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Int. J. Mol. Sci. 2012, 13(1), 1066-1094; doi:10.3390/ijms13011066

Article
On the Several Molecules and Nanostructures of Water
Cynthia Kolb Whitney
141 Rhinecliff Street, Arlington, MA 02476, USA; E-Mail: Galilean_Electrodynamics@comcast.net; Tel.: +1-781-643-3155; Fax: +1-781-643-3155
Received: 30 September 2011; in revised form: 4 January 2012 / Accepted: 5 January 2012 /
Published: 19 January 2012

Abstract

: This paper investigates the water molecule from a variety of viewpoints. Water can involve different isotopes of Hydrogen and Oxygen, it can form differently shaped isomer molecules, and, when frozen, it occupies space differently than most other substances do. The tool for conducting the investigation of all this is called ‘Algebraic Chemistry’. This tool is a quantitative model for predicting the energy budget for all sorts of changes between different ionization states of atoms that are involved in chemical reactions and in changes of physical state. The model is based on consistent patterns seen in empirical data about ionization potentials, together with rational scaling laws that can interpolate and extrapolate for situations where no data are available. The results of the investigation of the water molecule include comments, both positive and negative, about technologies involving heavy water, poly water, Brown’s gas, and cold fusion.
Keywords:
Algebraic Chemistry; Brown’s gas; boiling; chemical bond; cold fusion; energy storage; freezing; ice; ionization potentials; melting; quantum chemistry; poly water; quantum mechanics; snow flakes; water chemistry

1. Introduction

Human beings are made mostly of water, and that perspective makes water a subject fitting for deep mathematical study. By ‘deep’ I mean looking at many possible ionic structures, and investigating the possible macroscopic consequences thereof. Water does a number of interesting things, not all of which we are intimately familiar with, since we live mostly within the circumstances of planet Earth’s surface. But we do know about interesting behaviors of some other molecules that are, in deep ways, similar to water. So this study includes some of those other molecules, to ponder as analogs of water, or vice versa, and guide us to look for behaviors we already know about from the other molecules. So this study includes, not just water, but also methane, other hydrocarbons, and other atoms/molecules involved with water in various technologies.

The analytical tool used throughout is ‘Algebraic Chemistry’ (AC). This is a quantitative model for predicting the energy budget for all sorts of changes between different ionization states of atoms that are involved in molecules or nanostructures undergoing chemical reactions or changes of physical state. This paper uses the model to develop information about water: its several possible isomer molecules, the ways in which they might interact, their implications in regard to macroscopic physical states. Analogies between water and other simple molecules are highlighted.

Section 2 reviews and expands information of a formulaic nature from [1], and, following the style of [2], introduces data in numerical form (included as Appendix 1). Section 3 applies AC to ordinary water in its liquid state. Section 4 discusses water in its different physical states, including solid state, which has to initiate with a nanostructure. Section 5 applies AC to discuss water molecules in unusual isomers, arguing that these isomers arise from unusual electron configurations. This leads to a discussion of the phenomenon known as ‘Brown’s Gas’ [3,4], and some parallels with hydrocarbons [5,6]. Section 6 discusses water molecules formed with isotopes of its constituent atoms. This leads to a discussion of the phenomenon known as ‘Cold Fusion’ [7,8]. Section 7 summarizes conclusions, and Appendix 1 collects numerical data in a convenient form for future use by readers.

2. Algebraic Chemistry

All atoms possess ‘Ionization Potentials’ that reflect the strength with which electrons are bound to them. Ionization potentials are generally measurable, and data about them is fairly abundant. As shown in [1], ionization potentials fall into reliable patterns that can be characterized algebraically. Ionization potentials constitute the basic information needed to support the calculations in the following Sections. So we review the formulaic information here, and present it in numerical form, convenient for current and future calculations, in Appendix 1. Some of the formulaic information is from [1], but some is new. The information that is newly developed since [1] is:

  • Higher-Order Ionization Potentials: These are rewritten to highlight use of ‘population-generic’ information and ‘element-specific’ information.

  • Ionization Potentials of Ions: These are developed here, starting from ‘population-generic information and ‘element-specific’ information.

2.1. Patterns in Ionization Potentials

Data on ionization potentials for most elements are generally available for at least several ionization orders. It has been discovered that, after applying a simple scaling, the data fall into a neat pattern. The scaling applied to a measured ionization potential is M/Z, where M is nuclear mass, and Z is nuclear charge. The resulting number is represented by the symbol IPIO,Z, where integer IO is the ionization order. Like the raw data from which it arises, it is denominated in electron volts.

Figure 1 (Fig. 2 in [1]) depicts the behavior of IP’s for all elements (nuclear charge Z = 1 to Z = 120 shown). Element Z actually allows Z ionization potentials, but for larger Z, many IP’s are not so easy to measure. Readily available data go only to seventh order, so that is how many orders are shown. The model is capable of producing plausible estimates for all M/Z -scaled IP’s for all IO’s, beyond those measured, and all Z’s, beyond those yet demonstrated to exist.

The points on Figure 1 are the IP data points. The lines on Figure 1 represent the algebraic model for the IP’s. The model consists of straight-line segments on a semi log plot. That implies simple power laws.

The most striking fact revealed by Figure 1 is that, apart from its first point, the curve for any IO is quite like the curve for IO = 1, but shifted right by IO − 1 elements, and muted in amplitude, more and more muted as IO increases.

The rightward shift of each model line means that each successive element reveals one additional bit of information about all subsequent elements. This fact speaks to the universality of chemical information: basic information about any one element can be inferred reliably from basic information about other elements.

The amplitude muting of successive model lines means the higher-order IP’s involve functions of IO that are not just linear, or just quadratic, or any one power. This fact speaks to the subtlety of chemical information!

2.2. First-Order Ionization Potentials

Since first-order ionization potentials determine everything else, let us begin with ionization order IO = 1. The most startling fact uncovered is that the total rise on every period is the same::

Total rise on every period = 7 / 2

The second most startling fact is that the fall from one period to the next is apparently very regular:

Period to period drop = 7 / 8 three times ; then  1 three times

On each period rise, there are sub-period rises. They are all of the form

Incremental rise = total rise × fraction

For the first sub-periods,

Fraction = 1 , 1 / 2 , 1 / 3 ; then  1 / 4 four times

For all subsequent sub-periods,

fraction = [ ( 2 l + 1 ) / N 2 ] [ ( N - l ) / l ]

where l is the traditional ‘angular momentum’ quantum number for nominal single-electron states being filled, and N is a non-traditional parameter that depends on the number L of elements in a period: 2N2 = L. Table 1 collects all the information about sub-period fractional rises.

In the model, sub-period rises are split between the two spin states, plus 1/2 and minus 1/2. That makes two distinct sub-segments. Further details and actual numerical data are given in Appendix 1.

2.3. Higher-Order Ionization Potentials

The model for atoms used here is based on Hydrogen. The Hydrogen-based model invites the division of each ionization potential IP1,Z into two parts, one being IP1,1 for the generic Hydrogen-like collective interaction with the nucleus, and the other being the increment ΔIP1,Z = IP1,ZIP1,1 for the element-specific electron-electron interactions, which do not exist for Hydrogen.

Higher ionization order is characterized by IO > 1. Figure 2 uses IP1,1 and the IP1,Z to express the IP’s for all IO > 1. (Ref. [1] gave a detailed development of the IP’s for IO > 1 and presented the information without using the decomposition of IP1,Z into IP1,1 and IP1,Z.)

The ‘etc.’ means that the pattern established at IPIO,IO+3 continues from there on. Indeed, even IPIO,IO+2 is a special case of the general pattern revealed in IPIO,IO+3. The first term in IPIO,IO+3 is universal. The second term is period specific. The third term is element specific.

The leading terms representing any IP are proportional to IO2. This dependence suggests that the physical process generating the data involves removing IO electrons all at once, and not removing just the single electron left after IO − 1 other electrons have already been removed, or possibly just skipped over and left in place. This distinction about removing IO electrons all at once, vs. any scenario that removes just one electron, is obvious from the mathematical factor IO2, but it is not obvious from a description by a typical text phrase, such as ‘third-order ionization potential’, for example. So when reading the existing literature on ionization potentials, always watch out for the possibility of confusion arising from inadequate language.

