in between effects seen in Special Relativity and in
Gravitational Relativity. In fact, properties commonly factored
for a star or black hole in Gravitational Relativity, can also
be factored in Special Relativity, and visa versa. This suggests
not necessarily a unified field theory, but definitely a connection
between certain properties in gravity, and in electro-magnetism.


 

 

ABSTRACT

 

 

 

Several facets are to be discussed in the following.


(Part 1) Arguments demonstrating an increase in mass by the
effects of gravitational relativity are shown through events
which occur in the solar system.

(Part 2) Effects for gravitational and special relativity are shown
to be synonymous for a given mass. Critical limits are uncovered in
the behaviors of both relativities. In specific situations, mass is
locked to a ceiling which is less than, but is determined from, black
hole mass equivalents. In this, it is found that the maximum original
mass which can be gathered before gravitational relativistic effects
are maximized, is that of a black hole's mass divided by a factor
of 1.618034 (a number constant known as the Golden Harmonic Ratio).
The maximum velocity attainable by this mass when moving in special
relativity, is the speed of light divided by the Golden Harmonic Ratio.


(Part 3) It is found that for any visible mass, there is a
maximum special relativistic limit on the mass. This limit can be
known in advance by knowing the maximum velocity the moving mass can
attain and still remain visible in the normal sense, when observed by
a stationary observer. The maximum effect is a derivative of the speed
of light reduced by the relativistic effect of the mass's gravity.
This is shown to define an upper limit velocity at which any given
mass can appear in the same state of the universe as the stationary
observer. Any rest mass reaches this barrier at a plateau that is
predictable, and so the mass cannot visibly expand to infinity.


(Part 4) Innuendos of a unified field theory are harking loudly,
popping out of the framework of relativistic physic. There is a
universality in obvious behaviors working directly between the
one field's venues (gravity) and the other field's venues
(electromagnetism). As to whether these equalities can constitute
segments of a full fledged unified field theory is not to be
addressed at this time, in the scope of the following disclosures.

 

 

PART 1

GRAVITATIONAL RELATIVITY

 

 

A little known (entirely unknown) fact is that certain solar
planetary masses can be connected as a direct consequence of
gravitational relativity. This is shown to be true when it is
surmised that relativistic effects of gravity may include an
intrinsic increase in the mass comprising the source of the
gravity.

The relativistic increase for the Sun mass is very small compared
to the mass of the Sun itself. Even though the increase in mass
is small at roughly 4.23 x 1027 grams, the increase
is nevertheless nearly 7 times the mass of Mars, and is marginally
less than the mass of Venus.

Such an increase in the Sun mass, when calculated to advanced
accuracy, is found to be exactly equal to the mass difference
between Venus and Mars. Another discrete relativistic potential
includes 1/2 the mass of Jupiter added to the mass of the Sun.
The existence of states makes it possible to infer a more
accurate estimate for the existing mass of the Sun.

The radius of the Sun is considered to be a constant for various
manifestations, shown to correspond to parameters which operate
between solar mass equivalents up to the masses of black holes.
In this, a link between gravitational and special relativity
is shown. The link is the subject of part 2.

 

 

PART 2

SPECIAL RELATIVITY

 

 

It can be easily demonstrated that a visible mass moving at
velocities nearing the speed of light, can never grow to infinite
quantities and remain visible in the normal sense, and so can never
achieve a velocity equal to the speed of light, in the normal sense. 


This is because gravitational relativistic effects have to be
considered for a moving mass, if it is assumed that gravitational
relativity includes an effect that increases the original state of
the mass which is the source of the gravity's relativistic effect.
It is readily shown that such gravity effect has significance to
special relativity.

There is a boxed in limit, where the moving mass (bumped in
value in special relativity) assumes a value equivalent to the
mass of a black hole, when the original rest mass is expanded by
the effect of special relativity, in direct accord with the mass's
radius contracted by the effect of special relativity.

When assuming the mass of a black hole equivalent, the
moving mass effectively drops from sight in the normal
physical view as seen by a stationary observer.

(See Appendix A at the end of this document, for a related
discussion involving elementary particles such as the proton).

One of the finite limits to which a mass can be accelerated
in special relativity, and to which a mass can be accumulated
in gravitational relativity, can be explicitly expressed for
both modes of relativity as factors of a number constant known
as the Golden Harmonic Ratio, 1.61803398875 .

In this, the Golden Ratio's significance is to the existence of
black holes. Specifically, a black hole's mass includes both an
original mass and an augmentive portion from the relativistic
effect of gravity, to comprise the total mass involved. The
relationship between original, gained, and final black hole
mass aggregations, can be expressed in exact terms of the
Golden Harmonic ratio.

In particular, however, in the dynamic behaviors of both
relativities, important boundaries are reached at a certain
critical limit whose mathematical significance is the Golden
Harmonic Ratio. The parameters here include a black hole's
mass aggregate and event horizon.
 

PART 3

THE GOLDEN HARMONIC RATIO

 

 

The effects of gravitational relativity can be generally related
to the effects of special relativity, to the extent that relativity
effects of gravity and of special relativity can be shown to be
equated through a single common factor.

The maximum velocity attainable by a visible moving mass, is
the speed of light reduced by the proportionate effect of the
gravitational relativistic effect in the mass being accelerated.

The critical limit (maximum velocity) possible, is restricted
by bounds achieved in special relativistic effect when the rest
mass has increased, and radius has contracted, to a point where
the moving entity reaches a state where it forms a black hole and
effectively disappears from view, relative to a stationary observer.

The barrier limit is easy to calculate and to mathematically
confirm, when given the original rest mass and radius.

It becomes clear that, generally a visible mass accelerated to
relativistic velocities cannot theoretically achieve an infinite
mass, and the velocity can never theoretically equal the speed of
light. The traditional interpreted statements in special relativity
which say any visible mass continues to expand toward infinity,
and the velocity continues to the speed of light, are in error
about such things.

 

 

 

 

     

 

GRAVITATIONAL RELATIVITY THEORY

 

 

 

 

GENERAL INTRODUCTION for part 1 The Solar System

     

 

In the following, the existing orbits of planets are not
considered as terms, and all of the events are shown to
occur as within a constant confinement radius which is
the existing radius of the sun.

A general relativistic equation is in common use for gravitational
effects. Such an equation has been around in physics since 1916.
Variations of the equation are also in common use. Given a known mass
for instance, a Schwarzschild radius for that mass confined as a black
hole can be immediately calculated.

Conversely, given a radius, how much mass would be needed to be
confined within that radius as a black hole can also be calculated.

Such effects are a steady state system. It is the amount of
mass within a specified radius which counts. The effects are
constant per given mass and radius, since no outside velocity
or acceleration is involved with the masses sitting stationary.

The same is true for mass aggregates which are not a black hole,
but which have mass sufficiently large, and a radius sufficiently
small, for gravitational relativistic effects to be discernible.

For stars the size of the Sun, for instance, there are discernible
effects, even though they appear to be very slight at first sight.
In a closer look, however, the slight effects can reveal many major
properties in the fundamental relativistic behavior of gravity.

 

       GRAVITATIONAL RELATIVISTIC EFFECT

 

In principle, gravitational relativistic effects are calculated via
the standard equation, for varying mass and radius, until a meeting
point is reached at which the mass and radius correspond to the
formal parameters of a black hole.

In the standard equation, a term for the relativistic effect
results, which has been mainly used to determine the slowing
of time in closer vrs more distant proximities to the field
generating the effect.

The same term can be used to find out how much a gravitational
mass's radius can further contract relativistically per given
increase in mass, when assuming that gravity relativistically
contracts its own confinement radius. The same term can be used
to calculate the gravity's relativistic effect on its own mass.

This term can be called E (for effect). The value of term E
suddenly nose dives toward 0 when the mass is sufficiently large,
due to a sudden relativistic upsurge in pull in the greater power
of the gravity itself, at which point the existing mass becomes
a so called black hole and the existing mass's radius no longer
appears to contract, rather, it will begin to increase given
further increases in mass.

This mass and radius stabilization is considered a physical
boundary called the Schwarzschild radius, or event horizon.

The stabilization is discussed in 'A Comparison Between
Gravitational And Special Relativity' (found directly
under the 'General Introduction for Relativity' Part 2',
below), and is formally described in Equations 3 to 5
in APPENDIX B at the end of this document.

        GENERAL MASS QUANTA EFFECT

 

In variations of the equations, when a quantity of mass is given
and the radius containing it is also known, then a simple solution
using term E can denote how much of a mass increase may occur in
the mass, due to a relativistic augmentation by the mass's gravity.

The augmentation can be conjectured to occur in two ways.
Either a measured mass is naked (original with no relativistic
augmentation), or is augmented (the measured mass includes
the augmentation).

Hence the augmentation can be conjectured to be in two
modes; either a decrease upon the originating mass, or
an increase.

In keeping with special relativity effects, a mass increase
in gravitational relativistic augmentation can be presumed
with no difficulties.

For instance the Sun (given its mass and radius) is surmised
to have a visible radius which is marginally reduced by
relativistic augmentation (shrunk), and so the Sun's apparent
mass is also surmised to be marginally augmented (expanded) in
a mass increase by an equivalent relative proportion.

The problem is that such a conjecture (relativistic augment-
ation in mass) is hard to prove, since it is not possible to
actually separate a given mass from its gravity and so observe
any change in the apparent mass, when the mass is compared with
vrs without the relativity of the gravity.

In which case, any evident mass augmentation will have to
be learned by some secondary means.

In this solar system such a means is provided mechanically,
by the fact that the amount of solar mass augmentation is a
meaningful quantity in company with the existing mass of some
of the planets.

The mass augmentation has a value which is in a quantum
correspondence to the existing masses of Venus and Mars.
This makes the mass augmentation clearly visible. The fact
that the relativistic mass is involved with these planets
(in relationship with small particles external from the Sun)
is very curious.

GRAVITATIONAL RELATIVISTIC EFFECTS

The standard equation for gravitational relativistic effect
is described as follows:

 

EQUATION A

E = √[ 1 - 2G(mass)/C2R ]                                

 

The square root of [1 - (the product of 2 times the
gravitational constant G, times a mass) /(the radius

of that mass times the speed of light squared) ],
yields a gravitational relativistic effect factor, termed E.

EQUATION B

The radius of the mass times the reciprocal of the
E factor, gives the originating radius of the mass,
ie., before contraction of the radius by the mass's
gravitational relativistic effect.

 

[ R x (1/E) ] - R = Re    Where Re is the amount of space by which the Sun's

                                             radius is contracted by the relativity in the Sun's mass

 

[    Ro   ]                       Ro is the original radius before effect

                                             R is the existing radius (the radius we see) which includes

                                             effect (Ro + Re)                  

 

These (Equations A and B) are well known and nothing new
has been so far stated.

The relativistic collapse in the Sun's radius
is very slight, hardly 1½ kilometers.

This is learned as the difference between the originating Sun
radius Ro, minus the existing (augmented) radius R. The difference
seems to be a remarkably close approximation of ½ the Schwarzschild radius needed for the Sun mass to be a black hole.

However this is not surprising, in that the smaller the mass and/or

the larger the radius, the closer the radius augmentation is to ½ the Schwarzschild radius. The ½ approximation grows closer, the

less the mass aggregate is a black hole.

In principle, with little mass and a large radius, there is
very little augmentation. Conversely, a very small radius for
the small mass is needed as the event horizon for the small mass
to become a black hole.

The point intended is that as the mass to radius ratio
approaches the primes of a black hole, the rates of
change due to gravitational relativistic effects climbs
up a steepening gradient.

At solar quantities, the effects are so slight as to be
normally thought of as negligible. But this is not so.

If for instance 1/2 the mass of JUPITER is added to that of
the Sun, and this enhanced mass sum is regarded as being within
the confines of the existing Sun radius, the relativistic mass
augmentation effect when applied to the mass of the Sun minus
1/2 the mass of Jupiter, equals the previously noted congress
involving Venus and Mars masses, (at the end of 'General Mass
Quanta Effect'
, above).

 

Such state arrays reveal a previously unsuspected property,
of relativistic mass quantal arrangements displaced at long
distance from the source generating the relativistic mass
effect. A first suspicion is that:

'THERE IS AN INCOMPATIBILITY BETWEEN A GRAVITATIONAL
FIELD AND THE RELATIVISTIC EFFECT IT GENERATES'

The appearance is that some aspect of the relativistic mass
effect generated in a field of gravity, does not stay within
the field generating it.

 

In supposition, it appears that some relativistic component
is expunged (externalized) from the originating field of
gravity. In the case of our solar system's example, the
masses of Venus and Mars, along with Jupiter, are external
and yet relativistically tied to the Sun mass.

 

         ESTIMATED ACCURACY OF SOLAR MASSES

 

Masses in the solar system are traditionally published in two
ways. A mass for each planet is given as a ratio between it and
the mass of the Sun. Since comparative ratios can be inferred to
considerable accuracy, the Sun to planet mass ratios for most of
the planets are well known.

On the other hand estimating the actual mass of a planet or
the Sun in terms of (say) gram units, is not so easy, since
there is no way of actually sitting a planet on a scale. For
that matter, estimating the real mass of the Sun (in say grams)
is also difficult since the Sun cannot be weighed on a scale.

The problem is compounded in that in order to know a real
weight (in grams) requires that the universal gravitational
constant (G) be known to high accuracy, which it is not.
Whereas determining the mass influences of one body on another,
as a ratio, is easier since (G) is not a critical factor for
the accuracy.

For these reasons the real mass of (for instance) the
Sun (in say grams) cannot be stated with great accuracy
by ordinary measuring methods.

The Sun's mass is currently given as somewhere between
1.989 x 1033 grms, and 1.991 x 1033 grms. Whereas
planet masses are currently given in gram figures accurate
to between 4 and 5 significant figures. The greater accuracy
for planet masses is assisted by the fact that the planets
tend to subtlety bounce each other around in orbit, and their
bouncing can be closely watched. Whereas the Sun is hardly
bounced by the less hardy influence of the planets.

The Earth - Moon combination gives the best look at bouncing.
But rigorous real weight analysis for the Earth is not so easy
when tried, because both the Earth and Moon also subtlety bounce
around as a unit.

 

If the gram weight of the Earth (5.976 ± .004 x 1027 grms)
is multiplied by the Sun to Earth mass ratio (332,995.9
± .4),
then the Sun's gram weight results as (1.9899834 x 1033 grms).

This value is actually deemed low to a very minor degree for the
equations which follow below. In the following, a Sun mass in the
vicinity of (1.990993 x 1033 grms) is explicitly inferred.

Another problem in any advanced accuracy is inherent in the weak
solar gravitational relativistic effects per se. Because the effect
for solar mass quantities is so slight, there is a loss of some
accuracy due to inherent truncation in doing the calculations.

In the equations which follow, accuracy has been maintained
to 13 significant digits, but inherent truncation results at
the 7th significant digit of certain of the terms.

Such truncation is diminished when dealing with larger
masses confined within small radii. The truncation disappears
completely when dealing right at the range of black hole masses.

Hence, black hole limits can provide a tool for comparing
calculations, to determine which calculations produce
exactitudes and which produce close approximations only.
This is actually more straightforward than it sounds.

 

         BASIC CONVENTIONS

 

 

In the following, the existing orbits of planets are not
considered as terms. All of the events are shown to occur
as within a constant confinement radius, which is the
existing radius of the sun.

For the sake of convenience, the mass of the
Sun is shown as a standard term labeled (MM).

 

In the following, the calculations are accomplished at
an accuracy of 10 to the 13 significant digits. Zeros are
used to fill gaps between available digits and the 13th
significant digit. As already mentioned, some of the terms
are accurate only to the 7th significant digit. In fact,
some terms cut off at the 7th digit. For this reason, the
highest maintained accuracy possible is very important.
 

For the universal gravitational constant G, a recent
revision having a digital value of 6.6720 x 10-8 is used.

The speed of light C of the following value is used:
2.99792458 x 1010 cm/sec.

The radius of the Sun is used as a constant R, having
the value 6.96265 x 1010 cm.

MASS CONVENTIONS

The following mass aggregates have been adopted as standards for
the involved quantities. The high accuracy given them has been
by the adjusting of repeated pure math experimental results until
a semblance of coherency in the mass standards looked viable.

The term 'aggregate mass' is used for denoting a mass (such as
the Sun, plus or minus another mass (such as ½ the mass of
Jupiter).

'Aggregate mass' is also used to denote any apparent
mass, since the mass is assumed to include relativistic
augmentation due to gravity.

Hence, the original mass before augmentation is

termed 'original mass', or 'originating mass'.

K has been adopted as a term to explicitly denote the
relativistic mass augmentation in the Sun's mass due
to the Sun's gravity.

In determining aggregate mass values, the value of MM for the
Sun's apparent mass was first determined, based on an assumed
equality that a so called K augmentation factor for the Sun mass
is indeed the mass difference between planets Venus and Mars.

Without doubt the real values for the mass aggregates (given
in grms for instance) will marginally change depending on
future adjustments of the universal gravitational constant,
and perhaps sharper astronomy techniques.

(For that matter, mass MM may not be the true real
mass of the Sun. It may turn out that MM is the mass
of the Sun
± something else).

