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This article is in four sections.
Emisson-Absorption-Scattering (EAS) Sub-Quantum Physics
EAS Nuclear Glue
EAS Neutron Beta Decay
EAS Mass Excess
EAS Mass Excess
Robert S. Fritzius
Installed sometime prior to 4 Mar 2001. Latest update 03 Nov 2017.
New or modified entries are in bold.
Serious reconstruction underway. Please drive Carefully.
This page started as an explanation for the difference between the mass
of a neutron and the sum of the masses of its ponderable decay products, i.e., a proton and
an electron. It is being modified to maybe provide a rationale for nuclear
Mass Excess/(Mass Defect).
On atomic and nuclear scales we deduce mass electromagnetically.
That is, if we want to know the masses of specific nuclei or of electrons,
we subject them to known electrical and/or magnetic fields and by
observing their trajectories or their changes in velocity we calculate
or deduce their masses. We do not actually measure ponderable amounts
Since neutrons are electrically neutral we "measure" the masses of
differing isotopes of an atom, then deduce neutron masses based on the
differences and energy input/output considerations.
(Added 26 Sep 2005.)
The EAS model of sub-quantum physics holds that the visibility of a
given nucleus or ion, with respect to its electrodynamic environment is
inversely proportional to what we call its mass. The model
also holds that the superposition principle (for calculating electrical
forces in many-body systems) does not strictly apply. In my
opinion, the superposition principle is a powerful tool
for first order effects, but in a many-body scenario it has a tinge of
action-without-reaction. It says that electrical charges
can be affected by an electrical field without the field expending any
energy in the process.
In the Emission-Absorption-Scattering (EAS) model, positively charged bodies
emit positive sub-atomic chargelets which are (elastically) scattered by other
positively charged bodies and are (inelastically) absorbed by negatively
charged bodies. Negatively charged bodies emit negative chargelets which
are scattered (elastically) by other negatively charged bodies and are
(inelastically) absorbed by positively charged bodies.
Because of the chargelet collisons just mentioned, like-charged particles
are more or less visibly opaque to one another. For
example, if a positive chargelet, which could have interacted with a
given proton, doesn't reach it, because it was scattered by an intervening
proton, then a kind of electrodynamic shielding would be taking place. The
opaqueness of like charged bodies for one another thus produces a reduction in the
effect of the external electrodynamic environment on bound systems of charges.
Similar shielding interactions between unlike charges will be about half that
for like charges because of the inelastic absorption events. (Where colliding masses
are equivalent, inelastic collisions produce half the momentum transfer of elastic
If a given nucleus is less visible than the superposition
principle would indicate, then its response to electrodynamic influences
(electrical fields for example) will be reduced. It would behave as though it were more
massive than expected. This would be a case of negativemass excess.
If a nucleus is more visible than the
superposition principle would have it, then it will respond more
readily to its electrodynamic environment than expected, and thus would
appear to be less massive than expected. This would be a case
of the expected mass defect. (The mass of the nucleus is
less than the sum of its parts.
Inside complex nuclei the nucleons compete for attention from the outside
universe. In that environment, using carbon 12 for our starting point,
the nucleons in less complex nuclides would tend be closer to free access
to external chargelet fluxes. They would be more electrically responsive
to the external environment and therefore would behave as though they were be
less massive than those back at the starting point. The general tendency
would be increasing mass defect with decreasing Z. This leaves a yet-to-be
spelled out EAS rationale for the mass excesses of nucleons of increasing
mass above Carbon 12.
[Added 19 Feb 2017. Re-worked on 3 Nov 2017.]
What follows is the original EAS argument regarding the mass of deuterium
compared to the sum of the masses of two protons and an electron. This section
may be moved to the top of this page.
Lets talk about measuring the masses three different particles:
a: An electron
b: A proton
c. A deuterium nucleus
We inject each of these objects at a known low energy at one end of a
linear accelerating cavity and let the electrical field impressed
across the cavity do its work. Each object's exit speed will mainly be a
function of its charge, its' "mass" and the voltage applied.
