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Natural Science Forum / Physics / Relativity / December 2005



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Challenge to Tom Roberts

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David Thomson - 24 Dec 2005 17:36 GMT
Hi Tom,

I guess it is safe to say that you cannot calculate the nuclear binding

energy or nuclear binding force using QCD.  So I have earned another
point by developing a simple nuclear binding force equation and nuclear

binding energy equation that does something the SM and its sub theories

cannot.

People might think you would have the decency to admit that my theory
is useful and worth further pursuing after this monumental presentation

(as simple as it was).  Well, do you?

Dave

David Thomson wrote:
> Hi Tom,

> I'm still waiting for your presentation of calculating the nuclear
> binding force and energy for H4 using QCD.

> Dave

> David Thomson wrote:
> >> Be more specific, provide an equation that shows the units and
> > dimensions of the strong force.  For example, calculate the strong
> > force between two protons and two neutrons (H4).

> > My equation is fairly simple.  Let us calculate the strong force of the
> > berylium isotope Be11:

> > Z = 4  N = 11

> > strong binding force equation:
> > BNDF = k.c * Z * e.pmax^2 * N * e.nmax^2 / w.C^2

> > BNDF = 4.32 newton

> > (k.c = Coulomb's constant, e.pmax^2 = strong charge of proton, e.nmax^2
> > = strong charge of neutron, w.C = Compton wavelength, Z = number of
> > protons, N = number of neutrons)

> > To find the nuclear binding energy, use this form of the above
> > equation:
> > BNDE = k.c * Z * e.pmax^2 * N * e.nmax^2 / w.C

> > BNDE = 65.416 MeV

> > The actual measured binding energy of Beryllium 11 is 65.481 MeV.  The
> > difference between my calculated value and the measured value is that
> > my calculation is simplified and does not take into account the
> > distortion caused by the twisting of the Aether.  Naturally I chose an
> > isotope with nearly zero net distortion.

> > But let us see the simple force law that you are discussing and how it
> > maintains the dimensions throughout the equations.
Eric Gisse - 24 Dec 2005 20:23 GMT
[snip]

Do you even know calculus?

You show no signs of having an education in either physics or
mathematics...
David Thomson - 24 Dec 2005 22:54 GMT
> Do you even know calculus?
>
> You show no signs of having an education in either physics or
> mathematics...

Do you know algebra?  I have presented a working formula using simple
algebra.  Can you beat that by calculating the binding forces or
binding energies of isotopes using *any* method of mathematics?

I can do calculus, but that is completely irrelevant to the challenge.
Tom wanted to see my theory do something, so I showed him how easy it
is to calculate nuclear binding energies and binding forces.  Are you
going to ignore the functionality of my theory, too, and just blow more
hot air?  What's wrong with you guys?

Dave
Tom Roberts - 24 Dec 2005 22:49 GMT
> Hi Tom,
> I guess it is safe to say that you cannot calculate the nuclear binding
> energy or nuclear binding force using QCD.

Yes, I cannot do that. <shrug>

> So I have earned another
> point by developing a simple nuclear binding force equation and nuclear
> binding energy equation that does something the SM and its sub theories
> cannot.

I have no idea what sort of "point" that would be.

More to the point, what _experimental_ test could be applied?

Tom Roberts    tjroberts@lucent.com
David Thomson - 24 Dec 2005 23:00 GMT
> > Hi Tom,
> > I guess it is safe to say that you cannot calculate the nuclear binding
> > energy or nuclear binding force using QCD.
>
> Yes, I cannot do that. <shrug>

Well, you wanted to see what my theory does that the SM does not.  Now
you have it. <shrug>

> > So I have earned another
> > point by developing a simple nuclear binding force equation and nuclear
> > binding energy equation that does something the SM and its sub theories
> > cannot.
>
> I have no idea what sort of "point" that would be.

The point is that I have once again delivered real results with my
physics theory.  You keep blabbing that it doesn't do anything.  I keep
showing you what the Aether Physics Model can do.  So what are you
going to do now?  Just ignore it?

> More to the point, what _experimental_ test could be applied?

What more do you need?  I have given you the equation, just calculate a
nuclear binding energy, measure it, and see how they compare.  You can
also use the nuclear force equation and see if the amount of force
needed to separate a deuterium atom matches the predicted force of the
equation.  

