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THE UNIVERSAL
GRAVITATIONAL CONSTANT It occurred to me some time ago that the Universal
Gravitational Constant—usually signified by the variable G—might be the
key to unlocking the secret to gravity, among other things. It has always
seemed puzzling that a constant should have so many unexplained
dimensions. A complex constant like that is normally a sign of incomplete
theory. All the known concepts are assigned variables and the unknowns are
lumped together in a constant. The numerical value is not such a puzzle,
since it may just be an expression of incommensurate initial definitions.
For instance, we chose the length of the meter and the second and so on
pretty much arbitrarily, so it shouldn't be a surprise when all our
numbers don't match up at first. But G is not just a number. It has lots
of dimensions, L3/MT2. Could there be a secret
locked up in those dimensions?
I am not the first to ask that question, but no one has yet
presented us with any major secrets. Historically, the door for serious
questioning was not open that long. Newton's theory became dogma so
quickly that very few scientists had the gumption to look hard at it. The
ones who did found it mostly convincing or mostly opaque. Since the time
of Einstein, no one has taken the constant seriously. It is a piece of
discarded and superceded math. To the contemporary physicist, G is about
as interesting as the constants of Archimedes or Toltec hieroglyphics.
Einstein gave us a new math to express the gravitational field, leaving
the mysteries of Newton behind. But Einstein's new math and theory did not
dispense with the old mysteries. In many ways it simply changed the text
of the mystery. It substituted a new problem for an old one.
This paper is not concerned with
critiquing the math of General Relativity. Here it is enough to point out
that the mechanism of gravity is admitted to remain a mystery to this day.
Relativity describes the gravitational field in ways that are
mathematically superior to Newton. It cannot be denied that Einstein at
the very least updated the math to include the finite speed of light c—a
constant that was unknown in the time of Newton. The finite speed of light
implied a difference in measurement of variables between an object and its
observer, as well as a difference among various observers, so that even
Newton would have admitted the necessity of a mathematical update. By
returning to Newton's equations I am in no way questioning the truth or
usefulness of Relativity as a whole. I feel I must preface every one of my
gravitational and relativistic papers by saying that I am convinced beyond
any doubt of time dilation, length contraction and mass increase; I will
say it again here. I am returning to Newton's gravitational math not to
argue for its historical superiority, but only to answer questions that
have remained even after Einstein. No one denies that these questions
remain; no one denies that gravity remains mysterious in many ways. Nor
will anyone deny that gravity has resisted being incorporated into QED or
unification theories. In
this paper I will show that by studying the foundational theory of gravity
a bit more closely we can arrive at a better understanding of both mass
and gravity. By doing simple algebraic operations on Newton's equations we
can derive new knowledge. This knowledge will allow us to discover many
things that have so far been hidden. The most important of these is tying
the classical equations of Newton to unexplained numbers coming out of
particle accelerators. In this paper I will provide the mathematical link
between Newton's classical equations of gravity and the equations of mass
increase of Einstein. In doing this I will mathematically derive the limit
for mass increase for the proton. Until now, this experimental limit has
been a mystery. Neither Relativity nor QED has been able to explain the
number 108 for the ratio of moving mass to rest mass for the proton. I
will derive it with simple high-school algebra and a few simple
theoretical postulates. Let there be two equal spheres of radius r
touching at a point. We know that according to the theories of Newton and
Einstein there must be a gravitational force at that point, but neither
math allows us to calculate it. Newton's math cannot apply since there is
no distance between the objects; Einstein's math cannot apply because
there is no field at a point. Both theories solve this problem in their
own ways, it is true. They add further theory that allows them to
calculate in this predicament. In a nutshell they both propose a field
centered about a point or a singularity. This causes further problems due
to the fact that the objects' gravitational strengths are determined by
their masses, and all mass cannot be found at a point. By current theory,
mass resides in matter, and matter is made up of atoms. These atoms have
real positions: they are found throughout the object—at its outer shell
just as at its core. If the mass is a summation of atomic masses, then the
force must be a summation of atomic forces. It is difficult to see how the
center of force can be behind (in a directional sense) half the mass that
causes the force. We can
bypass these further theoretical questions by continuing to propose simple
new theory. To do this, let us move our twin spheres s distance apart for
a moment. If there is a gravitational force, then after a time interval
Δt, this distance will diminish by Δs. Why has the distance diminished?
Because a force between the two spheres pulled them closer—this is the
classical and current interpretation given to the situation. But can we
give it another interpretation? Yes, we can say that both spheres are
expanding and that they moved into the distance between them. By the
classical interpretation, the centers of the spheres moved toward
eachother. By my interpretation, they did not. Of course, people living on
the surface of the spheres would define "getting closer" by the idea of
"less distance between the spheres," especially if they did not know the
spheres were expanding. With
my change in theory, you can see that we no longer have to assign Δs to
the diminishing distance between the spheres. We can assign it to a change
in the radii of the spheres. This being so, we can move the spheres back
together, touching at a point. After a time Δt, the radius of each sphere
will have changed Δs/2.