In the EAS model the electrical accelerating
influence of an electrical field is brought about by collisions of
negative or positive chargelets with the test charge. In the
acceleration cavity there will be a net flux of negative chargelets
traveling from the negative electrode to the positive electrode and
likewise a net flux of positive chargelets traveling from positive
In this model protons and electrons are semi-opaque to the passage of
positive and negative chargelets, which are the neutrino-like (or
virtual photon-like force carrying particles. . . .
Elastically colliding negative chargelets (emanating from the negative
electrode) hit the electron approximately twice as hard as do positive
chargelet inelastic absorptions (from the positive electrode) so the net
flux of negative chargelets will accelerate the electron toward the positive
In similar fashion, elastic positive chargelet collisions with a
proton will pack twice the punch as those of the negative chargelets
that are absorbed, so the proton will be accelerated from positive to
Deuterium nucleus acceleration
(Keep in mind that in the EAS model a neutron is a proton with an electron
in close orbit.) As before, the net positive chargelet flux will
impel both protons toward the negative electrode and the net negative
chargelet flux will be impelling the nuclear electron toward the
The "push-of-war" will be won by the two protons.
The following paragraphs will have to be reworked regarding how much
shielding unlike charges provide to one another.
If we focus on just the neutron part of the deuterium nucleus (by
"neutron" I mean the proton that happens to have the electron at
the moment) the electron will be out of sight of the accelerator's net
negative chargelet flux roughly half the time, because it's shielded by the proton.
(It is assumed that the electron is of smaller radius than the proton,
This "blockage" is equivalent to having the electron's electrical response
to the external field reduced to near zero half the time. The electron
will thus experience half the expected linear acceleration from the applied
flux. This is like having a proton and a "half time" electron for
acceleration purposes. If the electron is being acted on half the time by
the impressed electrical field then it will accelerate half as much.
Again, people generally "infer" mass from the observed accelerations
imparted to objects when we use known (electrical, magnetic, or
gravitational) accelerating influences. If we get reduced accelerations
for an object, and all else that we think we know remains unchanged, we
interpret it as increased mass. (Our currently accepted paradigm says
that charge is constant and that no shielding takes place. Superposition
reigns.) In the case being discussed, the "nuclear electron" thus is
observed to behave as though it were twice as massive as a free electron.
I did not do my homework before writing the following
paragraph. The mass of a deuteron is less than the combined masses
of two protons and an electron, or of a proton plus a neutron.
Mass-defect at work! See Philosophy paragraphs above for where
this is going to go.
[This cautionary note added 8 September 2005.]
The electron will provide some blockage of positive chargelets that
would ordinarily collide with the protons, so the "collective" proton
responses to the applied electrical field will be less than that expected
based on the non-shielding aspect of the superposition theorem.
(The protons themselves should fractionaly shield one another as well.
The deuteron (two protons plus nuclear electron) will
"measurably" seem more massive than expected. The amount of this
"increase" will be a proportional to the ratio of the cross-sectional area
of the electron to that of the protons. The trick will be to refine the
hypothesis so as to make the total apparent increased mass, electron and
protons, come out to be equivalent to 1.51 electron masses.
The electrical blockage (or electrical shielding) discussed here may be
applied to more complex nuclei. The EAS model may provide an avenue for
evaluating the peculiarities of nuclide mass relations.
Perhaps this Thayer Watkins study can bail me out on this mass deficit
problem (or make it worse).
A Possible Error in the Mass of a Neutron and Its Implication for the
Binding Energies of Nuclides - [Added 28 Sep 2016.]
Binding Energy and the Mass Defect - Duffy [Added 19 Feb 2017]
Atomic Mass Adjustment -
G.Audi, A.H.Wapstra and C.Thibault - Nuclear Physics A729 p. 337-676, 22 Dec 2003.