The Haisch - Moddel patent has a better accepted theoretical foundation for 
fractional hydrogen than Mills but is also flawed in not
recognizing the relativistic nature of the effect. I disagree with both Mills 
and H-M about the energy transfer when a monatomic
atom translates to a fractional state. I am convinced that Naudts suggestion of 
a relativistic translation is correct and the atom simply
transitions to a different inertial frame which only appears smaller from our 
perspective. My position is that the noble gases in the H-M patent will simply 
reverse this relativistic translation upon exiting the cavity without releasing 
any energy or producing any plasma. Mills also enlists this non radiative 
transition of monatomic atoms claiming energy is released through dipole to 
dipole action but recognizes the need to employ diatomic bonds and chemistry to 
rectify energy from matter in this translated state. A relativistic explanation 
for the energy gain is that a fractional diatom opposes any change in Casimir 
force in opposition to motion induced by gas law, once a certain threshold is 
exceeded the bond is broken restoring atoms to their monatomic state. The atoms 
translate to the new fractional value and are primed to reform diatomic bonds 
again for as long as they remain in the Casimir field.  In the patent extract 
below Haish describes the orbital decays as a rapid linear contraction as 
opposed to the normal quantum jump where this balance between absorption and 
emission must be maintained and the difference emitted as heat energy. If the 
Naudts theory is correct then this was a wrong assumption in the patent, Yes 
the "translation" is smooth but there is no difference in energy to radiate 
away, instead the contraction of the orbit already represents a balance between 
the suppressed energy level in the cavity and the orbital. The only "energy" to 
be gained in this environment is by using orbital bonds to lock the fractional 
states in opposition to further change.
Regards
Fran


The following material appears in U. S. Patent #7,379,286
Haisch, Moddel
/ May 27, 2008

QUANTUM VACUUM ENERGY EXTRACTION

Abstract: A system is disclosed for converting energy from the electromagnetic 
quantum vacuum available at any point in the universe to usable energy in the 
form of heat, electricity, mechanical energy or other forms of power. By 
suppressing electromagnetic quantum vacuum energy at appropriate frequencies a 
change may be effected in the electron energy levels which will result in the 
emission or release of energy. Mode suppression of electromagnetic quantum 
vacuum radiation is known to take place in Casimir cavities. A Casimir cavity 
refers to any region in which electromagnetic modes are suppressed or 
restricted. When atoms enter into suitable micro Casimir cavities a decrease in 
the orbital energies of electrons in atoms will thus occur. Such energy will be 
captured in the claimed devices. Upon emergence form such micro Casimir 
cavities the atoms will be re-energized by the ambient electromagnetic quantum 
vacuum. In this way energy is extracted locally and replenished globally from 
and by the electromagnetic quantum vacuum.


This process may be repeated an unlimited number of times. This process is also 
consistent with the conservation of energy in that all usable energy does come 
at the expense of the energy content of the electromagnetic quantum vacuum. 
Similar effects may be produced by acting upon molecular bonds. Devices are 
described in which gas is recycled through a multiplicity of Casimir cavities. 
The disclosed devices are scalable in size and energy output for applications 
ranging from replacements for small batteries to power plant sized generators 
of electricity.

BACKGROUND OF THE INVENTION

Max Planck proposed the concept of zero-point energy in 1912. The idea was then 
studied by Albert Einstein and Otto Stern in 1913. In 1916 Walther Nernst 
proposed that the Universe was filled with zero-point energy. The modern field 
of stochastic electrodynamics is based upon these ideas.

At that same time the structure and stability of the atom were puzzles. The 
Rutherford model of the atom was based on analogy to the motions of planets 
(electrons) around the Sun (the nucleus). However this was not feasible. The 
orbiting electron(s) would emit Larmor radiation, quickly losing energy and 
thus spiraling into the nucleus on time scales less than one-trillionth of a 
second, thereby rendering stable matter impossible. It is now known within the 
context of stochastic electrodynamics (SED) theory that a possible solution 
involves the absorption of zero-point energy. It was shown in 1975 by Boyer 
that the simplest possible atom and atomic state, the hydrogen atom in its 
ground state, would be in a state of equilibrium between Larmor radiation and 
absorption of zero-point energy at the correct radius for a classical 
Rutherford hydrogen atom.