a = m/r2 Notice that
L3/T2 may be thought of as the acceleration of a
volume, or a three-dimensional acceleration. This is very
suggestive. This passing idea
of Maxwell caused me to reconsider the concept of mass. His math is true,
except for one thing. His first equation is not really correct. As written
it should be a proportionality. To be an equation requires the constant
G. a = Gm/r2 The dimensions of G are L3/MT2,
which gives the mass and acceleration the correct current dimensions. But
what if G is a sort of mirage or misdirection? To pursue this further, I
went to Newton's gravity equation, like Maxwell had. F =
Gmm/r2 We must have a 2 on the
right side, since the force equation for gravity is the force between two
masses, but the force that causes an acceleration on the other side of the
equality applies to only one of the masses. It is customary to give all
the acceleration to one of the masses, but in my thought problem the two
equal spheres both accelerate. Now let us apply this equation to our twin
spheres touching at a point. There is no distance between the spheres, so
r would normally apply to the distance from center to center. But since
the spheres are the same size, let us re-assign r to the radius of each
sphere. The distance from center to center is then 2r. We have assigned Δs
to a change in the radius instead of a change in the distance between the
spheres, and this allows us to calculate even when the spheres are
touching. For clarity let us make Δs into Δr. a/2 =
Gm/(2r)2 The only
remaining problem is the variable r. If the spheres are expanding, then r
must be expanding. After time Δt, the radius will be r + Δr. After any
appreciable amount of time, r will be negligible in relation to Δr, so
that Δr ≈ r + Δr. Therefore we may simply drop the r variable as a
variable that approaches zero. 4Δr2/Δt2 = Gm/Δr
Now all we have to do is reassign the dimensions of
L3/T2 to the mass, as Maxwell implicitly suggested.
We will drop the dimension M altogether. This gives G no dimensions at
all. It is just a number. This is actually much more sensible, since
constants with dimensions are a sign of incomplete theory. That is what
drew me to this solution in the first place. Newton had to give the
dimensions L3/MT2 to G only because he had
mistakenly assigned mass a new dimension. Mass is not a new dimension. It
is reducible to the old fundamental dimensions of length and
time. Our last problem is
plugging known values into this new equation. At first it looks like the
mass should be changing over time, since the radius is changing. But no.
The mass is dependent on Δr/Δt2, and that is not changing over
time. As the radius gets larger, so does the change in time, so that the
ratio is constant. It is a constant acceleration. A constant acceleration
gives us a constant mass. Therefore we can plug known values for m into
this equation. m = 4Δr3/GΔt2
For the proton, this yieldsa = 6.06 x
10-13m/s2 So, at this point we have not applied
the math to density. The math above applies to simple structural spheres,
and in this case the mass is no function of density—since the sphere has
no content. A proton may be assumed to act (nearly) like a simple
structural sphere, but a large object like the earth will not. Therefore
these equations may not be applied to complex masses without further
additions of theory and math. Clearly this math will provide us with an
acceleration of the outer shell of the complex mass given its composition.
This composition will include factors like density, since a summation of
internal motions must take into account the number of particles in the
composition and their effects on one another. In fact, this calculation of
a summation will mirror the current calculation, except that current
calculations explain the genesis of micro-forces in one way and my theory
does so in another way. That is, current calculations would find a
summation of atomic masses. My calculations would find a summation of
atomic motions. Mathematically my new equations may not much affect the
calculated accelerations of large objects, although they will drastically
affect the foundational theory. Treating the proton as a composite itself, as we believe that it
is, will undoubtedly affect my math above in small ways. The proton cannot
be treated as an expanding shell anymore than the earth can. However, my
intent with this paper is not to achieve numbers that are correct all the
way down to the quark, it is to suggest foundational changes in theory
that will allow us to explain various phenomena that are so far
unexplainable. I have done that, and adding the more complex math to this
paper would only undercut its clarity. If the proton has a residual
acceleration due to mass, then in any one direction it will have a
velocity at any given time. If we suppose that the age of the proton is on
the order of the age of the universe, then we can estimate the current
velocity of the shell of the proton. "Velocity relative to what?" you may
ask. "If everything is expanding, then what is our background?" The
velocity we will find must be relative to two things. It is relative to
the velocity of the radius at t0, which we define as zero. And,
it is relative to the speed of light, c. Einstein defined the speed of
light as the universal background, and I continue to accept that
definition. If we accept
(one of) the current estimates for the age of the universe as around 20
billion years, then the current velocity of the proton's shell would be
3.8 x 105m/s. v = at = (6.06 x 10-13m/s2 )(6.3 x
1017s) = 3.8 x 105m/s That seems ridiculously large at first, except that we have
experimental confirmation of a number in that ballpark from accelerators.
As I have shown in my paper on accelerators, there is a limit to the speed
achieved by the proton. This limit is a final energy of about 108 times
the rest energy. Using gamma, this translates to a velocity of
.999957c, which is 1.2 x 104m/s short of c. If we theorize that
the gap between c and the limit in velocity is caused by a residual
velocity or velocity equivalent that the proton already has, then the
limit is explained. That is the link between this paper and my paper on
the accelerator. But there
is more. My correction to gamma and to the mass increase equations
predicts a limit in velocity for the proton of .9930474c, which is 2.1 x
106m/s short of c. This turns out to be a much better number.
Using gamma gives us an age of the universe of only 600 million
years. My correction gives us an age of 110 billion years. This only
exceeds current models by a factor of five. Estimating the age of the
universe or elementary particles is very speculative, and estimates have
continued to increase over the last 50 years. On the other hand, we know
that protons must be older than 600 million years. The earth is almost ten
times older than that itself. .7/x = x/r As an example,
we now use the cesium atom to define time. The baseline data in the cesium
atom is an oscillation from one energy level to the other, or an atomic
wobble. This oscillation is a motion, and all motion implies a distance.
If the cesium atom gets bigger, then the distance increases, and the time
period increases. Time is dependent on distance. This is even clearer with
a pendulum clock. If all material lengths increase, then the length of the
pendulum will of course increase, which will increase the length of the
second. Time is connected definitionally and operationally to distance,
therefore any increase in universal length will cause a proportional
increase in universal time. Since velocity is defined as one over the
other, velocity will not change. The numerator and denominator both get
bigger at the same rate. |