It is anticipated that any such changes would nevertheless
prove to continue to be coherent within the realms of the
gravitational relativistic state equations which involve them.

Several tables and basic equations follow. Following these,
a discussion begins on how a mass of MM was inferred for the
Sun, via gravitational relativistic effects.

Table 1 which follows, lists important mass aggregations,
and the highest resolved real mass values possible as used
to explore their relativistic highlights.

 

 

INFERRING A GRAVITATIONAL RELATIVISTIC
 AUGMENTED MASS VALUE FOR THE SUN

 

 

                                   TABLE 1:  INFERRED VALUES

 

MM 

= Existing Sun mass, presumed to include
   original mass plus mass augmentation K

=1.9909930 x 1033 grms

 

 

= Gain in original mass of the Sun, the
   amount of relativistic augmentation 
   due to the Sun's gravity

= 4.226490 x 1027 grms

 

 

Mbh

= Mass of a black hole having an event 
   horizon equal to the Sun's radius R

= 4.689536679 x 1038 grms

 

 

                             TABLE 1-A ESTABLISHED VALUES

 

= Existing Sun radius

=6.96265 x 1010 cm

 

 

C

=  Speed of light

= 2.99792458 x 1010 cm/sec

 

 

G

= Universal gravitational constant

= 6.6720 x 10-8 cm3/grms sec2

 

 

CR

= A physical constant for Mass/Radius
   ratio of a black hole

= 6.735275620 x 1027 grms/cm

 

 

GH

= Golden Harmonic Ratio

= 1.61803398875

√GH = 1.272019649

 

 

                            TABLE 2

 

Planetary masses - Data is from tables found at the
                     back of the following reference:          

   UNIVERSE by Don Dixon, Houghton Mifflin Co.,  Boston, 1981

Moon     = 0.0735 x 1027 grms
Venus    = 4.8683 x 1027 grms
Earth     = 5.976   x 1027 grms
Mars      = 6.4181 x 1026 grms
Jupiter  = 1.901   x 1030 grms

Sun       = 1.9888 x 1033 grms

 

 

                            TABLE 3

                            Certain terms are used to generalize  certain types of masses:

 

Low mass            

-

Masses in the range of those  found in this solar system

Enhanced mass   

-

Solar mass aggregates other than the Sun, added or subtracted to  the Sun mass

 

 -  Specifically the mass of the Sun   

plus 1/2 Jupiter, and mass of the Sun minus 1/2 Jupiter, also mass of the Sun minus mass of Venus

Higher mass    

-

Mass of a black hole, and in mass range of a black hole

-  Specifically the mass for a
 black hole whose event horizon
 is the radius of the Sun

 

Originating mass

-

Original mass accumulation without
any relativistic augmentation

Augmented mass

-

Existing mass assumed to include
 a change from the originating
mass due to relativistic effect
of gravity

Existing mass

-

As physically measured, with
any assumed augmentation present
in the measurement

Real mass

-

A real weight, in terms of a  physical weight, for instance
measured in grms as if weighed
on a scale

 

 

 

Certain equations are used to generalize mass effects
due to gravitational relativity. Certain term conventions
are adopted for the sake of convenience in bookkeeping:

 

EQUATION C

 

Determining a relativistic effect factor Em
for a mass aggregate, in particular the Sun:

[using Equation A above]

Em=√[1 –  2G·MM/C2·R]              where MM is the mass of the Sun

                                                         and R the radius of the Sun

EQUATION C-1

 

Determining how much mass augmentation relativistically
occurs in the mass aggregate of the Sun:

MM – (MM x Em) = Km       Where K is the actual mass
                                         augmentation increased on
                                         the Sun's original mass
                                         due to gravity

EQUATION C-2

 

Determining a relativistic effect factor for a mass
aggregate, such as the Sun plus X, where X is anything:

Ex=√[1 –  2G·(MM+X)/C2·R]      

 

EQUATION C-3

 

Determining how much mass augmentation relativistically
occurs in a mass aggregate, such as the combined mass
of the Sun + X , when both are confined in radius R :

(MM+X) – [(MM+X) × Ex] = Kx   [originally K+x]

 

EQUATION C-4

 

For example, determining a relativistic effect factor
for such as the Sun plus ½ Jupiter combined:

E+½j=√[1 –  2G·(MM+ ½j)/C2·R]       [ E+½j originally E+½j ] 

 

EQUATION C-5

 

Determining how much mass augmentation relativistically
occurs in a mass aggregate, such as the combined masses
of the Sun and ½ Jupiter, when both are confined in
radius R :

(MM+½j) – [(MM+½j) × E+½j] = K+½j  

                                              [ E+½J originally E+½j  , K+½J originally K+½j ] 

 

 

 VERIFYING A MASS OF MM FOR THE SUN 

 

 

An aggregate mass MM (being the mass of the Sun) found to have
intrinsic relativistic consequences, can be easily verified.

If starting with an estimated Sun mass, for instance;
(1.989 x 1033 grms); and assuming that the Sun mass is
already relativistically augmented, the gravitational relativistic
mass increase of a Sun mass of (1.989 x 1033 grms) is found
(using Equations C and C-1), to be slightly less than the mass
difference between Venus and Mars.

That is:    Venus mass       is      4.8683     x 1027 grms
                Mars mass         is        .64181   x 1027 grms
                Venus - Mars     is      4.226490 x 1027 grms

whereas the mass augmentation Km of a
Sun mass of (1.989 x 1033 grms) is
(4.218033 x 1027 grms), which is low.

If the Sun's mass is gradually increased, eventually a
mass aggregate will be found, in which the relativistic
mass augmentation K is precisely (Venus - Mars), that is:

K = 4.226490 x 1027 grms.

                       

The point of agreement occurs when the mass aggregate
for the Sun MM is found to be (1.990993 x 1033 gms).

 

For instance, suppose arbitrary units of Neptune's mass are
systematically added to a base mass of (1.989 x 1033 grms).
A break point will be reached. At + 18N units of Neptune's mass
the relativistic augmentation (Km) of the aggregate mass will be
marginally less than (Venus - Mars). And at + 19N units of
Neptune's mass, the relativistic augmentation (Km) of the
aggregate mass will be marginally more than (Venus - Mars).

 

And so somewhere between (base + 18N) and (base + 19N) is a solar
mass component whose resulting augmentation (K) is exactly equal
to (Venus - Mars). The search can now be narrowed to (base + X),
where (+ X) falls somewhere between (+ 18N and +19N).

Fine tune fiddling back and forth using smaller and smaller
increments for X, eventually closes in on a result for;

(base + 18N + X)

 

in which the relativistic mass augmentation
from (base + 18N + X) when using Equation D
below, equals (Venus - Mars) exactly.

EQUATION D

 

E =√[1 –  2G·(b+X)/C2·R]     Where b is a base mass

                                                   =(1.989 x 1033 grms)

                                                     And so  (b+X) – [ (b+X) × E ] = K,

                                                     and K=(Venus-Mars) exactly,

                                                     when (b+X) is exactly 1.990993 x 1033 grms

 

EQ D can be written so that (b+X) is standardized as MM, so that:

 

 

EQUATION E

Em=√[1 –  2G·MM/C2·R]       Where MM is an inferred Sun mass,

                                                                so  MM – (MM× Em) = K

                                                                                     where K =(Venus-Mars),

                                                                and Em is the relativistic

                                                                effect factor for mass MM

In other words the inferred Sun mass MM presents a solar
mass factor whose relativistic gravitational augmentation (K)
is exactly equal to the mass difference between Venus and Mars.

 

That is:     Equation E determines Em
     and:    
MM (MM × Em) = K
     and:    
K = 4.226490 x 1027 grms

 

                                            which is precisely (Venus - Mars)
  which also is:            4.226490 x 1027 grms

 

This instantly presents an interesting situation. The inferred
mass of the Sun MM appears to involve a relativistic gravitational
mass amalgamation which is greater than the mass of the Sun alone.

The interesting kink is that the masses of Venus and Mars
are found expunged into space, at long distance orbits around
the Sun. This orbital existence is not explained at this point
and so is noted only as a comment.

The other interesting point of view is that although the mass
of Mars for instance is very small compared to the mass of the
Sun, the mass of Mars is nonetheless highly visible. This is
something like the high visibility of the electron's tiny
binding energy unit in comparison to the mass of the Proton.

 

 

 

 SPECIFIC MASS QUANTA EFFECT

 

 

As described under 'A Comparison Between Gravitational And Special
Relativity' (found directly under the 'General Introduction for
Part 2', below), gravitational relativity includes at least two
variable source terms for its effect. These source terms are the
aggregate mass, and the mass's confining radius. It means that
different quantities of mass can be said to occupy the same area.
In which case there can be (in result) different or identical
relativistic mass augmentations, depending on discrete combinations
of how much mass is said to be added or subtracted to the initial
mass aggregate, confined in the same or in different radii.

For instance in mass aggregates which are in the range
of the size of the Sun, here, discrete extra mass in the
same radius (the Sun's radius) can produce a relativistic
factor Ex which when arbitrarily applied to yet another
discretely different mass aggregate, can produce a K
augmentation which is otherwise gained from yet another
different mass aggregate.

For instance, the Sun mass MM, plus ½ the mass of Jupiter,
can provide via EQ C-2 an effect factor
E+½j which when
applied to the same mass aggregate, via EQ C-3, results in
K+½j .     [ K+½j originally K+j ]

  

But if E+½j is applied to a different mass aggregate, for
instance to MM-½j, a value slightly departed from
K+½j must
result. The resulting slightly lower value in fact once again
happens to be K exactly (the mass difference between Venus
and Mars).

The formal description for this enhanced mass state is:

EQUATION E-1

E+½j=√[1 –  2G·(MM+ ½j)/C2·R]      MM+½j is the

                                                                          aggregate of the Sun

                                                                          mass plus ½ the mass of

                                                                         Jupiter, confined in the

                                                                         existing Sun radius R

EQUATION E-2
 

( MM-½j ) – [ ( MM ½j ) x E+1/2j] = K

where K equals the mass of (Venus - Mars), and
E+1/2j is the relativistic effect of the slightly
denser aggregate of the inferred Sun mass MM plus ½
the mass of Jupiter, when confined in the Sun's radius R.

In keeping with state-like mass aggregates, if EQ E-1 is
rewritten so that the initial mass aggregate used in EQ E-1
is now MM-½j, and a resulting effect (called E-½j) is
used in a rewritten form of EQ E-2, then a relativistic mass
augmentation equal to K once again results; that is:

 

EQUATION E-3

( MM+½j ) – [ ( MM+½j ) x E–1/2j] = K
where K equals the mass of (Venus - Mars).
 

EQUATION E-4

The bifurcation of Jupiter mass around the mass of the Sun
to form coherent relativistic states can be generalized as:

E+1/2j   of mass   M+½j   applied to   M–½j   yields K
Em        of mass   MM        applied to   MM       yields K
E-1/2j    of mass   M–½j    applied to   M+½j  yields K

 

EQUATION E-5

Such a bifurcation around the mass of the Sun
can be generalized as:

E+x  of mass  M+x   applied to   M–x    yields Kx
E     of mass  M       applied to   M       yields Kx
E-x   of mass  M–x    applied to   M+x   yields Kx

However, the augmentation quantity Kx only equals known
augmentation value K, when M+x and M-x are specifically
MM+½j, and MM½j. That is, when ½ quantas of Jupiter's
mass are added, and subtracted, to the inferred mass MM of
the Sun.

 

(It should be noted that the bifurcation results of EQ E-4
are not perfect exactitudes. The three resulting values of
K happen to look the same for masses in the range of this
solar system. For higher mass densities for example MM
times 1000, confined in the same radius R, the three K
values (shown as Kx in EQ E-5) are noticeably separated).

         VERIFYING THE COHERENT ½j STATES

 

 

Equations E-1, E-2, E-3, and E-4, were not easily found without a
prior insight and a discovery. In question is how come a unit of 1/2
the mass of Jupiter has been arbitrarily used to arrive at a seeming
non arbitrary result, this result being where K is twice again
calculated, as summarized in Equation E-4.

An original intention was to see if the total mass of the solar
system could be inferred to be in any way involved in some sort
of interphasing between different mass aggregates in this solar
system's gravitational relativity. This thought itself came from
an original impression that the real mass of the Sun was in the
range of base (1.9891 x 1033 grms), and inferred mass MM
would be the real Sun mass (base) plus Jupiter's mass, since
(MM - base) closes in on an excellent approximation of Jupiter's
real mass at (1.901 x 1030 grms), when using EQ D to infer
mass MM.

For a while it was looking good. It seemed that if MM was the
mass of the (Sun + Jupiter), and a mass value just slightly
larger than the total mass of the solar system was substituted
in EQ C-2, then a mass augmentation of K was again found when
the factor Ex of EQ C-2 was substituted in EQ C-3, when
Jupiter's mass was subtracted from the solar total mass
aggregate and the result of this reduction substituted for
MM+X in EQ C-3.

In the exploration, a mass term Mt was adopted for the solar
mass total, plus some little extra, to give mass term Mtx.
And mass term Mtx–j denoted the solar total minus the mass
of Jupiter.

The value of Mtx could be rigorously inferred, as being
exactly the mass aggregate needed in EQ C-2 to result in
a mass augmentation effect equal to K in EQ C-3, when mass
aggregate Mtx gave augmentation effect Etx, which was used
to find the augmenting effect on mass Mtx-j, as in:

 

EQUATION F

Etx=√[1 –  2G·Etx/C2·R]       

and a mass aggregate of (Mtx - Jupiter) was substituted
in EQ C-3, giving:

 

EQUATION G

(Mtx–j) – ((Mtx–j) x Etx) = K

In other words, the thinking was heading along a line that a
sort of formal relativistic interphasing might be occurring,
whose boundary was spread between the base mass of the Sun,
and the total mass of the solar system. For instance between
the Sun, and (Sun + Jupiter), and (Sun + planets + moons),
and (Sun + planets + moons - Jupiter). The problem was in that
little extra mass bit, (the x of Mtx). What might it represent?

It was suddenly and unexpectedly found that the value
of Mtx as rigorously inferred, turned out to be exactly
(MM + ½ Jupiter). This was not a percentage of error
type of equality. The figures that suddenly appeared on
hand were identical to 8 significant digits.

In other words, the rigorously determined value for Mtx,
and MM + ½j, were identical to 8 significant figures.

Which dramatically changed the picture.

It was now easy to think that MM instead of being
a (Sun mass + Jupiter) aggregate, represented the
real mass of the Sun itself. In other words, MM
could well be the real mass of the Sun.

It was also easy to perceive a formal verification for the
quanta bifurcation factor involving
½ the mass of Jupiter.

By using Equations F and G to find a result equal to K,
a mass quanta increment of (+X) added upon MM eventuates in
an interphase involving (MM-X) for the K result, only when
X is exactly
½Jupiter, when using the same inferencing
technique as was used to infer MM in the first place, as
described above under 'Verifying a Mass of MM For The Sun'.

A slightly more accurate inferencing for MM itself was thus
made possible. In order for Equations E-1 to E-4 to yield
results definitely equal to K, the value of MM is adjusted
to the greater accuracy of (1.99099305 x 1033 grms).

It made the explorations involving solar mass total aggregates
Mt and Mtx not important. This avenue of reasoning was dropped,
and is mentioned above only to reveal how a quantal value of
±
½ Jupiter as displayed in Equations E-1 to E-4 came to be
an issue.

         OTHER MASS AGGREGATE STATES

 

 

In applying such interphasing logic to the solar system, the
study is narrowed to include only mass quantities which currently
exist; these being the Sun, and certain planets.

In the case of a bifurcated Jupiter mass, a theoretical attribute
is identified. This is where mass aggregates and resulting
gravitational relativistic effects can phase in and out (in a
continuation of certain coherent effects), through a range of
mass densities confined within a single constant radius.

A form of harmonic interphasing through a realm of masses
is definitely sensed.

In gist; a higher relativistic effect from an enhanced mass
aggregate is applied to a lower mass aggregate, such that
the resulting augmentation is lower or different than would
be expected for either the originating enhanced mass, or the
reduced mass.

This type of reasoning should only be speculative, except that
the mass augmentation which actually results when +1/2 Jupiter
and -1/2 Jupiter are involved, is already a recognized quantity,
this being mass term K, already independently seen for a mass
aggregate which is other than an effect that is expected
straight across for an enhanced or diminished sum of the Sun
plus or minus 1/2 Jupiter.

 

 

         OTHER MASS EFFECT COHERENCIES

 

 

Other mass effect coherencies seem to occur. One involves the
mass of the Earth (Me), which, when subtracted from mass MM,
yields an aggregate mass whose relativistic effect factor
(herein called Ee), which when applied to mass aggregate MM,
results in a discrete mass split which is precisely equal to
the mass of the Earth Me minus K.

This formula (as exemplified in EQ H and I below), might at first
seem tautological until further studies show that a relativistic
factor Ex for any mass aggregate (M + X) or (M - X) does not phase
in perfectly to an exact result for
(MM - (MM x Ex)) = X - Kx for
any value assumed for mass X. Only certain precise values of
± X
are seemingly phased in a coherency. For instance when:

1. X equals the mass of Earth
2. X equals the mass of Venus
3. X equals
± ½ the mass of Jupiter

The case of X being equal to ± ½  the mass of Jupiter
has already been demonstrated in Equations E-1 to E-4.

