Between August 1895 and October 1933, Charles W. Leadbeater and Annie
Besant of the Theosophical Society conducted clairvoyant studies of the
atomic structure of the elements. Both of these individuals had previously
awakened kundalini; Leadbeater has described his having done so by pranayama,
which is the same method I used. After kundalini has been awakened, and
after the ajna chakra (brow chakra) is fully functioning, it is possible
to extend one's consciousness, specifically the faculty of vision, through
great ranges in magnification capability, and either up or down in objective
size. In yogic writings, this is part of what is allegorically referred
to as the ability to make oneself very small or very large at will. These
are the first and second of the eight major siddhis, the Sanskrit Anima
and Mahima. The actual nature and extent of many of the siddhis, or paranormal
powers, are often (intentionally) described allegorically, and so are widely
misunderstood. Anima and Mahima actually each refer to several different
One of these, or what actually happens, and is being referred to in
the case of these observations, is that a projection from the ajna chakra
is formed by the yogi; the functional aperture and gain of this protuberant
projection or filament can be controlled by the yogi, according to the
scale of the object under observation. This extended faculty is symbolically
depicted in ancient Egyptian iconography by the small serpent on the pharaoh's
forehead, which is dismissed by most Egyptologists as being just a part
of the headdress. By its means, one is capable of seeing objects far smaller
and far more distant than is possible by means of any man-made instruments
yet devised. Leadbeater, for example, describes an entire spectrum of particle
sizes below the subatomic particles which make up physical atoms.
The results of Leadbeater's and Besant's investigations were published
serially as articles in the magazine, The Theosophist. The material was
later arranged and published in 1909 in a book titled "Occult Chemistry",
which was revised in a second edition in 1919. In 1951, a much enlarged
and revised third edition (396 pages) was published in Adyar, Madras, India.
I am fortunate to have copies of these two later editions. Over twenty
years ago, in the 1970's, I corresponded at length with the Theosophical
Society's Olcott Library, and they graciously provided me with a good deal
of further information. Since that time, and during my own studies, I have
awaited in hopes that the Theosophical Society would reprint all the original
material. This has not yet occurred, though I continue to hope for it.
Editions of Occult Chemistry are now very rare and difficult to find. [R.
A. Kessinger has done a reprint of this book. It is available from them
at: P.O. Box 160, Kila, MT 59920, phone (406) 756-0167, fax (406) 257-5051,
e-mail : firstname.lastname@example.org]
However, a British physicist named Stephen Phillips became aware of
this material, and in 1980 published a book titled "Extra-Sensory
Perception of Quarks", describing the two Theosophist's work and interpreting
it in the light of modern atomic theory. Though the atomic structures observed
by the yogic faculty, as described by Leadbeater and Besant, did not make
much sense to their contemporaries, present day theories of atomic structure
and particle physics make their descriptions much more recognizable, validated,
and startlingly accurate, as Dr. Phillips was amazed to discover.
Phillip's book was published before the high spin state was recognized,
and so he does not discuss it from this aspect. However, he does notice
how the observations match the Higgs superconducting vacuum model, recognizes
non-Abelian monopoles with Nielsen-Olesen vortices as carrying quantized
flux, and identifies the mechanisms at work underlaying quark stability,
among many other things. All in all, he did a fine job of it. [Extra-Sensory
Perception of Quarks, by Stephen M. Phillips, PhD, 1980, Theosophical Publishing
House, Wheaton IL, ISBN 0-8356-0227-3, US $15.00]
David's ORME patent literature specifically names cobalt, nickel, silver,
gold, palladium, platinum, ruthenium, rhodium, iridium, and osmium as exhibiting
the orbitally rearranged state, with the attendant room temperature superconductivity.
Later, he announced in his lectures, that he finds that mercury also exhibits
the same behavior. As far as I am aware, he has not yet publicly suggested
any other elements (excepting only mercury) are capable of stable ORME
states and high temperature superconductivity, beyond those listed in his
Now, as Leadbeater and Besant's work has already been published, presenting
a great deal on this subject (even if it is not widely known), and it has
been available for some time now, and monatomics are also now becoming
more widely recognized, and a certain requisite amount of discussion has
taken place regarding it, (thanks to Dr. Phillips), it is at last permissible
to comment on the information that has been released occultly, with greater
openness, and from the perspective of monatomic research.
Based on these published materials, and on certain studies I have done,
I may now relate some further information regarding monatomic forms of
the physical elements, their shapes as monatomics, some additional light
on superdeformation, superdeformation's relation to the high spin state,
and what these several factors have to do with the manifestation and development
As monatomics (single, isolated atoms), the elements are yogically observed
to display shapes, which turn out to resemble certain of the platonic solids
and other unanticipated shapes, more than the Bohr atom most people think
of. However, valence structures, subatomic structures, and numerous other
complex phenomena can be identified, given patient study, so that the physical
basis for our theories are nearly all seen to be revealed, even if they
are not implemented quite as we had supposed. The valences take the form
of rod-, bar-, and funnel-like shapes, with the large end of the funnel
cone pointed outwards. The valence shapes, nuclei shapes, and other observed
macro features are of course not solid forms, but are swept volume envelopes,
made by the rapidly moving particles which compose the atoms. I will be
referring to the "valence structures" etc.; these are equivalent
to "orbitals" as used in the ORME acronym.
Dr. Phillips has observed that incongruencies exists between the valences
observed yogically, and those predicted by theory, that the number and
nature of the valence structures actually observed (in the monatomic state)
are not as would be expected, according to present scientific theories
of atomic structure. And he has made an effort to reconcile the two, theory
and observation. Valency, as observed, can be seen in some cases to be
comprised of sets of half valences, so that there are two valence structures
for each of the valences allotted in our present theory, and other variations
in other cases. Dr. Phillips puzzles over this at length in his book. Unfortunately,
he never quite makes the connection (though he comes to within a hair of
it), or it fails to occur to him, as to how these sets of "half"
valences (for instance) relate to, and are responsible for, the forming
of Cooper pairs. But he seems so pleased to at last be seeing how atoms
really work, that he doesn't greatly mind this "problem".
Phillips concludes that the majority of the atoms observed by the investigators,
and presumed to be monatomic, are actually diatomic, and points out that
this assumption clears up most of the apparent difficulties. In this article
I will refer to the observed forms as monatomic, for continuity with the
original investigators, as much as for any other reasons.(1)
Dr. Phillips' book, sadly, has not received much attention. Scientists
do not enjoy giving up their theories, but few would argue that the theories
as they stand today shall forever remain unchanged. I recommend that those
interested read his book, for a hint at what the theories will be... changing
The physical structural arrangement of elemental atoms, and particularly
how the valence structures are arranged in the atom, are observed to develop
as several recurring periodic patterns of form. Leadbeater and Besant soon
found that the structural patterns do not fit well into the Mendelyeev
table (which has been found so useful for predicting chemical properties),
but the observed structural periodicity is nicely predicted by the periodic
system proposed by Sir William Crookes, which was later refined by Jinarajadasa
into a quadruple leminscate. Crookes-type tables, which can be represented
by a multi-level 3-dimensional figure 8 pattern, fit the data far better
from a structural characteristics standpoint, **for the purely singular
and monatomic forms of the elements**. This is an important point to remember,
as the elements have dramatically different shapes when they are observed
in chemical combinations.
The elements in Table 1 (below) are yogically or paranormally observed
to have shapes which appear as moderately high aspect symmetrical dipoles,
when examined as single atoms; ie, apart from chemical-, cluster-, lattice-,
or crystalline- influences. They all show symmetry of rotation about their
major axis, as well as mirror symmetry about a plane bisecting their major
axis. They were aptly termed "dumbbell shaped" by Leadbeater
and Besant; the valence funnels are dipolarly disposed on either end of
the atom, giving them a distinctive dumbbell shape.
Dumb-Bell Shaped Atom
In the case of the dumbbell shaped atoms, which might be considered as one of the most puzzling shapes to someone seeing it for the first time, it is arranged as follows. The main or central body envelope is a swept volume which is approximately represented by imagining an elliptical solid, or ellipsoid of revolution, formed by spinning an ellipse on its major axis. The aspect ratio of the major/minor axes (speaking only of the central structure) is greater for smaller atoms in this family, like sodium, where it is approximately 4:1, and becoming relatively "fatter" in the heavier atoms. Monatomic gold has a central body of about 2:1 aspect.
Each element in the dumbbell shaped group has a total of 24 valence
funnels; there are 12 at each end of the atom, representing 6 sets of half
valences. The 12 funnels are arranged a bit like blades of a ceiling fan,
which rotate on the major elliptical axis of the central body, hence the
dumbbell look. The ends of the valence funnels are slightly staggered,
alternating up and down slightly as you go around the atom.
Within the central ellipsoid form and the valence structures are found
smaller forms (and similarly so for the other element family shapes), which
Phillips has managed to relate to protons, neutrons, quarks, and their
components. Of course quarks, let alone baryons, leptons, omegons, etc.
were unheard of when this information was first published. The smallest
particles which make up the physical atom are referred to by Leadbeater
and Besant as "ultimate physical atoms", since they seem to be
the constituent particle from which all the subatomic particles are built
up. They have called these "Anu", after the Sanskrit name for
the ultimate particles of matter (it is the same root term used in Anima,
"the size of an atom"). There are two types of these, termed
+ and -. The Anu "particles" are composed of whirls of energy
which spin in opposite senses between the + and - varieties. These whirls
of energy, when magnified under increasing power by yogic vision, are themselves
composed of smaller spirals, and those of smaller spirals, and so on, down
through 7 layers of nesting.
The Anu are many orders of magnitude smaller than the subatomic particles,
and the subatomic particles are in turn many orders of magnitude smaller
than the elemental physical atoms of the periodic chart. The Anu, and more
complex particles, all move at enormous velocities, sweeping out the shapes
that I am referring to, and the atom is an extremely active thing to see.
