Secrad Geometry at the Atomic Level

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Paranormal Observations of ORMEs Atomic Structure

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 things.

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.

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)

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 patent literature.

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 of superconductivity.

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. 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 to.

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.

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 ceaselessly throbbing, pulsating, spinning, gyrating and processing 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.

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.

Table 1 "Dumbbell" group monatomics, predicted to exhibit the ORME superconducting state.

Sodium Chlorine Copper + Bromine Silver + Iodine Samarium Erbium Gold + Astatine Berkelium Lawrencium+ 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 conditions.

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 axis.

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 exteremely 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 Meissner fields.

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. 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 the earth.

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 catalyst."

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 off.

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. 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. 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. 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 temperatures.

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.

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 formation.

Table 2 "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.

Iron Cobalt * Nickel * Ruthenium * Rhodium * Palladium * Osmium * Iridium * Platinum * Plutonium Americium Curium

* Already specifically named in David Hudson's patent literature.

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 longer, proportionately.

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 vaproized 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 occaisionally 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 occuring, or are needed to explain the results. Only ordinary associative/dissociative reactions, acting on some very unordinary orbital arrangements.

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 occuring 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 isnt. 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 interesting topics. I invite everyone 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.

from a Theosophical student