The secondary terms representing any arbitrary IP are linear in IO. These terms implement the ‘shift right’ behavior seen in Figure 1. They also determine the numerical pattern that the period rises follow. For IO ≡ 1, the period rises are all 7/2. For all IO > 1, all but the first period are the same, but less than 7/2, gradually approaching unity as IO increases.

A formula for the period rises can be determined by looking at the ratio IPIO,IO+10/IPIO,IO+2:

I P I O , I O + 10 I P I O , I O + 2 = 1 2 I P 1 , 1 ( I O 2 + I O ) + 1 2 Δ I P 1 , 3 ( I O 2 - I O ) + Δ I P 1 , 10 I O 1 2 I P 1 , 1 ( I O 2 + I O ) + 1 2 Δ I P 1 , 3 × ( I O 2 + I O ) ,

Here Δ I P 1 , 3 = - 1 8 I P 11 and Δ I P 1 , 10 = ( 7 8 × 7 2 - 1 ) I P 1 , 1 = 33 16 I P 1 , 1. From these values, one finds that period rises, except for the first period, follow the simple formula (IO + 6)/(IO + 1), which reduces to 7/2 for IO = 1.

The exception for first-period rises when IO > 1 demands an explanation. To begin developing the explanation, note the factor of 2 in the formula for IPIO,IO for IO > 1:

I P I O , I O = 2 × I P 1 , 1 × I O 2

Why does this formula not come out, as it must for IO ≡ 1, as IPIO,IOIP1,1 × IO2 ? A possible explanation is that, unlike first-order ionizations, these total ionizations are not best characterized as ‘removal of electrons from the atomic system’; they are better characterized as ‘expulsion of the nucleus from the atomic system’. Note that electrons have a lot of kinetic energy; on average, an amount equal to half the magnitude of their (negative) potential energy in the atomic system. By contrast, the nucleus has almost no kinetic energy. So expelling the nucleus from the atomic system takes essentially twice the energy that removing all of the electrons together from the atomic system would take. But the fragility of the electron subsystem probably prevents the latter scenario.

Next, consider the formula for the scenario that starts with IO + 1 electrons, and ends up with one electron:

I P I O , I O + 1 = I P 1 , 1 × 2 × I O 2 + 1 2 × I P 1 , 1 × I O + 1 2 Δ I P 1 , 2 × I O

The first term, IP1,1 × 2 × IO2, is identical to the formula for starting with io electrons and ending up with no electrons. So this part of the scenario looks like the blow-the-nucleus-out scenario, but not with just the nucleus alone; instead, this nucleus takes one electron with it, so that what is blown out is a nucleus-plus-electron system that is like a nucleus with charge IO instead of IO + 1. That leaves an electron system with IO electrons still to dispose of.

The second term, 1 2 × I P 1 , 1 × I O, defines what it means to ‘dispose of’ IO electrons. Each electron is blown away with enough energy, 1 2 × I P 1 , 1, so that any pair of them has energy IP1,1, sufficient to keep them away from each other.

The third term, 1 2 Δ I P 1 , 2 × I O, suggests a possible structure for the system of IO electrons. If the system is a ring, or several rings, it takes IO binary cleavages to destroy the system. So there is the factor of IO multiplying ΔIP1,2. But why is there also the factor of 1 2 multiplying ΔIP1,2? Well, consider that when every electron gets energy 1 2 Δ I P 1 , 2, then any pair of them has enough energy, ΔIP1,2, to resist reuniting as a pair.

Next, consider the scenario that starts with IO + 2 electrons, and ends up with 2 electrons. We have:

I P I O , I O + 2 = 1 2 I P 1 , 1 ( I O 2 + I O ) + 1 2 Δ I P 1 , 3 × ( I O 2 + I O )

The first term, 1 2 I P 1 , 1 ( I O 2 + I O ), contains 1 2 I P 1 , 1 I O 2, which is quite different from the IP1,1 × 2 × IO2 seen in the cases of IO and IO + 1: it has the overall factor of 1 2 instead of 2. This means that there is no expulsion of a nucleus-like system consisting of the nucleus plus two electrons, which would have charge IO instead of IO + 2. Instead, IO electrons are blown away from the atom, leaving the nucleus-like system behind. The factor of 1 2 on 1 2 I P 1 , 1 I O 2 means the nucleus-like system and the expelled electron system have between them enough energy, IP1,1IO2, to keep them away from each other.

The first term here also contains 1 2 I P 1 , 1 × I O, which was present in the IO + 1 case as the second term there. The 1 2 I P 1 , 1 × I O means the same thing here: each electron is given enough energy, 1 2 × I P 1 , 1, so that any pair of them has energy IP1,1, sufficient to keep them away from each other.

The second term here, 1 2 Δ I P 1 , 3 × ( I O 2 + I O ), is actually negative, because Δ I P 1 , 3 = - 1 8 I P 11. The second term scales down the energy increments recommended by the first term as being necessary to keep away the IO electrons, either as a group (the IO2 term), or as individuals (the IO term). The scale-down reflects the fact that an electron system consisting of just two electrons by themselves is the most stable electron system seen anywhere in Nature. Like a paper currency note, it can seem too big to break.

Next, consider the scenario that starts with IO + 3 electrons and ends up with 3 electrons. We have:

I P I O , I O + 3 = 1 2 I P 1 , 1 ( I O 2 + I O ) + 1 2 Δ I P 1 , 3 ( I O 2 - I O ) + Δ I P 1 , 4 I O

The first term is the same as it was in IPIO,IO+2, and has the same meaning here. The second term, 1 2 Δ I P 1 , 3 ( I O 2 - I O ), differs by the internal minus sign from the second term 1 2 Δ I P 1 , 3 ( I O 2 + I O ) in IPIO,IO+2. That minus sign on the already negative ΔIP1,3 effectively adds to the energy requirement to keep individual electrons from coming back. The third term, ΔIP1,4IO, further raises the energy needed to keep individual electrons from coming back, inasmuch as ΔIP1,4 is positive. The message is: three electrons is a really an unstable situation. As with small coins, something is likely to get lost.

2.4. Ionization Potentials of Ions

The events described by higher-order ionization potentials are very vigorous, even violent: stripping IO electrons off an atom all at once. This takes explosions, particle beams, etc. There is a much gentler way to end up with the same end result: strip the electrons off one at a time. (Or add them one at a time.) The distinction is usually not made clear, but it is well captured in [2] with the attribution ‘Pauling’ for the ‘all-at-once’ event, and the word ‘spectroscopic’ for the ‘one-at-a-time’ process.

The gentle subtractions or additions are what most chemical reactions do. So we need to work out how to model them. Above we separated ΔIP1,1 and ΔIP1,Z. For first-order ionizations, the IP’s scale with Z/M. This means that the constituent parts, IP1,1 and ΔIP1,Z, both scale with Z/M too. But for an already ionized atom, the modifications to Z/M will be different for the two parts, IP1,1 and ΔIP1,Z. Now instead of just Z, we need to recognize a separate ZP for proton count and Ze for electron count, and instead of just M, we need to be clear that we mean M(ZP).

For single electron removal, we generally need the scaling of IP1,1 as:

I P 1 , 1 Z / M I P 1 , 1 Z p Z e / M ( Z p )

For the destruction of the original electron cluster, we need scaling of ΔIP1,Z as:

Δ I P 1 , Z Z / M Δ I P 1 , Z e Z e / M ( Z p )

along with an energy associated with the creation of the resultant electron cluster:

- Δ I P 1 , ( Z e - 1 ) ( Z e - 1 ) / M ( Z p )

This last energy increment will be cancelled if the electron removal process continues. Otherwise, depending on sign, it can represent heat lost to the environment, or taken from the environment.

For single electron addition, we need similar terms with some signs reversed. First, the baseline energy for adding (opposite of removing) an electron:

- I P 1 , 1 Z / M - I P 1 , 1 Z p Z e / M ( Z p )

with the energy for destruction of the original electron cluster

Δ I P 1 , Z Z / M Δ I P 1 , Z e Z e / M ( Z p )

and the energy for the creation of the resultant electron cluster:

- Δ I P 1 , ( Z e + 1 ) ( Z e + 1 ) / M ( Z p )

The use of these formulae is illustrated with the analyses in the next Sections.

3. Ordinary Water

Ordinary water is made of two ordinary Hydrogen atoms and an ordinary Oxygen atom. To conduct an analysis of it, we need basic information about Hydrogen and Oxygen.