When X equals the mass of Venus, then a mass split resulting
in a discrete relativistic augmentation, also incorporates the
mass of Mars. This is shown further below in Equations Q to S.

A formal description for the interphasing state involving
the Earth is as follows:

 

EQUATION H

 

Ee=√[1 –  2G·(MM– Me)/C2·R]      Where (MM-Me) is mass MM

                                                                    minus the mass of the Earth Me.

                                                                    MM is the mass of the Sun

 

 EQUATION I

MM - [(MM + Me) x Ee] = Me - K     Where Me is the mass of Earth,
                                                                   and K is (Venus - Mars)

This formula (as exemplified in EQ I), might at first seem
exciting until it is recognized that it is rather a sort of
strange tautology.

That is, further exploration shows that a relativistic factor Ex
for any low mass aggregates in the range available for this solar
system, for instance (MM + X) or (MM - X), phases in to a seeming
predictable result where:

when Ex is determined as the relativistic effect factor
for mass MM-X (for instance using EQ H), then:

MM – [ (MM+X) x Ex ] = Xx = (X - K)

where
Xx = (X - K) results for any
reasonable value assumed for mass X.

But for higher masses (much beyond MM), the equality actually
breaks down, demonstrating that there was no tautological
equality to begin with.

A formal description for showing the breakdown is:

EQUATION J

Ee=√[1 –  2G·(MM–Me)/C2·Rx]      Where (MM-X) is mass M minus

                                                                    any other mass X, and radius

                                                                    Rx is the same for any values

                                                                    of (M-X), then:

 

EQUATION K

M - [(M) x Ex] = Kx                          And:

 

EQUATION L

M - [(M+X) x Ex] = Xx                     And:

 

EQUATION M

Xx - X = K                                       Where:

Xx + Kx = X                                And:

Xx = X - Kx                                 Where X is the original arbitrary
                                                  mass that was subtracted from M in
                                                  EQ J, and was then added to M in EQ L

 

         STRANGENESS IN A SEEMING TAUTOLOGY

 

 

This section covers general ground and seems to ramble, rather
than to leap straight ahead from one event to a next. Read if
interested.
This section concludes with information of importance
to the following section 'A Coherent Phase in This Solar System'.

The discussion resumes in earnest in PART 2 a few pages further below.

Do not be fooled by the implied authority of Equations J to M.
Equations J to M are not a perfect tautology. Even though they are
presented above as such. Instead, they are strange, in that their
results can actually vary in several ways, under the microscope
of vigorous scrutiny.

For instance terms X and Xx begin to noticeably separate for larger
values of M, for instance when M begins to assume a mass approaching
that of a black hole having radius Rx. In these higher mass regions,
the value of Kx can begin to rapidly escalate over and above any
amounts of increase given to mass M.

 

In other words Kx begins to itself take on high value
(pursuant to gravitational relativistic augmentation),
but always is less than the value of M.

The value of Kx is in fact somewhat periodic in two ways.
(Kx is said to be the mass augmentation due to the gravitational
relativistic effect of mass M acting on itself, ie. on mass M).

Firstly: the digital value of Kx is dependent almost entirely upon
the digital value of M. For example a Kx digital value ranging
from (4.21 x 1027) up to (4.79 x 1037) is found for mass M values

ranged from (1.989 x 1033) up to (1.989 x 1038), when the

confinement radius Rx is held constant at (6.96256 x 1010 cm),

through greater and greater magnitudes in the concentrations

of mass M.

Secondly: it will be seen that for every increase of M by a factor
of 10, the value of Kx increases by a power of 100 (actually just
slightly more than 100), until the Value of Kx vrs M closes suddenly
in a very rapid crunch toward unity as the value of M approaches a
last iota in becoming the mass of a black hole. The power of just
above 100 in the increases of Kx, is due to the modest increase in
the digital value of Kx identified in the previous paragraph.

At the junction at which the confinement radius Rx becomes the
same as an event horizon of a black hole, Then the augmentation Kx
vanishes from the picture, because when M is the mass of a black
hole having a radius Rx, then Kx can no longer be calculated.

Related events can be closely watched for permutations by
keeping certain parameters constant. For instance Rx is the
same constant radius, in Equations O to O-4 which follow.

Then, given the basic equation:

EQUATION O

Ex=√[1 –  2G·Mh/C2·Rx]      Where Ex is the relativistic
                                                            effect factor of a high mass Mh

                                                            having a confinement radius Rx,

                                                            and:

EQUATION O-1

M – [(Mh x Ex) = Kx 
 

But when Mbh is the mass of a black hole of radius Rx, then:

EQUATION O-2

2GMbh/C2Rx =1                   And therefore:

 

EQUATION O-3

Ex=√[1 –  2G·Mbh/C2·Rx]      Is no longer valid, since:
 

EQUATION O-4

Ex=√[1 – 1]                                 The square root of 1-1=0

                                                             is impossible.

However, in looking back to Equations J through M, where terms X
and Xx are featured, certain important distinctions can be observed
to occur for high masses M that are not yet a black hole. For instance
if variable amounts of mass M
± X are confined within the same radius Rx
so as to provide a consistent point of view via a constant Rx, then in
particular:
 

ITEM A.        If X is closer in value to the higher value M, (for
                    instance if X is  1/100th  the value of M), then Xx of
                    EQ L can be substantially lower than X, and Xx can
                    also be substantially lower than Kx.

 

ITEM B.       If X is substantially lower than the higher value
                   M, (for instance if X is 1/100000th the value of M),
                   then Xx can increase substantially above X. In fact Xx
                   approaches the value of Kx for the mass M (as will be
                   found when in using Equation K, above).

These above mentioned 'drifts' are inherent in the gravitational
relativistic arena. It was possible to see them only because
for the instances of ITEMS A and B above, the value of radius
Rx was held constant, so that the consequences of different
masses (M-X) and (M+X) through different values of M and X can
be followed in the varying results.

The above 'drifts' have been discussed here at length because
if their insights are not known, certain confusions may seem
to occur in doing high mass calculation in the denser levels
up to that of a black hole, vrs doing low mass calculations
involving values of mass M that are on par with the mass
aggregates available in this solar system.

In such low mass calculations, conditions similar to ITEM A
above are found. Except in low mass calculations for this solar
system, the value of Xx can be rather close to the value of Kx,
and Xx + Kx can be rather close to the value of X.

In fact in mass regions on par with this solar system, any difference
between X and (Xx + Kx) of Equation M above, in which the Earth mass Me
is X, is hardly discernible, so indiscernible that X and (Xx + Kx) seem
the same, (as indicated in EQ I above, where Xx would be Me - K). But X
and (Xx + Kx) are not truly identical.

Yet there are certain precise values phased in a certainty
for all values of M right up to that of a black hole.

For instance there is a condition in which Xx and Kx can
both turn out to be identical. This is as follows:

 

 

EQUATION O-5.

Ex=√[1 –  2G·(Mass)/C2·Rx]      And:
 

Mass - [(Mass) × Ex] = Kx             Then:

EQUATION O-6. (A zero result occurs in using the reciprocal 1/Ex)

Mass - [ (Mass - Kx) × (1/Ex) ] = 0    This is true for both
                                                        low mass and high mass calculations

 

         A COHERENT PHASE IN THIS SOLAR SYSTEM

 

 

In this solar system there is one precise value of X
which seems phased in a genuine coherent certainty, when
viewed through the scope of Equations J through L.

Specifically, when the mass aggregate equals MM, and X
equals the mass of Venus (Mv), the strange tautology of
Equations J through L become a seeming genuine equality,
wherein the resulting X = (Xx + Kx) mass split in relativistic
augmentations, also incorporates the mass of Mars. Specifically,
Xx is the mass of Mars.

 

 The formal description for this state is as follows:

EQUATION P

Ex=√[1 –  2G·(MM-Mv)/C2·R ]     Where (MM-Mv) is mass MM of the mass

                                                                    of the Sun minus the mass of Venus Mv.

                                                                    R is the exiting radius of the Sun.


EQUATION Q (Determines a value K)

Ek=√[1 –  2G·(MM)/C2·R ]            This is the same as EQ E, so that:

                                                                  

MM - [(MM) x Ek] = K                      Such that:

EQUATION R

MM - [(MM+Mv) x Ev]= Ma              Where Ev is the effect
                                                                   factor of EQ P above,
                                                                  and Ma is the mass of Mars, so that:

EQUATION S

Mv - Ma = K                                   In which also K + Ma = Mv
 

With Equations P to S there is established a formal second
(albeit obvious) identification for the previously noted
condition; that the relativistic augmentation (K) of the inferred
mass of the Sun MM is identical to the mass difference between
planets Venus and Mars.

 

 

 

 

 

PART

GRAVITATIONAL AND SPECIAL RELATIVITY THEORY

 

 

 

 

GENERAL INTRODUCTION for part 2 

 

 

 

 

         A COMPARISON BETWEEN GRAVITATIONAL AND SPECIAL RELATIVITY

 

 

It is traditionally thought that gravitational relativistic
effects differ in kind from special relativistic effects, in that
in special relativity, an approaching equality between a velocity
and the speed of light is theorized to lead to an escalating mass
increase which continues toward infinity as the velocity closes in
on the speed of light. In this view of special relativity, there is
only the one ultimate source of the effect, this being the varying
velocity. The velocity of light can never be reached in an onrush
of mobile matter, due to the infinity in mass which would result.

In gravitational relativity, at least two source parameters are
variable. Specifically, there is a given mass and a given radius,
each of which can change independently, and so can ultimately
combine in combinations where various equalities exist. For
instance a radius of a mass can vary depending on ambient mass
density, for example between a gas such as hydrogen, and a solid
such as gold.

But for any mass of sufficient size, gravitational collapse
can theoretically lead to a black hole.

 

1.        In a mathematical convenience, more mass added to the same
radius can produce the collapse. In this sense there are
equalities involved. The equalities are when the mass's
existing radius is normal and when the same radius is the
boundary of a mass's black hole event horizon.


1A.      A sort of double flip flop occurs at this boundary. If
extended beyond this equality, any increase in mass in the
black hole results in an increase in radius (rather than
decrease in radius). But conversely a decrease in a black
hole's radius results from a decrease in mass, ie., if the
mass does not decrease the radius does not decrease).
 

2.        This stable equality can exist because both the input terms
for mass, and confining radius, are variable. For instance a
low density gas cloud can have a high mass but large radius,
resulting in very weak relativistic consequences, whereas
the same mass concentrated in a very small area can have
substantial relativistic consequences.

 

3.        Further, mass can be removed or added within the same radius,
dramatically changing the aggregate's relativistic components.
Conversely the same mass can be drawn closer together or spun
farther apart, thus changing the radius, thus again dramatically
effecting the aggregate's relativistic components.

 

4.         A similar though not identical property can occur in less
dynamic realms, for instance in mass aggregates which are the
size of the Sun. In this case extra mass in the same radius
(the Sun's radius) can for instance produce a relativistic
factor E which when imaginarily applied to another mass
aggregate, can produce a Kx augmentation which is otherwise
gained from a different mass aggregate.

 

In the case of the solar system, the Sun's radius and resident mass
aggregate are not the total quantities involved in the aggregate's
relativistic components. Planet masses in the bodies of Jupiter,
Venus, and Mars, are also involved. It means that the relativistic
components include something which is manifesting in an external-
ization of the effect, occurring at long distances from the field
which is generating the relativistic effect. What these external-
izing influences are is not immediately known. Nonetheless the
evidence of their existence is unmistakable.

The evidence in fact does infer that a mass augmentation is
present in a field of gravity. In truth, the evidence does not
immediately prove whether the mass augmentation is a relativistic
increase, or decrease, on an original mass. The equations herein
shown have assumed that the augmentation is an increase.

The evidence on its own raises questions which are not answered
at all. For instance, how come the particular planet orbits for
Jupiter, Venus, Mars, and also the Earth? And what linkages
might angular momentum and/or planetary spin have, if any? Etc.

The gist of Part 2 is not in the speculation, but in certain
understandable exactitudes which do occur. These exactitudes
are particularly easy to see in high mass ranges closing in
right on black hole masses, and so can be extrapolated back to
less easily seen low mass effects in gravitational relativity.

What is more important, is that a direct tie-in between
gravitational and special relativity becomes obvious.

 

 

 

 

A UNISON BETWEEN GRAVITATIONAL AND SPECIAL RELATIVITY

 

 

There is a direct connection between the effects of gravitational
relativity, and special relativity, to the extent that; given a
gravitational mass and its confining radius (so that its mass
augmentation effect on original gravitational mass is known),
the same quantity in mass augmentation can be determined for
special relativity, according to the mass increase gained by
the same original mass if traveling at some portion of the
speed of light.

Specifically, the gravitational relativity equation provides
a term which allows that the exact velocity of the mass if
moving can be perfectly known, in terms of special relativity.

The predictability between the two relativities is, as said,
exact. That is, the gravitational relativity effect factor from
gravity is related to the proportion by which the speed of light
is reduced, so that the same mass travelling at the stated velocity
(predictably reduced below the speed of light) will experience a
special relativity effect on its mass identical to the effect on
its mass experienced by gravitational relativity.

(This assumes that gravitational relativity indeed has
an effect on a gravitational mass, such that there is for
instance an augmentive relativistic gain in the mass itself
when the mass is standing still. This mass gain by gravitational
relativity, and by the instantly predicted velocity in special
relativity, are identical amounts of gain).

 

 

THE GRAVITY - SPECIAL RELATIVITY CONNECTION IN DETAIL

 

The connection between gravitational and special relativity is
not quite so naive as first suggested above, when it comes to
actually working out a connection between a given gravitational
mass and its special relativistic equivalent.

To begin with, a certain parameter must be determined for the
gravitational effect. To wit, the radius involved is a control
parameter. Given the radius, the amount of mass needed to have
a black hole confined in the radius as an event horizon, is
determined. (A black hole silent partner for the given mass,
so to speak). The ratio of the partner black hole mass, over
the mass in question (see equation T below), supplies an essential term.

Let's call this term Nx. Let's call the black hole silent
partner mass equivalent Mbh. And let's call the original
given mass M. The ratio of Mbh divided by M, is our ratio Nx.

The speed of light C is divided by the square root of Nx, to
give a velocity that is less than C. Lets call this velocity
Vx. If mass M is traveling at velocity (Vx), then mass M will
experience the same gain in rest mass enhancement via special
relativity, as is otherwise gained when the mass is standing
still but is augmented by its own gravitational relativity.

In a further comment, in the scenes of gravitational relativity,
it turns out that ratio Nx (gained as the ratio of a given mass
divided into its black hole silent partner mass) is a different
view of the relativistic effect factor Ex, which is gained by
calculating the given mass's gravitational relativistic effect.
This puzzling statement has an easy explanation.

For a fact, when:

EQUATION T

Mbh/M = Nx                        Then relativistic effect Ex is:

EQUATION T-1

Ex=√[1 –  1/Nx ]              Gravitational relativistic effect Ex

                                                     is calculated from ratio (Mbh/M), when

                                                      the mass of black hole silent partner Mbh

                                                     is calculated from the radius of M, by:

EQUATION T-2

Mbh = C2R/2G                  As in:

 

EQUATION T-3

Ex  =

 

 

 

 

 

 

 

 

 

1

     

 

1

 

 

 

 

     

 

 

C2·R

 

 

 

 

 

 

 

2G

 

 

 

 

 

 

 

M

 

 

 

 

         A COMPARISON BETWEEN GRAVITATIONAL AND SPECIAL RELATIVITY

 

 

In Equations U through X which follow:

 

(Eg) :

is the effect (in gravity) for a mass M in gravitational relativity

 

(Es) :

 is the effect (in special relativity) for mass M in
motion at a significant velocity in special relativity

 

(Mbh) :

 is a black hole mass from a given radius Rx, as
calculated in EQ V below or EQ T-2 above. Mbh
is the silent partner mass for any given mass M

 

(Nx) :

 is the ratio of the black hole mass Mbh,
divided by the given mass M

 

 

EQUATION U

Eg=√[1 –  2G·M/C2·R ]            

EQUATION U-1

Eg=√[1 –  V2/C2·R ]            

 

EQUATION U-2

Gravity relativity                            Bare bone version

Eg=√[1 –  1/Mbh/M ]           =√[1 –  1/Nx ]          

 

EQUATION U-3 

Special relativity                               Bare bone version

Es=√[1 –  [C/√Nx]2/C2 ]           =√[1 –  1/Nx ]          

 

As seen in Equations U-2 and U-3, a fundamental statement for both
special and gravitational relativity are indistinguishable when given
in a Bare bones manner containing term 1/Nx. This is not false, but
misleading, in that term Nx is found from the ratio Mbx/M of EQ U-2.
In the Bare bones version of EQ U-3, term Nx cannot reveal what the
velocity that mass M is moving at in order to have a relativistic
effect factor Es in EQ U-3 that is equal to Eg in EQ U-2.

This is by no means a critical shortcoming. Without knowing term Nx,
the velocity of a moving M can nevertheless be determined directly,
if a substitution is made for term Nx in EQ U-3. This substitution
cannot be easily shown in the full equation in a typed manuscript
such as this. However, the factor to be substituted in EQ U-3 is
easily shown. It is Term 1 shown below in EQ U-4. Term 2 of EQ U-4
is taken straight from EQ U-3.
 