Dave
Bilge - 25 Dec 2005 16:32 GMT
David Thomson:
>> > Hi Tom,
>> > I guess it is safe to say that you cannot calculate the nuclear binding
[quoted text clipped - 4 lines]
>Well, you wanted to see what my theory does that the SM does not.  Now
>you have it. <shrug>

 The standard model also isn't useful for comparing the mass of
two cannon balls from a measure of muzzle velocity obtained from
a carefully measured amount of powder.

[...]

>> I have no idea what sort of "point" that would be.
>
>The point is that I have once again delivered real results with my
>physics theory.

 You mean by comparing apples to oranges? How about a test that
compares apples to apples, like say your model against the nuclear
shell model?

[...]

>> More to the point, what _experimental_ test could be applied?
>
[quoted text clipped - 3 lines]
>needed to separate a deuterium atom matches the predicted force of the
>equation.  

 And what does your model say about the shape of the deuteron?
Why is there no 2He or dineutron? How about 5H, 5He, 5Li, 5Be,
etc.? What does your model say about 8Be?
David Thomson - 25 Dec 2005 22:31 GMT
>  >> > I guess it is safe to say that you cannot calculate the nuclear binding
>  >> > energy or nuclear binding force using QCD.
[quoted text clipped - 7 lines]
> two cannon balls from a measure of muzzle velocity obtained from
> a carefully measured amount of powder.

Bilge, of all people, I would expect better from you.  You are quite
aware how important a Unified Force Theory and nuclear binding energy
equation should be to modern physics.

>   You mean by comparing apples to oranges? How about a test that
> compares apples to apples, like say your model against the nuclear
> shell model?

The Aether Physics Model incorporates the Linus Pauling Spheron model.

>  >> More to the point, what _experimental_ test could be applied?
>  >
[quoted text clipped - 7 lines]
> Why is there no 2He or dineutron? How about 5H, 5He, 5Li, 5Be,
> etc.? What does your model say about 8Be?

Are we jumping through hoops again?  How about some feedback on the
questions I have already answered?

My model predicts the shape of the deuteron as seen on this page:
http://www.jlab.org/highlights/nuclear/Nuclear.html

I'm aware that the shapes of other isotope nuclei have been determined
by the SM, but I haven't gone as far down this road.  Having deduced
the shape of the space-time in which the subatomic particles exist, I
was able to predict the simple condition of one proton and one neutron
quite easily.  I'm sure the geometry of the other isotopes can be
predicted from the theory and that doing so will increase the accuracy
of the nuclear binding energy and nuclear binding force equations to
near exact.  This is one of the things I have not yet had the resources
to pursue.  If you were so inclined, you could be the first to
determine this and get the credit for yourself.

Dave
Bilge - 26 Dec 2005 08:52 GMT
David Thomson:
>>  >> > I guess it is safe to say that you cannot calculate the nuclear binding
>>  >> > energy or nuclear binding force using QCD.
[quoted text clipped - 11 lines]
>aware how important a Unified Force Theory and nuclear binding energy
>equation should be to modern physics.

 I am aware of a lot of things, one of which is that you don't have
a model than answer anything related to those topics. I have plenty
of examples you can use to try and make your case, though. So far, you
have successfully avoided making your case.

>>   You mean by comparing apples to oranges? How about a test that
>> compares apples to apples, like say your model against the nuclear
>> shell model?
>
>The Aether Physics Model incorporates the Linus Pauling Spheron model.

 I don't care if incorporates cake frosting, you didn't answer
the question.

[...]
>>   And what does your model say about the shape of the deuteron?
>> Why is there no 2He or dineutron? How about 5H, 5He, 5Li, 5Be,
>> etc.? What does your model say about 8Be?
>
>Are we jumping through hoops again?

 Since you are claiming to have a theory of something, jumping
through hoops is your job. If you don't like the work, don't do
it. If you can't get through the few simple tasks I've set out,
you have no chance under any serious scrutiny.

>How about some feedback on the questions I have already answered?

 You haven't answered any questions.

>My model predicts the shape of the deuteron as seen on this page:
>http://www.jlab.org/highlights/nuclear/Nuclear.html

 Last time I checked, you weren't the jefferson labs. If I wanted
the information on that url, I could have just asked myself for it.
The next time you post a reference to work that is not yours and
claim you can reproduce it, I'm going to be a lot less user friendly.
 