The development of the relevant information about Hydrogen goes as follows:

Write Formulae:

H 1 H 1 + : I P 1 , 1 × 1 / M 1 H 1 H 1 - : - I P 1 , 1 × 1 × 2 / M 1 - Δ I P 1 , 2 × 2 / M 1

Insert Data (eV):

H 1 H 1 + : 14.250 × 1 / 1.008 eV H 1 H 1 - : - 14.250 × 1.4142 / 1.008 - 35.625 × 2 / 1.008 eV

Evaluate Formulae:

H 1 H 1 + : 14.1369 eV H 1 H 1 - : - 19.9924 - 70.6845 = - 90.6769 eV

The development of the relevant information about Oxygen goes as follows:

Write Formulae:

O 8 O 8 + : I P 1 , 1 × 8 / M 8 + Δ I P 1 , 8 × 8 / M 8 - Δ I P 1 , 7 × 7 / M 8 O 8 + O 8 + + : I P 1 , 1 × 8 × 7 / M 8 + Δ I P 1 , 7 × 7 / M 8 - Δ I P 1 , 6 × 6 / M 8 O 8 O 8 - : - I P 1 , 1 × 8 × 9 / M 8 - Δ I P 1 , 9 × 9 / M 8 + Δ I P 1 , 8 × 8 / M 8 O 8 - O 8 - - : - I P 1 , 1 × 8 × 10 / M 8 - Δ I P 1 , 10 × 10 / M 8 + Δ I P 1 , 9 × 9 / M 8

Insert Data (eV):

O 8 O 8 + : 14.250 × 8 / 15.999 + 13.031 × 8 / 15.999 - 13.031 × 7 / 15.999 eV O 8 + O 8 + + : 14.250 × 7.4833 / 15.999 + 13.031 × 7 / 15.999 - 7.320 × 6 / 15.999 eV O 8 O 8 - : - 14.250 × 8.4853 / 15.999 - 20.254 × 9 / 15.999 + 13.031 × 8 / 15.999 eV O 8 - O 8 - - : - 14.250 × 8.9443 / 15.999 - 29.391 × 10 / 15.999 + 20.254 × 9 / 15.999 eV

Evaluate Formulae:

O 8 O 8 + : 7.1254 + 6.5159 - 5.7014 = 7.9399 eV O 8 + O 8 + + : 6.6652 + 5.7014 - 2.7452 = 9.6214 eV O 8 O 8 - : - 7.5577 - 11.3936 + 6.5159 = - 12.4354 eV O 8 - O 8 - - : - 7.9665 - 18.3705 + 11.3936 = - 14.9434 eV

Summarize for Convenience:

O 8 O 8 + + : 7.9399 + 9.6214 = 17.5613 eV O 8 O 8 - - : - 12.4354 - 14.9434 = - 27.3788 eV

Water is known to dissociate into the naked proton H+ and the hydroxyl radical OH. The hydroxyl radical has to be the combination of ions O− − + H+, the formation of which takes −27.3788 + 14.1369 = −13.2419 eV; there is not an alternative form using H, because then O would have to be neutral.

So it is natural to consider H2O as H+ + OH, or equivalently 2H++ O− −. Forming water as H+ + OH, or equivalently 2H++ O− −, takes 14.1369 − 13.2419 = + 0.8950 eV, or equivalently 2 × 14.1369 − 27.3788 = +0.8950 eV, a slightly positive energy.

A molecule with a positive energy is not completely stable. It will tend to dissociate into the ions H+ and OH, as ordinary water in fact does. But ordinary water does not dissociate very much. Only about one part in 107 will be dissociated at any given moment. So water as 2H++ O− − isn’t the complete story.

I have previously considered [5] an additional feature that is analogous to pair formation between electrons, known in Physics as Cooper pairing, and very evident in Chemistry in the first ionization potential of Helium. The posited additional feature is pair formation between two H+’s; i.e. two naked protons.

But here I want to consider another possibility first. A plausible ionic configuration for water is 2H+ O++. The transition 1H → H takes −19.9924 − 70.6845 + 0 = −90.6769 eV, and the transition 8O → 8O++ takes 17.5613 eV. So making H2O as 2H and O++ takes 2 × (−90.6769) + 17.5613 = −163.7925 eV. This is much more energetically favorable than making H2O as 2H++ O− −, at +0.8950 eV. So 2H+ O++ is a better candidate for the ionic configuration of ordinary water.

This ionic configuration helps explain why the normal water molecule is bent to an angle that recalls a tetrahedron? Indeed it does help. Imagine the heavy O++ ion with four satellites around it: two H nuclei (protons), and the two 2e subsystems (electron pairs). The two protons go to two corners of the tetrahedron, and the two electron pairs go to the other two corners.

And how about the polarization of ordinary water molecules? Does the ionic configuration explain that? Of course it does: The typical tetrahedral water molecule with two negative corners and two positive corners is, of course, polarized.

4. Physical States of Water

The polarization of ordinary water helps one water molecule attract another, and gradually form into a solid crystal: ice. There is an interesting feature about ordinary water ice: unlike just about anything else, water expands upon freezing. Does the vision of normal water as 2H+ O++ in a tetrahedral arrangement help explain that odd property? Indeed it does help. The electron pairs have to orbit their respective protons, and being identical, they orbit in synchrony. That makes the whole tetrahedron spin about an axis that is the tetrahedron edge connecting the two protons. A tetrahedron spinning on an axis that is an edge is a lop-sided occupier of space. It sweeps out a volume that is larger than that of the tetrahedron, shaped like two regular cones joined at their circular bases, and slightly truncated at their apexes. That double-cone sweep volume is the minimum volume that a water molecule can occupy.

When the water is liquid, the spinning tetrahedrons can tolerate other spinning tetrahedrons temporarily invading any temporarily vacant space: they can bounce, or otherwise adjust. But when water is frozen, adjustments are not possible. Each spinning tetrahedron needs to have sole ownership of the volume of space in which it spins. So upon freezing, water expands.

We could really think about the freezing of water the other way around: upon melting, water contracts, because the flexibility of the liquid state permits ‘timesharing’ of the physical ‘real estate’.

And what of snowflakes? Why do they have their obvious hexagonal symmetry? The double-cone image helps with this question too. Obviously, the most efficient packing arrangement on a plane is one double cone surrounded by six others; i.e., hexagonal packing.

Snowflakes originate with nanostructures of seven molecules. Those nanostructures are perhaps the first ever to produce wonder in the human mind! Beyond this lovely thought, water is a pretty good example with which to talk about the physical states of matter generally.

This Section investigates the relationships between the macro states of matter—solid, liquid, gas, and plasma—and the micro states of ionization—neutral, singly ionized, doubly ionized, and so on. Readily available data show that boiling points and melting points follow a pattern, related to the pattern that first-order ionization potentials follow. Such patterning suggests that observed boiling and melting are related to hidden changes in ion populations. That would mean that the macroscopic states of matter are related to the microscopic states of atoms. This chapter poses a hypothesis about the relationship, and investigates the hypothesis in a quantitative way. The story involves the Planck energy distribution for black body radiation as a background for transitions between ionization states.

It is a source for photons of appropriate energy to provoke transitions, and it is a dumping ground for waste heat from spontaneous transitions. The state changes themselves often have a cascade character: the background supports the first change, and then some subsequent changes occur spontaneously. That scenario can make macroscopic state changes look as abrupt as they do.

This story goes far back to antiquity. Aristotle identified the macroscopic states of matter as Earth, Air, Fire, and Water. Seen in retrospect, that is an amazingly good categorization. The modern view has those same four macro states, but reordered as Earth, Water, Air, and Fire, and renamed as Solid, Liquid, Gas, and Plasma.

But now there are also many sub-categories that are specifically acknowledged. A Solid can be Conductor, a Super Conductor, a Semi Conductor, an Insulator, etc. A Liquid can be a Fluid, a Super Fluid, a Solvent, an Oil, a Plastic, a Pyroclastic, a Glass, a Conductor or an Insulator, a Solution, a Suspension, etc. A Gas can be Inert, Explosive, and so on, A Plasma can be Hot, Cold, etc.

4.1. Macroscopic Physical States and Microscopic Ionization States

It is reasonable to consider the possibility that macroscopic states of matter have some correlation with the microscopic ionization states, especially since one of the four main macroscopic states, namely the plasma state, has absolutely everything to do with ionization states.

What is the key similarity between macroscopic states of matter and ionization states? It is energy.