EQUATION U-3 

                    

                     Term 1                             Term 2              Term 3

                                                                                      an exact velocity V

Substitute    [C/√(Mbh/M)]/C  For  [C/√Nx]/C       = V/C

 

Term 1 of EQ U-4 gives the exact velocity V (as used in EQ X
below), at which mass M must be moving, in order to have a special
relativistic effect (Es) identical to a gravitational relativistic
effect (Eg).

In this connective equality between relativities, identical augmenting
effects on the moving rest mass (Mass)(1/Es) of special relativity, and
aggregate mass (Mass)(1/Eg) of gravitational relativity, are gained for
an original mass when moving (special relativity) and when standing still
(gravitational relativity).

Inter-combinant mathematics between the two modes of relativity
have so far been shown strictly for the effect of one mode (gravity)
on the other mode (motion). There are other potentials. For example,
would the motion's effect increment upon the gravity effect. If this
is so, than Equations T to X need to be expanded to include modifying
terms giving the velocity needed when other effects on mass are
considered. Such potential views in the mathematics are not herein
pursued.

 

 

 

         A Support equation for gravitational relativity follows next

 

 

EQUATION V

 

(Mbh) can be determined from the gravitational
relativistic effect (Eg). Given a calculated
effect (Eg), as determined in EQ U above, then:

Mbh = M × [ 1/( 1-(Eg)2 ) ]

 

EQUATION V-1   However:

 [ 1/(1-(Eg)2) ]                 also equals   [1 –  1/Nx ]

 

EQUATION V-2   So that EQ V simplifies to:

M ×  Mbh/M =  M × Nx     So that         Nx = Mbh/M

(The result of Equations V is obvious for very high masses,
for instance for masses approaching that of a black hole. However,
in lower mass calculations (such as for gravitational effects for
masses found in the solar system), there is an intrinsic truncation
eroding the accuracy, leading to imprecise seeming solutions for
Equations V to V-2).

The simplification of EQ V into EQ V-2 has been shown, because
soon we want to watch very closely certain effects involving Nx,
when Equations T through U-4 are used to explore particular aspects
of both gravity and special relativity modes in masses which work
backwards starting at the limit of black hole masses.

As seen in Equations V to V-2, term Nx can be made to have an
overly complex look (EQ T-3), or overly simplistic look (EQ V-2).
The general confusing looks vanish when certain exact values are
attached to ratio Nx.

In an exploration which follows after the next section, a
constant number already well known as the Golden Harmonic
Ratio, becomes apparent as a term of fundamental importance
when things are looked at through a certain point of view.

         Summary equations for the two modes of relativity follow next

 

 

EQUATION W     Basic Gravitational relativity equation

Eg=√[1 –  2G·(Mass)/C2·R]      EQ W is the  

                                                   same as EQ C further above
 

(Gravitational effect Eg is known to slow time in the
vicinity of a (Mass) which is generating effect Eg).

 

EQUATION W-1

(Mass) - ((Mass) x Eg) = Kx              Where Kx is an augmentation
                                                       of (Mass) by gravitational
                                                       relativistic effect Eg

EQUATION X         Basic special relativity equation

Ex=√[1 –  V2/C2]      Many text books cite a greek letter for effect

                                             Es, and for ratio V2/C2

Effect 1/Es increases the mass. Es decreases the
radius, and slows time for an entity moving at
velocity V relative to the speed of light C

EQUATION X-1    Basic black hole mass calculation

 

(Mbh) of EQ X-1 is the mass of a black hole mass as gained
when radius R is the event horizon (Schwarzschild radius)
of the black hole, whose mass is calculated as:

Mbh = C2R/2G                 Finding the mass (Mbh) needed for

                                         a black hole whose Schwarzschild

                                         radius is given as R. EQ X-1 is

                                         the same as EQ 5 of APPENDIX B below

 

INTERPRETATIONS

It is worth noting that Equations T through X are true for an
existing mass. Specifically, there is a given (existing) gravitational
mass M which has an augmentation (Kx) included. The augmentation (Kx)
is easily found in its exact amount (by Equation W-1). How fast does
the existing (Mass) have to be in motion to experience the same
degree of augmentation as Kx via special relativity? This simple
question has been addressed by Equations T to U-4.

 

However otherwise the equations of gravitational relativity theory
lead to this, (which is the same as saying the energy equivalent
in forward escaping light is pulled backward (or bent) by powerful
gravity at the same rate of acceleration as the forward velocity C
of the light), from Term 1 of Equation U-4 above it is clear that
at the mass limit of a black hole, the ratio 1/Nx of the black hole
mass Mbh to aggregate mass M, is equal to 1.


And so in Term 2 of Equation U-4 the ratio of the speed of light C
divided by the root of Nx (as in C/√Nx) will also be equal to 1.

Special relativistics then will no longer have effect, as in:

EQUATION X-2

 

 

Term 1

 

 

 

Term 2

 

 

Term 3

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

Exact

Velocity

 

 

 

 

 

 

 

C

 

 

 

 

 

 

C

 

 

 

 

 

 

 

For

1

=

C

=

1

 

Mbh

 

 

 

 

 

 

 

C

 

 

 

 

Mbh

 

 

 

 

C

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

C

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

However, the situation here is actually more deceptive.

For instance how can the rest mass of a relativistically moving mass
aggregate increase toward infinity as its velocity ratio V/C  from
(C/Nx divided by C in EQ U-5) approaches 1, to keep in step with a
stationary gravitational mass aggregate approaching its black hole
mass limit Mbh as defined in EQ X-1 above, according to the aggregate
mass's radius R ?

This is no question to be sneezed at.

It implies an idealized stable situation, where A = B. That is,
the ratio of Mbh/M  as A, equals the ratio of velocities V/C  as B,
such that masses approaching infinity should be possible, as ratio
Mbh/M  approaches 1.

However, the wrinkle is that mass M can never exceed mass
Mbh. Not via any mass increases gained by higher and higher
gravitational relativistic effects on mass M. And therefore
extreme mass enhancements in special relativity as velocity V
over C approaches 1, are not possible, if velocity V is gained
as an Nx factor directly from the ratio of Mbh/M .

 

 

THE CONUNDRUM

 

In the real world, the situation is in no way idealized. For
instance masses approaching infinity should begin to appear, as
the equivalent mass aggregate M begins to home in on the final
iotas before becoming a black hole, if the A = B relationship
is in all ways exact.

But, the contingency of a mass said to approach infinity in the
special relativity side is not proof that mass infinities can be
achieved by M plus mass augmentation Kx at higher and higher
plateaus of gravitational relativistic mass effect.

How might this conundrum be explored as an intellectual exercise?

If the confining radius of a mass aggregate itself is being
relativistically contracted by effects of the mass's gravity,
then the real world situation is very different than the idealized
version. For instance, increasingly less mass is required to
aggregate in a diminishing radius to form a black hole.

It would now seem that the mass aggregate could bleed away toward
nothing as the gravity increases in tune with a relativistically
diminishing (contracted) confining radius.

What would prevent this is two things.

First, the mass aggregate increases in relativistic proportion
to the decrease in radius. Since both terms are found in the
same equation, as in:

EQUATION Y

Eg=√[1 –  2G·(Mass)(1/Eg)/C2·R(Eg)]      Mass is increased by 1/Eg 

                                                                   Radius is decreased by Eg

which results in the ratio portion (Mass)(1/Eg)/R(Eg)
being increased by the square of the reciprocal of Eg.

In a second prevention, if 2G (twice the gravitational constant) is
decreased by Eg while the square of the speed of light is increased
by 1/Eg, as in Equation Y-1:

 

EQUATION Y-1

Eg=√[1 –  2G·(Eg)(Mass)/C2·(1/Eg)·R]      Gravity is decreased by Eg,

                                                                                    is increased by 1/Eg

then the ratio portion (2G)(Eg) / C2(1/Eg)
is decreased by the square of Eg.

In which case all relativistic augmentations found in Equations
Y and Y-1 internally cancel each other, as in Equation Y-2:

 

EQUATION Y-2

Eg=√[1 –  2G(Eg)(Mass)(1/Eg)/C2·(1/Eg)·R(Eg)]     

and the net internal effect is again simply
2G (Mass) / C2R, as in Equation W above.

But this type of intellectual exercise does not solve
the above posed conundrum. The conundrum's answer is
introduced immediately below.

 

 

 

 

THE GOLDEN HARMONIC RATIO IN RELATIVITY THEORY.
A CRITICAL LIMIT IN THE FOUNDATION OF GRAVITATIONAL RELATIVITY

 

 

 

GENERAL INTRODUCTION for part 3 

 

 

 

 

                        TABLE 4

 

KEY TERMS

Mbh  

-

Mass of a black hole, having radius Rbh

Mo

-

An original mass (before mass augmentation due to gravitational relativity)

Ko

-

Mass augmented upon mass Mo due to
gravitational relativity

M

-

An existing mass, which includes: Mo + Ko

Mc

-

 A Critical Mass Limit, where Mc is an Mo which is less than Mbh by precisely the Golden Harmonic Ratio

Rbh

An event horizon radius for black hole Mbh, and for other masses such as Mo, M, and Mc which are evaluated with the same Rbh radius but are not yet at the black hole mass limit.

 

 

 

 

                      TABLE 4 Continued

 

1/Ng  

-

 Ratio  Mbh/Mc = 1/Ng when Mc = Mo, as when: Mbh/Mo = 1/Nx
 

GH

-

Golden Harmonic Ratio 1.61803399, also called Golden Ratio, having a digital value equal to 1/2 the square root of 5, plus 0.5, as in:
1.1603398875 + .5 = 1.61803398875

 

Vc

-

 A critical limit velocity in special relativity, where the ratio C/Vc is equal to the square root of the Golden Harmonic ratio GH = 1.61803398875

 

 

 

 

          FUNCTIONAL INTERPHASE BETWEEN
          GRAVITATIONAL AND SPECIAL RELATIVITY

 

 

The thing about speculations is that many words can be used
to discuss a point which has no convincing answer. Whereas
a simple equation can state it all for a self evident truth.

However, the simple equation may be obvious to only
the soul who wrote it. For others, the simple equation
may need elaborate support such as explanation and
interpretation.

The following sets forth a question which begs an answer.
The answer being self evident is then quickly stated. But
the stating is accompanied by explanation and interpretation.

QUESTION

 

One important question which comes immediately to mind (already
asked further above in 'The Conundrum') is how can the rest mass of
a relativistically moving mass aggregate increase toward infinity as
its velocity ratio V/C from EQ U-4 approaches 1, to keep in step with
a stationary gravitational mass aggregate which is approaching its
black hole mass limit?

 

ANSWER

 

The answer is that a gravitational mass can only increase to a
certain limit, reached before the black hole mass. At this reached
limit, the increase in gravitational relativistic augmentation on
the mass, raises the overall mass in a final bump to the black hole
limit. The final range closing in on the black hole limit is bypassed
by the bump.

 

 

INTERPRETATION

 

The problem is that the conundrum is only apparent and not real;
that: as a mass aggregate rapidly approaches its black hole limit,
the ensuing special relativity mass increase counterpart will rapidly
begin to climb toward infinity, and such an infinite mass is not
possible in the sense of real events.

For instance, assuming the conundrum is real, in the following
thoughts let Rbh be a given radius. Let's say a mass aggregate M
of radius Rbh is at 99% of the Mbh black hole mass limit for radius
Rbh. The gravitational relativistic effect (Eg) is roughly about
Eg = .09950, which translates into a special relativistic mass
enhancement effect of roughly (10.049 x M) on the mass travelling
at roughly (root 99%) of the speed of light).

 

Effect Es = 10.049 is reciprocally equivalent to effect Eg = .09950.

The problem here is that the special relativistic enhancement
on the mass will be roughly 10 times the black hole limit for
the mass in question.

The problem here is also that if mass M is increased by a
gravitational relativistic effect Eg of 10.049, then the
resulting augmented mass will exceed its own black hole limit
by a factor of roughly 10 times.

How, then, does an aggregate mass M of radius Rbh increase
only to a black hole mass Mbh of radius Rbh, in keeping with
a committed tie-in to special relativity, without the moving
mass M impossibly increasing to infinity as the aggregate
mass M closes in on Mbh, and without the stationary mass
increasing wildly above its own black hole limit due to
its own gravitational relativity?

The question is a thought balloon which seems to go in
several directions. But actually has a unique answer.

 

EXPLANATION

 

In a fundamental point of view, events are explored from
the outlook of an original mass, which is augmented to
become an apparent mass.

Specifically, let an original mass Mo (before mass augmentation) be
used in an Mbh/Mo ratio, to give ratio term 1/Ng (instead of 1/Nx).
And let velocity (C divided by the root of Ng) be the velocity the
original mass is travelling in special relativity, to have the same
enhancing effect on Mo as would be found when the gravitational
relativity effect augments mass Mo.
 

 

THE GOLDEN HARMONIC RATIO - A CRITICAL LIMIT

 

When ratio Ng is equal to the Golden Harmonic Ratio,
then several striking things happen. The Golden Harmonic
Ratio is 1.6180339. It is typically given as a number quantity
from (1/2 of root 5, plus .5).

Let the Golden Harmonic Ratio be GH. And so let Ng = GH.

 

 

THE CRITICAL LIMIT in gravitational relativity

 

When Mbh/Mo is GH, a vital event occurs. The gravitational
effect Eg precisely turns out to be 1/GH (the reciprocal of
the Golden Harmonic Ratio).

And so mass (Mo x 1/Eg) = (Mo x 1/GH), which
precisely turns out to be mass Mbh. Effectively,
mass Mo leaps uphill to become mass Mbh in one
final single bump.

This is a box, where one thing specifically yields another. In
interpretation, a mass augmentation (Eg) on an original mass Mo,
raises the quantity of the original mass Mo to that of a black
hole mass Mbh, when ratio Ng = Mbh/Mo is precisely the Golden
Harmonic ratio GH.

In which case, in special relativity, when the original mass
Mo is moving at a velocity V which is root GH less than the
speed of light, the special relativistic effect Es increases
mass Mo to mass Mbh in a final single bump. In which case mass
Mbh becomes a black hole and disappears from sight, relative
to a stationary observer watching the mass move.

There is a locked in equality here. Explicitly, Mbh/GH is a
critical limit preceding mass Mbh, at which an original mass
Mo is raised to the black hole limit Mbh by the mass effect
of its own gravitational relativity. Let Mc be the critical
mass limit.

Effectively, it establishes that if gravitational relativity
includes a mass augmentation effect, the original mass cannot
exceed the critical mass limit Mc. And so the original mass can
never be the same as a black hole mass, or even a fraction less
than a black hole mass, since the black hole mass includes an
original mass Mo at the critical mass limit Mc, raised to Mbh
through a quanta bump equal to the Golden Ratio GH.

In this locked in state, Mbh - Mc = Ko, where Ko is the
actual mass augmentation, the same as is otherwise said to
be Kx, except in this instance, Ko is fundamentally related
to the Golden Ratio GH. In exactitude,
Ko = Mbh - (Mbh/GH).

It means that when the critical mass limit Mc is reached prior
to a black hole, the original mass Mo is augmented by effect 1/Eg
to become a black hole equivalent, and no more mass can confine
in the same radius Rbh. (More original mass added would serve to
increase the confining radius to greater than Rbh).

As already said, the Mc critical mass limit
(for radius Rbh) is simply (Mbh/GH), where
(GH) is the Golden Harmonic Ratio.

 

THE CRITICAL LIMIT in special relativity

 

It also means that in special relativity, when the critical
mass Mc is a rest mass in motion at a velocity equal to C
divided by the square root of GH, the original rest mass
Mc expands via 1/Es in a single bump to a mass value where
it also becomes a synonymous black hole of mass Mbh.

In consequence there never is a condition where the original
mass Mo in special relativity expands toward infinity as
mass Mo closes in on mass Mbh in gravitational relativity,
because the convergence in gravitational relativity for an
original mass Mo closes off completely at the critical mass
limit Mc, when Mc is less than mass Mbh by a ratio equal
to GH. This is a simple and elegant exclusion clause here
in the realms of the two modes of relativity, gravitational
and special.

EQUATION Z

In gravitational relativity, the critical limit is:

Mo = Mc = Mbh/GH

Where: Eg is the gravitational relativistic effect of Mc

Such that:
Eg = 1/GH

And
Mbh = Mc + Ko, where Ko = (Mc x 1/Eg) - Mc

And also:
Mc x 1/Eg = Mk, and Mk - Mc = Ko

And so:
Mbh = Mc x 1/Eg = Mk

Only when:
Mc = Mbh/GH

So that:
Mbh = Mk

 

Where Mk an apparent mass equals its own black hole silent partner
mass equivalent. This physical condition occurs because the Golden
Ratio GH constantly defines Mo as Mbh/GH.