It is ceaslessly throbbing, pulsating, spinning, gyrating and precessing
with amazing rapidity and vigor when so viewed. Not at all like the billiard
ball protons and neutrons with the spherical electron shells many would
expect to see. But our dashed expectations are our own fault, rather than
Nature's. Still, we are better prepared now than at any time before to
understand the remaining secrets of atomic structure; we must only recognize
that things are far more complex than we have ever previously supposed.(2)
Table 1 elements are all structurally similar, despite the fact that
under our present periodic arrangement samarium (for example) inserts columnarly
in VIII between ruthenium and osmium, and sodium falls in group IA with
the alkalis. Most of the nonmetallic halides are found, by this faculty,
to similarly be dumbbell shaped in their monatomic states. Of the elements
in this family, David has already observed ORME state superconductivity
which develops in gold, silver, and copper.
"Dumbbell" group monatomics, predicted to exhibit the ORME superconducting state.
+ Already specifically named in David Hudson's patent literature.
The inclusion of an alkali metal like sodium, most of the halides, and
so on, flies in the face of existing interpretations as to the underlying
causes of the ORME phenomena (which is presently postulated to be a consequence
of partly filled orbitals). Many of the elements I suggest in this article
to possess superconducting ORME states are, of course, nowhere near the
center of the Mendelyeev periodic table, where elements with partly filled
orbitals are placed.
It would be good to recall at this point that the periodic table was
originally developed only as a means of helping us understand the laws
governing the elements' chemical properties, and we should not fall into
the trap of extrapolating its fine success in this regard to imply that
it also applies to, or continues to hold true for, monatomic shapes. To
assume that chemical properties are a reflection of an element's monatomic-form
structure is not supported by yogic observations. There is little hope
in discovering an element's atomic propensity for having an ORME state
by peering at the Mendelyeev periodic table. This phenomena has little
to do with orbital filling as shown there. However, the phenomena and the
reasons behind it become clear and plain when viewed yogically.
The actual reasons that certain elements exhibit stable ORME states,
form Cooper pairs, and display Type 2 superconductivity (as David has correctly
described them as doing), lies in their structural characteristics, and
these particular structural characteristics only occur in the monatomic
forms of elements, and then only among certain monatomic-form structural
families. The valence forming structures (ie, 'orbitals') of the elements
named in David's patent literature (as well as mercury, and others), are
seen to "rearrange" precisely as David has indicated, and this
rearrangement is indeed what leads to their extraordinary properties. Other
elements, discussed in this article, not yet acknowledged as ORMEs by David,
shall eventually be found to exhibit this same behavior, under appropriate
The elements which can potentially exhibit room temperature (and higher)
superconductivity do not necessarily immediately or spontaneously rearrange
themselves into a superconducting ORME state upon disaggregation. They
first require an impetus to set them rapidly spinning. High spin is a necessary
condition for this rearrangement to occur; it is the first step in how
the ORME state is reached. (It should be apparent that to have a rapidly
spinning single atom means that it is monatomic.) However, the relatively
low energy of thermal collision forces is sufficient to get them spinning
fast enough. Simple glancing thermal collisions knock the monatomic atom
into a rapid spin, and that is how the high spin state leading to ORME
transition is most commonly achieved. That is the reason behind why David
had to heat the monatomic material in order to transform it into a superconducting
ORME state. It is indeed a strange consequence that thermal energy transfer,
in the form of a spin-imparting collision, may act to lower the atomic
energy temperature, but it is an observationally evident effect.
The spin of the atom centrifugally causes the valence structures to
deflect from the normal positions they have as single (monatomic) atoms.
Rearrangement of the valence structures into the ORME configuration then
occurs, which, once formed, is extremely stable for some elements. [For
some other elements capable of forming ORMEs, much greater excitation levels
are required, and stability is also lower.]
Here is how the transition into an ORME works from an observational
standpoint. Assume an atom of one of the appropriate families has just
become disaggregated (let us say, by some means that does not impart substantial
kinetic energy to it) from a lattice, or crystal, or chemical combination,
so that it is free to assume its normal monatomic (family) shape, and is
just floating around without much velocity or spin. In its initial condition,
upon disaggregating, its valence structures will be arranged in their "normal"
symmetrically disposed manner as a monatomic chemical atom. In this shape
and condition, it is stable, though it is, of course, able to chemically
combine in normal ways, since its valences are as yet unaltered.
How long the atom has to wait for a suitable collision depends on the
temperature and population density of its environment. This may be very
brief, as some atoms can make this transition at only moderate temperatures.
Even if its environment is relatively cool, an energetic collision may
still occur, it is just less likely. Eventually (assume), a collision occurs
causing it to tumble or spin about its center of mass.
There is a statistical probability that the collision will impart rotation
to the atom, in (or reasonably near to) one of the possible spin planes
which will deform the valences into one of the possible ORME configurations
for the particular atom.
When an atom is set properly spinning and on its way to forming an ORME
configuration, the outreaching valence structures are flung centrifugally
from their normal orientations, and this always happens in the manner that
most increases the atom's moment of inertia in the closest ORME spin plane.
For example, in the case of the dumbbell shaped atoms of Table 1, this
would be a tumbling of the major axis itself (ie, the major axis is rotating
around a line passing through the atom's center of mass and orthogonally
bisecting the major axis), and all the valence structures at either end
of the dumbbell swing outwards, away from the center of mass of the atom,
to align or cluster towards parallelism with the atom's tumbling major
The atom thus deforms as centrifugal forces overcome the forces which
hold the valence structures in their "normal" positions. It just
happens fortuitously that the Coulomb forces which want to keep the valence
structures separated, and the centrifugal forces the valences actually
experience under high spin conditions are similar in magnitude. The atoms
and their substructures are extremely stretchy and springy; this should
not come as a big surprise, since after all, they are basically bundles
of forces and masses. As rearrangement of the valence structures takes
place, it acts to reduce the spin of the atom, similar to how spinning
ice skaters can slow down by extending their arms outwards.
However, if enough angular velocity has been achieved, the valence structures
("orbitals") rearrange into two groups, like two bouquets of
funnel-like flowers, with one group swung centrifugally outwards on each
end of the tumbling, now highly elongated atom. In this superdeformed condition,
their outermost ends (where the chemical bonds form) approach each other.
When (and if) the coupling ends of the valence structures come into close
enough proximity, they link together in pairs in a specific manner. In
other words, in this superdeformed condition, the atom becomes able to
bond to itself, much the same way it would bond to another atom, only more
tightly. When this happens, it looks a bit like the atom is "hugging"
itself with its multiple valence "arms", all joined together
in pairs. It is like when you stick your hands into the opposite sleeve
of your coat on a cold day. To yogic vision, this is what actually happens
physically and structurally, corresponding to what is termed in modern
scientific theory as the formation of Cooper pairs. It is the forming of
a micro-cosmic orbit, so to speak, at an extremely tiny atomic scale. In
a sense, it seems ORMEs are metaphysical, even from a structural standpoint;
they are like the atomic equivalent of the ancient adage: "Turn inwards,
and know thyself."
When the valences are all paired together, the atom will look nothing
like it used to, from a chemical properties or analytical standpoint. No
free bonds are left to form compounds. Externally it appears inert, all
closed up, not a valence to be seen. Its spectral emissions will be entirely
different. David's statements here are right on the mark. This closed-up-armadillo-like
structure is why they are insoluble in the strongest acids, capable of
withstanding great temperatures, and so forth. The internally closed circulating
flow, through the self-joined valences, is the source of their individual
It is important to note that it is also possible to have partial ORMEs,
in which some of the valences are "normal", and free to form
chemical bonds, while the others, on the same atom, are coupled as Cooper
pairs. These "partial" ORMEs may result from either a marginal
collision, resulting in an incomplete ORME formation; from an odd collision
event that knocks two valence structures together just right to cause them
to join; from a fully paired ORME that experiences a partial uncoupling
of its paired valences; and from other less probable events. Varying degrees
of "partiality" are possible, in steps of one valence structure
pair at a time, from all to none. (3)
This is a bit like the Cheshire cat, who gradually disappears, a little
at a time, till all you have left is the smile. Partial ORMEs are less
stable; when the still exposed valence portion of a partial ORME enters
into a bond with another element, etc., this can introduce other internal
changes in the partial ORME which disrupt the remaining Cooper pairs, causing
them to decouple. Partial ORMEs having chemical bonds to other atoms may
eventually relax their Cooper pairing and drop back into a normal metallic
or chemical atom state.
There is no question but that many of the naturally occurring and manufactured
ORMEs David has been working with are, in fact, partial ORMEs. The natural
ORME materials found in the tailings and volcanic deposits Dave is using
contain or comprise a mixture of both completely and partially formed ORMEs.
The partially formed ORMEs components exist in varying levels of completeness
in their Cooper pairing. Of this raw material mix, the natural, partially
formed ORME atoms which still remained semi-uncoupled were able to bind
with his cyanide solution. That is why they were able to be caught by the
chemical leaching process of his tailings recovery operation, leading Dave
to his path of discovery. This was only possible, and only happened this
way because partially formed ORMEs still retain some of their metallic
attributes. The fully formed ORMEs do not act like metals at all, and do
not in the least interact chemically with the leaching process cyanide.
If all the ORMEs in the tailings had been 100% Cooper paired, they would
all still be sitting in those tailings piles, and Dave would still be growing
cotton; the cyanide would have never caught them.
It was only the incompletely or partially formed ORMEs, still weakly
metallic, which were picked up by the recovery solution. Fortunately however,
the partially formed ORMEs still form linkages with fully formed ORMEs
through their Meissner fields, even though the fields of partial ORMEs
are weaker. And so both varieties were carried along together by the recovery
process. The partial ORMEs reacted with the cyanide (using what free metal
bonds they had left) and were washed out with it. These captured partial
ORMEs in turn dragged the fully formed ORMEs along for the ride, pulling
them by their Meissner fields like a big dog on a leash, towing its owner.
The 100% ORMEs are easy for these partial ORMEs to pull around, since the
full ORMEs offer no resistance at all. No other chemical attachment forces
can act on them (chemically speaking they are as slippery as a greased
pig), and so they obligingly follow their more chemically attached partial
ORME partners, being pulled along as if they were riding on ball bearings.