In the case of the four main macroscopic states of matter, state transitions can be correlated with changes in temperature and pressure, which relate to thermal and mechanical energy.

As for the various sub-categories within the four main macroscopic states, those too must have something to do with energy, but more in the nature of chemical-energy change, or configuration-energy change.

It appears that generally the difference between one macroscopic state of matter and another is some pressure × volume-change energy and/or some temperature × entropy-change energy.

In the case of ionization states, the difference between one state and another is electromagnetic energy, and, possibly, some thermal energy. To accomplish a change of ionization state, electromagnetic work may be invested, and heat may be dumped. The final energy of an ionization state is the cumulative sum of work increments invested and heat increments dumped in getting from the neutral state to the ionized state.

This Section is limited to just the four macroscopic states of matter: solid, liquid, gas, and plasma. Data about these macroscopic state changes are usually provided as point values of temperatures: melting points and boiling points. (As for excitation to the plasma state, that seems more difficult to document with temperature data.)

Figure 3 shows reported melting points and boiling points, in comparison to first-order ionization potentials. The horizontal axis is the nuclear charge Z of the elements. The vertical axis is electron volts for ionization potentials, and degrees Kelvin for boiling points (series 1, squares) and melting points (series 2, triangles). The vertical scale is logarithmic to accommodate a large dynamic range. The solid line (series 3) reproduces the first order IP’s, or M/Z-scaled ionization potentials from Figure 1.

Observe that the dynamic range of boiling and melting temperatures is huge compared to the dynamic range of IP’s: we need four decades for temperatures, vs. one decade for IP’s. The temperature range for the liquid state varies from nearly a factor of 5.5 (i.e., very substantial range for liquid state) down to nearly a factor of 1 (i.e., no range at all for liquid state). There is a clue here that the liquid state is rare, so we are lucky that our planet, at least, has plenty of liquid water for us.

Despite the huge difference in dynamic range, the temperature data are clearly correlated with the IP data. The correlations are rough, but very compelling. What is actually going on here? To investigate this question, we require a hypothesis to test. My candidate hypothesis is that:

  • The solid state involves ions and/or radicals existing in pairs that are in negative energy states;

  • The liquid state involves neutral atoms and/or molecules, along with some ions existing in pairs that are mostly in negative energy states;

  • The gas state involves neutral atoms and/or molecules, along with some ions existing in pairs that are mostly in positive energy states;

  • The plasma state is composed significantly of ions existing in pairs that are in positive energy states.

4.2. Physical States and Ionization States

Figure 4 offers a conceptual structure for the problem. The horizontal axis represents temperature, ranging from absolute zero to some very high temperature, represented by the ‘1’ at the right end. The vertical axis represents the population fraction of atom pairs in different ionization states. The energy of an ionized state is the cumulative result of work increments required and heat increments dumped in getting from the neutral state to the ionized state. It can be negative, positive, or zero. The three curves represent these three regimes of ionization state energy. The left curve, consistently descending with temperature, represents the fraction of ion pairs that are to be found in negative energy states. The right curve, consistently increasing with temperature, represents the fraction of ion pairs that are to be found in positive energy states. The middle curve, first increasing with temperature and then decreasing with temperature, represents the fraction of atom pairs to be found in the neutral, un-ionized state.

Figure 4 is quite generic. Its particular realization for a particular substance may be shifted right or left, or have the middle crossing point higher or lower, with the middle bump correspondingly lower or higher. Much higher is possible; you know this is true if you think about water: the proportion of H+ is only about 1 × 107.

The three curves exhibit three crossing points, and they thereby define four temperature ranges. This situation invites consideration of the possibility that these four temperature ranges correlate with the four top-level states of matter: solid, liquid, gas, and plasma.

But temperature T is not the only independent variable. There is always at least one other. Pressure P can be taken as the other one. So macroscopic state changes are not adequately characterized as a point over a one-dimensional temperature axis; they need a line on a two-dimensional P, T phase diagram.

Figure 5 shows what a generic phase diagram looks like. The horizontal axis represents temperature T, and the vertical axis represents pressure P. The 1 on the horizontal axis corresponds to absolute zero temperature. The 101 means the plot is constructed from 101 temperature data points. The 0 on the vertical axis means zero pressure, and the 1 means the maximum pressure plotted, whatever that might actually be.

The left side of the picture corresponds to low temperature, and hence the solid state. The middle part of the picture represents higher temperature and hence the liquid state. The bottom of the picture represents low pressure, and hence the gas state.

The short curved line segment in the lower left marks transitions directly between solid and gas states, called ‘sublimation’ in the direction of solid-to-gas. Sublimation is an example of a situation wherein not all four states of matter occur. At low pressure, the liquid state does not occur; the solid state goes directly to the gas state.

The nearly vertical line marks the more usual transitions between solid and liquid. Observe that over most of the pressure range, these transitions occur at nearly the same temperature. So that is why the idea of ‘melting point’, or ‘freezing point’, is a pretty reliable one to put a single number to. However, pressure does affect melting temperature a little bit. You know that this is true, if you ever go ice-skating. The second curved line segment marks transitions between liquid and gas. It depends noticeably on pressure. You know that this is true, if you ever go camping at various mountain altitudes. That makes the idea of ‘boiling point’ or ‘condensation point’ tough to put a single number to.

The point on Figure 5 where the three lines meet is called the ‘triple point’. Three states of matter, solid, liquid, and gas, can co-exist there.

The point on Figure 5 marked by a big black dot is called the ‘critical point’. The distinction between liquid and gas simply disappears there. Matter in this condition simply goes ‘opalescent’. This is a big mystery, worthy of much research. It begs the questions: what about points not beyond, but beside the critical point? Where exactly does the distinction between liquid and gas reappear?

Figure 5 overall begs an even bigger question: what about the plasma state? Unfortunately, it hasn’t been customary in the past to include the plasma state on phase diagrams. So including it constitutes an open research topic. Here we can only offer a few remarks. Consider Figure 6.

If the plasma state were included on phase diagrams, where might the transitions to plasma state go? I suspect a nexus to the critical point. I don’t really believe Nature does a ‘termination’ at the critical point; it more likely does another triple point, this one involving liquid, gas, and plasma. If so, where would the transition lines for liquid/plasma and gas/plasma likely go? It seems clear that for temperatures high enough, the plasma state trumps the gas state, and for pressures high enough, the solid state trumps the plasma state. So I expect the lines missing from Figure 5 to go generally diagonal, downward to the right, as illustrated by the new straight line shown on Figure 6. I do not mean to imply that the new lines should actually form this straight line; they could curve, they could change direction sharply at the critical point, or do whatever one can imagine; at present, we have no knowledge about such details. We only know that we should now go looking for them.

Observe that Figure 6 shows the liquid state limited to the totally surrounded, approximately triangular, area in the center. This means that, over the cosmological range of temperatures and pressures out there, the liquid state is something very rare. You know that this is true, if you are interested in space exploration, and follow NASA’s search for water.

Observe too that Figure 6 suggests yet another triple point, somewhere near the left top of the Figure. This third triple point involves the solid, liquid, and plasma states. It is my prediction that such a triple point exists, and will some day be observed.

Observe too that there are two more transitions of the sublimation type: a state of matter being skipped. Besides the transition from solid to gas, there is a transition from solid to plasma and a transition from liquid to plasma.

Can water illustrate for us any of these anticipated phenomena? It all depends on whether water can have anything like a plasma state. That question brings us to the next topic.

5. Isomers of Water

If water has anything like a plasma state, the molecule approaching that state is certainly not the ordinary tetrahedral water molecule. So we need to search out one or more isomers of water.

5.1. A Linear Isomer of Water

A linear isomer of water is thought to be the important constituent of the plasma-like phenomenon known as ‘Brown’s gas’. See, for example, [3,4]. Brown’s gas is of technological interest because it can perform welding and other technologically important tasks. One particularly interesting property of Brown’s gas is that it causes no harm when impinging on human flesh. Evidently, that is because the human flesh does not have metal content; flesh is essentially water, like the Brown’s gas itself is.

The ionic configuration 2H++ O− − previously displaced by 2H+ O ++ as the candidate for ordinary tetrahedral water is actually quite interesting in this new context: it could be the ionic configuration for the linear isomer of water in Brown’s gas. Because all of the electrons in 2H++ O− − are in the possession of the Oxygen nucleus, the two naked Hydrogen nuclei can settle along the poles of the Oxygen system. So unlike the 2H+ O ++ isomer, the 2H++ O− − isomer is not polarized.