EQUATION Z-1

In special relativity, there is a companion critical
velocity limit Vc for velocity V, where Vc is the speed
of light divided by the square root of the Golden Harmonic,
such that a critical velocity limit Vc constantly exists
for mass Mc, when C is the speed of light, as in:

Vc = (C/GH) ;

where Vc is actually:

Vc = [C/(Mbh/Mc)] or also (C/GH)

when: Mc = Mbh/GH or also GH = Mbh/Mc
so that when: Mc is traveling at velocity Vc
the special relativity effect is: Es
and the special relativity effect 1/Es increases
rest mass Mc to black hole mass Mbh in a bump
because Eg is equivalent to 1/GH.

 

                                           A TEST CASE:                           
          GOLDEN HARMONIC RATIO IN THE TWO MODES OF RELATIVITY

 

Let's look at the critical limit situation in more detail.

An apparent mass aggregate Mk contains an original mass, plus
an augmentation in mass due to gravitational relativity. And
so let the originating mass be Mo, the augmenting mass be Ko,
and the resulting mass be Mk. And therefore:

For Gravity relativity

EQUATION Z-2

Eg=√[1 –  2G·Mo)/C2·R]      Mo is an original mass

                                                           before augmentation,

EQUATION Z-3

(Mo x 1/Eg) – Mo = Ko          Ko is the mass augmentation
                                                        on Mo, due to effect 1/Eg

EQUATION Z-4

Mo + Ko = Mk                        Mk is the measured (apparent)
                                                         mass, consisting of original
                                                         plus augmentive masses

EQUATION Z-5
When

Mo = Mc = Mk/GH                          Where Mc is a critical mass
                                                                    value for original mass Mo

then:

Eg=√[1 –  (2G·Mk/GH)/C2·R]      Mk is black hole mass with

                                                                    horizon radius Rbh, and GH is

                                                                    the Golden Harmonic Ratio equal

                                                                    Rbh to the number 1.61803398875

EQUATION Z-5-1

Eg=√[1 –  (2G·Mbh/Ng)/C2·R bh]  Mass Mbh is the same as mass

                                                                    aggregate Mk.

                                                                    Ng is ratio Nx when the value

                                                                    of Nx is GH, which is the

                                                                    Golden Harmonic Ratio.

EQUATION Z-6

With digits substituted for GH, then:

Eg=0.61803398875=√[1 –  (2G·Mbh/1.61803398875)/C2·R bh] = 1/1.61803398875  

 

EQUATION Z-7
because:

1/Nx=√[1 –  1/Nx]             When and only when Nx = GH.

                                                      The Golden Ratio contains

                                                      this self appreciating

                                                      mathematical property.

and so:

1/GH=√[1 –  1/GH]             GH is the Golden Ratio

                                                       1.61803398875

 

 

For Special relativity

EQUATION Z-8

Es=[1 –  (C/√Nx)2/C2] =[1 –  (VC)2/C2] 

EQUATION Z-9

Es=[1 –  (C/√GH)2/C2] =[1 –  (VC)2/C2] 

EQUATION Z-9-A   And so:
 

(Mc x 1/Es) = (Mc x GH) = Mbh, because (Es = 1/GH)

when 1/Es is the special relativitistic effect on
mass Mc which is moving at velocity Vc of EQ Z-9

EQUATION Z-10      As in:

0.61803398875=√[1 –  (C/√1.61803398875)2/C2]

       FOR SPECIAL RELATIVITY EFFECT ON BOTH MASS AND RADIUS

 

There is yet another factor to consider. In special relativity
the radius of a mass contracts in reciprocal proportion to the
enhancement of mass. In this regard, when the radius is contracted,
less mass will be required to form a black hole in the relativist-
ically reduced radius.

How does this effect the status of the critical limit Mc,
where the original mass Mo is the black hole mass divided
by the Golden Ratio?

Specifically, what mass will now form the black hole,
when the original mass's radius is concomitantly reduced
by special relativity's effect?

The new mass is easy to find.

EQ Z-9 is abruptly rewritten to accommodate both a reduction in
radius, and expansion in mass, upon original (critical) mass Mc.
The correct velocity for mass Mc can be labelled as (Vbh), as in
'Velocity for black hole', and is easy to find. It turns out to be:

Vbh = (C/GH)                    Given as:

EQUATION Z-11

Es=[1 –  (C/GH)2/C2] =[1 –  (Vbh)2/C2] 

 

Es turns out to be the reciprocal of the square root
of the Golden Harmonic. That is; Es = (1/√GH).

It means that when a mass Mc is physically moving at velocity
Vbh relative to a stationary observer, its radius Rbh contracts
by (1/√GH), as its rest mass Mc expands by (√GH), with the result
that a new black hole is formed, having a lesser mass equal to
(Mc x √GH), and a lesser radius equal to (Rbh x 1/√GH).

As already said, this occurs when velocity Vbh is equal
to the speed of light divided by the Golden Harmonic Ratio.

The new mass can be labelled as Mbh–, which is less than the
gravitational black hole mass Mbh, by a factor of √GH. As already
indicated, Mbh/Mc = GH, but the special relativistic mass result
Mbh– is not the same as Mbh. There is a series:

EQUATION Z-12

Mc x √GH = Mbh–  x  √GH = Mbh

It means that a visible mass cannot expand to infinity,
because velocities can approach but can never reach the speed
of light, due to built in limiting factors. This statement
is true specifically for visible masses.

For instance, the maximum velocity possible for mass Mc is Vbh
which is C/GH, but this is only when the original mass Mo is at
the critical mass limit Mc which is a black hole mass Mbh divided
by GH. Whereupon the mass becomes a new black hole of mass Mbh
and disappears from view, relative to a stationary observer.

The ratio C/GH is (C/1.61803398875)

(The preceding does not take into account any effect that
gravity might have to relativistically reduce the radius of the
mass causing the gravity's relativistic effect. It is realized
that if a reduction in gravitational radius is also needed as a
key term, than the parameters of the critical mass limit Mc regards
the black hole final limit Mbh, will adjust accordingly, as will
the exact factors related to the Golden Harmonic Ratio).

(The question of such possible adjusting is not addressed in
this disclosure, whose prime intention is to simply show that
certain critical limits and equalities do synonymously exist
in the domains of gravitational and special relativity. And
that the Golden Harmonic Ratio is a fundamental primary term).

A REMARK


The Golden Ratio was not a term pulled with a sleazy wink from
a magician's hat to fit an idea. The Golden Ratio turned out
to be a resulting term that provided a theory; whose gist is
as follows:

How can a limiting velocity (thus a universal barrier to infinite
expansion of visible mass relative to a stationary observer), be
determined for any visible mass, in special relativity?

The answer to this is straight forward and demonstrates that
a visible mass can never expand to infinity. A discussion
regards this answer begins further below under:

'Special Relativistic Effects on any Mass and Radius'.

       SUPPLEMENTAL REMARKS

 

The following remarks are included to complete the discussion
regards relativity theories and the Golden Harmonic Ratio. These
supplemental remarks cover the subject of how the Golden Ratio
was found to be a constant in critical limit situations.

The remarks discuss the issue from firstly; effects on the critical
mass only; and secondly for effects on the critical mass and radius.

Golden Harmonic Relativistic Effects on Mass Only

How was the Golden Harmonic found to be the critical
ratio factor Ng for Nx in Equations Z-5 and Z-5-1 ?

A value of (square root of 2) was first tried for Nx, yielding
a mass augmentation result (1/Eg x Mo), which was greater
than mass Mbh, when root 2 for Nx was ratio (
Mbh/Mo = Nx).

In intuitional trial and error, an Nx value arbitrarily
selected as 1.8 was next tried. It yielded an (1/Eg x Mo)
value which was slightly less than mass Mbh.

So the two Nx values were averaged as in 1/2(√2 + 1.8)
to yield a value of 1.608. Since this number was close to a
known number (1.61803398875), this known number was tried to
see how close the Es result (1/Es  x Mo) came to Mbh, using
this familiar number as Nx for a point of reference.

It turned out that 1.61803398875 happened to be the very
term wanted, because the result was perfect. This fast
found number was given the label GH.

When GH was Nx, then
(1/Es x Mo) = Mbh.

And so this particular Nx was
labeled Ng (for Golden Ratio).

And Mo was understood to be
the same value as mass Mc.

Equations Z-6 and Z-7 show why Ng is a constant. The
set of Equations Z to Z-10 followed as a consequence
of knowing this.

Golden Harmonic Relativistic Effects on Mass and Radius

 

But Equations Z to Z-10 consider only the special relativistic
effect on mass, and left unanswered another question which was:

'What modifications would occur in the parameters of
mass when the radius of the mass is also conjointly
changed by special relativity effects'.

The answer to this was also quickly forthcoming, but
in hindsight seems to reflect a very fortuitous guess.

Trial and error was started again. A velocity was needed,
to determine at what rate mass Mc would be travelling to
relativistically increase to mass Mbh-, when radius Rbh
of mass Mc was conjointly contracted to radius Rbh-.
In this thought balloon, Mbh- and Rbh- would be the
parameters forming a new black hole when mass Mo was
travelling at sufficient high velocity.

 

At this point the rate of joint contraction on mass Mbh
and radius Rbh was not known. And neither was the velocity.

The intention was to find what term Nx is
divided into C to yield the significant velocity.

In a remarkably lucky guess, the first Nx
term tried was GH itself, (in EQ Z-11).

To begin, radius Rbh was modified by (Es × Rbh) as gained
from (EQ Z-11) with Nx equal to GH in the ratio C/GH, to give
contracted radius Rbh-. Then, using EQ 5 of APPENDIX B below
to find the mass of a black hole formed in radius (Es × Rbh-),
a new mass Mbh- was the result. It turned out that the ratios
of masses (Mbh/Mbh-) and (Mbh-/Mc) both equaled the square
root of ratio GH.

It had thus been found that when (C/GH = Vbh), then
EQ Z-11 yielded the square root of GH as the Es value.

The result is that with Es equaling the reciprocal of the
square root of the Golden Ratio, when Rbh is multiplied by
Es to yield radius Rbh-, and mass Mc is multiplied by the
reciprocal of Es to yield mass Mbh-, then radius Rbh- and
mass Mbh- are the correct parameters to form a new black
hole from the special relativity effects on both mass Mc
and radius Rbh, when Mc is travelling at a (C/GH) velocity.

How was this verified ?

 

The 'dual effect' event was easily
verified by the following:

 

A.     Radius Rbh- was found from radius Rbh,
        by using the Es effect of EQ Z-11 in:

Rbh x Es = Rbh-

B.     Using radius Rbh- to find mass Mbh- in:

 

Mbh- = C2Rbh-/2G                  Finding mass Mbh- needed for a

                                               black hole whose Schwarzschild

                                               radius is given as Rbh-

C.   Mbh- turned out to be mass  Mbh/(1/√GH)
      when effect Es (of EQ Z-11) was 1/GH.

D.   It meant mass Mbh- and radius Rbh- form a new black hole,
      which is less than a black hole of mass Mbh and radius Rbh,
      by a factor of the square root of the Golden Ratio for
      both Mbh- and Rbh-.

E.   This is true when mass Mc is travelling in special
      relativity, at a reduced velocity Vbh, as gained
      from EQ Z-11.

F.   The synonymous special relativistic 'dual effect' event
      for a gravitational relativistic event at the critical
      mass limit Mc, is gained by using term Nb = GH (as used
      in EQ Z-5-1), to find velocity Vbh in EQ Z-11.

 

SPECIAL RELATIVISTIC EFFECTS ON ANY MASS AND RADIUS

 

 

Only certain critical limit cases
(for masses Mo and Mc = black hole mass Mbh/GH)
have so far been considered.

 

QUESTIONS

What if instead of Mc there is given any general mass Mo,
having a radius said to be Ro. Would there still be critical
limits involving Golden Harmonic factors that would limit a
general test case to a state that is less than infinite mass,
at a velocity which can never tightly approach the speed of light?

For that matter are other, more general, limits possible,
besides those already shown to be related to the Golden Ratio?

And if general limits are in the fabrics of physics, how to
determine them, given a general mass quantity that to begin
with is not known to be related to anything else, especially
when it is NOT RELATED to the Golden Ratio ?

 

ANSWER

This questioning also came to a quick answer, although
the finding of the answer was not all that straightforward.

The answer demonstrates that any visible mass travelling at a
relativistic velocity in special relativity, reaches a limiting
barrier, beyond which the mass does not visibly increase any further
toward infinity, and its velocity closes no further toward equaling
the speed of light.
 

The first insight is that any entity (in its most general
sense) comprises a mass and a radius. With mass is some
gravity. For instance a typical Sun sized star is an
ideal test case entity.

For example, the ratio of the Sun's existing mass M over
the Sun's existing radius R is its (mass/radius) ratio,
ie., M/R

(Note that Mo would be the Sun's original mass before any
mass augmentation effect due to gravitational relativity.
The Sun's original mass Mo is less than its existing
mass M, since the existing mass as physically measured
is assumed to include a mass augmentation upon mass Mo).

The Sun's black hole Mbh mass (silent partner mass)
is easily found by:

EQUATION Z-13

Mbh = C2R/2G                  Finding mass Mbh needed for a

                                          black hole whose Schwarzschild

                                          radius is given as R when

                                          R is the radius of the Sun

so that another ratio is found, this being (Mbh/R)
which is the Sun's (black hole mass/radius) ratio.

But actually, term Mbh of EQ Z-13 is worthless. What
we really want to find is what (Mbh-/R-) ratio forms a
black hole out of the original Mo/R parameters, when Mo is
travelling at increasingly faster velocities approaching the
speed of light.

We need a comparative term, to study any differences between
the Sun when standing still, and when moving at a relativistic
velocity. The comparative term we want to know is found as:
 

EQUATION Z-14

Mbh/R= C2/2G                 Where ratio C2/2G is a constant,

                                          when C is the speed of light, and

                                          G is the universal gravitational

                                          constant.

R is the original radius of original mass Mo

Mass Mbh is instantly found from EQ Z-13.

The logical argument formed in advance, was that
any mass result M+, and radius result R-, ensuing
from special relativistic effects on original states
Mo and Ro, should also equal the black hole constant
ratio
 C2/2G, if mass M+ and R- were relativistically
altered sufficiently to form a new black hole.

Ratio C2/2G can be labeled ratio CR (for 'constant ratio') and
has the value of (6.735275620 x 1027 grs/cm), given a speed
of light whose digital value is 2.99792458, and a gravitational
constant whose digital value is 6.6720 x 10-8.

Ratio C2/2G is known as a constant
for the given values of C and G.

What we can do is follow special relativistic changes upon
both Mo and Ro through successively greater velocities, until
the combined ratios (1/Es x Mo) / (Es x Ro) equals the ratio
C2/2G, as in:

EQUATION Z-14A

[ (1/Es x Mo)/(Es x Ro) ] = (M+/R-) = C2/2G

where Es is the special relativistic effect.

Finding a significant Velocity value, which results in ratio CR

It was useful that a good test model was available in the
solar system's Sun, where given the Sun's existing mass as M,
and existing radius as R. The Sun has to be accelerated to such
an extent that through the parameters of special relativity, the
Sun's modified mass M+ and radius R- reach a point where they
transfigure into conditions which form a new black hole.

It was assumed that such a transfiguration should
occur, and that the transfigurating velocity in
special relativity could be inferred.

How could the velocity needed for the transfiguration, be
determined for an arbitrary general case such as the Sun ?

At this point, some intuitively lucky guesswork again prevailed;
a 'seeing around corners' so to speak. To make a long story short,
it is easy to predetermine the prerequisite velocity. How, is
outlined as follows:

 

1.     Given an existing Sun mass M of 1.99099305 x 1033 gms
        (mass MM from Part 1 above)

1A.   Given a Sun radius R of 6.96265 x 1010cm

1B.   Given constant ratio
CR =  C2/2G
                                              
= 6.735275620 x 1027 grms/cm

2.    Given the black hole radius parameter
       of EQ 4 of APPENDIX B, as:

 

       EQUATION Z-14-1

       R'= 2G·M/C2         Finding the Schwarzschild

                                      radius R' of a black hole's

                                      event horizon, when given

                                      mass M

 

3.    And given Equation 5 of APPENDIX B, rewritten as:

 

       EQUATION Z-14-2

       Mbh= C2R/2G         Finding mass Mbh needed for a

                                      black hole whose Schwarzschild

                                      radius is given as R.

                             Mass Mbh is the black hole silent
                             partner mass for any given mass M.

 

4.   Given Equation Z-8 above for special relativistic effect
      on both an original rest mass and its original radius, based
      on a term Nx to determine a velocity, so that:

 

       EQUATION Z-15

       Es=[1 –   (C/Nx)2/C] =[1 –   (Vx)2/C2 ] 

 

 

5.   Given that (1/Es × M) = M+

6.   Given that
(Es × R) = R-

7.   Given that
(1/Es × M+) / (Es × R-)   =  C2/2G   =  M+/R-

8.   Then it should be possible to find a velocity for EQ Z-15-1
      below such that the resulting
M+/R- ratio = C2/2G

9.   A first arbitrary value for Nx was tried, being 1.0001, which
      produced results that were too low for the above Item 7 to be
      correct.

10.  A second arbitrary value for Nx was tried in EQ Z-15, being
       1.00001, which was of the right magnitude for a mass M+, but
       Item 7 was still not correct.