Later, when the solution mix of partial and complete ORMEs is subjected
to further chemical separation methods, the Meissner leash connection between
them eventually gets severed. This is usually through the full ORME's stronger
attraction to the Meissner fields of other full ORMEs, thus breaking up
the partnership. The partials are eventually removed through their still
semi-functional metallic reactivity, as an "impurity" along with
the precious metals. This leaves behind the fully formed ORMEs, clogging
up Dave's process solution, and causing David and his associates so much
bafflement when they were found to resist all known forms of analysis.
Fully formed ORMEs will not react with hydrogen cyanide any more than
they do with aqua regia or anything else. Their main interaction with external
world is through their Meissner fields. In Nature, only other ORMEs, partial
or complete, speak their language. They all ride along together in a world
of their own on the waves of magnetic and electric fields that pass through
David's patent literature says the following:
"Further, the applications to which the ORMEs are directed will
establish their relationship to a specific T-metal by virtue of the manner
in which the ORME performs in that application as compared to the performance
of commercially available derivatives of the T-metal. An example is the
performance of commercial rhodium as a hydrogen-oxidation catalyst compared
with the performance of the rhodium ORME as used in a hydrogen-oxidation
Partial ORMEs will still work, to some extent, depending on the degree
of partiality, in fuel cell catalysis, for the same reason they react with
cyanide; a consequence of the weakened metallic properties they retain.
Dave has indicated in his lectures that some elements in his patent are
susceptible to nitric oxide destabilization as ORMEs (specifically excluding
gold, which of course does not react with nitric oxide, even in its metallic
form). This then, strongly suggests that these are not 100% coupled ORMEs,
in which he has observed this effect. 100% coupled ORMEs, regardless of
element, will not react with nitric oxide. They will not do anything in
a fuel cell. Nor will they form bonds with cyanide, acids, etc. By definition,
a 100% ORME is one which has nothing -no bonds- remaining but Cooper pairs,
so it *cannot* react chemically; it has become incapable of doing so. Only
partial ORMEs may react with nitric oxide, or other chemicals. To repeat
myself, in 100% ORMEs, all the valence structures are coupled and closed
Dumbbell group atoms of Table 1, with their 24 valence structures capable
of forming up to 12 pairs, thus have from 0 to 12 levels or stages of partiality
(ie, orbital rearrangement), with zero being a normal chemical atom.(4)
Bars group atoms, listed in Table 2 (and discussed later in the article),
with 14 valence bars, may form from 0 to 7 distinct levels of partiality.
Presently, I do not believe Dave or his associates are aware of the
distinction which exists between full and partial ORMEs.(5)
It is obvious that determinations as to whether 100% Cooper paired ORMEs
are best suited to, and should be supplied for, medical and philosophical
uses are not possible as long as there is no such awareness. Depending
on the element, only a partial complement of Cooper pairing may be needed
to prevent heavy metal toxicity in the body. For example, partial pairing,
from a toxicity standpoint, is not even an issue for a nontoxic element,
such as gold. But fully paired ORMEs are more effective and efficient in
the intended applications, due to their stronger Meissner fields, which
is the number one active ingredient.
But I shall also suggest that a complement of partial ORMEs helps the
body to utilize ORMEs better. Perhaps, I shall suggest, the body may wish
to have a certain amount of certain partial ORMEs to act as tethers, to
keep the 100% ORMEs on a leash, at the place where they are needed. Perhaps
the partial ORMEs are a natural "handle", provided by Nature
to help hold onto their more slippery cousins. The fact that partial ORMEs
that have first been reacted with HCl are reported to be most effective,
eg when administered by injection, strongly suggests this is so to some
degree. [These were partials or the HCl could not have reacted with them.]
Or perhaps partial ORMEs are a hidden danger, waiting for those who ignore
them to learn a tragic lesson from. Perhaps all these things. The subject
of partially formed ORMEs needs to be closely examined, in the context
of its implication for each of these elements.
The subject of partial ORMEs is the main reason I have decided to submit
the information in this article. There is a present lack of understanding
here, and hopefully these explanations will be plain and obvious enough
to help remedy this. I would rather that someone else had pointed out,
but this hasn't happened.
Reasonably high yields of fully coupled ORMEs are obtainable by simply
processing monatomics in a finely divided form for a sufficient length
of time at optimum temperature and pressure in an inert gas atmosphere.
The inert gas atoms provide an effective spin-inducing collision mechanism.
The lack of external valencing of the inert gases results in more effective
spin-inducing collisions than for any other medium. Batch yield, or a determination
of partial ORME content can be gauged by screening a sample with aqua regia,
fluorine, hydrocyanic acid, or other powerful reactants, depending on the
ORME elements involved. If it doesn't react with those, it is certifiably
highly Cooper paired, and obviously safe for the body. There are no doubt
other partially paired gaussian distributions for each of the various elements,
which may be certifed as safe under less stringent criteria, but these
determinations need to made in an informed, intelligent, and demonstrative
way. There will always be some partials produced by any practical process.
David's methodology, as gleaned from his lectures, presently seems to include
no provision or means to analyze, monitor, regulate, or optimize the product
ratios of these partial forms, let alone assay or separate partials out
according to the discrete levels or stages of their Cooper pairing.
The stability (or actually, lack of stability) of the ORME states of
some of the other elements I speculate about in this article may render
them unsuitable for consumption. However, any ORME elements which are observed
in any quantity in Nature are arguably stable enough, or they would have
long since disappeared as such forms. I suggest that less stable ORMEs
shall nevertheless be found to be of great interest in other exciting ways.
Loading the ORME atoms with more energy than they can handle will also
break up the Cooper pairs. One way this can happen is as when Dave exposed
the material to direct sunlight. When overloaded, the links between the
ends of the valence funnels or bars burst apart like the joint of a water
pipe when forced to carry too much pressure. This is the structural observation
of what happens in a superconductor collapse, such as occurs with experimental
and commercial superconducting-ring energy storage devices, when too much
energy is pumped into the Meissner field. Most of these devices develop
Type 2 superconductivity using cryogenic temperatures, but the formation
of Cooper pairs in the metal lattices of low temperature superconductors
follow valence behavior principles related to those occurring in ORMEs.(6)
The self-bonding of ORMEs has the decided advantage of not having to contend
with local lattice thermal jitter, and thus functions at high external
It appears that overloading is what is occurring in the electro-winning
method Dave uses in his patent literature to reconstitute the group VIII
ORMEs into metals. On this the patent states:
"ORMEs are transformed into their original T-metal by means of a chemical bonding with an electron-donating element, such as carbon, which is capable of d orbital electron overlap and "spin flip". When the G-ORME is chemically bonded to carbon in an aqueous solution of ethyl alcohol under a specific potential, carbon monoxide is formed and the ORME forms Au+(Au+, a black precipitate, which under continued application of potential and dehydration reduces to Au+1 (Au-1, a metallic bonded diatom of gold. **This invention establishes that a high potential applied to the solution forces an electron into the d orbital, thus eliminating the electron pair.** The first potential, which for G-ORME is approximately -2.2 V and for other ORMEs is between -1.8 and -2.2 V, re-establishes the d orbital overlap. The final potential of -2.5 V overcomes the water potential to deposit gold onto the cathode."
( **'s added.)
And again, later:
"An ORME can be reaggregated to the T-metal form using conventional
wet chemistry techniques, by subjecting the ORME to a two-stage electrical
potential to "oxidize" the element to the metallic form."
It seems that what is happening here, in the description of converting
gold ORMEs (or G-ORMEs, as they are termed) to metal, is that the partial
ORMEs are reacting mildly with the cyanide solution (the carbon referred
to), dragging fully formed ORMEs along in the process, just as I have described
earlier as happening for Dave's heap leaching process. The chemistry that
is referred to as going on is all associated with the weakly metallic aspects
of the partial ORMEs only. The 100% ORMEs don't participate in it. The
part I have highlighted (between **'s), is where the energy loading that
breaks the Cooper pairing occurs, coming from the electric potential in
the cell, and Dave is specifically recognizing that and pointing it out
in a subtle way. The mistake is in failing to understand that partially
formed ORMEs are involved, and what their role is in the process. This
is not intended as criticism; the best present theories of atomic structure
which he is applying to the phenomena are simply not yet able to provide
many clues as to the true explanation of what is going on.
In Dave's lectures and in the 5/26/96 interview with binga, he indicates
he uses a chemical analysis on test materials, to determine their ORMEs
content, which appears to take several days of running to complete. This
is a proprietary method he has not given any details on, but has released
on disclosure to certain parties such as MIU. Without knowing the details
on this, it is likely for the reasons I have discussed, that Dave's analysis
method (being chemical) acts on partial ORMEs, though the process may well
also accumulate full ORMEs, by Meissner linkages, similar to the way his
tailings recovery process did. I tend to suspect that this is the case,
even though it seems to not yet be apparent to Dave that a distinction
exists in ORMEs, between full and partial varieties.
In determining whether a particular element in the periodic table may
exhibit structural bistability, having both a stable chemical atom state
and an ORME state, there are several factors to consider. Everything about
these ORME's behavior is structural in nature. In order to form a true,
complete ORME state, all the valences must be paired up as Cooper pairs.
Ideally (though not in practice) only elements having a number of valence
structures divisible by 4 can exhibit ORME behavior: the valence structures
divide into 2 opposite groups under high spin. There must also be an even
number of valence structures in each spin-divided group in order to form
Cooper pairs, so all the valences "disappear". Hence the factor
of 4. Element families which have a number of valence structures that is
a multiple of 4 meet this ideal, and form symmetrical ORMEs. There are
three atomic structural families among the physical elements that satisfy
this "ideal" criteria. These are called the dumbbell, octahedron,
and tetrahedron families by Leadbeater and Besant (viewed as monatomics),
and have 24, 8, and 4 valence structures, respectively. Gold, silver, and
copper from David's patents are from the dumbbell family. Mercury is from
the tetrahedral family.
All the other elements in David's patent are from another family shape,
which doesn't meet the criteria of having a valence structure count divisible
by 4, but manages to get around this (and very successfully) by utilizing
an unbalanced spin in forming ORMEs. This is the "bars" family,
each element having 14 valence structures. These are called bars, as the
valence structures resemble bar shapes, radially projecting from the center
of the atom. The valence bars are (monatomically) disposed towards the
6 face centers and 8 corners of an imaginary cube (the cube shape is not
visible in the atom, but that is how the bars arrange themselves). When
bars elements form monatomics, they form (when spinning) an unbalanced
dipole, with 6 bars (3 Cooper pairing sets) grouped on one end, and 8 bars
(4 Cooper pairing sets) on the other end.