Since this solution was not known in 1913, Niels Bohr followed a different path 
by simply postulating that only discrete energy levels were available to the 
electron in an atom. This line of reasoning let to the development of quantum 
theory in the 1920s. The concept of classical zero-point energy was forgotten 
for a decade. However the same concept found itself reborn in a quantum context 
in 1927 with the formulation of the Heisenberg uncertainty principle. According 
to the principle, the minimum energy of a harmonic oscillator has the value 
hf/2, where h is Planck's constant and f is the frequency. It is thus 
impossible to remove this last amount of random energy from an oscillating 
system.

Since the electromagnetic field also must be quantized in quantum theory, a 
parallel is drawn between the properties of a quantum oscillator and the waves 
of the electromagnetic field. It is concluded that the minimum energy of any 
possible mode of the electromagnetic field, consisting of frequency, 
propagation direction and polarization state, is hf/2. Multiplying this energy 
by all possible modes of the field gives rise to the electromagnetic quantum 
vacuum, which has identical properties--energy density and spectrum--to the 
classical zero-point energy studied by Planck, Einstein, Stern and Nernst a 
decade previously.

The line of inquiry involving classical physics plus the addition of a 
classical zero-point field was reopened in the 1960s by Trevor Marshall and 
Timothy Boyer and has been named stochastic electrodynamics (SED). SED asks the 
question: "Which quantum properties, processes or laws can be explained in 
terms of classical physics with the only addition being a zero-point 
electromagnetic field." Two of the early successes were a classical derivation 
of the blackbody spectrum (i.e. one not involving quantum physics) and the 
discovery that a classically orbiting electron in a hydrogen atom emitting 
Larmor radiation but absorbing zero-point radiation would have an equilibrium 
orbit at the classical Bohr radius. An initial approach to this problem by 
Timothy Boyer (1975) was perfected by H. E. Puthoff (1987). Their analyses 
treated the orbiting electron as a harmonic oscillator.

This result underwent a major new development with the recent work of Daniel 
Cole and Y. Zou which simulated the orbit of a classical electron in a true 
Coulomb field of a hydrogen nucleus and found that such a realistic electron 
would find itself in a range of distances from the nucleus, in agreement with 
quantum mechanics, owing to the random nature of the emission and absorption 
processes. The mean position is at the correct Bohr radius, but the actual 
distribution of positions very precisely duplicates the electron probability 
distribution of the corresponding Schrodinger equation in which the electron is 
regarded as being represented by a wave function. (In the SED representation 
the electron is "smeared out" not because it is a wave function, but because as 
a point-like particle it is subject to the continuous perturbations of the 
electromagnetic quantum vacuum fluctuations.)

A clear consequence of this theory is that a reduction of the electromagnetic 
quantum vacuum at the frequency corresponding to the orbit of the electron will 
result in a decay of the orbit since there will thereby be an imbalance in the 
Larmor radiation vs. absorption.

The electromagnetic quantum vacuum energy spectrum is proportional to the cube 
of the frequency. If the vacuum energy is suppressed at the frequency of the 
"normal" orbit of the electron, this will cause the electron to spiral inward 
to a higher frequency orbit. In this fashion it will then encounter a new 
equilibrium situation with the electromagnetic quantum vacuum energy spectrum 
owing to that spectrum's increase with the cube of the frequency.

If the SED interpretation is correct for the hydrogen atom as the analyses of 
Boyer, Puthoff, Cole and Zou indicate, it must apply as well to all other atoms 
and their multi-electron configurations. In that case, a transition of an 
electron from an excited state to a lower energy state involves a rapid decay 
from one stable orbit to another, not an instantaneous quantum jump. The 
details of the bases for stability of electron orbits has yet to be determined 
by SED theory, but the logical extrapolation from the single-electron hydrogen 
case is clear: electron orbits in all atoms must be determined by an emission 
vs. absorption balance and thus are subject to modification involving mode 
suppression of the electromagnetic zero-point field at appropriate frequencies.