11.  However, it was noticed that 1/1.00001 by itself was in the
       magnitude range of gravitational relativistic effect Eg from
       the Sun's mass, as determined in EQ C of Part 1 further above.
       (MM in EQ C is the same value as Sun mass Mo given in EQ Z-2,
       and immediately above in Item 1. And Eg of EQ Z-2 is the same
       as Eg used immediately below in Item 12).

12.  And so Eg was determined for the Sun's mass M = MM = Mo in
       EQ Z-2, and conveniently labelled Egs (for 'effect gravity Sun
       mass'), and was substituted as term 1/Nx in EQ Z-15 immediately
       above, to give:

 

       EQUATION Z-15-1

       Es=[1 –   (C×Egs)2/C] =[1 –   (Vx)2/C2 ] 

              where velocity Vx is (C × Egs),
              and special effect Ess conveniently
              means an Es effect related to the
              gravitational mass via term E
gs
.

13.  Then; Sun mass M in (M × 1/Ess) = M+

14.  And; Sun radius R in
(R x Ess) = R-

15.  And; ratio
(M+/R-) = 6.73527458 × 1027 grms/cm
       As found in:

EQUATION Z-15-2

 

(M x 1/Ess) / (R x Ess) = CR = (M+/R-)

16.  Which turned out to be an excellent approximation of ratio
       CR (being C2/2G as created in Item 1B immediately above)

Well, this was very good for a first found attempt. How
about for other masses, and how did the ratio result of
Item 15 favorably equate in truth to Item 1B above, in
that the CR result in Item 15 is marginally below the
CR constant in Item 1B ?

17.  The mass of the Sun was arbitrarily raised by a factor
       of 1000, so that now M = 1.99099305 × 1036 grms

18.  A new Egs effect factor was determined using the
       larger mass of Item 17, in EQ Z-2 above

19.  The new Egs factor was substituted in EQ Z-15-1
       to give a new Ess factor

20.  The new Ess factor was substituted in the
       terms of Items 13, 14, and 15

21.  The result
M+/R- = 6.735275620 × 1027 gms/cm = CR,
       which is exactly the constant of
Item 1B

Two things were instantly made clear.

It is clearly evident that Equations Z-15, Z-15-1,
and Z-15-2, are correct for any mass, to yield (M+/R-)
ratios equal to C2/2G.

It is clearly evident that ratio (M+/R-) closes
in on ratio C2/2G, the closer that given original
mass M is to the black hole silent partner mass Mbh
as determined in EQ Z-14-2

(It is also clear from preceding explorations, that
when relativistic effects are to act upon an original
mass, the original mass M can never approach its black
hole silent partner equivalent Mbh any closer than by
Mbh divided by factors of the Golden Ratio).

Finding that terms M+ and R- are properties of a black hole

 

At this point we are still not finished. The final question is;
are terms M+ and R- (as determined by Equations Z-15-1 and Z-15-2),
in fact the terms of a new black hole whose mass is M+ and whose
radius is R- ?

This final question was very easy to test by a double check:

22.   The value of M+ from Equation Z-15-1 and Item 13 for the
        Sun mass arbitrarily increased by a factor of 1000, as in
        Item 17, yielded an Ess value in Item 19, which as applied
        to Item 13, was:
                                 3.055623494 × 1027grms

23.   The value of R- from the same Ess in Item 19, applied
        to Item 14, was:
                                4.536746031 × 109cm

24.   Looking to Equations Z-14-1 and Z-14-2, it was found in
        EQ Z-14-2 (given mass M+ of Item 22), and found in EQ Z-14-1
        (given radius R- of Item 23), that (M+/R-) = CR. This is shown
        in the following three equations:

EQUATION Z-15-3

        R'=  2G·M+/C2        Finding the Schwarzschild

                                         radius R' of a black hole's

                                         event horizon, when given

                                         mass M+

R' was 4.536746031×109 cm,
    exactly the same as R- in Item 23

EQUATION Z-15-4

        M'=  C2R-/2G           Finding mass M' needed for a

                                         black hole whose Schwarzschild

                                         radius is given as R-

                                        

M'  was 3.055623493 × 10 to 27 grms,
     exactly the same as M+ in Item 22

 

EQUATION Z-15-5


And so  :  M' of EQ Z-15-4, divided by R' of EQ Z-15-3, = CR
as in     :
 (M'/R') = CR
where   :  CR is the constant of Item 1B
proving :  that M+ of Item 22 and R- of Item 23 are the
                correct parameters of a new black hole created
                by relativistic effect Ess of Item 19, on higher
                mass M of Item 17, using EQ Z-15-1 to determine
                Ess, after using EQ Z-16 to determine Egs.

 

       SUMMARY EQUATIONS

 

The delineations of Items 1 to 23, and Equations Z-14 to Z-15-5,
once understood, resolve into a quick series of steps, used to
determine a relativistic barrier for any given mass M and its
radius R, as in:

 

EQUATION Z-16

Egs=[1 –   2G·M/C2·R  ]                     M is any mass, R is its

                                                            radius, and Egs is the

                                                            gravitational relativistic

                                                            effect of mass M.

EQUATION Z-16-1

Ess=[1 –   (C×Egs)2/C] =[1 –   (Vx)2/C2 ]

 

Ess is the special relativistic effect ensuing from
velocity Vx, determined as the direct consequence of
the speed of light reduced by the mass's gravitational
relativistic effect Egs.

EQUATION Z-16-2

(M x 1/Ess) = M+

 

EQUATION Z-16-3

(R x Ess) = R-
 

EQUATION Z-16-4

M+/R-  = C2/2G  = CR

 

and mass M+ and radius R- are a relativistic transfiguration of
M and R into the parameters of a black hole, when
ratio (M+/R-) = CR.

CR is a physical constant in black holes,
whose value is given as the speed of light squared
divided by twice the gravitational constant, and
whose value is 6.735275620 x 1027 gms/cm.

EQUATION Z-16-5

And ultimately, Ess can be determined directly
from Egs, by:

 

Ess2 = 1 - Egs2
 

Ess is not the same value as Egs. Ess can be higher
or lower than Egs. The exact relationship between the
value of Egs and Ess is known by:

EQUATION Z-16-6

Ess =√[1 - Egs2]
 

Egs =√[1 - Ess2]
 

Why this relationship occurs is explained
further below, beginning with EQ Z-17),
and explicitly in EQ Z-19.

In a nutshell, Equations Z-16 to Z-16-6 fully show that
fundamental terms in both gravitational (stationary) and
special (moving) modes of relativity are synonymous.

 

 

 

 

UNIFIED EFFECTS IN FIELD BEHAVIOR

 

 

 

GENERAL INTRODUCTION for part 4   Unified Fields 

 

 

 

'The best information seems to come after you think you
have it wrapped up and have stopped thinking about it'.

'For example, the following floated into
consciousness as an afterthought'.

In a broad sense, relativity synonymy evokes innuendoes
of unified behavior between the fields of gravity and
electromagnetism (a unified field theory).

But wait, this is not a fully fledged unified field theory. What
is under review here are only parts of what appear to be a unified
field theory environment. What is shown are exactitudes whereby
gravitational effects of an assumed mass changing character on a
body, result explicitly in equivalent special relativistic effects
synonymous to the body moving at characteristic velocities.

Certain rules of behavior define these two modes of relativity in
their unified behavior. These rules are easy to understand, once
clearly seen, but can be very confusing until their characteristics
are shown in an obvious way. This next section (Part 4) explores
the rules.

To do the job, a particular environment is arbitrarily created. Exact
test cases are followed to the nth degree. The created environment is
in violation of certain conditions already outlined in Part 2 above;
to wit: that certain critical limits exist in the rate of mass
expansion, where the maximum expansion oscillates between a black hole
mass equivalent Mbh, and plateaus below this, articulated as functions
of the Golden Harmonic Ratio 1.61803398875.

For the test cases, it is desirable to see what happens
mathematically for events which are right at the brink of
a black hole mass, compared to masses well below the brink.
The phenomenology is thus most easily watched in detail.

For this, such masses are arbitrarily created, and assumed to exist
in violation of the statements in Part 2 above (which delineate that
a mass of black hole equivalent includes an original mass Mo, a mass
augmentation unit Ko, and resultant mass aggregate which is that of a
black hole or less. If the mass is that of a black hole, the original
mass is at a critical mass limit Mc, and the ratio Mbh/Mc = Ng is a
function of the Golden Ratio. For masses other than than Mc, ratio Ng
is given the general label Nx).

In the following, the cases for Mc and Ng parameters are ignored by
conveniently looking the other way. In the test cases which follow,
the existence of discrete portions denoted by terms such as Mo, Mc,
and Ng, are expeditiously put aside, and a mass value is assumed which
can be anything less than Mbh, even if less than Mbh by a few parts in
a thousand. This is called a HIGH mass, for convenience.

 

 

TEST CASE

 

 

 

In a test case, a HIGH mass value is studied which hangs right
below the mass of a black hole Mbh. This is in a deliberately
selected HIGH mass range which as already said ignores properties
such as a critical mass factor (Mc) outlined in Part 2 above.

The intention this time is to follow test case examples in
excruciating digital detail, so that the effects and their
changes are unmistakable.

The sole intention of the following, is to observe how certain
properties are universally united in a general way through various
transformations between gravity and electromagnetic field behaviors.

And so a new study model is created, based on the arbitrary
criteria that any job needed to do a certain job is good enough
for the purpose intended.

A HIGH mass gravitational event and a LOW mass event are thus
arbitrarily created from the same Mbh term, which is the mass
of a black hole confined in the Sun's radius. Mbh for the Sun's
radius is (4.689536679 × 1038 grms).

The Sun's radius (6.96265 × 1010cm) has been chosen as an
easily recognized radius for use as a constant to investigate
the effects of different mass densities confined in a fixed
(unchanged) area. Otherwise, the Sun's radius has no physical
significance when tied to the following arbitrary mass aggregates.

To supply the study, a small ratio Nx has been selected for a
control in the study. Nx is meaningless other than its value
is the charge to mass ratio of the hydrogen atom, ie.:

((Proton + electron) / electron) = 1.000544617 = Nx.

(The interpretation is that the negative electron charge
of the lightweight electron influences the heavy proton
by only 1.000544617 of the effect the proton has on the
electron, since both particles have the same quantity of
charge (opposite) despite widely divergent rest masses.
This is mentioned only to satisfy curious minds. As said,
the real value for the above ratio Nx has no intrinsic
significance in the following).

 

MASS1    In our study model, Mbh is arbitrarily reduced by the
               small ratio Nx to give a HIGH Mass1 term, which is very
               slightly below Mbh.


MASS2    Mass1 is then arbitrarily reduced by a factor of 100,000 to
               give a LOW Mass2 term having the same digits but much lower
               magnitude then Mass1.

 

The intention is to be able to follow certain relativistic field
effects in detail by following the digital results of both the
HIGH mass term (Mass1), and LOW mass term (Mass2), to more openly

follow the unifying effects between the two fields (being gravity
and electromagnetism).

In the study model, as already said, the value of Nx has no
significance except that it provides a convenient low value
Nx ratio to arrive at a HIGH mass term for the study model.


Nx      is given to 13 significant digits as gained from the
          ratio (P 938.2796 mev + E .5110034 mev) / (P 9382796 mev)
          = 1.000544617404

 

                        TABLE 4-A

 

   ARBITRARY STUDY MODEL DATA

 

 

Nx      =   1.000544617404 = (P + E) / E
Mbh   =   4.689536679 × 1038 grms

 

 

HIGH mass1     =   Mbh / Nx
                        =   4.686984066 × 1038 grms
                 Nx   =   1.000544617404
 
LOW mass2      =   Mass1 / 100,000
                        =   4.686984066 × 1038 grms
                 Nx   =   100054.4617404 

 

 

In the following, Equations Z-17-1 and Z-17-3
are the same as EQ Z-15-1 above, except, the real
digit value of each Egs ratio is substituted for
the algebraic term Egs.

 

 

EQUATION Z-17 HIGH gravitational Mass1 results:

Egs =√[1 - 2G (4.686984066 × 1038 grms)/C2R]

Mass1 has been given in
terms of a real weight.

Radius R is the radius of the Sun.
Egs is the gravitational relativistic effect of Mass1.

HIGH gravity field effect

Egs is closing toward 0

 Egs =

0 .023330687

EQUATION Z-17-1             Electromagnetic field effect results
                                          (Ess is special relativistic effect)

Ess=[1 –   (C × 0.023330687)2/C] =  (Vx)2/C2

0.023330687 is effect Egs
of EQ Z-17

Ess =   [1 - Egs2]
As in:
 [1 - 0.0233306872]= 0.999727802
 

LOW special field effect

Ess is closing toward 1

V velocity is starting to
close toward 0

 

 Ess =

0.999727802
 

EQUATION Z-17-2            LOW gravitational Mass2 results:

Ess=[1 –   (2G × 4.686984066 ×1033 grms)2/C2R  ]

                                                                             Mass2 has been given in
                                                                             terms of a real weight.

LOW gravity field effect

Egs is closing toward 1

 

 Egs =

0..999995002
 

EQUATION Z-17-3           Electromagnetic field effect results
                                       (Ess is special relativistic effect)

Ess=[1 –   (C × 0.999995002)2/C2  ] =  (Vx)2/C2

                                                                            0.999995002 is effect Egs
                                                                                                  of EQ Z-17-2

Ess =   [1 - Egs2]
As in:
 [1 - 0.9999950022]= 0.003161416
 

HIGH  special field effect

Ess     is closing toward

V        velocity is closing toward 1

 

 Ess =

0.003161416
 

 

       COMPARING M+ AND R- RESULTS FOR HIGH AND LOW MASSES

 

 

As delineated in Items 22 to 24 above, and in Equations Z-15-3
to Z-15-5 which immediately follow Items 22 to 24, two terms
M+ and R- represent the enhanced mass and reduced radius on
an object due to special relativistic results ensuing from the
proper ratio of the speed of light divided by the proportionate
relativistic effect of the object's gravity.

And so the synonymity of related behaviors, (the resulting
effects of Ess from Equations Z-17-1, and Z-17-3), when applied
to the HIGH mass of EQ Z-17, and LOW mass of EQ Z-17-2, will yield
appropriate M+ and R- terms for each of the masses. These are
listed in the following:

TABLE 5

 

HIGH MASS GRAVITY

 

                 MASS1   =   (4.686984066 x 1038 grm)

 

             RADIUS R  =   6.96265 x 1010 cm

 

          Ess EFFECT  =   0.999727802 ; from EQ Z-17-1

 

                    M+ =    (Mass1 x 1/Ess)

                          =    4.688260199 x 1038 grms

 

                     R- =    (radius R x Ess)
                          =    6.9607547839 x 1010 cm

 

                    CR =    ratio (M+/R-)
                          =    6.735275620 x 1027 grms/cm

 

 

TABLE 6

 

LOW MASS GRAVITY

 

                 MASS2   =   (4.686984066 x 1033 grm)

 

             RADIUS R  =   6.96265 x 1010 cm

 

          Ess EFFECT  =   0.003161416 ; from EQ Z-17-3

 

                    M+ =    (Mass1 x 1/Ess)

                          =    1.482558107 x 1036 grms

 

                     R- =    (radius R x Ess)
                          =    2.201183848 x 108 cm

 

                    CR =    ratio (M+/R-)
                          =    6.735276152 x 1027 grms/cm

 

 

      It is seen that results M+ , though higher than an
      originating mass, are lower than the ceiling mass Mbh
      in LOW mass results, and close in on ceiling mass Mbh
      in HIGH mass results. (Ceiling mass means a black
      hole mass equivalent Mbh formed in radius R.
      In HIGH mass situations, M+ can look like the high
      mass itself, but in low mass situations, M+ is far
      removed from the low mass itself.
      Also, it is obvious that M+ of LOW mass results can
      gain substantially over the LOW mass itself, yet still
      remain substantially below the final mass Mbh, whereas
      M+ hardly gains over its originating HIGH mass, and
      can also look very much like final mass Mbh, when
      the HIGH mass itself looks closely like Mbh.
      In real situations, the HIGH mass will be fixed at a
      maximum ceiling of critical limit Mc. In this current
      test case situation M+ looks neither like Mc, or Mbh.
      Yet M+ will be explicitly Mc x √GH, and Mbh/√GH, when
      GH the Golden Ratio 1.618034 is term Nx.
      (Ratio CR in the LOW mass situation, is seen to be
      marginally more than CR = C2/2G . This shift might
      be due to intrinsic truncations in the digital
      accuracy of the equations for lower mass densities.
      It is hard to tell, in the scope of a digital
      accuracy limited to 13 significant figures).

 

 

FIRST INTERPRETATION

 

Thus M+ can approach but never equal or exceed Mbh. As the Egs
effect approaches 0 (greatest power in gravity field strength),
the Ess effect approaches 1 (the least power, no effect), in
velocity related relativistics.

At the point where the gravity effect has its greatest value;
at Egs = 0 ; the special relativistic effect ceases to exist
(comes to a standstill), because there is no velocity, as when:

 

EQUATION Z-17-4

(C/0)/C = 0/C = 0 .
 

This closes right in on a clear insight regards the question
of how maximum potential relativistic gravity effect can
contain light - effectively cancel the velocity of light.
The velocity of light is not cancelled. The ability to have
a velocity related to any special relativistic effect is
cancelled. It appears this amounts to the same thing as a
counteracting of the velocity of light.