Section 3 determined that the formation of water in the ionic configuration 2H++ O− − takes 14.1369 − 13.2419 = + 0.8950 eV, or equivalently 2 × 14.1369 − 27.3788 = + 0.8950 eV. This is a slightly positive energy. By contrast, the formation of water in the ionic configuration 2H+ O ++ takes 2 × (−90.6769) + 17.5613 = −163.7925 eV. This is a very negative energy.

Section 4 posited an association between the energy of ionic configuration and physical state of matter. Observe that Brown’s gas fits the posited association: under conditions where ordinary tetrahedral water is liquid, the linear isomer is a gas. Observe too that, in an application like welding, Brown’s gas can be described as ‘burning’. But it doesn’t burn in the usual sense: by oxidation. It need not consume any oxygen; it can just revert to its normal water isomer. The release of energy makes a release of light, and at that moment the Brown’s gas may reasonably be regarded as being in the plasma state.

The whole situation with Brown’s gas can be compared to that of methane CH4. I previously analyzed the ionic configuration C4− + 4H+ [5]. The relevant information about Carbon is developed as follows:

Write Formulae:

C 6 C 6 - : - I P 1 , 1 × 6 × 7 / M 6 - Δ I P 1 , 7 × 7 / M 6 + Δ I P 1 , 6 × 6 / M 6 C 6 - C 6 - - : - I P 1 , 1 × 6 × 8 / M 6 - Δ I P 1 , 8 × 8 / M 6 + Δ I P 1 , 7 × 7 / M 6 C 6 - - C 6 3 - : - I P 1 , 1 × 6 × 9 / M 6 - Δ I P 1 , 9 × 9 / M 6 + Δ I P 1 , 8 × 8 / M 6 C 6 3 - C 6 4 - : - I P 1 , 1 × 6 × 10 / M 6 - Δ I P 1 , 10 × 10 / M 6 + Δ I P 1 , 9 × 9 / M 6

Insert Data (eV):

C 6 C 6 - : - 14.250 × 6.4807 / 12.011 - 13.031 × 7 / 12.011 + 7.320 × 6 / 12.011 eV C 6 - C 6 - - : - 14.250 × 6.9282 / 12.011 - 13.031 × 8 / 12.011 + 13.031 × 7 / 12.011 eV C 6 - - C 6 3 - : - 14.250 × 7.3485 / 12.011 - 20.254 × 9 / 12.011 + 13.031 × 8 / 12.011 eV C 6 3 - C 6 4 - : - 14.250 × 7.7460 / 12.011 - 29.391 × 10 / 12.011 + 20.254 × 9 / 12.011 eV

Evaluate Formulae:

C 6 C 6 - : - 7.688 - 7.5945 + 3.6566 = - 11.6267 eV C 6 - C 6 - - : - 8.2197 - 8.6794 + 7.5945 = - 9.3046 eV C 6 - - C 6 3 - : - 8.7184 - 15.1766 + 8.6794 = - 15.2156 eV C 6 3 - C 6 4 - : - 9.1900 - 24.4701 + 15.1766 = - 18.4835 eV

Summarize for Convenience:

C 6 C 6 4 - : - 11.6267 - 9.3046 - 15.2156 - 18.4835 = - 54.6304 eV

About Hydrogen, we already know 1H → 1H+: 14.1369 eV, so we have

4 1 H 4 1 H + : 4 × 14.1369 = 56.5476 eV .

So forming methane as C4− + 4H+ takes −54.6304 + 56.5476 = +1.9172 eV. This is just over twice the +0.8950 eV that it takes to make water as 2H+ + O−−. So both of these molecules in these ionic configurations are respectable fuels. The difference is that to release energy, methane has to burn oxygen, whereas linear water does not; it only has to revert to its tetrahedral isomer.

It is interesting that, like water, methane too has an alternative ionic configuration with charge signs reversed: C4+ + 4H. To analyze this, the relevant information about Carbon is developed as

Write Formulae:

C 6 C 6 + : I P 1 , 1 × 6 / M 6 + Δ I P 1 , 6 × 6 / M 6 - Δ I P 1 , 5 × 5 / M 6 C 6 + C 6 + + : I P 1 , 1 × 6 × 5 / M 6 + Δ I P 1 , 5 × 5 / M 6 - Δ I P 1 , 4 × 4 / M 6 C 6 + + C 6 3 + : I P 1 , 1 × 6 × 4 / M 6 + Δ I P 1 , 4 × 4 / M 6 - Δ I P 1 , 3 × 3 / M 6 C 6 3 + C 6 4 + : I P 1 , 1 × 6 × 3 / M 6 + Δ I P 1 , 3 × 3 / M 6 - Δ I P 1 , 2 × 2 / M 16

Insert Data (eV):

C 6 C 6 + : 14.250 × 6 / 12.011 + 7.320 × 6 / 12.011 - 2.805 × 5 / 12.011 eV C 6 + C 6 + + : 14.250 × 5.4772 / 12.011 + 2.805 × 5 / 12.011 - 9.077 × 4 / 12.011 eV C 6 + + C 6 3 + : 14.250 × 4.8990 / 12.011 + 9.077 × 4 / 12.011 - ( - 1.781 ) × 3 / 12.011 eV C 6 3 + C 6 4 + : 14.250 × 4.2426 / 12.011 + ( - 1.781 ) × 3 / 12.011 - 35.625 × 2 / 12.011 eV

Evaluate Formulae:

C 6 C 6 + : 7.1185 + 3.6566 - 1.1677 = 9.6074 eV C 6 + C 6 + + : 6.4982 + 1.1678 - 3.0229 = 4.6431 eV C 6 + + C 6 3 + : 5.8122 + 3.0229 + 0.4448 = 9.2799 eV C 6 3 + C 6 4 + : 5.0335 - 0.4448 - 5.9321 = - 1.3434 eV

Summarize for Convenience:

C 6 C 6 4 + : 9.6074 + 4.6431 + 9.2799 - 1.3434 = 22.1870 eV

About Hydrogen, we already know 1H → 1H+: −19.9924 − 70.6845 = −90.6769 eV

So we have

4 H 1 4 H 1 - : 4 × ( - 90.6769 ) = - 362.7076 eV

So forming methane as C4+ + 4H takes 22.1870 − 362.7076 = −340.5206 eV.

This methane molecule appears to be extremely stable energetically. But it might not be so stable geometrically, because H is very large compared to H+. So forming methane as C4+ + 4H might require high pressure.

One place that automatically provides high pressure is the deep ocean. So C4+ + 4H looks like a good candidate configuration to expect within the vast deposits of methane known to exist at the bottom of the world’s oceans.

Both of the two methane isomers mentioned above, C4− + 4H+ and C4+ + 4H, are tetrahedral in shape, and are not polarized.

5.2. Isomers of Water Involving Proton Pairs

So far, water and methane have a lot in common: each has one fairly inert isomer, and one fuel-ready isomer. Let us now consider one more potential variation on the molecules involving H+’s, i.e., naked protons. Suppose that naked protons can do what electrons most like to do: form binary pairs. Let such pairs be represented the notation (2H+).

Applied to the C4− + 4H+ fuel-ready isomer of methane CH4, such a process could produce another isomer. Let this new isomer be represented by the formulaic notation C4− + 2(2H+) showing that it involves two protons pairs. Let it be represented by the pictorial layout (2H+) : C4− : (2H+), showing that it is an un-polarized linear molecule with two strongly positive ends. This isomer of methane could exist, but it’s potential utility is unclear.

But the pairing process could also produce yet another isomer, with only one proton pair. The formulaic notation would be C4− + 2H+ + (2H+), and the pictorial representation would be H + · H + · C 4 - · ( 2 H + ). (The little dots mean ‘chemical bonds’, a mysterious concept worthy of a whole book on its own.) This molecule is not symmetric, and so it is polarized. Its polarization can trigger a cascade process that can lead to heavier and heavier hydrocarbons. That is, polarized methane CH4 can lead to ethane C2H6, propane C3H8, butane C4H10, and so on.