Bar Group Atoms
Besides the dumbbell and bars families, there are also atomic families
with shapes resembling octahedrons, cubes, tetrahedrons, spikes (shaped
similar to carpet tacks), and 6 pointed stars. There is a separate group
for hydrogen. I will not discuss these groups except for briefly mentioning
a few elements from some of them, that appear to have potential for ORMEs
"Bars" group monatomics, predicted to exhibit superconducting
ORME states. This group has the highest thermal-collision statistical probability
to form an ORME state, based on number of possible spin planes, resulting
in their having lower average temperature transition points.
The "bars" family, followed by the "dumbbell" family
have more possible spin planes than the "octahedral" and "tetrahedral"
families, which can all (potentially, -even the cubics) form complete sets
of Cooper pairs. This gives bars and dumbbell group elements a statistical
advantage, by reducing the number of thermal collisions necessary for a
successful valence rearrangement transition. This seems to explain why
such a high percentage of these elements (bars group in particular) occur
in Nature as ORMEs, and hence why the majority of the ORMEs David has discovered
to date are in this category. The bars group have long extended valences
which bend together to couple relatively easily, and the large number of
them means the required angular deflection (the angle between the valence
bars) is comparatively small compared to the octahedrons, cubics, and tetrahedrons.
All these factors tend to make the bars family ORME states highly stable
and easily formed.
On the other hand, the unbalanced high spin state of bars group elements
make them distinctly more susceptible to the formation of partial ORMEs.
This conclusion also appears substantiated in the higher relative ratio
of partial to complete bars family ORMEs, as found in Nature. Since these
elements are the largest constituent for ORMEs in Dave's volcanic mineral
deposits, it is unavoidable that the production process will generate large
amounts of partial ORMEs, with or without awareness of the fact.
The dumbbell family has an infinite number of spin planes, but they
are not uniformly distributed, being all planes which make up the set that
include the line of the major axis. In other words, if you imagine a spin
plane which includes the line of the major axis, then rotate the spin plane
using the major axis line as a pivot, every angular position the plane
can have, as it rotates in this manner, represents a possible spin plane;
there are an infinite number of such spin planes in 2PI radians. The bars
family, on the other hand, while actually having no "ideal" spin
plane possibilities (its valence structures are not multiples of 4) is
nevertheless statistically more likely to benefit from a particular collision.
Its '6+8 arrangement' unbalanced spin plane combinations are evenly distributed,
and valence positional variance, plus the tolerance window for collision
angles, eliminates nearly all non-ORME-forming collision "blind spots".
As a result the bars family enjoys a much greater total number of potentially
transitionable thermal collision vectors.
Among the octahedrals, titanium, and zirconium appear to have potential
for ORME formation, based on their structural proportions. Titanium and
zirconium are oddities within this family, each having 4 long narrow valence
arms which bifurcate at the very ends. They have a strong affinity for
carbon, as their valence terminations are identical in structure to that
of carbon's valences. Most of the other octahedral elements (and more so
with cubics and tetrahedrals) have short broad valence funnels, which would
have a hard time of it, trying to reach around to each other to form a
Cooper pair coupling. Of the other octahedrals, lead looks like it would
be the next most likely possibility; its valence structures are a little
Once the valence structures of an atom have been self-coupled into Cooper
pairs, the atom may (or may not!) remain this way. Upon fully coupling,
the valences have a strong mutual affinity to staying paired; after all,
it is coupling to itself, and so the compatibility factor is pretty high.
Many elements highly prefer being in the ORME state.
Some of Nature's elements form extremely stable and tightly clenched
ORMEs. Other elements simply cannot, or else barely can, bridge the distance
to make the connection, even when spinning enormously fast. These latter
cases are much less stable as ORMEs, though they may still form under appropriate
conditions. Elements having stubby valence structures must be spinning
much faster to deform the valence positions, than elements with longer
more gangly valences. Greater "at rest" separations between valences
means that more deformation must take place before Cooper pairing can occur.
Elements with platonically shaped monatomics having fewer faces are more
disadvantaged in this way. Elements which are less structurally disposed
to forming an ORME state will require proportionately higher collision
temperatures, to get to the coupled superconducting condition, once they
have been disaggregated into monatomics.
Consequently, even though the elements of certain structural families
may potentially form ORMEs, some of them, such as many of the octahedrons,
cubics, and especially the tetrahedrons, can only do so under extraordinary
conditions. Even then, once formed they may not have sufficient stability
to remain rearranged when their spin drops below a certain rate. The restoring
forces trying to pull the valences apart will become stronger than the
self-coupling forces, if the atom's spin rate drops too low.
Of the cubics, some of the heavier elements, most notably tantalum and
lutetium, have relatively long valence funnels and may be able to successfully
form Cooper pairs under suitable conditions. Like the bars family, these
cubics would have to enter an unbalanced spin in order to form ORMEs. That
is, the cubic elements must spin so that there are two valence funnels
(1 Cooper pairing set) on one end, with the other four valence funnels
(2 Cooper pairing sets) on the opposite end of the spinning atom, in order
for complete pairing to be possible.
Mercury is a special case, coming as it does from the tetrahedral structural
family, with only 4 possible spin planes (2+, 2-) which might form an ORME
superconducting state. How is it that mercury has managed to have this
capability and be discovered already? One might think that the tetrahedrals
would be among the least likely families from which would appear a stable
ORME. To yogic vision, mercury (like Ti and Zr) is seen to be a bit of
an oddity, compared to other elements in its family. It has some major
subatomic structures in common with gold, and while showing the expected
structural family features, it is oddly proportioned quite differently
than it might be expected to be as a tetrahedral family element. These
nonconformities enable it to deform more than other tetrahedrals with the
same amount of spin, allowing it to rearrange and achieve a superconducting
state more easily. When it superdeforms, it winds up looking more like
a gold atom that has two big valence structures on each end, rather than
like the other tetrahedrals.
Vaporizing mercury in an inert gas atmosphere of sufficient temperature
and pressure will form Hg-ORMEs. This is an effective means of forming
ORMEs for any element. Seeding this process with some already formed ORMEs
will help catalyze the transition. Occasionally this even occurs in a minor
way in mercury vapor turbines, but has not been recognized. With only four
valence structures, there are only three free state possibilities in the
case of mercury: metallic (chemical) atoms, 50% partial ORMEs (1 set of
valence structures paired), and complete ORMEs (all 4 valence structures
paired, into 2 sets).
In David's patent literature, he uses this process in the case of gold:
G-ORME was prepared from metallic gold as follows: ... (19) The monoatomic
gold is placed in a porcelain ignition boat and annealed at 300 C under
an inert gas to remove hydrogen and to form a very chemically and thermally
stable white gold monomer....
This step appears to say that the 300 C temperature and inert gas are
mainly there in order to facilitate removing the hydrogen. The description
might leave one with the impression that if the hydrogen could only be
removed in some other lower temperature manner, perhaps the process would
still succeed, and that the ORMEs form spontaneously. Well, they do, in
a manner of speaking, but it is because of the high temperature, and the
presence of the inert gas that the "spontaneity" happens. As
soon as they become monatomic, their exposure to these conditions gives
them an excellent opportunity to experience thermal collisions, knocking
them immediately into the high spin state that leads to their forming into
Cooper paired ORMEs. The environmental conditions are the most important
parts of the equation. Though he has mentioned using welding grade argon,
David says nothing in his patent about the pressure he is doing the annealing
at, and has not mentioned in his lectures whether he has experimented with
gas pressure as a variable. The gas pressure is not a critical factor to
success, but it does impact the process rates.
For each particular element, there shall be found to exist a range,
or window, of conditions of pressure and temperature, depending on which
inert gas is used as the atmosphere, which will result in ORMEs (and partial
ORMEs) formation. Besides the associative ORMEs formation process, there
is also a dissociative process operating simultaneously. As in all other
thermally driven reactions of this nature, the rates of both processes
increase with temperature. Optimum ORMEs formation will occur under specific
conditions, and may be arrived at computationally, but these may also be
determined empirically (simple trial and error) for specific cases. Once
the process has remained at some fixed conditions long enough for the rates
to stabilize and reach equilibrium, no significant further change in product
quantity will occur. In ALL cases, the process result will be a combination
of complete and partial ORMEs, to some degree. The object is to set up
the process to maximize or peak the full/partial ORMEs ratio for each element.
Remember the 300 second spectroscopic burn David refers to in his lectures?
I suggest the following be considered as an explanation of what was happening
there, in illustration of how these two process rates I've just discussed
operate. As a premise, I believe the samples Dave was using in these spectroscopic
experiments were most likely 100% paired ORMEs to start with. The sample
material (I am supposing) had inadvertently been selectively concentrated
that way (as 100% ORMEs), by his tailings recovery process, as explained
earlier. I think he may have had quite a bunch of this material around,
that nearly all the partials had been removed or excluded from, as a side
effect of his refinement operation, and that this was where the materials
he was using at the time came from. But any other 100% source he may have
had would produce the same results. The spectroscopic arc is inert gas
shielded, and very hot. Just like what I've described as an efficient ORMEs
formation process, and just like what is in Dave's patent for making ORMEs.
What do you suppose would happen to 100% ORMEs, under those conditions?
They obviously cannot follow the association process function, since they
already are all 100% paired. The only thing they can do is begin to dissociate,
once the temperature drives the function high enough. Dissociation will
continue until the partial population count (within a particular minute
volume in the arc) becomes high enough that the two rates, associative
and dissociative, come to equilibrium. Dissociation will be the strongly
dominant process. ORMEs vaporized off the sample will be turning into partial
ORMEs, as a dissociative process, as collisions with inert gas atom break
their Cooper pairings.
Dissociation for the first element (palladium) seems to commence at
70 seconds into the burn. At that time, the ORMEs start vaporizing. As
soon as the ORMEs leave the sample's surface, partials begin to form, and
spectral lines begin to show up. Only when ORMEs vaporization and dissociation
starts, do platinum group spectral lines appear, those metal lines being
emitted by the unpaired portions of the newly-dissociated partial ORMEs.