 

 

 

DIRECT  INTERPRETATION

 

A first interpretation of the consequences of Equations Z-17 to
Z-17-3, is that a HIGH gravitational mass density results in a
LOW special relativistic synonymity. And a LOW gravitational
mass density results in a HIGH special relativistic synonymity.

It has the immediate interpretation that things run faster in
LOW gravitational events, and slower in HIGH gravitational events.

It adds another picture to the experimentally
confirmed property that proximity to gravity,
relativistically causes time to slow.

Intuitively, it answers a question as to how gravity at
its highest can confine light. A see saw (or yin yang)
characteristic in the works is summarized in the following:

TABLE 7

HIGH mass gravity                Effect     Egs     approaches 1
                                             Effect     Ess     approaches 0

LOW mass gravity                 Effect     Egs     approaches 0
                                             Effect     Ess     approaches 1

You can see at a glance how gravity can confine
light. As gravity effect Egs closes in on 1,
Special effect Ess closes down toward 0 velocity.
When Egs is right at 1, Ess is closed down right
to 0 and the velocity of light C in a V/C ratio
is vanished when 0/C = 0

Conversely, when Egs is low and closing down to 0,
effect Ess intensifies with a velocity approaching
1, which is equivalent to approaching the full
speed of light.

In another sense, it is clearly seen that events
are free to move more rapidly in activities of a
HIGH velocity, in a LOW gravity field density.

And in a HIGH gravity field density, events are
constrained to low velocity activity approaching
0 velocity, when the gravity field approaches the
density of a black hole, re: special relativity.

 

Notes:

In real events, as summarized above in Part 2,
if a mass augmentation is assumed for gravity
effect Egs, then when a mass's density (without
augmentation) reaches a critical mass factor Mc,
the mass augmentation amount Ko is sufficient to
jump the mass amalgamation in one whole bump to a
black hole quantity Mbh, such that effect Egs = 1.
And thus effect Ess = 0; which is the equivalent
of a 0 velocity for light.

The proportionate bump of mass Mc to Mbh is a
function of the Golden Ratio 1.61803398875.

It means there never is a situation where effects
Egs and Ess slowly converge to 1 and 0, as is
fictitiously indicated in Equations Z-17 and
Z-17-1. As show in Part 2 further above, effects
Egs and Ess will jump in a final leap to 1 and 0
in a single bump via Golden Ratio functions, when
the gravity mass density reaches Mc before ³
reaching black hole mass Mbh

 

 

 

PURE MATH CONNECTORS

 

Terms Nx, Egs, and Ess, can be shown to be mathematically
connected by direct steps which bypass the physical dynamic
terms. This does not mean the physical dynamic terms do not
exist, it only means that it is possible to quickly work back
and forth between Ess, Egs, and Nx, when a few connector rules
are known. These rules include the following:

Given an Nx term:

            then:   Egs  = √(1 - 1/Nx)
             and:  
Nx    = root 1/[1 - (Egs)2]
             and:  
Ess  = root 1 - (Egs)2
             and:  
Ess  = √(1/Nx) = 1/√Nx

These connector rules can be more readily shown in a table,
as follows:

TABLE 8

FOR EXAMPLE, GIVEN THAT Nx = √3 = 1.732050807

Then: for GRAVITY relativity

 

1.              Egs  = (1 - 1/√3)                =  .650115167

 

So that:     Nx  = 1/(1-Egs2)                 = 1.732050807

 

Then: for SPECIAL relativity

2.              Ess  = (1/√3)                     = 0.759835685

Then: for GRAVITY relativity

 

                Ess  = (2GM/C2R)            = 0.759835685

 

And:       Ess2  =  2GM/C2R                = 0.577350269

 

So that  :   M  =  Ess2· C2 ·R/2G

      And :   Ess  = 1 - (Egs)2               =  0.759835685

      And :   Egs  = 1 - (Ess)2               =  0.650115167

      And :   Ess  = 1/Nx                      =  0.759835685

So that  :   Nx  = 1/Ess2                      =  1.732050807

      And :   Vx = C / 1/Egs                  =  Velocity  

 

 

 

 

NOTE:    There are specific similar distinctions
              between the Nx terms for the two relativities,
              and first given Egs and Ess terms, shown in
              TABLE 8 as 1, and 2.

 

These above shown pure math permutations are
true when given any value for Nx, or Egs, or Ess.
With these rules it is possible to freely move back
and forth to arrive at key terms for gravitational
and special relativites.
For instance, given a special effect (Ess) for a
body moving at a high velocity, then equivalent
gravitational effect (Egs) in relativity is directly
known by a single step calculation, for instance
by:

       Egs  = 1 - (Ess)2             

And what portion the given moving body's mass 
is to a black hole silent partner equivalent,
is directly known by a single step calculation,
for instance by:

      Nx  = 1/Ess2       because: Nx = Mbh/M

 

When dealing with real events which occur at the critical
mass limit Mc, where then Mbh/Mc = GH (the Golden Harmonic
Ratio 1.618034), then pure math connectors can appear slightly
confusing, in that certain pure math factors exactly occur through
functions of the Golden Ratio, rather than through relativistic
field dynamics.

For instance:

 

TABLE 9

GIVEN THAT Nx = 1.61803398875 = The Golden Ratio

 

Then also:

                 Egs  = 1/GH = GH-1           =  0.6180339

      And :   Egs  = 1 - (Ess)2               =  0.6180339

      And :   Nx  = Egs+ 1                      = 1.6180339

 

 

 

And:         Ess  = Egs                       = 0.7861514

And:         Nx   = (Ess x 1/Egs)2         = 1.6180339

And:         Nx   = Ess2 + 1                  = 1.6180339

                                                            Etcetera


BUT THESE ARE TRUE ONLY WHEN NX = THE GOLDEN RATIO

 

 

WHY Egs AND Ess ARE INTRINSICALLY RELATED

 

 

In a closer look at the preceding, some
further facets are learned. In particular:

EQUATION Z-18

      For example:   Taking data for Ess and Egs from EQ Z-17-3 ;
                   and:   M+ from table 6
                 then:    in EQ Z-18 ;

     Ess = 1 - (Egs)2

              where:    M+/M = Nx                 when Nx = Mbh/M

      and so:   in EQ Z-18-1

EQUATION Z-18-1

                     Ess of 0.003161416    =   1 - (.999995002)2

    because:   M+/M = Nx

     

      and so:   in EQ Z-18-2 ;

 

 

EQUATION Z-18-2

 

 (1.482558107 x 10 to 36 grms)    = 316. 313878376 = √100054.469653
 (4.686984066 x 10 to 33 grms)

 

      where:   100054.469653 = Nx × 100,000
 

   because:   Nx is ratio 1.000544617404
          and:   Mbh / 1.000544617404        gave Mass1 for our study model
          and:   Mass1 / 100,000                  gave Mass2 for our study model

 

       NOTE:   The true value of √(Nx × 100,000) = 316.313865868 =
                    √100054.4617404, is slightly departed from the actual Nx
                    value for Mass2 shown immediately above. The departure
                    is due to intrinsic truncation in accuracy, where a few
                    digits are clipped from the tail end of the HIGH special
                    relativity Ess term 0.003161416, and the LOW Egs term
                    0.999995002.

 

 

 

 

 

SPECIFIC CONCLUSIONS

 

 

 

 

It is now clear, according to the above derivations which begin
with EQ T and continue through EQ Z-18-2, that a fundamental
barrier exists in physics, which limits special relativistic
effects on a visible moving mass entity to a pre-determinant
black hole gravitational mass equivalent, gained by a
pre-determinant limit in velocity.

The pre-determination on the entity is as seen by a stationary
observer watching the mass entity move at relativistic velocities.
At its pre-determinant limit in velocity, the mass entity
transfigures into a black hole and disappears from view.

(This does not mean that the black hole cannot keep acceler-
ating. What it means is that the possibility of such further
acceleration is not addressed in any way, in the scope of this
disclosure. This exploration ends with the original radius R
transfigured into an event horizon R– = R'. And so as an event
horizon radius R- will thereafter behave in dissimilar ways
than in the physical form of a radius R. Such dissimilarity
in behavior of radii is discussed further above at the start
of Part 2, as Items 1 and 1A under: 'A Comparison Between
Gravitational and Special Relativity').

In outlook, a visible mass is any mass of radius R.

The visible mass has to be capable of radiating light to be
seen in the universe. Its black hole M+ and R- equivalent at
the relativistic limiting barrier does not radiate light, and
so no longer physically exists in terms of basic electromagnetic
radiation.

Generally, a visible mass accelerated to relativistic
velocities cannot achieve a theoretical infinite visible mass,
and the velocity of the visible mass can never theoretically
equal the speed of light.

The interpreted statements in special relativity which say a
mass (obviously visible) continues to expand toward infinity,
and the velocity continues to the speed of light, are wrong, when
they do not take into consideration the black hole barrier effect.

The maximum velocity attainable by a visible moving mass, is
the speed of light reduced by the proportionate ratio of the
gravitational relativistic effect of the mass being accelerated.

The velocity barrier limit (maximum velocity) possible, is
restricted by the bounds achieved in special relativistic
effect when the mass has increased, and its radius has
contracted, to a point where the moving entity forms a
black hole and effectively disappears from view.

As already said, this point is easily calculated, as
being the velocity resulting when the speed of light
is divided by the proportionate effect of the mass's
gravitational relativistic effect.

This point will vary from mass to mass, and from radius to
radius per given mass, but will inevitably appear somewhere
before the speed of light is reached, when the visible mass
is being accelerated to relativistic velocities.

A further limiting factor is reached, when the original
mass factors and augmented mass factors are summed, to
reach an absolute prior limit at which the total mass
transforms into a black hole equivalent in single bumps,
which are proportionate factors of the Golden Harmonic
Ratio 1.618034.

 

 

 

GENERAL CONCLUSIONS

 

 

 

 

The fundamental point of view adapted for much of the
preceding, is to consider that gravitational relativistic
effects are steady state. I.e., the gravitational source is
simply sitting there doing its relativistic thing.

And so there are no gravitational accelerations of a kind
which involve motions of points of center, when understanding
certain of the effect's basic properties, such as the effect
on the original mass of the gravity causing the effect.

Throughout the gravitational relativity explorations of Part 1,
the perspective was entirely from the perception of different
mass aggregates being squeezed within the same unchanged radius.

In practice, the only radius used was the radius of the
Sun, as it is presently measured empirically in this solar
system. That the Sun's radius can be presumed to be reduced
slightly by the relativistic effect of gravity has been taken
into consideration, but has not been explored through any of
the possible permutating effects that changes to the radius
might have. In short, the studies involved variable densities.

The very nature of gravitational relativity implies permuting
effects due to gravity on all of the parameters involved, for
instance on all of the terms in EQ W. The sheer magnitude of the
job of trying to explore all possible combinations of permutations
involving just R vrs M for this solar system, for instance, has
not been explored here.

Which leaves wide open a very important question. In the
circumstances so far described, there is no proof that the radius
of a mass aggregate is the bottom line through which important
gravitational relativistic manifestations are to be observed.
This in no way suggests that a proof should not be forthcoming.

It so happens that a constant radius (in this case the radius
of the Sun) is very convenient for displaying many important
manifestations of gravitational relativity and black hole
correspondences. It appears to hold together a thread of logic
though many physically dissimilar events, including standing stark
still (gravity relativity) and in motion (special relativity).

Such stark realism between the relativities would be a hard
(if not impossible) task to monitor if the confinement radius
was allowed to be mutable.

So, the Sun radius is freely used as a constant
for exploring different stark manifestations.

 

       MASS DENSITIES IN A CONSTANT RADIUS

 

It is clear (as shown in many of the preceding demonstrations)
that the existing Sun radius might in some way be of fundamental
importance. Not necessarily in core physics of the universe as
a whole, but at least in core physics of the solar system.


This is seen in the interphased mass congress states involving
½ units of Jupiter's mass, as discussed in Part 1.

In the various relativistic explorations, the Sun's radius has
been willfully maintained as a constant value through different
discrete changes in mass aggregates studied. (This applies to the
corresponding planet masses explored, and is not meant to apply
to any special relativistic effects explored).

Dynamically, a change in mass within the same radius usually
translates into a change in density of the aggregate.

In other words, density pressure may be a part of the cause
and effect, or at least may have originally been a part of
the cause and effect, prevailing at the time of this solar
system's formation.

This may be a clue regarding the unusual solar characteristics
observed; where different discrete units of mass (including
mass particles said to be a part of total mass aggregates)
are seen externalized as planets orbiting far from the major
field of the Sun.

The mystery is that the particles are orbiting well
beyond the significant radius of the inducing effect.

The external factors include planet masses which are a
part of the mass aggregate inducing significant effects.
One particular planet is Jupiter. Other planets are
clearly related to the induced effects, but their masses
do not seem to be included in the mass aggregates. These
planets are Venus and Mars.

It may be that concomitant to gravity relativistic
effects gained with the Sun's mass, special relativistic
effects are also gained. But rather than being produced
in the form of increased mass per se, the special effects
become produced in the form of velocity which can translate
directly into angular momentum, resulting in at least some
of the induced influences being flung into orbit thus carrying
away discrete units of relativistic effect in the form of
discrete quantities of angular momentum. This is only a
thought, probably ridiculous.

(In a casual thought, if a gravitational body also
induces a synonymous relativistic effect (motion) the
motion has no real way to go forth in itself, since
ideally all of the effect of motion is equidistantly
applied to a sphere (the gravitational body). In this
scenario, the motion portion is thrown off (externalized)
in order to be expressed).

 

A QUESTION REGARDING RELATIVISTIC
MASS EFFECT AND QUASARS

 

These following remark are purely conjectural.

Let's suppose that certain relativistic effects induced by
gravity seem to be incompatible with the basic gravity itself.
In other words there are two aspects to gravity: the original
(naked) gravity for any material, and the relativistic effects
caused by that gravity. In this supposition, some relativistic
nature cannot exist within the naked nature, and so is
externalized at long distance.

The externalizing is guessed as either by a throwing off
(forcibly casting forth) or by a remake (as if in leaping
from here to there, where 'there' is a predetermined position
in some kind of latent underscore pattern involving the gravity
field). (In high energy physics, many sub atomic particle
interactions are depictable as occurring simultaneously in two
places at once, where an event at one place directly effects
the event in another place even though nothing but thought
can transfer between the two places). A third form of ejection
might be by the simple virtue of an outthrow of discrete bits
by angular momentum.

In the workings of gravitational relativity, several things are
at issue. There is an original mass, plus the original mass's
augmentation due to the relativity of the mass's gravity. There
can also be more mass added into the conglomerate at any time.
Which results in a hike in the augmentation effect due to
strengthened relativity.

It can be supposed that if an increase in mass takes place within
a given radius, resulting in a hiked relativistic mass augmentation
due to the added mass, which in turn causes jitters so that
something of the hike has to be expunged or externalized from the
gravity field which is generating the effect in order to satisfy
an esoteric yearn to solve the jitters, then where added mass is
accreting into a large black hole some of the relativistic gain
is transferred to an external position outside the black hole.

Since very high energy effects are involved with the black
hole anyway, it is not difficult to picture that the expunging
can appear highly energetic. What the mechanism is that could
transfer the effect to an external place is not here conjectured
but can be supposed. For instance:

A long arm recurrence (here and also there) is one mode.

An intense radiating away (or bleeding away) of some of
the change upon the event horizon boundary, in alternative
to allowing a change to go ahead in the relativistic regions
of the boundary size itself, is another mode. This is made more
viable if it is suggested that the black hole yearns to maintain
some form of internal density which has no further relativistic
influence inside the black hole.

And finally, a conversion of units of intrinsic spin
as energy, (conversion from spin to propagational energies),
is another, if possible.

A QUESTION REGARDING RELATIVISTIC
EFFECT ON THE GRAVITATIONAL CONSTANT 

 

There is also the prospect that the gravitational constant itself
is modified by the relativistic effect of gravity. In retrospect,
it is not readily apparent as to whether the gravitational constant
would weaken, or strengthen, relativistically, given larger and
larger masses. The present day mode of thought is to consider that
the gravitational constant might grow relativistically stronger.

On the other hand, Equations Y to Y-2 above suggests that
the gravitational constant relativistically weakens through
increasing mass aggregates.

On yet another hand, it has not been proven that a mass
relativistically increases (as opposed to decreases) by
gravitational relativity. A stable picture should ensue,
albeit not exactly the same as the picture described in
Equations T through Z-11-4, if a mass decreases by its
gravitational effect, such that the mass's confining
radius might increase, or decrease, and the gravitational
constant also might increase, or decrease, etc.

Such possibilities are not considered in the above shown mass
congresses involving the Sun and certain planet masses. If the
gravitational constant is in fact modified by relativity, then
the apparent mass of the Sun is still valid, but the original
mass should not be precisely that as determined by the apparent
mass MM, minus the apparent mass times the effect; as shown in
EQ W-1.

In fact all of the parameters of Equation 1 below in APPENDIX B
(except for the speed of light) might be in states of modification.
These parameters include G and M, where a mutable value of
G therefore
is internally influencing the value of M.