It is claimed that modification of electron orbits is in essence the same 
process as natural transition between energy levels of electrons in atoms and 
therefore that the energy released in such a process can be captured in the 
same way as ordinary transition energy.

By moving an atom into and out of a microstructure that suppresses appropriate 
modes of the electromagnetic quantum vacuum, an extraction of energy from the 
electromagnetic quantum vacuum may be accomplished. This can be done with micro 
Casimir cavities.

The electromagnetic quantum vacuum as a real source of energy is indicated by 
the Lamb shift between s and p levels in hydrogen, van der Waals forces, the 
Aharanov-Bohm effect, and noise in electronic circuits.

However the most important effect of the electromagnetic quantum vacuum is the 
existence of the Casimir Force, a force between parallel conducting plates 
which may be interpreted as a radiation pressure effect of electromagnetic 
quantum vacuum energy. Electromagnetic waves in a cavity whose walls are 
conducting are constrained to certain wavelengths for reasons having to do with 
transverse component boundary conditions on the wall surfaces. As a result, in 
a Casimir cavity between parallel plates there will be, in effect, an exclusion 
of radiation modes whose wavelengths are longer than the separation of the 
plates. An overpressure of electromagnetic quantum vacuum radiation on the 
outside then pushes the plates together. An extensive literature exists on the 
Casimir force and the reality of the force has moved from laboratory 
experimentation to micro-electro-mechanical structures (MEMS) technology both 
as a problem (so-called "stiction") and as a possible control mechanism.

The exclusion of modes does not begin all at once at the wavelength equivalent 
to the plate separation, d. Mode suppression will be strongest for wavelengths 
of d or greater, but will begin to occur as well for wavelengths falling in 
between the "stairway" d/n, with the effect diminishing as n increases. We 
propose to use the partial suppression of modes for wavelengths shorter than d 
occurring in this fashion in order to be able to employ Casimir cavities of the 
maximum possible physical size.

Researchers have shown that thermodynamic laws are not violated when energy is 
"extracted" from zero-point energy, as energy is still conserved and the second 
law is not violated. Cole and Puthoff have carried out and published 
thermodynamic analyses showing that there is no violation. Indeed, a thought 
experiment by Forward (1984) showed a simple, but not practical, energy 
extraction experiment.

In the stochastic electrodynamics (SED) interpretation of the hydrogen atom, 
the ground state is interpreted as effectively equivalent to a classically 
orbiting electron whose velocity is c/137. The orbit is stable at the Bohr 
radius owing to a balance between classical electromagnetic emission and 
absorption from the electromagnetic zero-point field. This view, first obtained 
by Boyer (1975) and subsequently refined by Puthoff (1987) has been further 
strengthened by the detailed simulations of Cole and Zou (2003, 2004) which 
demonstrate that the stochastic motions of the electron in this interpretation 
reproduce the probability density distribution of the Schrodinger wave 
function. Note that one apparent difference between this interpretation and 
that of quantum mechanics is that in quantum mechanics the 1s state of the 
electron is regarded as having zero angular momentum, whereas in the SED 
interpretation the electron has an instantaneous angular momentum of 
mcr/137=h/2.pi.. However SED simulations by Nickisch have shown that the 
time-averaged angular momentum is zero just as in the quantum case owing to the 
zero-point perturbations on the orbital plane. Thus averaged over enough 
"orbits" this "classical electron" will fill a spherical symmetric volume 
around the nucleus having the same radial probability density as the 
Schrodinger wave function and zero net angular momentum, completely consistent 
with quantum behavior.