In more detail, the ethane C2H6 molecule with a proton pair would have formulaic representation 2C3− + 4H+ + (2H+), and pictorial representation

H + · H + · C 3 - · ( 2 H + ) · C 3 - · H + · H +

The propane C3H8 molecule with proton pairs would have formulaic representation 3C3− + 6H+ + 2(2H+) and pictorial representation

H + · H + · C 3 - · ( 2 H + ) · C 3 - · ( 2 H + ) · C 3 - · H + · H +

The butane C4H10 molecule with proton pairs would have formulaic representation 4C3− + 4H+ + 3(2H+)and pictorial representation

H + · H + · C 3 - · ( 2 H + ) · C 3 - · ( 2 H + ) · C 3 - · ( 2 H + ) · C 3 - · H + · H +

What is happening at each step here is that a polarized methane unit H + · H + · C 4 - : ( 2 H + ) with its proton pair meets the growing molecule, reacts with it in a way such that one hydrogen gas molecule gets expelled, and the next longer molecule gets formed. This process is a kind of ‘polymerization’, although not the usual kind, with addition onto the end of the molecule; instead, it features insertion somewhere into the middle of the growing molecule. (The vision that heavy hydrocarbons are created from light hydrocarbons under extreme temperature / pressure conditions comes from [6])

All of the chain hydrocarbon molecules can be thought of as polymer molecules, and of course polymer molecules can be thought of as nanostructures. So, is there, as there was so often above, some analogous situation and ensuing process with water? Consider the linear isomer of water, 2H++ O− −. The proton pairing process would produce another isomer. Its formulaic representation would be O− − + (2H+) and its pictorial representation would be O− − (2H+). This is a doubly polarized, linear molecule that is more compact than 2H++ O− − is. The polarization and the linear shape would encourage such water to form linear polymeric structures. But the situation is very different from that with methane. The water polymerization process just features molecular alignment. The first polymer formed just has formulaic representation 2O− − + 2(2H+) and visual representation O− − (2H+) O− − (2H+). There is no chemical reaction to cement that alignment once it is achieved. That is, there is no analog to the expulsion of the Hydrogen molecule that occurs in the creation of the hydrocarbon polymers. So there is nothing to keep the aligned water molecules from reverting to their un-aligned condition.

Back in the late 1960’s and early 1970’s, there was a lot of controversy in the chemistry literature and the popular press over the purported existence of so-called ‘polywater’. The name refers to water that was put through a physical gauntlet involving passage through narrow quartz capillary tubes. The physical properties of the resulting ‘polywater’ were described as rather polymer-like. But the claimed phenomenon of polywater could not be reliably reproduced at the time, despite much investment and effort, and was eventually dismissed as an unreal phantom. The whole episode is today regarded as an example of ‘pathological science’.

Now we can see why nothing came of polywater. Polymerization of water is possible, yes, but it has absolutely no staying power whatsoever. One simply cannot create samples of polywater, package them, and carry them about to independent testing laboratories—as was attempted way back then.

Polywater is, however, worth remembering, and studying more rationally, since the polymerization idea involved in it has its analog in the important area of hydrocarbon fuels.

Presumably, the corresponding water process has to begin with the ordinary tetrahedral isomer of water, 2H+ O ++. Then the 2H++ O− − linear isomer of water has to be created. The process for making this linear isomer is not fully revealed in the literature. But perhaps AC can offer some reasonable guesses about it. Variables that can be controlled include temperature and pressure and electrical current. Electrical current appears to be the most important one.

Then the proton-pairing process has to be triggered. This is probably not so difficult, considering how easy, even unavoidable, it is in the case of electron pairing.

Then the polarized molecules have to be brought into close proximity. The combination of low temperature and high pressure would help put molecules into the requisite close proximity.

Then the polymerization has to be sensed immediately, in situ. Optical methods involving polarized light could be useful for this.

6. Water Containing Isotopes of Its Constituent Atoms

Both the Hydrogen and the Oxygen in water can occur in isotopes, with different neutron counts in the nucleus. The technologically important isotopes are those of Hydrogen. There are three of them: normal Hydrogen (with only the one proton), Deuterium (one proton with one neutron) and Tritium (one proton with two neutrons).

The heavy isotopes of Hydrogen are found in all water, but in greater concentration in so called ‘heavy water’. Heavy water can be produced by evaporation of ordinary seawater, because the lighter water molecules will evaporate before the heavier water molecules.

Heavy water is a raw material for all sorts of fusion experiments. Fusion experimenters typically get heavy water from special-purpose vendors. The experimenters may not fully understand how hard heavy water is to make, or exactly what the vendor has actually provided. For example, suppose the production process starts with seawater, and uses boiling to remove normal H2O, and/or centrifuging to increase the concentration of heavier species, which include DHO and D2O and THO and TDO and T2O. In what proportions do these heavier species occur? Who knows! But my guess is that DHO is the dominant heavy-water species available, not D2O (and certainly not anything involving T), and that significant ordinary H2O is still left in any heavy-water sample. But fortunately, that doesn’t matter, so long as at least some heavy nuclei are present.

What matters more is to find a way to meet the fundamental requirements for fusion to occur. These include:

  • Removal of electrons from the immediate environs of nuclei to be fused;

  • Forcing of the naked nuclei into proximity sufficient for their attraction by nuclear forces to dominate their natural Coulomb repulsion.

The traditional Hot Fusion (HF) does these jobs in a brute-force way. To meet Requirement 1, the oxygen is separated out, leaving gas molecules H2, HD, D2, etc., which are heated into its plasma state. To meet Requirement 2, the plasma is confined and compressed with a huge magnetic field.

All of that is exceedingly difficult, and difficulty creates motivation to seek alternatives using less brute force and more subtlety and guile. In recent decades, many efforts to develop alternatives to HF have been characterized by the title ‘Cold Fusion’ (CF).

Arising from empiricism rather than from theory, CF has been much maligned. But Algebraic Chemistry (AC) offers at least a quantitative modeling tool with which to approach CF objectively. The following Sub-Sections develop this story.

6.1. Data on Isotopes of Hydrogen

The development of the relevant information about all the individual Hydrogen isotopes follows. Notice that the masses of the individual isotopes are integers, as opposed to the real-number average value seen earlier in the paper.

For normal Hydrogen:

Write Formulae:

H 1 H 1 + : I P 1 , 1 × 1 / 1 ; H 1 H 1 - : - I P 1 , 1 × 1 × 2 / 1 - Δ I P 1 , 2 × 2 / 1

Insert Data (eV):

H 1 H 1 + : 14.250 × 1 / 1 eV ; H 1 H 1 - : - 14.250 × 1.4142 / 1 - 35.625 × 2 / 1 eV

Insert Data (eV):

H 1 H 1 + : 14.250 × 1 / 1 eV ; H 1 H 1 - : - 14.250 × 1 / 1 - 35.625 × 2 / 1 eV

Evaluate Formulae:

H 1 H 1 + : 14.250 eV ; H 1 H 1 - : - 20.1525 - 71.2500 + 0 = - 91.4025 eV

For Deuterium:

Write Formulae:

D 1 D 1 + : I P 1 , 1 × 1 / 2 eV ; D 1 D 1 - : - I P 1 , 1 × 1 × 2 / 2 - Δ I P 1 , 2 × 2 / 2

Insert Data (eV):

D 1 D 1 + : 14.250 × 1 / 2 eV ; D 1 D 1 - : - 14.250 × 1.4142 / 2 - 35.625 × 2 / 2 eV

Evaluate Formulae:

D 1 D 1 + : 7.125 eV ; D 1 D 1 - : - 10.07625 - 35.625 = - 45.70125 eV

For Tritium:

Write Formulae:

T 1 T 1 + : I P 1 , 1 × 1 / 3 eV ; T 1 T 1 - : - I P 1 , 1 × 1 × 2 / 3 - Δ I P 1 , 2 × 2 / 3

Insert Data (eV):

T 1 T 1 + : 14.250 × 1 / 3 eV ; T 1 T 1 - : - 14.250 × 1.4142 / 3 - 35.625 × 2 / 3 eV

Evaluate Formulae:

T 1 T 1 + : 4.750 eV ; T 1 T 1 - : - 6.71745 - 23.750 + 0 = - 30.46745 eV

6.2. Comments on Cold Fusion

Here I wish to comment on some beliefs about cold fusion that are commonly articulated, and might be wrong, and some other ideas that haven’t been articulated before, and may deserve some study.