>I'm aware that the shapes of other isotope nuclei have been determined
>by the SM, but I haven't gone as far down this road.

 Apparently, you aren't aware of what the standard model is, since
you keep invoking it to refer to nuclear physics but not any of
the nuclear physics of interest to the standard model.
David Thomson - 26 Dec 2005 15:16 GMT
>   Since you are claiming to have a theory of something, jumping
> through hoops is your job. If you don't like the work, don't do
> it.

If I don't like the fact that you have ignored all my answers in the
past, I will just continue to ignore your disingenuous hoopla.

> If you can't get through the few simple tasks I've set out,
> you have no chance under any serious scrutiny.

That's what you think.  I have actually been getting lots of interest
in my theories, lately.  I just met with a former government contractor
who has worked closely with certain prominent universities, who made
phone calls and arranged for my work to be carefully reviewed.

You're just a hobby to me.

>  >How about some feedback on the questions I have already answered?
>
>   You haven't answered any questions.

Go back and read my posts, rather than make assumptions.

>  >My model predicts the shape of the deuteron as seen on this page:
>  >http://www.jlab.org/highlights/nuclear/Nuclear.html
[quoted text clipped - 3 lines]
> The next time you post a reference to work that is not yours and
> claim you can reproduce it, I'm going to be a lot less user friendly.

LOL.  When have you *ever* been friendly?  If you want to see how my
theory predicts the structure of the deuteron, then read it.  Don't ask
me to continually reproduce it in plain text.  When you get up off your
duff and actually start commenting on my work, rather than
demonstrating your lack of critical analysis skills, I'll reconsider
just how genuine I think your intentions are.

>  >I'm aware that the shapes of other isotope nuclei have been determined
>  >by the SM, but I haven't gone as far down this road.
>
>   Apparently, you aren't aware of what the standard model is, since
> you keep invoking it to refer to nuclear physics but not any of
> the nuclear physics of interest to the standard model.

You are so lame.

Dave
Bilge - 27 Dec 2005 15:52 GMT
David Thomson:
>>   Since you are claiming to have a theory of something, jumping
>> through hoops is your job. If you don't like the work, don't do
>> it.
>
>If I don't like the fact that you have ignored all my answers in the
>past, I will just continue to ignore your disingenuous hoopla.

 You've never answered any question you've ever been asked.

>> If you can't get through the few simple tasks I've set out,
>> you have no chance under any serious scrutiny.
[quoted text clipped - 3 lines]
>who has worked closely with certain prominent universities, who made
>phone calls and arranged for my work to be carefully reviewed.

 The University of PO Box 2005 doesn't count.

>You're just a hobby to me.

 Flattery will get you nowhere.

>>  >How about some feedback on the questions I have already answered?
>>
>>   You haven't answered any questions.
>
>Go back and read my posts, rather than make assumptions.

 Non-reponsive.
Bilge - 25 Dec 2005 16:02 GMT
David Thomson:
>Hi Tom,
>
[quoted text clipped - 3 lines]
>binding energy equation that does something the SM and its sub theories
>cannot.

 Care to test your equation for the nuclear binding? OK, since
you insist, calculate the mass difference between, 3He-3H,
41Ca-41Sc, 57Ni-57Cu and explain the masses. Note that each of
those are single particle mirror nuclei, so the the differ
by the difference in the neutron/proton mass and the difference
in coulomb energy (plus whatever explanation you have for anything
left over). You should be able to match all of the experimental
data including the nuclear radius and a structure which is
consistent with the observed transitions between states (esp.
the beta decay between the mirror nuclei.)

>People might think you would have the decency to admit that my theory
>is useful and worth further pursuing after this monumental presentation
>(as simple as it was).

 Why is that? I can find lots of empirical and semi-empirical
binding energy formulae for nuclei. The last thing anyone needs
or cares about is yet another empirical mass formula. Finding
one that can explain the detailed nuclear structure is a little
harder.
David Thomson - 25 Dec 2005 22:58 GMT
>   Care to test your equation for the nuclear binding? OK, since
> you insist, calculate the mass difference between, 3He-3H,
[quoted text clipped - 6 lines]
> consistent with the observed transitions between states (esp.
> the beta decay between the mirror nuclei.)

I will gladly calculate the above masses using my equations.  But
first, I would like to see your calculation of 11Be nuclear binding
energy using QCD.  I'm curious to see whether or not it can be done.