The dissociation, is occurring in an ordinary manner, by means of thermal
collisions between the ORMEs and the hot inert gas atoms occasionally breaking
some Cooper pairings in the ORMEs.
When Dave stopped the burn at 68 seconds, thinking (in those early days)
that he should then have only metals left, he had only succeeded in further
purging his 100% paired sample of extraneous impurities of lower boiling
point. No transmutations were occurring, or are needed to explain the results.
Only ordinary associative/dissociative reactions, acting on some very unordinary
Later, when the sample was analyzed, no evidence of metals could be
found in it. Why? Because the sample was still 100% ORMEs, as it had started
out. The dissociation was occurring among the ORME atoms in the arc, just
where you would expect it to be occurring, not in the relatively cooler
sample body. These vaporized and Cooper-dissociated partials, after emitting
their spectral lines, get carried off in the draft of the inert gas. So
no metals (or partially metallic ORMEs) would be expected to remain in
the sample. Had the arc vapors been trapped and condensed, a small quantity
of weakly metallic ORMEs would have been found there. What if the original
sample had not been 100% ORMEs, as in my premise? That seems improbable
to me, as the unpaired metallic portions of the partial ORME atoms would
then have shown up in the quantitative chemical analysis of the sample,
both before and after the burn.
In his lectures, Dave often speaks of how the atoms are undetectable,
don't match any known spectral lines, defy analysis, and can't be dissolved
in aqua regia. Then in almost the same breath, he tells of seeing platinum
group spectral lines though no metals can be found, that the material works
in fuel cells, can be analyzed in things like Acemannan, carrot juice,
and cow brains using chemical means, and recovers in his cyanide to the
point of clogging things up. Now it's chemically reactive... now it isn't.
These are incongruous statements, and I sense he is uncomfortable with
them. I believe many others sense a problem here, too, though they haven't
been able to put their finger on it. I have tried to explain here, that
the seemingly dual personalities of this stuff are not at all as contradictory
as they seem on the surface. There is an explanation. It just requires
a deeper understanding of what the materials are doing, way down there
in the tiny world of Anima. When you look very, very closely, and see that
Cheshire cat smiling at you, it all makes sense. I hope some of Dave's
friends will take this to him. This is what he needs to know.
At some future time, it may be possible to comment further on these
I invite forum subscribers to pursue this area of study as a potentially
fruitful direction for new discovery. Science has indeed come a long way.
But do not rest just yet.
Gary describes himself as a kundalini awakened American engineer. Gary
is a single white male in his mid 40s who works as an engineer with a very
big US company. Gary has "a background in physics, electronics, and
knows a few things about chemistry and the elements."
To state this plainly, the "monatomic" ORMEs in Hudson's patents
are, in fact, diatomic. It is also clear to me that most of these elements
do not exist stably in an isolated, monatomic state, but quickly disintegrate
when forced by the Will to assume that condition, although they are perfectly
stable as such when in chemical combinations.
(I chose to refer to the elements in my original article as monatomic,
prefaced by an explanation of why I was doing so (quoted above), so that
anyone sufficiently interested in studying the article material carefully
would note this and take it into account in understanding the rest of what
I wrote in the article. I knew full well that this brief note would be
lost on most who would read it, but I also knew that those few who would
read it very carefully, which should include any scientists, would pick
This was done in the hope of making the content of my discussion at
least appear to stand on familiar ground, and so be more acceptable to
David Hudson, et al, through a commonality of sorts in terminology.
My taking this approach also considerably reduced the amount of explanation
I would have had to include, to make the subject intelligible to everyone,
who have been (in the absence of anything else being available) only familiar
with ORMEs theory as propounded by David Hudson. Even so it was a large,
rather lengthy article.)
For diatoms, the number of valences will obviously always be even, ie
divisible by 2, and so Cooper pairing is freed from the objection that
atoms with uneven numbers of electrons could not be completely Cooper paired.
The valence funnels "rotate" (as a consequence of the motion
of the particles forming them) in alternating senses, as viewed in a sequence
going around the atom (e.g. a gold dumbbell - See below). It should be
clear that two adjacent funnels, one rotating clockwise, and one counter-clockwise,
will coincide in rotation if the funnels are distorted into a loop so that
the mouths join. They then form a continuous rotating tubular vortex. This
is the physical action corresponding to two electron spins joining and
canceling to form a Cooper pair. A similar effect occurs in metal lattices
at cryogenic temperatures, except that funnels join between neighboring
atoms, rather than on the same atom for an ORME.
Describing ORMEs as monatomic is still justifiable in a sense (albeit
technically inaccurate) since the ORMEs state is still the smallest atomic
level division that most of those elements remain stable and intact at
I will also suggest that, (if you will expand on what I have written
in my original article) it should then be obvious that, in addition to
the electromagnetic flux carried by the closed loop funnels of ORMEs, other
energies may (and do) also flow through these circuit paths, and may (and
do) do so in parallel with electromagnetic energy. Since this flux, in
moving around this atomic-level closed circuit, passes through the very
heart of the atom, it should not be at all surprising, and should indeed
readily suggest itself to anyone reading my article and thinking about
it that the nuclear strong and weak forces may also participate in this
flow (they do). This ORMEs circuit is one of the few cases in Nature in
which these internal forces may thus develop macroatomic fields, extending
beyond the outer envelope or perimeter of the atoms, and each of these
forces (and others still more esoteric) generates a field, which, like
the electromagnetic Meissner field, has unique properties, according to
the laws governing each of the underlying forces generating those distinct
yet co-spatial fields. Like the electromagnetic Meissner field (which Hudson
and others have erred in rushing to suppose to be the same as the aura)
each of these may vary in the amount of energy they contain, as a function
(by specific type) of their flow in the circuit.
Speaking now, in stricter use of the concepts 'monatom' and 'diatom',
I offer some further comments which may be of interest. This is in regards
to Brown's gas.
Diatomic hydrogen is observed to be an ovoid, containing two triangular
"monatoms", each composed of 3 quarks (having 3 anu each). The
triangular H atoms are not identical in the types of their constituent
quarks; each hydrogen in the diatom has the same mass, but differs from
the other as a consequence of their quark components. When dissociated
into monatoms, the two separated hydrogen atoms are stable (ie do not spontaneously
dissociate further) but I would suggest that they would prefer to be paired.
As monatoms, they loosely associate with free particles, forming something
like the atomic equivalent of the double-layer of continuous-phase charge
which forms around colloidal particles to neutralize their remaining charge;
it is a less defined layering for a gaseous continuos phase than for a
liquid as far as colloids are concerned, and this (gas case) is a close
analog of what happens in the atomic state, where the atomic-level vacuum
is the continuous phase, and the myriad of loose and undifferentiated subatomic
particles are the matter that the layers are (dynamically) formed from
around the monatoms, as a loose aggregate.
Diatomic oxygen is also an ovoid, containing two spiral shapes, looking
very much like helices of 5 turns each, with each being "wound"
in the opposite direction. Like the hydrogen, each monatom of the O2
diatom is dissimilar, being more positive or negative, respectively, from
its mate. Oxygen is also stable as a monatom, but also prefers to be paired.
It too can use loose matter to neutralize its monatomic charge, but is
entirely much less happy about the situation.
Three such oxygen monatoms may unite to form ozone. These will either
be +-+, or -+-. The helices arrange with their axes parallel, and triangularly
spaced as an isosceles, when viewed end on. Leadbeater noted that the positive
variety of ozone (+-+) tends to rise, though no tendency to move either
up or down is noted for the negative variety. This is further confirmed
in that for observations performed at high altitudes, nearly all the ozone
found in the atmosphere is of the positive type. In any practical ozone
generation system, equal amounts of each type will be formed. While I have
not tried it, it appears that it should be possible to separate these according
to species, once formed, by placing ozone gas in a potential gradient (-
on the upper electrode surface) that draws the two types apart. Ozone that
is thus separated by species is substantially more stable and far less
explosive in nature than ordinary heterogeneous ozone.
Oxygen is a very energetic and active element, and is capable of mediating
several type of energies, some of which are not as yet recognized by Science.
There are several forces, flowing between and linking individual anu
into associations of the different subatomic particles, and these forces
are seen to originate from, and return to, higher dimensions. They well-up
and later disappear, in a source/sink fashion, associated with anu forming
the ends of their flow paths in our 3 dimensions. Several types of distinct
forces transit along the different coils or whorls of the anu themselves.
Still other types of forces act through larger particles and atoms, and
linking monatoms (for instance) together into diatomic arrangements. Describing
all the forces which can be observed at work is a real challenge. It will
take a great deal of work to separate and quantify these forces, to reduce
them to physics.
As far as I can tell, none of the high energy experiments we can perform
actually "create" (or destroy) matter. But this statement must
be qualified. Under appropriate conditions, particles already existing
in the atomic-level background-vacuum, but still too small (or for other
reasons) to be detectable by us, may be caused to thereby associate, and
this association forms a larger particle, which *is* detectable. This may
make it appear that an energetic photon (for example) was transformed into
matter, whereas the photon actually did no more than provide the energy
of association for number of (unseen) particles that were already present.
Likewise, the mass-to-energy losses that are observed, to balance the
equations in nuclear disintegrations, etc., are also related to the binding
energy of particle associations. The flux between anu is a stream of tiny
"particles" (though these are not hard "particles"
any more than the anu are). These tiny particles each have a minute mass.
The mass of this binding energy stream is a function of the length of the
stream; larger particles typically have longer binding streams, since they
are composed of more anu. It is the mass represented by the inter-anu energy
streams, which represents the mass change in (at least many of) our nuclear
equations, apparent as energy. The anu do not change mass, and both types
are the same. The larger particles of matter we observe thus have masses
which are integer multiples of the anu mass, plus however much mass is
represented in their linking, or binding energy stream. There are a number
of different ways (lengths of stream paths) any particular number of anu
may be linked. This general statement on atomic and subatomic particle
mass quanta does not, of course, apply to particles smaller than one anu,
such as electrons, photons, etc.