Those who are skeptical about CF have often pointed to its meager generation of neutrons, which are common byproducts of many of the more familiar nuclear fission processes. But there is a flaw in this sort of objection. When we study the Periodic Table, we see that the proportion of neutrons in stable isotopes increases with atomic number. That means fission reactions typically start with elements that have more neutrons than the daughter elements will need for stability. So the excess neutrons are liberated in the fission process. By contrast, fusion reactions do not occur between the abundant isotopes of input elements because those isotopes do not have enough neutrons to make a stable isotope of the product element. Fusion reactions need some heavy isotope(s) as input. And even then, the neutrons provided may be too valuable for any to be liberated. Observe that the chemical/nuclear reactions

2 DHO He + H 2 + O 2 and  H 2 O + THO He + H 2 + O 2

can produce energy without producing any neutrons at all. Even though no other reactions seem able to do exactly that, do take note that:

The fact that neutrons are absent from, or at low concentration in, the environs of a purported CF experiment does not mean that there is no fusion occurring.

Those who are proponents of CF are obliged to justify the occurrence of any nuclear reaction at all in circumstances so modest as a CF cell provides: no high temperature, no high pressure, no magnetic confinement; in short, no big hardware.

A possible explanation is that the conditions of the CF cell produce a heavy version of Brown’s gas, including not only the linear isomer of H2O, but also linear isomers of DHO and THO, and possibly D2O and DTO and T2O too. The full set of linear isomers puts not only naked H’s, but also naked d ’s and naked T’s, in exposed positions, unshielded by electrons. Nuclear reactions are then possible: two D’s, or one T and one H, can fuse to make a normal 4He nucleus, or two D can make a T and an H, or a 3He and a neutron, etc. My guess is that the dominant nuclear reaction is 2D → 4He + γ, where γ is a gamma ray carrying the energy released. Other reactions can also produced some neutrons, which can then trigger other elements present to undergo fission. All these reactions amount to transmutations.

And what condition is it that the CF cell provides to make the linear isomers of water and heavy water? Basically, I believe it is an environment of chemical catalysis. The cathode in a CF cell is typically Palladium. That element comes from an area of the Periodic Table where famously catalytic metals are found. Some others are Silver, Platinum, and Gold. The CF anode is usually Platinum. Gold also sometimes appears, as a cathode. I have not seen Silver yet, but would not be surprised to see it. All these metals prefer not to be neutral, and upon encountering any other atom, will negotiate to give or take electrons. That is how they catalyze further reactions.

With Algebraic Chemistry, it is possible to calculate the energy costs and benefits of various electron rearrangements. So we can find out why a DHO molecule might get catalyzed into linear configuration in the CF cell.

The development of the relevant information about Palladium goes as follows:

Write Formulae:

P 46 d P 46 d + : I P 1 , 1 × 46 / M 46 + Δ I P 1 , 46 × 46 / M 46 - Δ I P 1 , 45 × 45 / M 46 P 46 d + P 46 d + + : I P 1 , 1 × 46 × 45 / M 46 + Δ I P 1 , 45 × 45 / M 46 - Δ I P 1 , 44 × 44 / M 46 P 46 d P 46 d - : - I P 1 , 1 × 46 × 47 / M 46 - Δ I P 1 , 47 × 47 / M 46 + Δ I P 1 , 46 × 46 / M 46 P 46 d - P 46 d - - : - I P 1 , 1 × 46 × 48 / M 46 - Δ I P 1 , 48 × 48 / M 46 + Δ I P 1 , 47 × 47 / M 46

Insert Data:

P 46 d P 46 d + : 14.250 × 46 / 106.420 + 2.701 × 46 / 106.420 - 1.980 × 45 / 106.420 eV P 46 d + P 46 d + + : 14.250 × 45.4973 / 106.420 + 1.980 × 45 / 106.420 - 1.289 × 44 / 106.420 eV P 46 d P 46 d - : - 14.250 × 46.4973 / 106.420 - 3.455 × 47 / 106.420 + 2.701 × 46 / 106.420 eV P 46 d - P 46 d - - : - 14.250 × 46.9894 / 106.420 - 4.242 × 48 / 106.420 + 3.455 × 47 / 106.420 eV

Evaluate Formulae:

P 46 d P 46 d + : 6.1596 + 1.1675 - 0.8372 = 6.4899 eV P 46 d + P 46 d + + : 6.0922 + 0.8372 - 0.5329 = 6.3964 eV P 46 d P 46 d - : - 6.2261 - 1.5259 + 1.1675 = - 6.5845 eV P 46 d - P 46 d - - : - 6.2920 - 1.9133 + 1.5259 = - 6.6794 eV

Summarize for Convenience:

P 46 d P 46 d + + : 6.4899 + 6.3964 = 12.8863 eV P 46 d P 46 d - - : - 6.5845 - 6.6794 = - 13.2639 eV

In [7], Gordon talked about ‘co-deposition’, meaning co-introduction of Palladium and Deuterium into the CF cell, both in solution form. The added Palladium is in the form of the salt PdCl2, which presumably dissociates into the ions Pd++ and 2Cl. The Deuterium is, I believe, in the form of DHO which, like normal water, does not dissociate very much, but stays as a molecule with ionic structure (D + H + O+ +). The available Pd++ ions can work on the normal DHO molecule to convert it to linear form, with ionic structure (D+ + H+ + O− −). There must be many pathways to this end result; indeed a ‘riotous profusion’ of possible pathways is typical of catalysis schemes. Here is just one reaction pathway, given for illustration of the principle involved:

( D - + H - + O + + ) + 10 Pd + + + 20 e - ( D + + H + + O - - ) + 10 Pd

From the data provided above, this reaction takes

45.70125 + 91.4025 - 17.5613 - 10 × 12.8863 + 7.125 + 14.250 - 27.3788 + 10 × 0 = 45.70125 + 91.4025 - 17.5613 - 128.863 + 7.125 + 14.250 - 27.3788 = - 15.32435 eV

Observe that the energy requirement for this reaction is negative, which means that this reaction will occur spontaneously.

Thus about the first requirement for fusion, removing electrons from subject nuclei, AC indicates that chemical catalysis can do the job. The catalysis converts normal DHO (analogous to normal water) into linear DHO (linear, like BG). The ionic structure of normal DHO keeps the D in association with two electrons, and so protected from intrusions to the nuclear level, but the ionic structure of linear DHO leaves the D exposed, unshielded by any electron.

With regard to the second requirement for fusion, confinement, CF does provide some of that in the form of Deuterium loading into the Palladium matrix of the cathode in the CF cell. But that is not enough confinement to cause neighbor-on-neighbor fusion inside the cathode [8]. Instead of fusion occurring interior to the cathode, fusion between the trapped cathode-loaded Deuterons and the exposed Deuterons in the electrolyte seems more likely. Basically, the Deuteron loading sets up the cathode like a dart board, and then the linear HDO molecules in the electrolyte, positively charged on the ends, are attracted to the cathode because it is negative, and they hit it like so many darts. When D ’s on those incident darts hit bull’s-eye D ’s on the target cathode, CF ensues.

7. Conclusions

This paper has shown that many physical behaviors of molecules and nanostructures are understandable in terms of ‘Algebraic Chemistry’. This name refers to a quantitative model for predicting the energy budget for all sorts of changes between different ionization states of atoms that are involved in chemical reactions and in changes of physical state. The paper states the formulae involved, and shows many examples of their use. The Appendix gives all the numerical data used here, plus similar data potentially useful for future studies involving additional elements.

The paper has suggested an association between macroscopic physical states of matter and microscopic ionization states of its constituent atoms. Some gaps in current knowledge are pointed out with the hope of stimulating future research.

About water in particular, the paper has argued that water does not ‘live’ in the ionization state to which it ‘dies’. If it did, it would dissociate more than it does. In detail, water lives with ionic configuration 2H + O2+, but it dies to H+ + OH, which has overall ionic configuration 2H+ + O− −.

The paper has argued that water also has several interesting isomers corresponding to different ionization states. The 2H+ + O− − ionization state is a linear isomer, apparently the key ingredient in socalled Brown’s gas, which is a fuel-like substance. The analysis developed here indicates that Brown’s gas works by a mechanism that is more akin to Spectroscopy than to Chemistry: it burns no Oxygen; it just relaxes to a less energetic ionic configuration.