>  >People might think you would have the decency to admit that my theory
>  >is useful and worth further pursuing after this monumental presentation
[quoted text clipped - 5 lines]
> one that can explain the detailed nuclear structure is a little
> harder.

First of all, I am not aware of a single formula for calculating *all*
the nuclear binding energies, let alone the nuclear binding forces,
other than my own formula.  My theory, as I have often explained on
these newsgroups, geometrically quantifies space-time, the subatomic
particles, and the force laws into a coherent Theory of Everything.
The nuclear binding energy equations I produce, while not yet
perfected, were derived from *first principles*, not from the empirical
data.  The equations describing the space-time, particulate, and force
structures of the quantum realm *were* derived from empirical data.
The empirical nuclear binding energy data merely confirms the formula I
derived from first principles is on the right track.

Also, my formula is not a "mass" formula per se, it is a "strong
charge" formula.  That is, because the Aether Physics Model quantifies
the strong charge in compatible dimensions with mass, we can directly
calculate the strong force and binding energies directly using a simple
force law.  Knowing there is a precise mass to strong charge ratio that
is consistent throughout the Universe, we can then convert the strong
charge to mass, and we can also directly convert the strong charge to
angular momentum via the universal conductance constant.

I await your demonstration of the QCD, or even a simple statement that
it cannot be done.  Then I will do the equations you requested.

Dave
Bill Hobba - 25 Dec 2005 23:28 GMT
>>   Care to test your equation for the nuclear binding? OK, since
>> you insist, calculate the mass difference between, 3He-3H,
[quoted text clipped - 8 lines]
>
> I will gladly calculate the above masses using my equations.

Then stop evading, shut up, and do it.

Rest of evasive junk snipped.

Bill
David Thomson - 26 Dec 2005 01:59 GMT
> > I will gladly calculate the above masses using my equations.
> Then stop evading, shut up, and do it.
> Rest of evasive junk snipped.

Don't be such a snot.  I have put up with you guy's crap long enough.
If you're going to make me jump through hoops, you can jump through of
few yourself.

Dave
Bill Hobba - 26 Dec 2005 08:19 GMT
>> > I will gladly calculate the above masses using my equations.
>> Then stop evading, shut up, and do it.
>> Rest of evasive junk snipped.
>
> Don't be such a snot.

Quit evading.  You claimed you can answer Bilge's question - do it.

>  I have put up with you guy's crap long enough.

More like we have put up with your crap for too long.  Answer the question
or be branded for what you so obviously are - both a liar and an idiot.

> If you're going to make me jump through hoops,

If you can't jump through the hoop don't claim you can.

> you can jump through of few yourself.

All you really are doing is confirming what Dirk has already documented -
namely your Sucking Logic, Sucking Algebra, Sucking Attitude, Sucking
Thumbs, the deadly combination of  IGNORANCE and ARROGANCE, topped with a
coulis of SELF-RESPECT as from now known under the name ARROGNORANCE
http://users.pandora.be/vdmoortel/dirk/Physics/ImmortalFumbles.html

Bill
David Thomson - 26 Dec 2005 15:17 GMT
<hot air snipped>

Did you say something?  

Dave
Bill Hobba - 26 Dec 2005 23:38 GMT
> <hot air snipped>
>
> Did you say something?

Yes -but as usual you were not listening.

Bill

> Dave
David Thomson - 27 Dec 2005 15:10 GMT
> > <hot air snipped>
> >
> > Did you say something?
>
> Yes -but as usual you were not listening.

I'm too busy working with actual science to be bothered listening to
your boring and unfounded personal opinions.

Dave
Eric Gisse - 27 Dec 2005 23:34 GMT
> > > <hot air snipped>
> > >
[quoted text clipped - 4 lines]
> I'm too busy working with actual science to be bothered listening to
> your boring and unfounded personal opinions.

So you are finally making the long-awaited sojourn to a library to be
introduced to mid-20th century physics?

> Dave
Bilge - 26 Dec 2005 08:34 GMT
David Thomson:
>>   Care to test your equation for the nuclear binding? OK, since
>> you insist, calculate the mass difference between, 3He-3H,
[quoted text clipped - 8 lines]
>
>I will gladly calculate the above masses using my equations.