If one takes an anu, and uses the Will to take it apart and completely
dissociate it, this can be done, but as soon as the Will is released, the
anu reforms again. It is like taking a piece of slinky spring, and unwinding
it by stretching it out and pressing it flat on the floor with your hands.
But as soon as you let go, it pops back. The individual anu are each (one
discovers) direct force-aspect manifestations of a higher Will, which generates
and sustains all the matter in the Universe. It is... in very fact, the
"Force", which is with us. This Force originates from a dimension
far higher than we (certainly, I) can reach while still clinging to corporeal
form. When we try to conceive of the stupendous number of anu, throughout
all matter of the visible galaxies, which are being held in existence in
such manner, the extent and scope of that Will is truly mind numbing.
If you are interested in gaining insight into the forces at work in
ORMEs systems, you might wish to read a book, first published in 1758,
by a Slavic Jesuit monk named Roger Joseph Boscovich. Its title is "A
Theory of Natural Philosophy - Reducing to a Single Law All the Forces
Which Exist in Nature" [Theoria Philosophiae Naturalis - Redacta ad
Unicam Legem Virium in Natura Existentium]. I believe it is still available
from MIT Press, where I got a copy about twenty years ago.
According to a reference in Scientific American [October 1991, Spin
Cycle - The Spectra of Super Deformed Nuclei, by Philip Yam] from David
Hudson's Dallas presentation:
"A spinning superdeformed nucleus slows down in discrete steps,
each time emitting gamma rays, or highly energetic photons. The emissions
produce a characteristic band of energy spikes all spaced equally apart.
The surprise: the spectra of some different superdeformed nuclei were almost
I suggest that these discrete stepped emissions are the result of rupturing
the valence circuits, one pair at a time, releasing their circuit energy
(as an emission). Since the emission energy is a function of the energy
stored in the valence circuit (and so not constant), when they are observed,
as reported, to be the nearly the same for different elements, then this
is only because the atoms were all charged in their circuits to nearly
the same energy level; this is most probably a consequence of conditions
imposed by the instrumentation environment that the atoms were placed in,
and were observed under.
Some of the elements, though capable of forming ORMEs states, are unstable
as such unless kept spinning quite rapidly, and would drop out of the ORMEs
condition as their spin decreased. The changing effect on atomic moment
of inertia is a result of the valence funnels deforming by swinging out
into the super elongated shapes, and the same is true in reverse as they
release while spinning down. This tends to keep angular velocity (spin
rate) from changing as it would normally be expected to, as angular momentum
is added or subtracted. If an observer using conventional methods is unaware
that this is happening, it can lead to incorrect conclusions about their
moments of inertia.
Although all elements with the dumbbell structure have 12 pairing levels
because each dumbbell has 24 funnels, and these combine by two's to form
12 pairs, this has little to do with the number of electrons (and positrons)
inside the atom.
Do not try to overlay the orbital theory of the atom, onto yogically
observed *real* atoms. You must recognize that while the orbital **model**
explains a great deal, it is, in the final analysis, only an analogy of
reality, and like all analogies, breaks down eventually. Comparing its
artificial constructs to real atoms can be confusing.
In reality, yogically observed atoms do not have electron orbitals.
They are not constructed as we were taught in school. They do not have
a single central nucleus. They have instead multiple "nuclear"
concentrations within the atom, and these move about rapidly. That is the
basis for the nuclear orbitals which Science has recently begun to appreciate.
Atoms are built differently than current theories predict; the forces which
hold them together and maintain their shapes are as yet little understood
by modern science. However, Science *has* observed, cataloged, measured,
and named many of their component particles.
If you will study the drawings of the atoms in the two references cited
at the beginning of this article, you will see that the funnels and bars
are formed by the motions of the groups of anu inside them.
The atom is observed to be built from anu, and the quantized energy-particle
flux between anu. Even the anu are essentially made of these energy-particles.
(Leadbeater has described how this is only an approximately correct statement,
so I won't go into that; see OC 3rd ed, p.19-20). Each anu is composed
of the *equivalent* of 49 smaller particles, on the first level.
The lines of force between the anu, are also streams of tiny particles.
These particles are the equivalents of electrons and positrons of conventional
physics. The positrons are basically the reality behind the "holes"
of conventional solid state physics. Their presence and number within the
atom comprises the total mass of the atom, both as (by equivalency) sub-components
of the anu and as energy streams.
I hope it is clear that each funnel or bar does not represent a single
electron, but only a valence. The valency arises as a result of the algebraic
sum of + & - charges in them, and is much less than the total charge
present. Hence sodium does not have 11 electrons and lawrencium 103 (they
do in modern theory, but not in real atoms). They each have many thousands
of electrons and positrons.
Those who wish to go into this further (the electron as the basis of
3 dimensional atoms) might hunt down a book titled "The Electron Theory
of Matter" by Owen Richardson, published in 1914 by Cambridge University;
612 pages. Owen shows quite elegantly how all atomic phenomena can be derived,
based on only electrons. Very good book. Pity no one reads it anymore.
In my opinion, the ORMEs David Hudson and others are working with under
the blanket term "ORMEs", are predominantly partials of various
levels, and in most cases high order partials, >65% paired, with some
100% species also present. This somewhat arbitrary division includes 4
partial levels of from 8-11 Cooper pairs for dumbbells, and two levels
of from 5-6 pairs for bars-family elements.
Partials rapidly become difficult to distinguish, using ordinary methods,
from one level of pairing to the next, and from completely paired ORMEs,
as the pairing complement increases. That is, they behave like 100% ORMEs
under most circumstances. So the behavior of 100% ORMEs is "typical"
of the ORME mixes David Hudson is working with, composed of mostly high
order partial and 100% ORMEs. I said the color (whether they are white
or not), does not particularly matter, because high order partials are
also white (& fluffy, recalcitrant, etc.), and are in most ways like
100% ORMEs. However, I remain concerned about the potential for long term
biological effects of certain partials, other than gold.
For your convenience, the following table may help to explain what is
happening. I have arranged bars element pairing to approximately match
up or correspond to pairing levels of the dumbbell family. This table simply
depicts the paired to unpaired funnel ratio, as a percentage.
Dumbbells (24 funnels)
Bars (14 bars)
|# Pairs||ORME Percent||# Pairs||ORME Percent|
This table should not be interpreted as describing the degree of manifestation
of ORME properties, which are usually not in proportion to pairing complement,
but are rather nonlinear for many properties. The table only shows ORMEs
With fewer pairing combinations, bars group elements are "lumpier"
in their partial steps, while dumbbells have a fairly fine gradation of
partial ORME stages or steps. There are also differences in behavior, for
the same number of pairs, depending on where the pairs are, relatively
speaking, on a particular partial ORME atomic specimen.
100% ORMEs are definitely scarcer in Nature, and in man-made processes
designed to create them, than are their less-perfect partial relatives.
Perfection is certainly not unheard of in Nature, but it is comparatively
rare. It is the pinnacle of achievement, not the rule or the norm. How
could it be otherwise? 100% ORMEs do not constitute anything like a majority
fraction in Nature's stores of these elements, though they certainly are
an important fraction, whose magnitude varies from element to element,
and which Science will soon quantify, once it learns how to detect them.
With understanding of how statistical processes function, and recognizing
how parallel thermal rate functions (referring here to internal geologic
processes) of association and dissociation work, as I describe elsewhere
in this article, it seems hard for me to see how someone could draw any
Though I believe David Hudson and company are certainly screening out
(e.g. by acid dissolutions, etc) most of the lower order, more metallic-like
partial species, and this increases the relative concentration of 100%
ORMEs (and high order partials) in their preparations. But again, remember
that acid solubilities of partials cannot be categorically defined, based
on pairing alone, since it depends strongly on the energy flowing in the
paired valence circuits. More energy flux brings out their ORME-ishness,
and increasingly screens their remaining chemical and metallic properties.
If the association and dissociation processes were symmetrical throughout
the ORMEs pairing range, this would result in a gaussian distribution,
or a bell curve, centered around 50% pairing, as the highest incidence
of occurrence. But there are non-lineraities that perturb this.
David Hudson's comments notwithstanding, it is noteworthy that partials
participate in metal clusters. They fit a bit awkwardly into the lattice,
but they still behave (partly) as metals, depending on their pairing levels.
That is why Hudson found that commercially prepared metal standards have
a second spectroscopic reading, which shows up late in the long burn, just
like his native ORMEs.
David Hudson has stated that ORMEs don't form metal-metal bonds, yet
offers no explanation for phenomena like this, other than pointing out
the obvious implication, that it is due to the presence of ORMEs. Many
low order partials exist in and among metals, rather than as monatomics.
They might be termed partial-ORME-to-metal alloys. They can markedly alter
the properties of the metal, when present in significant amounts. When
partial ORMEs are understood, their occurrence and effects in metals should
come as no surprise.
An individual, free mon-atom may drop to a 0% ORME state (by any of
a number of mechanisms), so that it technically becomes an ordinary metal/chemical
atom. But unless it joins an aggregate of metal atoms, it remains susceptible
to collisions and other events, which now in all probability would knock
it back into some level of ORME state. Joining a metal cluster is an unlikely
event, since it has been existing as a free and independent mon-atom, and
is not likely to be close to a metallic cluster. So being a mon-atom is,
statistically, a hard habit to kick.
It is more likely that a metal atom will get knocked off its cluster,
and become a mon-atom (ORME or otherwise), than the chance that a metallic
mon-atom will get attached *to* the cluster. That is because mon-atoms
are free, and subject to dispersive forces, so concentrations of them tend
not to develop. So there is a distinct statistical bias, moving metallics
into the ORME state. The rates of these opposite processes (in Nature)
only equalize when there are substantially more ORMEs than metal in the
region around a state system interface at which such processes are active.
Within an ORME population, where all the members are monatomic (including
0% paired metal atoms), there are also important non-linearities. For internal
geophysical processes, the process rates that drive population distributions
are **typically** such that the rate of Cooper pair formation and the rate
of Cooper pair loss, do not balance until a population average above 50%
pairing is reached. There is at least one identifiable factor at work accounting
for this. It is that pairings, once formed, are not only stable (referring
only to dumbbell and bars elements), but tend to increase in stability
as a result of energy subsequently building up and increasing, flowing
through the closed valence circuits. So it typically takes less collision
energy to form a pair, than to break it apart, once it has existed for
a while. In breaking apart, the acquired energy of stability is sometimes
all released, or may be absorbed to varying degrees by other circuits that
may be present.