An ionization state involving pairing of naked protons, analogous to the well-known Cooper pairing of electrons, is discussed. It could produce transient polymerization. So-called ‘polywater’ has a checkered past, and stands in need of rehabilitation. If it ever exists at all, it is totally ephemeral. But it may yet be detectable. It does not have an obvious practical utility, but the analogous process with hydrocarbons could be useful to know about.

The paper finally worked out some details for water with isotopes of Hydrogen in it. This information is useful for explaining what can be happening in ‘cold fusion’. This technology too has a difficult past. But it appears to have a potentially useful future.

Acknowledgments

The author thanks the reviewers and the editors for advice about this presentation. The author is grateful to the Natural Philosophy Alliance and its member individuals who have done experiments, and presented data and interpretive ideas, at its conferences.

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Appendix 1 Basic data on first-order ionization potentials

Table Periods 1, 2 and 3.

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Periods 1, 2 and 3.
ElementCharge ZMass MRaw Data IPScaled Data IPModel IPModel ΔIP
H11.00813.61013.71814.2500
He24.00324.60649.24449.87535.625

Li36.9415.39412.48012.480−1.781
Be49.0129.32621.01123.3279.077
B510.8118.30917.96617.0552.805
C614.00711.26622.55121.5707.320
N714.00714.54429.10127.28113.031
O815.99913.63127.26027.28113.031
F918.99817.43836.81034.50420.254
Ne1020.18021.58743.56243.64129.391

Na1122.9905.14510.75310.910−3.340
Mg1224.3057.65615.50616.5652.315
Al1326.9825.99612.44414.9230.673
Si1428.0868.15416.35718.8744.624
P1530.97410.49821.67723.8719.621
S1632.06610.37320.79023.8719.621
CI1735.45312.97727.06330.19215.942
Ar1839.94815.77835.01738.18623.936

Note above: l = 0 and l = 1 sub-periods are tied to the beginnings and ends of periods. Note following: l = 2 sub-periods float mid period, with their mid points tied to the overall period-rise.

Periods 4 and 5.
ElementCharge ZMass MRaw Data IPScaled Data IPModel IPModel Δ IP
K1939.0984.3468.9449.546−4.704
Ca2040.0786.12012.26513.057−1.193
Sc2144.9566.54614.01313.057−1.193
Ti2247.8676.82614.85113.638−0.612
V2350.9426.74314.93414.244−0.006
Cr2451.9966.77414.67614.8770.627
Mn2554.9387.43816.34515.5391.289
Fe2655.8457.87316.91115.5391.289
Co2758.9337.86317.16316.2291.980
Ni2858.6937.64516.02616.9512.701
Cu2963.5467.72816.93417.7053.455
Zn3065.3909.39820.48518.4924.242
Ga3169.7236.00613.50914.4940.244
Ge3272.6107.90517.93617.8603.610
As3374.9229.82422.30322.0077.757
Se3478.9609.76122.66922.0077.757
Br3579.90411.82626.99827.11612.866
Kr3683.80014.01532.62333.41219.162

Rb3785.4684.1809.6579.546−4.704
Sr3887.6205.69513.13213.057−1.193
Y3988.9066.39014.56713.057−1.193
Zr4091.2246.84615.61413.638−0.612
Nb4192.9066.88815.60814.244−0.006
Mo4295.9407.10616.23214.8770.627
Tc4398.0007.28216.59715.5391.289
Ru44101.0707.37616.94215.5391.289
Rh45102.9067.46917.08016.2301.980
Pd46106.4208.35119.31916.9512.701
Ag47107.8687.58317.40317.7053.455
Cd48112.4119.00421.08718.4924.242
In49114.8185.78813.56314.4940.244
Sn50118.7107.35517.46217.8603.610
Sb51121.7608.65120.65522.0077.757
Te52127.6009.01522.12022.0077.757
I53126.90410.45625.03727.11612.866
Xe54131.29012.13729.50833.41219.162
Period 6.
ElementCharge ZMass MRaw Data IPScaled Data IPModel IPModel Δ IP
Cs55132.9053.9009.4259.546−4.704
Ba56137.3275.21812.79613.057−1.192
La57138.9065.58113.60012.393−1.857
Ce58140.1165.47713.23212.583−1.667
Pr59140.9085.42512.95712.776−1.474
Nd60144.2405.49813.21712.972−1.278
Pm61145.0005.55013.19213.171−1.079
Sm62150.3605.63313.66013.374−0.876
Eu63151.9645.67413.68713.579−0.671
Gd64157.2506.14115.08913.579−0.671
Tb65158.9255.85114.30513.787−0.463
Dy66162.5005.93414.60913.999−0.251
Ho67164.9306.02714.83614.213−0.037
Er68167.2606.11015.02914.4310.181
Tm69168.9346.18315.13714.6530.403
Yb70170.0406.25515.46314.8780.627
Lu71174.9675.43613.39517.8603.610
Hf72178.4907.05417.48718.7554.505
Ta73180.9487.89419.56819.6965.446
W74183.8407.98819.84420.6846.434
Re75186.2077.88419.57421.7217.471
Os76190.2308.71421.81121.7217.471
Ir77192.2179.12922.78822.8118.560
Pt78195.0769.02522.57123.9559.705
Au79196.9679.23223.01925.15610.906
Hg80200.53010.44626.18426.41812.168
Tl81204.3836.11015.41716.5152.265
Pb82207.2007.42718.76819.6965.446
Bi83208.9807.29318.36123.4909.240
Po84209.0008.42320.95823.4909.240
At85210.00028.01513.765
Rn86222.00010.75727.76933.41219.164

Note: l = 3 (like l = 2) sub-periods float mid period, with their midpoints tied to the overall period-rise.

Period 7.
ElementCharge ZMass MRaw Data IPScaled Data IPModel IPModel ΔIP
Fr87223.0009.546−4.704
Ra88226.0005.28013.56013.057−1.193
Ac89227.0006.95017.72712.393−1.857
Th90232.0386.08915.69912.583−1.667
Pa91231.0365.89214.95912.776−1.474
U92238.0296.20316.05012.972−1.277
Np93237.0006.27615.99413.171−1.079
Pu94244.0006.06815.75213.374−0.876
Am95243.0005.99615.33713.579−0.671
Cm96247.0006.02715.50713.579−0.671
Bk97247.0006.23415.87513.787−0.463
Cf98251.0006.30716.15413.999−0.251
Es99252.0006.42116.34514.213−0.037
Fm100257.0006.50416.71614.4310.181
Md101258.0006.58716.82714.6530.403
No102259.0006.66016.91114.8770.627
Lf10317.8593.610
Rf10418.7554.505
Db10519.6965.446
Sg10620.6846.434
Bh10721.7217.471
Hs10821.7217.471
Mt10922.8118.561
Ds11023.9559.705
Rg11125.15610.906
Cn11226.41812.168
Uut11316.5152.265
Uuq11417.0192.769
Uup11523.4909.240
Uuh11623.4909.240
Uus11728.01513.765
Uuo11833.41219.162
Ijms 13 01066f1 1024
Figure 1. Ionization potentials, scaled appropriately and modeled algebraically.

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Figure 1. Ionization potentials, scaled appropriately and modeled algebraically.
Ijms 13 01066f1 1024
Ijms 13 01066f2 1024
Figure 2. Behavior of higher-order IP’s (IO > 1).

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Figure 2. Behavior of higher-order IP’s (IO > 1).
Ijms 13 01066f2 1024
Ijms 13 01066f3 1024
Figure 3. Correlation between state-change temperatures and ionization potentials.

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Figure 3. Correlation between state-change temperatures and ionization potentials.
Ijms 13 01066f3 1024
Ijms 13 01066f4 1024
Figure 4. Population fractions of three regimes of ionization state energy.

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Figure 4. Population fractions of three regimes of ionization state energy.
Ijms 13 01066f4 1024
Ijms 13 01066f5 1024
Figure 5. A generic phase diagram.

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Figure 5. A generic phase diagram.
Ijms 13 01066f5 1024
Ijms 13 01066f6 1024
Figure 6. A phase diagram with the plasma state included.

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Figure 6. A phase diagram with the plasma state included.
Ijms 13 01066f6 1024
Table Table 1. First-order IP’s: fractional rises on sub-periods.

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Table 1. First-order IP’s: fractional rises on sub-periods.
periodLNlfractionlfractionlfractionlfraction
12101
28201/213/4
38201/313/4
418301/425/1812/3
518301/425/1812/3
632401/437/4825/1619/16
732401/437/4825/1619/16
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