 No, you won't and in any case, I asked for more than just the
masses. As I have mentioned previously, there are lots of formulae
one can use to obtain the mass of a nucleus, the liquid drop model
and the garvey-kelson mass formula are but two.

>But
>first, I would like to see your calculation of 11Be nuclear binding
>energy using QCD.  I'm curious to see whether or not it can be done.

 You don't read very well. One cannot calculate the mass of a large
nucleus using QCD, nor is it ever likely anyone would expect such
a calculation to be done any more than anyone expects to start with
the coulomb interaction and predict global weather patterns. Do
you really have even a hint of what qcd is or are you just engaging
in self-promotion by picking up buzzwords? Try comparing your model
to the nuclear shell model and see if you can even get within striking
distance of the most naive shell model predictions. What you have
done is called fitting data.

>>   Why is that? I can find lots of empirical and semi-empirical
>> binding energy formulae for nuclei. The last thing anyone needs
[quoted text clipped - 4 lines]
>First of all, I am not aware of a single formula for calculating *all*
>the nuclear binding energies, let alone the nuclear binding forces,

 Since I've told you before of a number of such formulae, that
ruse won't fly. In any case, if you are going to claim to be doing
research, it's your responsibility to know.

>other than my own formula.  My theory, as I have often explained on
>these newsgroups, geometrically quantifies space-time, the subatomic
>particles, and the force laws into a coherent Theory of Everything.

 Can the crap. You can't even explain nuclear structure, much less
anything more difficult. Don't say you can unless you are in a
position to demonstrate it using an example or two that I will
supply.

>The nuclear binding energy equations I produce, while not yet
>perfected, were derived from *first principles*, not from the empirical
>data.

 Be serious. There is nothing remotely resembling first, second or
even third principles in your fits.
kenseto - 26 Dec 2005 14:26 GMT
> >   Care to test your equation for the nuclear binding? OK, since
> > you insist, calculate the mass difference between, 3He-3H,
[quoted text clipped - 41 lines]
> charge to mass, and we can also directly convert the strong charge to
> angular momentum via the universal conductance constant.

One dumb question:
If your equations are different than current physics then how come they give
the same correct numerical predictions as current physics equations for all
experiments??

Ken Seto
David Thomson - 26 Dec 2005 15:05 GMT
> One dumb question:
> If your equations are different than current physics then how come they give
> the same correct numerical predictions as current physics equations for all
> experiments??

Hi Ken,

If you read the posts carefully, you'll notice that there are no
equations in the SM that compare to mine.  The only way the SM can
calculate nuclear binding energies is to measure them first and then
back calculate a so-called "mass defect."  This mass defect is then
reused to "calculate" the nuclear binding energy.

My equations are based upon a strong force law, and recently I have
also been able to refine the equation to account for the proton and
neutron's magnetic moments.  As it stands right now, my equation when
applied to all the known isotopes, calculates the nuclear binding
energies to within an average 92.58% accuracy.  The equation as it
stands now is particularly accurate for the isotopes near the elements
of iron and nickel, the most stable in terms of binding energy per
nucleon.

You might think there are equations that predict the nuclear binding
energies in the SM, but they simply do not exist.  There have been some
particularly numerical attempts to predict the nuclear binding
energies, but they were truly data fitting techniques.  My equations
are firmly rooted in a strong force law I have developed and the
relationships of subatomic particle magnetic moments.  I suspect the
third part of the equation will be related to the spin structure of the
space-time in which the subatomic particles exist (Aether).  I've had
some insights into how this might work just recently and have been
working on it.

Dave
Dirk Van de moortel - 26 Dec 2005 15:29 GMT
> > One dumb question:
> > If your equations are different than current physics then how come they give
> > the same correct numerical predictions as current physics equations for all
> > experiments??

:-))

> Hi Ken,

Beaten by the biggest imbecile of the club.
Congratulations.
To both of you.

Dirk Vdm
kenseto - 26 Dec 2005 15:44 GMT
> > One dumb question:
> > If your equations are different than current physics then how come they give
[quoted text clipped - 8 lines]
> back calculate a so-called "mass defect."  This mass defect is then
> reused to "calculate" the nuclear binding energy.

I was under the impression that you have different equations for all
interactions....not just the nuclear binding energies. I am wrong on that
assumption? Also what about relativity?...do you have different equations
than SR/GR? Thanks.