A second factor is that, once an atom has been knocked into a high spin
state and some pairs have been formed, these tend to be (obviously enough)
on opposite ends, so the bar or dumbbell is more elongated in aspect than
it was before. This increases the likelihood that a subsequent collision
will knock it into a spin on the same spin plane again. This is particularly
true for dumbbells, which tend to have their population peak at a higher
number of pairs than do bars elements.
In Nature, populations of most geothermally formed ORMEs elements peak
at 8-10 pairs for members of the dumbbell group, and 4-5 pairs for elements
in the bars family. Common ORME configurations for many bars elements,
is for the ORME to have two pairs on each end, ie roughly opposite each
other as head and tail, and 6 free valence bars sticking out in between,
around the "waist"; or else three pairs on one end, two on the
other, and 4 free valence bars in between.
These pairing level distributions are sufficient to give those elements
"ghost gold" properties, making them somewhat detectable, though
not recoverable as metals by ordinary methods, since they won't coalesce
into the metal lattices, characteristic of their respective elements. That
is about the level (coming straight from natural materials) that Hudson
experienced, when his dore' button would shatter like glass when hit with
a hammer. As solids, their abnormal valence structures don't produce a
regular symmetrical lattice, and that is why they seem like ceramics. Low
order partials are essentially glassy or amorphous in their micro-structure.
So 100% ORMEs (within natural monatomic populations) are not as rare
as metal mon-atoms, but still by no means dominant.
As I have mentioned, there are ways of precisely separating each pairing
species from one another, and also similarly paired species of related
elements. David Hudson and company are presently unable to do this. Actually,
hardly anyone working with ORMEs at this point even understands or admits
partial pairing exists as a feature of atomic structure, and so experimenters
don't even know there is anything **to** separate.
The potential hazards of partial ORMEs should not be under-estimated.
Low order partials are inherently dangerous when taken indiscriminately,
by those oblivious to the very real effects of their remaining metallic
factors. Gold, even when metallic (let alone in its partial forms), is
non-toxic, so less caution is necessary. However, when someone is suffering
from a life-threatening condition, then it is sometimes necessary to take
extraordinary measures, and to weigh relative risks.
While I have previously referred to ORMEs as exhibiting type II super-conductivity,
this is only superficially correct, and ORMEs (in my opinion) deserve to
be given a separate, distinct classification, such as type III.
In conventional type II Superconductors (SCs), for temperatures within
their superconducting regime, as the external field is increased, the Meissner-generating
currents flowing through the SC (necessary to expel the external flux)
reach a level at which superconductivity in the sample can no longer be
sustained, and superconductivity is destroyed. I have described this event
as a wholesale rupturing of bonds between valence funnels of adjacent atoms
in the lattice. Removing the external field (and hence the current) results
in reforming the Cooper pair bonds, and restoration of superconductivity
(assuming the sample temperature hasn't changed).
However, in the case of ORMEs, superconductivity (transmittance across
the sample body) occurs through Meissner field linkages between individual
ORMEs atoms - an entirely different mechanism. This is true whether the
ORMEs are a continuous body, like an ORMEs glass (small ORMEs-glass particles
are merely small examples of continuous bodies), or an aqueous dispersion.
(Of course, observing superconductivity in aqueous phase dispersions is
not even a possibility for other SC materials, because they are cryogenic.)
At Hc2 (Hc2 is the energy field level at which superconductivity ceases)
for ORMEs, the external Hc2 field only succeeds in establishing itself
*between* the ORMEs atoms, suppressing, or causing their individual atomic-level
Meissner fields to withdraw or be pushed back sufficiently so that the
Meissner-mediated energy transfer between atoms is blocked, interrupting
macro-current flow in the sample. To restate this, the macro Meissner-generating
currents, which act to expel an external flux from an ORMEs body, flow
*between* ORMEs, not *within* individual ORMEs. The function or role of
the ORME atom is to establish the macro-current *path* (via a continuous
chain of Meissner fields), not to produce the expelling current itself.
It is, in fact, a DOUBLE-NESTED system of superconductors: the macro body
superconducts via Meissner field linkages, and within that the individual
ORMEs each superconduct on an atomic level through their individual closed
Cooper pair circuits.
An individual ORME atom in such a population is not much affected by
the presence of an Hc2 field, even despite its stopping of macro-current
flow in the sample body. The ORME atoms' own Meissner fields are only moderately
changed at best; they only must scrunch up a bit, so as to make room for
the external Hc2 field, which is now passing between them. The currents
in the ORMEs atomic circuits thus do not change very appreciably, since
most of the external flux passes around (between) them.
This leads one to the conclusion that Hc2 for ORMEs is not a constant
(though unlike type IIs, it does not depend on temperature). Instead, for
each element, it depends (primarily) upon the energy contained in the Meissner
fields of the individual ORMEs (I am also assuming the ORMEs as being arranged
at their preferred atomic spacings). The strength of these individual atomic
fields ultimately determines how much external field will be required to
force them apart, and supplant them from their inter-atomic connections.
If the Meissner fields are pumped up (or conversely, drained down) and
the Hc2 measurement experiment is tried again, a different value for Hc2
will be found.
Hc2 for ORMEs is still defined as the external field which destroys
super-conductivity in the macro-body of the sample. On the surface it seems
the same as the definition for type II SCs, despite entirely different
mechanisms at work, and despite ORMEs' temperature independence. Furthermore,
like type II SCs, removing the external field restores superconductivity
in ORMEs bodies. (The ORMEs themselves never lost their atomic-level ORMEs
circuits; if they had, removing the external field would not result in
a resumption of superconductivity, which it does). Because of these similarities,
it can be seen how ORMEs could easily be mistaken as a type II material,
and how casual reference to it as such is even reasonably accurate for
So these are laws at work behind the observed phenomena by which ORMEs
particles may sometimes flee the approach of a magnet or hand; first act
inertly when in an intense magnetic field and then resume their flightiness
when it is withdrawn; and so on.
Hopefully, the superficiality of the similarities between type II and
ORMEs behavior are now clear. The following few statements summarize these
conclusions about ORMEs.
1 ORMEs superconductivity is essentially temperature independent.
2 Macro currents are transmitted by inter-atomic Meissner field linkages
through an ORMEs body.
3 Hc2 is the level at which macro-currents in the ORMEs body cease.
4 The Hc2 level for an ORMEs body is a function of Meissner field strengths
of the individual ORMEs.
5 The atomic-level Meissner fields of individual ORMEs are distinct
and largely independent of the macro Meissner field of the ORMEs body,
and only moderately increase at Hc2.
6 Cooper pairs of the ORMEs themselves are typically unaffected by Hc2
field levels, unless the ORMEs Cooper pair circuits are already carrying
flux at or near their critical capacity.
ORMEs are somewhat hydrophilic, and tend also to be hygroscopic. How
much so is in a proportion to how strongly their fields are charged. In
"solution", the Meissner field of each ORME is capable of controlling
a significant number of water molecules; how many, again depends on the
ORME's charge. In such a solution of ORMEs, the separation between ORMEs,
specifically, the distance at which energy normalization can occur between
them is extended by the presence of the water molecules, for a given strength
of Meissner field. It is similar to how inserting a dielectric material
increases the capacitance between two plates. The plates may be much more
widely separated when the intervening space is filled with a material of
hi-dielectric constant, than without it, for the same capacitance. Likewise,
the ORMEs can be further apart in water, and still communicate energy between
The effect of the Meissner fields in such a situation is to artificially
increase the apparent viscosity of the water. It produces a "stiffness"
or pseudo-viscosity which is a function of the concentration of ORMEs,
and of the field strength. The field strengths naturally normalize between
ORMEs under such conditions, so all individuals within the population come
to an equivalence in energy level (assuming mixed species), or to an identical
energy level between identical species. This is the explanation behind
the slimy, gelatinous consistency of aqueous ORMEs dispersions.
The "viscosity" of the suspension may be altered drastically
and dramatically, as a function or cause of anything which affects the
Meissner fields. For example, placing a sample drop in a magnetic field,
well in excess of Hc2, will suppress the extent or range of the individual
Meissner fields and (unless other field types, as I alluded to elsewhere,
are operative) the viscosity may be observed to diminish, particularly
if any macro-currents were present.
The possibility of achieving high-temperature superconductivity with
Tc>300K was predicted over 30 years ago by W.A. Little [Phys Rev A 1964,
vol. 134, p 1416]. You may also be interested in reading D.M. Eagle's paper
in Physica C [1994, vol. 225 p 222-234] on observed room temperature superconductivity,
and other discussions of same delivered at Brookhaven National Laboratory
in April 1994. This is related to the earlier work by LN Grigorov, et al.
Lets suppose that a small pile of lumpy and granulated ORMEs powder
and particles are the sample of an experiment. Let us also presume that
these ORMEs are only weakly or minimally charged, so that Hc2 for them
is considerably below the field strength of a test magnet, at a distance
of a few centimeters. What will happen then...when the magnet is brought
In their initial states, the weakly charged ORME atoms are fixed in
position and orientation, within the solid particle they are a part of.
For individual ORME atoms, sufficiently dispersed in a matrix of other
ORMEs or non-ferrous material, with the ORMEs being sufficiently low in
atomic-level Meissner field strength so as to not be in Meissner linkage
with one another, they may be seen to be capable of something superficially
approximating ferromagnetic behavior. Due to the atomic-level circuits
each ORME atom possesses, some flux will always be present (whenever there
are closed valence circuits), and this will result in a small, net magnetic
moment; this is what I am referring to when I assume they are only weakly
charged. Another way of saying it is that this means a tiny magnetic field
is associated with each ORMEs atom, because of their individual circuit
The nature of the magnetic field of a single ORME atom (although I am
using "atom", I am doing so loosely, so keep in mind that these
are diatoms) depends on which element it is (specifically, what its elemental
atomic shape or form is), how many closed valence circuits it has, and
(for partial ORMEs) where these circuits are located on it, among the possible
pairing locations. The resulting field shapes are not simple dipoles, but
are complex multi-polarizations, depending on the permutations of these
several factors. Nevertheless, in many cases, there will be some net dipolar
or quasi-dipole component, which will be particularly apparent and dominant
in near-field aspect. The net effect of these tiny ORMEs dipoles generally
will produce a gross dipole of some degree in a particular sample particle,
though it is also possible that the sample particle will also display a
more complex field.