The Bohr radius of the atom in the SED view is 0.529 A (Angstroms). This 
implies that the wavelength of zero-point radiation responsible for sustaining 
the orbit is 2*.pi.*0.529*137=455 A (0.0455 microns). It is claimed that 
suppression of zero-point radiation at this wavelength and shorter in a Casimir 
cavity will result in the decay of the electron to a lower energy state 
determined by a new balance between classical emission of an accelerated charge 
and zero-point radiation at .lamda.<455 A, where .lamda. depends on the Casimir 
plate separation, d. Note that the tail end of the quantum probability density 
of the electron (as well as the SED simulation of Cole and Zou) extends beyond 
five Bohr radii, so that some change in the energy balance could be 
accomplished even at considerably longer wavelengths of perhaps 0.1 microns-0.2 
microns

Since the frequency of this orbit is 6.6.times.10.sup.15 s.sup.-1, no matter 
how quickly the atom is injected into a Casimir cavity the process will be a 
slow one as experienced by the orbiting electron. We therefore assume that the 
decay to a new sub-Bohr ground state will involve gradual release of energy in 
the form of heat, rather than a sudden optical radiation signature.

Since the binding energy of the electron is 13.6 eV, we assume that the amount 
of energy released in this process would be on the order of 1 to 10 eV for 
injection of the hydrogen atom into a Casimir cavity of d=250 A or thereabouts 
(and perhaps even a larger cavity as noted above). Upon exiting the cavity the 
electron would absorb energy from the zero-point field and be re-excited to its 
normal state. The energy (heat) extracted in the process comes at the expense 
of the zero-point field, which in the SED interpretation flows at the speed of 
light throughout the Universe. We are in effect extracting energy locally and 
replenishing it globally. Imagine extracting thimbles-full of water from the 
ocean. Yes, the ocean is being depleted thereby, but no practical consequences 
ensue.

Since naturally occurring hydrogen at standard temperature and pressure (STP) 
is a two-atom molecule, a dissociation process would need to precede an 
injection of hydrogen atoms into a Casimir cavity. We avoid this complication 
and take advantage of multi-electron modification by working with monatomic 
(noble) gases which also have the advantage of being safe and inexpensive.

We work with naturally occurring monatomic gases for three reasons: (1) No 
dissociation process is required. (2) Heavier element atoms are approximately 
two to four times larger than hydrogen and thus can utilize and be affected by 
a larger Casimir cavity which is easier to fabricate. (3) Heavier elements have 
numerous outer shell electrons, several of which may be simultaneously affected 
by the reduction of zero-point radiation in a Casimir cavity.

The following five noble gases are potentially suitable: He (Z=2, r=1.2 A) Ne 
(Z=10, r=1.3 A), Ar (Z=18, r=1.6 A) Kr (Z=36, r=1.8 A) Xe (Z=54, r=2.05 A).

All of these elements contain ns electrons. He has two 1s electrons. Ne has two 
each of 1s and 2s electrons. Ar has two each of 1s, 2s, and 3s electrons. Kr 
has two of each of 1s, 2s, 3s, and 4s electrons. Xe has two of each of 1s, 2s, 
3s, 4s and 5s electrons.

Assuming an outermost electron which is completely shielded by the other 
electrons (a crude assumption), its orbital velocity would scale as r.sup.-1/2 
(the familiar Keplerian period squared proportional to semi-major axis cubed 
relationship) and thus .lamda. proportional to r/v) will scale as r.sup.3/2. If 
that is the case, then the larger radii translate as r.sup.3/2 into larger 
Casimir cavities having an effect on the energetics of the outer electron 
shells. We would therefore expect that a Casimir cavity having d=0.1 microns 
(or perhaps even as large as one micron would have an effect on reducing the 
energy levels of the outermost pair of s electrons . . . and possibly also p 
electrons and intermediate shell s electrons as well.

It is reasonable to expect that a 0.1 microns Casimir cavity would result in a 
release of 1 to 10 eV for each injection of a He, Ne, Ar, Kr or Xe atom into 
such a cavity.