Ken Seto

> My equations are based upon a strong force law, and recently I have
> also been able to refine the equation to account for the proton and
[quoted text clipped - 17 lines]
>
> Dave
David Thomson - 30 Dec 2005 17:42 GMT
> "David Thomson" <google@volantis.org> wrote in message
> > If you read the posts carefully, you'll notice that there are no
[quoted text clipped - 7 lines]
> assumption? Also what about relativity?...do you have different equations
> than SR/GR? Thanks.

No, I do not have different equations for all interactions.  My
equations are based upon the known equations and interactions.  I have
developed a completely new level of physics, which describes the
*structure* of the quantum realm.  The only thing my theory replaces
are the nonsensical interpretations of wave/particle duality,
probability functions, force particles, and such.  I provide a
quantified alternative to these mythological descriptions of quantum
structure.  I determined this quantified structure from analyzing the
same empirical data and equations that these mythological
interpretations were attributed to.

My theory also shows an alternative explanation to General Relativity
theory.  Instead of seeing the Einstein tensors as being gravitational,
they are shown to be electrical.  The tug is not between a geometric
curvature tensor and mass/energy tensor, but between the electrostatic
charge of the Aether and the strong charge of matter.  My theory
clearly and simply quantifies the dimension of mass as being orthogonal
to the dimension of charge, and thus the two are always directly
proportional to each other.  Thus, Einstein can develop GR based upon
gravity and I can explain it based upon charge, and we would come up
with the same result.  The difference, however, is that the electrical
interpretation has far more practical use in engineering than does the
gravitational interpretation.  With the electrical interpretation, the
Electric Universe theory comes alive but we can also understand the
electrostatic propulsion effect, engineered distortions of space-time,
signalling without photons, tapping the vast sea of dark matter for
free energy, and numerous other applications.

Einstein's simlifed field equation is:

G = 8pi T

mine is:

e^2 = 8pi (e.emax^2 * a)

where e^2 is the electrostatic charge, e.emax^2 is the strong charge,
and a is the fine structure of the electron.  The above equation is an
expression of the Unified Charge Equation and there exists a unique
unified charge equation for each subatomic particle.

My theory does not forage deeply into the physics of describing *how*
things work.  It is from the physics of *how* things work that the APM
can describe *what it is that is doing the work."  From this
quantification of quantum structure it is then possible to extend
physics into areas that today are merely called "anomalies."  Also,
from this quantification of quantum structure we can clearly eliminate
the nonsensical interpretations that attempted to describe the quantum
structures.

Dave
Eric Gisse - 30 Dec 2005 18:16 GMT
> > "David Thomson" <google@volantis.org> wrote in message
> > > If you read the posts carefully, you'll notice that there are no
[quoted text clipped - 18 lines]
> same empirical data and equations that these mythological
> interpretations were attributed to.

HA HA HA HA.

You propose to overwrite all of quantum physics yet you can't replicate
any of its' predictions?

You claim you base your theory off "empirical data" yet you cannot even
be bothered to search the archives of the two journals you have access
to for evidence that blatently contradicts your theory?

> My theory also shows an alternative explanation to General Relativity
> theory.  Instead of seeing the Einstein tensors as being gravitational,
[quoted text clipped - 12 lines]
> signalling without photons, tapping the vast sea of dark matter for
> free energy, and numerous other applications.

More babble which means f.ck-all.

> Einstein's simlifed field equation is:
>
> G = 8pi T

Are you even capable of solving this field equation? If I gave you the
stress-energy tensor for a perfect fluid could you give me all, if any,
of the nonzero connection coefficients?

> mine is:
>
> e^2 = 8pi (e.emax^2 * a)

This isn't a field equation.

> where e^2 is the electrostatic charge, e.emax^2 is the strong charge,
> and a is the fine structure of the electron.  The above equation is an
> expression of the Unified Charge Equation and there exists a unique
> unified charge equation for each subatomic particle.

Why don't you use your 'field equation' to develop these 'unified
charge equations' ?

> My theory does not forage deeply into the physics of describing *how*
> things work.  It is from the physics of *how* things work that the APM
[quoted text clipped - 4 lines]
> the nonsensical interpretations that attempted to describe the quantum
> structures.

Just because you don't understand it does not mean it is nonsense.

> Dave

I thought you were going to spend more time doing 'real physics' or
somesuch?
 
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