The degree to which the net dipoles of the individual ORMEs in a given
particle are aligned to form a gross dipole obviously depends on the history
of the particle, such as what aligning conditions were present at the time
the ORMEs became solidified and fixed into their matrix, and what other
relevant influences were present at the time. They usually tend to align,
individually relative to their neighbor's influences, and as a group relative
to external influences.
When an ORMEs body is placed within an external magnetic field, only
three things may happen, as regards the flux of this field. It may pass
around the body, it may pass through the body, or it may terminate on a
pole or poles associated with the body; each magnetic flux line originates
from, and eventually terminates on, a pole, and these are the only possibilities
(which I shall discuss) that will satisfy this, as far as the ORMEs body
As the test magnet approaches, under a watchful eye, two main things
The first thing is, some of the magnet's flux engages, and terminates
on, the pseudo-dipoles of the ORMEs atoms (those that are aligned attractively
with the external field), whose fields then become continuations or a nexus
for it. While the individual ORMEs do not move about or flip, fixed as
they are within the solid, the particle as a whole may move to orient itself,
under action of the magnetic forces, so that it is aligned most attractively
with this external field, according to its gross dipole or the net disposition
of the ORMEs within it, and that will be its natural inclination, in seeking
a condition of lowest potential energy. This results *initially* in an
apparent ferromagnetic attraction of the gross ORMEs particle to the magnet.
They start to line up in whiskers as if they were iron filings, mapping
the local field of the test magnet.
The second thing that happens is, some of the magnet's flux penetrates
*between* the individual ORMEs atoms (I don't mean between the particles
of powder, but actually between the atoms in each particle), separating
the atoms and cutting off any inter-atomic Meissner linkages which might
have been present. (Remember, I have assumed that the ORMEs were weakly
charged, so Hc2 is below the magnet's strength, allowing this penetration
In penetrating the particle, the field attempts to pass through where
the ORMEs atoms themselves are also, and in doing so it tries to scrunch
their tiny atomic fields up, close to the atoms. This latter mentioned
action, by induction, causes a current in the superconducting ORMEs valence
circuits, opposing the magnet's encroaching field, and forcing it back,
away from the atom. The superconducting valence circuits act as a perfect
If it were only one atom that we were talking about here, that is where
things would stop, but that is not the case. There is a community of atoms,
and the atom has other atom neighbors, on every side of it, and above and
below, in a 3-dimensional arrangement. Consequently, while the first atom
is excluding the field from near itself, it has several neighbors which
are each doing the same thing. As these neighbor atoms exclude the field,
they are at the same time pushing the unwanted flux toward the first atom
again, just as the first atom is pushing it towards them. It is a case
of everybody saying "Not in my neighborhood!", all at the same
This is the source, nature, and mechanism of the field amplification,
within the ORMEs population, that would be needed in order for the ORMEs
to behave as has been observed, in levitating in the earth's half gauss
field, note also that type II SCs do this.
The squeezing of the external field between the ORME atoms greatly increases
the local strength (flux density) of the external field, as seen from the
viewpoint of each individual ORME atom. (The actual degree of flux compression
(field strength amplification) that takes place in this inter-atomic flux
pinch depends in part on the separation between the ORME atoms, but is
very, very great, and may certainly exceed the factor of 10^6 that is required.
The evidence that it does is plainly obvious to anyone, in that ORMEs *do*
As the field compression progresses, each ORME atom continues, in this
runaway induction, to increase the strength of the Meissner-generating
currents which flow in its superconducting closed valence circuits until
a state of equilibrium is reached, as the flux compression function runs
into an asymptotic wall. From the standpoint of each ORME atom, it looks
as though a wall of flux surrounding it is increasing almost without limit
(a near approximation to the hypothetical... Irresistible Force), when
all they are really doing is pushing against each other with the external
flux trapped in between, like a veneer. The magnet's flux that succeeded
in penetrating the particle is now trapped in the inter-atomic spaces it
intruded into. The particle is (for the moment) something like a bead strung
on the lines of external flux.
Just about the same time as this is going on, something else happens.
As the external magnet's flux becomes more and more confined, and the Meissner
fields of the individual ORMEs atoms become increasingly powerful, they
are also forming increasingly efficient field linkages between themselves.
The atoms begin to become capable of (more and more efficiently) transferring
energy with one another, which is another way of saying that the Hc2 value
for the system is increasing.
As this inter-atomic coupling begins to develop, macro "currents"
begin to flow (only in small localized regions of the particle at first).
These localized effects begin expelling the external flux from their area.
As the atoms come into communication with each other, and external flux
continues to be expelled, this sort of cascades and the whole population
transitions into a superconducting state as contiguous, extended particle
In other words, the first thing they do when linkages form is to promptly
develop Meissner-field-generating currents in the macro-particle, to exclude
the external magnet's flux that has, just before, become trapped between
the ORME atoms. As the flux is expelled, the growing diamagnetic field
opposes that of the test magnet's field, and the particle's attraction
changes to being repelled from it.
The rate of development of diamagnetism (or repulsive force) starts
slow, as inter-atomic linkages begin to form for the most closely spaced
atoms, increases as more linkages form and larger currents are possible,
and then finally levels off, as nearly all interatomic linkages which are
possible within a given particle have formed, even for the more widely
spaced ORMEs atomic neighbors. At that point the diamagnetic field stops
It takes a certain amount of time for the ORME atoms, working cooperatively,
to move the embedded external field's lines from being inside to being
out of the particle. Its like when you see somebody being passed across
the room, above the heads of the audience at a rock concert, by everyone's
arms gradually handing them from person to person. But eventually the lines
get expelled from the particle. This migration time (which depends on several
factors) causes a delay before significant repulsion begins to become apparent.
In finally flying away from the magnet, the particle then obeys kinematic
laws (a=f/m) as the acceleration (integrating into velocity) is determined
by the instantaneous repulsive force, as a function of instantaneous field
So the particles first appear to ferromagnetically attract, but before
long change their minds and fly away in diamagnetic repulsion. Please allow
me to point out, that all these behavioral phenomena are consequences (as
put forth in the inductive reasoning of the foregoing explanation) only
of the fact that ORMEs have closed valence circuits. Showing in a compelling
way that the same observed behaviors are required by theoretical atomic
concepts or models, which do not admit to or include closed Cooper pair
valence circuits, may be very difficult indeed, and certainly not as compelling,
I would say.
Zero point coupling is also related to ORMEs' ability to interact with
water, producing the pseudo-viscosity discussed in the previously. The
electromagnetic zero point in these phenomena is an important mechanism
by which energy moves to and from the vacuum energy field, and out of or
into our own space-time.
There exist many zero point doublets, within reach of our experience
(ie, associated with matter and energy phenomena we are capable of manipulating).
They are points where physical and transcendental resonances occur simultaneously,
ie, highly non-linear natural interactions between matter, energy, and
space-time. Each of these zero points represents a point of communication,
through which energy may enter (or exit) our 3 dimensional world from higher
dimensions, the ultimate source of the vacuum energy.
The important thing to understand, is, that it is not necessary for
a particular wave's frequency to "match" the mid-frequency of
a particular zero point doublet, to experience this sort of transition.
It is only necessary that coupling exist between energy (or matter, or
both) in our dimensions (for example) and a zero point resonator. The presence
of the appropriate coupling circumstances with a zero point notch or doublet
results in the entrainment or discharge of energy, by means of coupling
transfer. It is the coupling to the doublet resonator (e.g. a water molecule,
ORME, etc.) which is important. The frequency "shift" of the
coupled energy occurs as a natural consequence of this, due to topological
properties associated with the zero points themselves. The zero points
are not merely the specific frequencies they happen to fall on, within
the electromagnetic spectrum, but are the result of the trans-dimensional
resonator, which just happens to have whatever frequency it has; tuning
the 'right' frequency without or apart from a zero point resonator does
not constitute a zero point.
Meissner effects may also affect taste. Strongly charged ORMEs might
be masked in their metallic properties by the Meissner fields. The manna
of the Israelites was described as tasting like "honey" (Exodus
16:31), or "fresh oil" (Num 11:8). In making it into cakes, the
Hebrews, of course, had to add water to it. Both honey and oil are viscous
substances, and these terms may also give us an indication of the amount
of charge present for those allusions in the account, with perceived taste
varying according to charge.
ORMEs, having individual atomic-level Meissner fields, differ in behavior
from that of type II superconductors, when an ORMEs suspension is exposed
to an external magnetic field. The external magnetic field direction (earth's
field), which penetrates a water suspension of ORMEs is nearly horizontal.
The reaction of the ORMEs population is to exclude the magnetic field.
But because the ORMEs population in suspension is both mobile and discontinuous,
some interesting things occur. The ORMEs nullify and confine the penetrating
field by forming current vortices around each of the quantal lines of flux.
This forms a vortex field, that is, a field made up of a great number of
tiny vortices, dispersed uniformly through the solution when viewed in
a direction parallel to the earth's field lines.
Despite being discrete entities, these vortices mathematically sum into
a single peripheral vortex encircling the flux. Because of the mobility
of the ORMEs in suspension, the ORMEs themselves gradually flow towards
an arrangement of lower energy, which shall eventually exclude all the
field lines from the container. As they do this, these small vortices gradually
coalesce into larger and larger vortices, containing and enveloping the
penetrating flux in larger and larger clumps, till it is all lassoed into
only one large bundle. This might look like a solar prominence. A large
ring current flowing through the arch (and continued in a circuit through
the material in the container), sufficient to exclude the flux from it.
If you broke the arch (physically), the ring current would be interrupted
and cease, and the arch would fall and collapse (no current left to sustain
it, once broken), and the flux trapped under it would escape out through
the point of the breach as the two limbs of the arch fell.