In any case, the resulting gravitational relativistic mass
congresses between the Sun and planets as viewed herein are
in their resultant apparent states (involving the masses as
seen in the domain of the solar system and empirically measured).

And finally, the direct tie-ins between gravitational and
special relativity are balanced correctly anyhow, according
to the parameter choices selected for the preceding, to
infer then portray their handshake nature.

In a casual thought, if a gravitational body also induces
a synonymous relativistic effect (motion) the motion has no
real way to go forth in itself, since ideally all of the
effect of motion is equidistantly applied to a sphere (the
gravitational body). In this scenario, the motion portion
is thrown off (externalized) in order to be expressed.

It is not hard to speculate that the special relativistic
mass gain for the stationary object (gravity source) can be
(at least in part) thrown off in the form of energy, since
e=mC2. In which case a lot of energy will be visible per
small quantities of involved gain in mass.


In this speculation, there is a pure (rather than nuclear)
conversion of mass to energy.

In unstated allusions are hints that gravity and special relativistic
effects work hand in hand, with perhaps the special relativity effects
being more and more suppressed the higher the gravity. But as already
said, any special relativity associated seems to be incompatible within
the naked gravity itself and so ends up externalized (for instance) as
certain planets, as if a velocity is induced in a gravity mass at rest
which can leave its source, via angular momentum in the velocity.

 

A QUESTION REGARDS THE GRAVITATIONAL
CONSTANT AND THE GOLDEN HARMONIC RATIO

 

Whereas in another conjectural possibility, going in the other direction,
it may be possible that the apparent quantum jump in relativistic effects
seemingly embodied in operators involving the golden section ratio (the
golden harmonic), do not actually occur in the physical universe.

For instance if the universal gravitational constant did change in
value under increasing relativistic influence, it may result in a
situation where such things as mass and space increase smoothly toward
infinity after all, with the quantum leap from a plateau straight to black
hole parameters smoothed out or voided by relativistic changes in the power
of the universal gravitational constant.

Ho hum, speculations can be rather boring.

 

 

 

 

 

 

APPENDIX A

 
   

ELEMENTARY PARTICLE MASSES

 

 

 

 

In high energy physics experiments, particles such as the
electron or Proton are being accelerated to velocities said
to be virtually at the speed of light.

How is this possible?

This is possible because the Mass/Radius ratio of the proton
(as an example) is extremely small, compared to the Mass/Radius
ratio of the Sun for instance. The Mass/Radius ratio of the Sun is:

(Mass 1.991 × 1033grms) / (Radius 6.963 × 1010cm)

= (2.859 × 1022 grms/cms)

which itself is very small compared to the ratio of a black hole
having the Sun's radius, in which the Mass/Radius ratio is then:

Mass = (C2 × R) / 2G = (4.689 × 1038 cm)

 

And:

 

(Mass 4.689 × 1038 grms) / (Radius 6.963 × 1010 cm)

= (6.735 × 1027 grms/cm) = CR

 

Note that value (6.735 x 1027 grms/cm) = CR is actually
a physical constant for every black hole, and is equal to the
ratio of the speed of light divided by twice the universal
gravitational constant, as in:
(C2/2G) = CR = (Mbh/Rbh)
when Mbh and Rbh are the Mass and Radius (event horizon) of
a black hole, C is the speed of light, and G is the universal
gravitational constant.

When, otherwise, a normal M and R are transfigured by special
relativity into a new black hole having mass M+ and radius R-,
then: CR = (M+/R-), where, CR still has the constant value:
(6.735 x 1027 grms/cm).

In the large scale world of normal events the magnitude of
the Sun's mass at (10+33 grms) is well above the magnitude
of the Sun's radius at (10+10 cm).

In the world of the very small, the situation is
quite reversed. For example the mass of the proton is:

1.672 x 10-24 grms

whereas its radius is reverse in magnitude,
in the much larger range said to be about:

1.32 x 10-13 cm.

This produces a Mass/Radius ratio (proton Mass/proton Radius) of:

= 1.239 x 10-11 grms/cm.

Clearly, a proton will have to accelerate to an extremely
high velocity, virtually to the speed of light, in order
for special relativistic effects to transfigure the proton's
effected mass M and radius R into the (M+/R-) = CR parameters
of a new black hole.

The Mass/Radius ratio of the proton will have to grow by a
magnitude of (5.435 x 1038), in order for the accelerated
proton to take on the look of a black hole having mass M+, and
radius R-, and a (M+/R-) ratio equal to CR.

A calculation to determine what velocity the proton needs to
move in order for the transfiguration, is impossible to complete
with devices having mediocre accuracies good to only (say) 13
significant figures.

The calculation to determine the proton's velocity first requires
knowing what the gravitational relativistic effect Eg is for the
proton's mass and radius. Effect Eg is too small by many magnitudes
to be mechanically calculated by a device of 13 significant figures.
Given a device with greater accuracy, the resulting Eg effect for
the proton is divided into the speed of light, to give the velocity
at which the proton must travel to relativistically transform into
a black hole. The velocity will be the same as the speed of light
to many significant figures, before the digits begin to deviate.

(Unless there is (previously unsuspected) a gate in the velocity
of light, at which a particle (for instance a proton) might in fact
make a quantum leap to black hole magnitudes at a point that is at
some measurable factor less than a total 100% of the speed
of light).

Proton Comparative Mass Density

 

To give a comparison on just how nebulous is the mass
density of the Proton (how little in the way of gravity
that Proton matter presents), the mass density of a Proton
is on par with about 1 gram of matter wisping in a shell
whose width is equivalent to 10 times the full diameter
of the orbit of the Moon around Earth.

If the on par Proton mass were gathered together for the protion
which occupied the actual orbit of the Moon, it would be a moon
weighing about .48 grams circling the Earth.

 

 

 

 

 

 

APPENDIX B

 
   

BASIC EQUATIONS

 

 

 

 

Advanced details of a black hole, such as a paradigm model
of a charge membrane for instance, are not considered.

 

 

RELATIVISTIC MECHANICS

 

 

EQUATION 1

 

Eg =  √ 1  2G·M/C2R

Finding gravitational relativistic

effect Eg, for a given mass M and

a given radius R

 

EQUATION 2

 

M  =  (  [1 – (Egs)2] × C2R ) /2G

Finding mass M for a given

radius R and a given

relativistic effect Eg

 

EQUATION 3

 

R  =  2GM /( C2 [1 – (Egs)2] )

Finding radius R for a given

mass M and a given gravitational

relativistic effect Eg

 

EQUATION 4

 

R'  =  2GM /C2

Finding the Schwarzschild

radius R' of a black hole's

event horizon. When effect

E = 1, then factor [1 – (Egs)2]

is 0, which drops from EQ 3
leaving EQ 4

 

EQUATION 5

 

M'  =  C2 /2G

Finding mass M' needed for a

black hole whose Schwarzschild

radius is given as R'

 

 

GRAVITATIONAL MECHANICS

 

 

EQUATION 6

 

M   =  V2R /G

Finding the mass M for

sustaining a body orbiting the

mass at a given velocity V at

a given orbiting distance R

 

EQUATION 7

 

R   =  GM/V2

Finding the orbit R of a

body around a given mass M

at a given orbital velocity V

 

 

 

 

 

 

 

 

 

APPENDIX C

 
   

PURE MASS CONGRESS

 

 

 

 

This information is presented as a separate tableau and
has no self evident bearing on any of the explorations
and conclusions of the above statements. The following
shows that generally:

 

(½ THE SUM OF THE MASSES OF MERCURY, VENUS, EARTH, MARS),
PLUS THE MASS OF THE MOON, EQUALS THE MASS OF THE EARTH.

(½ the sum of masses N1 to N4) + N5 = N3

 

TABLE 10

Masses

 + N1   

  Mercury

=

   0.33020 × 1027 grms  
  + N2      Venus

=

   4.8683 × 1027 grms  
  + N3      Earth

=

   5.9760 × 1027 grms  
 

+ N4   

  Mars =    0.64181 × 1027 grms  
     

=

  11.81631 × 1027 grms  
 

½

 

=

     5.908155 × 1027 grms  
 

+ N5  

  Moon

=

    0.07350 × 1027 grms  
Equals

N3x

  Earth =     5.981655 × 1027 grms  
Inequality     N3x - N3

=

    0.005655 × 1027 grms  

There is an extra (+ .005655 × 1027 grms) in the N3x
result, which is unexplained. There is no other Moon in
the inner region of the solar system for instance.

The aggregate mass of the asteroids seems to be too
small by a factor of 10 to be this inequality. So the
extra (.005655  × 1027) does not meaningfully represent
the mass of the asteroids. What the mass inequality may
represent is not clear at all.

 

 

 

GENERAL MASS CONGRESS             (summary)                                                               

                

 

The Sun's mass plus ½ the mass of Jupiter added, can be shown
to induce a gravitational relativity mass increase effect which
is exactly equal to the mass difference between the planets Venus
and Mars.

 

(Sun effect ratio) =  √ 1  2G×(Sun mass + 1/2 Jupiter mass)/C2×R

                  C = Speed of light
                  G = Gravitational constant
                  R = Radius of the Sun

K (Mass augmentation) =  Sun mass     -  [Sun mass x (Sun effect ratio)]

K (also equals)              =  Venus mass  -  Mars mass

The same result is handled (in a slightly different way)
in the section beginning with TABLE 1 of file RELATIVE.1 .

                                                               See TABLE 11 next below.

TABLE 11

 

K                           =        4.226490 × 1027 grms

                             =        (Venus mass - Mars mass)

C                           =        2.99792458 × 1010 cm/sec
G                           =        6.6720 × 10-8 cm3/grms sec2
R                           =        6.96265 × 1010 cm

Planetary masses                      Data is from Table 1 in
                                                 the file RELATIVE.1

Moon                    =        0.0735 × 1027 grms

Venus                   =        4.8683 × 1027 grms
Earth                    =        5.976 × 1027 grms
Mars                     =        6.4181 × 1026 grms
Jupiter                 =        1.901 × 1030 grms

Sun                      =        1.9888 × 1033 grms

 

 

 

 

 

 

APPENDIX D

 
   

FOOTNOTES

 

 

 

 

 

Footnote 1

 

 

       RELATIVITY EQUIVALENCE PRINCIPLE

 

 

EQUATION Z-21

1 - Eg2 = 1 - Es2

One minus the square of gravity's relativity effect,
equals one minus the square of special relativity's effect.


EQUATION Z-22

 

1

=

1

=         Nx

1 - Eg2

Es2

The reciprocal of one minus the square of gravity's relativity
effect, equals the reciprocal of the square of special relativity's
effect.

This equality is equal to the ratio of a gravitational mass divided
into the mass equivalent of a silent black hole partner for the
gravitational mass.

 

Footnote 2

 

 

There is recent speculation that events in electroweak theory and
gravitational theory may converge to similar kind at very small
distances of the order of (10 to -28 cm) to (10 to -33 cm), said
to be possible at the time of a so called big bang. Whether or not
the unified field behaviors as disclosed in the above equations are
favorable or distasteful to such a big bang outlook is not in any
way considered to be of our concern, here.

 

 

 

Footnote 3

 

 

In use of the Sun's radius as a constant confinement delineator for
various mass aggregates and equivalent black hole masses, it is
acknowledged that the amount of extra mass poured into the existing
size of the Sun has to be very large to make a black hole.


For example the amount of mass is about 235,000 times the mass of
the Sun, poured into the space occupied by the Sun, to make a black
hole. This is of course physically unrealistic, (that that mass can
pour into the Sun and the Sun stay the same size). But having a
constant radius makes it far easier to keep track of various effects.

The physical universe is actually quite different. For instance the
radius of the Sun will dramatically expand with any appreciable amount
of mass poured into it.

But this is iffy. For example if the extra mass is iron, the Sun's area
will expand according to high material density. If the matter is helium
or hydrogen, the enlargement of the Sun's radius will be substantially
more.

In either case, since the radius is expanding (with more matter
poured in), a black hole mass plateau will be eventually reached
at a much different enlargement in mass than the factor of 235,000
times mentioned above. As you can see, pinning down parameters into
'look and see' constants, with this sort of thing going on, is like
trying to pin down the behavior of silly putty.

And so events herein have been scrutinized in detail from the point of
view of a single unchanged basic radius (the Sun radius), used as a
convenient point of reference to compare significant related events
that involve that single radius.

 

 

Footnote 4

 

 

The Golden Harmonic Ratio 1.61803398875, cited in this disclosure, is
an absolute number value gained as
(½ of √5) plus .5. This number is
also known as the Golden Section. The number can functionally permutate
through a bewildering array of directions on its own, with many
particular permutations appearing in the construction of 5 sided
geometrical figures. A particularly well known physical manifestation
of the Golden Section is the proportion of a Golden Rectangle. Other
well known manifestations include spirals and progressions occurring
in nature, some based on the Fibonnaci number series. These are said
to include galaxy spirals and Bode's Law for the solar system, however
some researchers think the astronomy occurrences appear to be as much
a case of co-incidence as anything.

 

 

Footnote 5

 

 

The Constant Ratio CR cited above as being M+/R- = C2/2G
also gives instant readout on such curiosity questions as:
 

1.  How much mass is contained in a black hole whose radius
     is 1 cm? The answer is

6.735275620 × 1027 grms                       In that:

 

M        =

C2R

 

Finding mass M needed for a

black hole whose Schwarzschild

radius is given as R = 1 cm

2G

 

Note that the mass has the same
digital value as ratio CR

2.  What confinement radius is needed for a black hole whose
     mass is 1 grm? The answer is:

1.484720234 × 10-28  cms                 Note that this is the digital
                                                               reciprocal of the value of the
                                                               mass M of question 1, in that:

 

R        =

2GM

 

Finding the Schwarzschild radius

R event horizon of a black hole

whose mass is 1 grm

C2

 

Footnote 6

 

 

In the most unusual circumstance of a velocity ratio V/C being
equal to a mass proportional ratio M1/M2, then gravitational
relativistic effect Egs is equal to ratio M2/M1.

For instance, let the ratio of one mass M1 divided
by a smaller mass M2 be called Rn.

 

Then:         Ess       =    √[1 –  (C/Rn)2/C2 ]       =    √[1 –  V2/C2 ]

 

And  :         Egs       =       1/Rn

 

 

 

Footnote 7

 

 

In case there is a concern over what has been done above, (in the
conjecturing of major effects as seen wrapping around changes in
the rest state of masses through two different synonymous modes of
relativity), there are no rules that exclude a direct synonymous
tie-in between both gravitational and special relativistic effects.

For example, it has been experimentally confirmed that time slows
in the proximity of a gravitational field. A main question which
can be asked is:

At what velocity does a mass have to be moving, to induce a
slowing of time (time dilation), that is equivalent to the
field effect from the gravity generating a relativistic
effect of equal magnitude on the flow of time?

The time dilation effect of a velocity in special relativity is
straight forward. That is, at a given velocity, events in time
for the moving object will seem slowed by a specific amount as
seen by a stationary observer.

In the case of gravity effect, the situation is more ambiguous.
The effect of time dilation depends on where the object is in the
vacinity of the field generating the effect. Closer to the field
means a greater time dilation. But in large scale objects such as
the Earth or more so the Sun, closeness empirically means close
to the surface with the observer also present, for example, rather
than close to a mathematical data point such as the center of the
Sun, or relative to a fixed velocity as when watching a Sun sail
by at high speed.

In our explorations above, real time positions moving here or there
in the embraces of a varying gravity field are not at all in the
picture. The basic 'need to know' speaks through simple statements
consisting of 'how much mass' in 'how much radius' to result in 'how
much effect' in the gravity will effect time.

The main point of view has been in terms of gravity as a mass source
extending in a boundry termed the gravity body's radius. In this view,
events can be measured from the radius and extending outward from the
radius, according to a mass total located at the radius, where the
radius itself is measured from a single point of center.

In questioning a mass augmentation effect in the gravity, the issue
can be more clear cut. Specifically, given a finite mass and a finite
radius, what gravity relativity effect is generated, and how much
does the effect increase the original mass generating the effect?.

From this steady stateness, it is obvious and easy to ask across to
special relativity wishing to know what velocity is required to generate
an identical effect.

However, in closer introspect, a greater question has also been asked.
And that is, given a mass enhancement and space contraction in special
relativity, at what velocity does a mass have to be moving in order
for it to transfigure into a black hole? Looking at things from another
point of view the question can be put in yet another way; to wit:

At what velocity does the mass have to be moving in order
for special relativistic effect (increasing the mass's mass
and collapsing its radius) to cause the mass's flow of time
to come to a standstill? The answer is found in the M+/R- ratio,
which is calculated through special relativity using the mass's
gravitational effect to state the equivalent relativistic velocity.

This type of thinking is out in the open in the material of Part 4.
It is summarized in the relationships enclosed in TABLE 8 under
'Pure Math Connectors' above.

 

 

 

FINISHED

 

 

 


Planetary Data is from the following reference source:

UNIVERSE by Don Dixon,       Houghton Mifflin Co.,
Boston, 1981                           (References found at
                                                the back of the book)


 

 

 

Signed:                                                          Greydon Moore

 

(C) 1990           Introduction to Mass Increases By Gravitational Relativity.
                        Greydon Moore Canada.

 

Peace Power and Plenty everyone.

 

 

 

ALL DONE