According to a Jordan Maclay, who has done theoretical Casimir cavity 
calculations, a long cylindrical cavity results in an inward force on the 
cavity. In the "exclusion of modes" interpretation of the Casimir force, this 
implies that a cylindrical cavity of diameter 0.1 micron would yield the 
desired decay of outer shell electrons and subsequent release of energy.

It is now recognized that an electromagnetic quantum vacuum field is formally 
necessary for atomic stability in conventional quantum theory (Milonni 1994). 
In the field of physics known as stochastic electrodynamics, this concept has 
been shown by theory and simulations to underlie the ground state of the 
electron in the hydrogen atom. The classical Bohr orbit is determined by a 
balance of Larmor emission and absorption of energy from the zero-point 
fluctuations of the electromagnetic quantum vacuum in SED theory. It follows 
that upon suppression of appropriate zero-point fluctuations the balance will 
be upset causing the electron to decay to a lower energy level not ordinarily 
found in nature with a release of energy during this transition. A Casimir 
cavity of the proper dimensions can accomplish this suppression of zero-point 
fluctuations. A Casimir cavity refers to any region in which electromagnetic 
modes are suppressed or restricted. Upon entering such a properly designed 
Casimir cavity the electron energy level will shift and energy will be 
released. Upon exiting the Casimir cavity the electron will return to its 
customary state by absorbing energy from the ambient zero-point fluctuations. 
This permits an energy extraction cycle to be achieved at the expense of the 
zero-point fluctuations. Although it has not yet been proven theoretically, a 
similar balance of Larmor emission and absorption of energy from the zero-point 
fluctuations must underlie the electron states of all atoms, not just hydrogen, 
permitting any atom to be used as a catalyst for extraction of zero-point 
energy (the energy associated with the zero-point fluctuations). An analogous 
process is also believed to underlie molecular bonds, yielding a similar energy 
extraction cycle.

SUMMARY OF THE INVENTION

A system is disclosed for converting part of the energy of the electromagnetic 
quantum vacuum available at any point in the universe to usable energy in the 
form of heat, electricity, mechanical energy or other forms of power. This is 
accomplished using an effect on the electron configurations of atoms predicted 
by the theory of stochastic electrodynamics (SED). Within the context of SED 
theory it is predicted that the electron energy levels in atoms are determined 
by a balance of Larmor radiation vs. absorption of radiative energy from the 
electromagnetic quantum vacuum. By suppressing electromagnetic quantum vacuum 
energy at appropriate frequencies a change may be effected in the electron 
energy levels which will result in the emission or release of energy. This 
change in energies is analogous to a standard emission of a photon as an 
electron makes a transition from an excited to a lower energy state, but on a 
longer time scale and with the change being a continuous one rather than a 
"jump" from one energy level to another. Mode suppression of electromagnetic 
quantum vacuum radiation is known to take place in Casimir cavities. A Casimir 
cavity refers to any region in which electromagnetic modes are suppressed or 
restricted. When atoms enter into suitable micro Casimir cavities a decrease in 
the orbital energies of electrons in atoms will thus occur, with the effect 
being most pronounced for outer shell electrons. Such energy will be captured 
in the claimed devices. Upon emergence form such micro Casimir cavities the 
atoms will be re-energized by the ambient electromagnetic quantum vacuum. In 
this way energy is extracted locally and replenished globally from and by the 
electromagnetic quantum vacuum. This process may be repeated an unlimited 
number of times. This process is also consistent with the conservation of 
energy in that all usable energy does come at the expense of the energy content 
of the electromagnetic quantum vacuum. Two example variations of a system are 
disclosed that permit multiple extractions of electromagnetic quantum vacuum 
energy during passage of a gas through a series of micro Casimir cavities and 
that operate in a self-sustaining, recycling fashion. Similar effects may be 
produced by acting upon molecular bonds. The disclosed devices are scalable in 
size and energy output for applications ranging from replacements for small 
batteries to power plant sized generators of electricity. Since the 
electromagnetic quantum vacuum is thought to permeate the entire Universe, 
devices drawing power from the electromagnetic quantum vacuum in the fashion 
claimed will be effectively inexhaustible sources of power.

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