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INTRODUCTION TO MASS INCREASES
BY
GRAVITATIONAL
RELATIVITY |
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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. |
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GRAVITATIONAL RELATIVITY THEORY
CONNECTS CERTAIN SOLAR PLANET
MASSES |
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ALSO, GRAVITATIONAL AND SPECIAL RELATIVITY
THEORIES ARE INTRINSICALLY RELATED |
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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.
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ABSTRACT |
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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.
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PART
1 |
GRAVITATIONAL
RELATIVITY |
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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.
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PART
2 |
SPECIAL RELATIVITY
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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.
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PART
3 |
THE GOLDEN HARMONIC
RATIO |
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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.
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GRAVITATIONAL RELATIVITY
THEORY |
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GENERAL
INTRODUCTION for part 1 The Solar System |
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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.
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GRAVITATIONAL RELATIVISTIC
EFFECT |
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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
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GENERAL MASS QUANTA
EFFECT |
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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. |
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GRAVITATIONAL RELATIVISTIC
EFFECTS |
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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.
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ESTIMATED ACCURACY OF SOLAR
MASSES |
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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.
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BASIC
CONVENTIONS |
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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.
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INFERRING A GRAVITATIONAL RELATIVISTIC
AUGMENTED MASS VALUE FOR THE SUN
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TABLE 1: INFERRED
VALUES |
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MM |
= Existing Sun mass, presumed to
include original mass plus mass augmentation
K
=1.9909930 x 1033
grms |
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K |
= Gain in original mass of the
Sun, the amount of relativistic augmentation
due to the Sun's gravity
= 4.226490 x 1027
grms |
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Mbh |
= Mass of a black hole having an
event horizon equal to the Sun's radius
R
= 4.689536679 x 1038
grms |
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TABLE 1-A ESTABLISHED
VALUES |
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R |
= Existing Sun
radius
=6.96265 x 1010
cm |
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C |
= Speed of
light
= 2.99792458 x 1010
cm/sec |
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G |
= Universal gravitational
constant
= 6.6720 x 10-8
cm3/grms sec2 |
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CR |
= A physical constant for
Mass/Radius ratio of a black hole
= 6.735275620 x 1027
grms/cm |
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GH |
= Golden Harmonic
Ratio
= 1.61803398875
√GH =
1.272019649 |
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TABLE 2 |
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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 |
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TABLE 3
Certain terms are used
to generalize certain types of masses: |
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Low
mass
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Masses in the range of those found in this solar
system |
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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 |
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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
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Originating mass |
- |
Original mass accumulation without any
relativistic augmentation |
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Augmented mass |
- |
Existing mass assumed to include a change
from the originating mass due to relativistic effect of
gravity |
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Existing mass |
- |
As
physically measured, with any assumed augmentation present
in the measurement |
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Real
mass |
- |
A
real weight, in terms of a physical weight, for
instance measured in grms as if weighed on a
scale |
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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 ]
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VERIFYING A MASS OF
MM FOR THE SUN
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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.
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SPECIFIC MASS QUANTA
EFFECT | |
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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 MM–½j. 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). |
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VERIFYING THE COHERENT
½j STATES |
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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. |
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OTHER MASS AGGREGATE
STATES |
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|
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.
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OTHER MASS EFFECT
COHERENCIES |
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|
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 =
Kx
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
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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
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A COHERENT PHASE IN THIS
SOLAR SYSTEM |
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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.
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PART
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GRAVITATIONAL AND SPECIAL RELATIVITY
THEORY |
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GENERAL INTRODUCTION for part
2 |
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A COMPARISON
BETWEEN GRAVITATIONAL AND SPECIAL RELATIVITY |
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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.
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A UNISON BETWEEN GRAVITATIONAL AND SPECIAL
RELATIVITY | |
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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).
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THE GRAVITY - SPECIAL
RELATIVITY CONNECTION IN DETAIL |
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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
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A COMPARISON
BETWEEN GRAVITATIONAL AND SPECIAL RELATIVITY |
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In Equations U through X
which follow:
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(Eg) : |
is the effect (in gravity) for a
mass M in gravitational relativity |
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(Es) : |
is the effect (in special
relativity) for mass M in motion at a significant velocity in special
relativity |
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(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 |
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(Nx) : |
is the ratio of the black
hole mass Mbh, divided by the given mass M |
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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.
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A Support equation
for gravitational relativity follows next |
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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. |
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Summary
equations for the two modes of relativity follow next
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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
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
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Exact
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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
.
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.
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THE GOLDEN HARMONIC RATIO IN RELATIVITY
THEORY. A CRITICAL LIMIT IN THE
FOUNDATION OF GRAVITATIONAL RELATIVITY
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GENERAL INTRODUCTION for part
3 |
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TABLE 4 |
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KEY TERMS
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Mbh |
-
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Mass
of a black hole, having radius Rbh |
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Mo |
- |
An
original mass (before mass augmentation due to gravitational
relativity) |
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Ko |
- |
Mass
augmented upon mass Mo due to gravitational
relativity |
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M |
- |
An
existing mass, which includes: Mo + Ko |
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Mc |
- |
A Critical Mass Limit, where Mc is an Mo which
is less than Mbh by precisely the Golden Harmonic Ratio
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Rbh |
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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. | |
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TABLE 4 Continued |
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1/Ng |
-
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Ratio Mbh/Mc = 1/Ng when Mc = Mo, as when: Mbh/Mo = 1/Nx |
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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
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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 | |
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FUNCTIONAL
INTERPHASE BETWEEN
GRAVITATIONAL AND
SPECIAL RELATIVITY |
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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.
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?
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.
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.
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.
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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.
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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.
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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.
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A TEST
CASE:
GOLDEN HARMONIC RATIO IN THE TWO MODES
OF RELATIVITY |
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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:
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
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] |
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FOR SPECIAL RELATIVITY
EFFECT ON BOTH MASS AND RADIUS |
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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).
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'. |
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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.
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. |
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|
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.
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 ?
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/C2 ] =√[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/C2 ] = √[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 Egs.
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.
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SUMMARY
EQUATIONS |
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|
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/C2 ] =
√[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.
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UNIFIED EFFECTS IN FIELD
BEHAVIOR | |
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GENERAL
INTRODUCTION for part 4 Unified Fields
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'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.
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TEST CASE |
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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
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TABLE 4-A |
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ARBITRARY STUDY MODEL DATA |
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Nx =
1.000544617404 = (P + E) / E Mbh =
4.689536679 × 1038 grms |
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HIGH
mass1 = Mbh /
Nx
= 4.686984066 × 1038
grms
Nx = 1.000544617404 LOW
mass2 = Mass1 / 100,000
= 4.686984066 × 1038
grms
Nx = 100054.4617404
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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. |
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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/C2
] =
(Vx)2/C2
0.023330687 is effect
Egs of EQ
Z-17
Ess = [1 - Egs2] As in: [1 -
0.0233306872]= 0.999727802
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LOW special field effect
Ess is closing toward
1
V velocity is starting
to close toward 0 |
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Ess =
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0.999727802 |
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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 |
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Egs =
|
0..999995002 |
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|
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
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HIGH special field
effect
Ess
is closing toward
V velocity
is closing toward 1 |
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Ess =
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0.003161416 |
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COMPARING M+ AND R- RESULTS
FOR HIGH AND LOW MASSES |
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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
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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). |
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FIRST
INTERPRETATION |
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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.
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DIRECT
INTERPRETATION |
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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 |
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PURE MATH CONNECTORS
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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
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WHY Egs AND
Ess ARE INTRINSICALLY RELATED |
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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.
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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. |
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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.
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MASS DENSITIES IN A
CONSTANT RADIUS |
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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.
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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.
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Advanced details of a black hole,
such as a paradigm model of a charge membrane for instance, are not
considered.
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RELATIVISTIC MECHANICS
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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
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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
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Finding mass M' needed for
a
black hole whose
Schwarzschild
radius is given as
R' |
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GRAVITATIONAL
MECHANICS |
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EQUATION
6
M
= V2R
/G
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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
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Finding the orbit R of
a
body around a given mass
M
at a given orbital velocity
V |
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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
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|
Mercury |
= |
0.33020
|
× 1027
grms |
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| |
+
N2 |
|
Venus |
= |
4.8683
|
× 1027
grms |
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| |
+
N3 |
|
Earth |
=
|
5.9760 |
× 1027
grms |
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| |
+
N4 |
|
Mars |
= |
0.64181 |
× 1027
grms |
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| |
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= |
|
11.81631 |
× 1027
grms |
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½ |
|
= |
|
5.908155 |
× 1027
grms |
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| |
+
N5 |
|
Moon |
= |
0.07350
|
× 1027
grms |
|
| Equals |
N3x |
|
Earth |
= |
5.981655
|
× 1027
grms |
|
| Inequality |
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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.
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GENERAL MASS
CONGRESS
(summary)
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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 |
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Footnote 1 |
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RELATIVITY EQUIVALENCE
PRINCIPLE |
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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
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. |
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Footnote 2 |
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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.
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Footnote 3 |
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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.
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Footnote 4 |
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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.
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Footnote 5 |
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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 | |
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Footnote 6 |
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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
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Footnote 7 |
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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.
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FINISHED |
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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)
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Signed:
Greydon Moore
(C)
1990
Introduction to Mass Increases By Gravitational
Relativity.
Greydon Moore Canada. |
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Peace Power and Plenty
everyone. |
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ALL
DONE |