US20030213696A1 - Pulsed electrolytic cell - Google Patents
Pulsed electrolytic cell Download PDFInfo
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- US20030213696A1 US20030213696A1 US10/461,285 US46128503A US2003213696A1 US 20030213696 A1 US20030213696 A1 US 20030213696A1 US 46128503 A US46128503 A US 46128503A US 2003213696 A1 US2003213696 A1 US 2003213696A1
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- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21B—FUSION REACTORS
- G21B3/00—Low temperature nuclear fusion reactors, e.g. alleged cold fusion reactors
- G21B3/002—Fusion by absorption in a matrix
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E30/00—Energy generation of nuclear origin
- Y02E30/10—Nuclear fusion reactors
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E60/00—Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
- Y02E60/30—Hydrogen technology
- Y02E60/36—Hydrogen production from non-carbon containing sources, e.g. by water electrolysis
Definitions
- This invention relates generally to the use of electrolytic cells for the creation of nuclear fusion and more particularly to a low energy nuclear reaction power generator that includes an electrolytic cell across whose anode and cathode electrodes electrical pulses are applied in a predetermined pattern conducive to fusion.
- Deuterons are positively charged particles and, therefore, repel each other.
- the force of the repulsion reaches its maximum value, it then creates what is known as the Coulomb barrier. It is only when this barrier is penetrated and the deuterons are brought to one ten-trillionth of a centimeter next to each other, that a strong nuclear force takes over and the particles then fuse. This is the same nuclear force that prevents nuclei which include positively-charged protons from flying apart.
- tritium nuclei for tritium is a heavy isotope of hydrogen, but its nucleus has a proton and two neutrons, whereas a deuterium nucleus has a proton and a single neutron.
- Thermonuclear fusion will occur when deuterons are combined at a high enough density and a high enough temperature for a time period sufficient to effect fusion.
- the center of the sun affords conditions conducive to thermonuclear fusion, for this fiery center is subjected to enormous gravitational forces and is at a temperature of about 10 million degrees Fahrenheit.
- the gravitational forces are much weaker and it therefore takes a much higher temperature, in the order of 100 million degrees Fahrenheit, to produce a deuterium-tritium (D-T) fusion reaction.
- the D-T thermonuclear reaction is the one currently being pursued, for it yields more energy than D-D fusion.
- Hot fusion overcomes the Coulomb barrier by ripping off atoms from the two heavy forms of hydrogen at extremely high temperatures to create a cloud of ions or plasma. Huge magnets produce the magnetic fields to hold the plasma together for a time sufficient for some of the nuclei to crash into each other and fuse. This thermonuclear fusion reaction produces tritium and helium nuclei as well as a shower of neutrons and gamma radiation.
- electrochemical techniques have been investigated as a possible technique for fusing nuclei for power generation.
- the investigations typically utilize an electrolytic cell whose electrolyte is heavy water that is water in which deuterium takes the place of ordinary hydrogen.
- the heavy water is rendered electrically conductive by a salt dissolved therein; i.e., lithium deuterhydroxide.
- Immersed in this electrolyte is an anode-cathode electrode pair composed of a strip of metal (such as palladium) surrounded by a coil of similar or another metal (such as platinum wire).
- the main object of this invention is to provide a low energy nuclear reaction power generator that includes a cell having a pair of electrodes immersed in an electrically-conductive heavy or light water electrolyte, to which electrodes electrical pulses are applied which are in a predetermined pattern.
- an object of this invention is to provide a low energy nuclear reaction power generator that yields far more energy in the form of heat than is applied to the cell in the form of electricity.
- a low energy nuclear reaction power generator provided with an electrolytic cell containing an electrically-conductive electrolyte in which is immersed a metallic electrode pair whose anode and cathode are formed of platinum, palladium, titanium, nickel or any other suitable metal.
- the electrolyte may be any suitable fluid such as light water, heavy water, and liquid metals, etc. or may also be a suitable solid material—e.g., a semiconductor. Applied across these electrodes is a train of voltage pulse packets, each comprised of a cluster of pulses.
- each packet of voltage pulses gives rise to a surge of current in the electrolyte which flows between the electrodes and causes the electrolyte (e.g., heavy or light water) to decompose, oxygen being released, for example, at the platinum electrode while hydrogen (or isotopic hydrogen, e.g., deuterium) ions migrate toward, for example, the palladium electrode.
- the successive surges of ions produced by the train of pulse packets bombard the metallic electrode to bring about dense ion packing.
- the dense ion packing preferably causes fusion which results in the generation of energy in the form of heat.
- the energy generated in the heat is greater than the energy of the voltage pulses applied to the electrodes.
- the dense ion packing may substantially increase the resistivity—i.e., the measure of a material's ability to oppose the flow of an electric current—of the metallic electrode by introducing hydrogen, or other, ions to the structure of the metal.
- This resistivity preferably can be measured in real-time by passing a current through the metallic electrode and measuring the change in current over time.
- the measured current over time is an indication of the change in resistivity, and, hence, the level of ion packing of the metallic electrode over time.
- a real time indicator of the ion packing may then be realized by continually passing a current through the metallic electrode and measuring the current.
- FIG. 1 schematically illustrates superlooping wave phenomena
- FIG. 2 schematically illustrates a low energy nuclear reaction electrolytic cell in accordance with the invention
- FIG. 3 illustrates the pattern of electrical pulses applied to the electrodes of the cell
- FIG. 4 illustrates the pattern of electrical pulses applied to the electrodes of the cell with pulse packets switched off during relaxation periods.
- the present invention represents a significant advance beyond the discovery at the Los Alamos National Laboratory that a greater production of excess heat is obtained in an electrochemical cell by pulsing the current flowing through the cell.
- applied to the electrodes of the cell are voltage pulses to produce a pulsed current flow in the cell.
- these pulses are not of constant amplitude and duration but are in a pattern in which the amplitude and duration of the pulses and the intervals therebetween are modulated to give rise to a dense packing, for example, of deuterium ions in the palladium electrode that promotes a fusion reaction.
- Every wave necessarily incorporates smaller waves, and is contained by larger waves.
- each high-amplitude low-frequency major wave is modulated by many higher frequency low-amplitude minor waves.
- Superlooping is an ongoing process of waves waving within one another.
- FIG. 1 (adapted from the illustrations in the Dardik article) schematically illustrates superlooping wave phenomena.
- FIG. 1 depicts low-frequency major wave 110 modulated, for example, by minor waves 120 and 130 .
- Minor waves 120 and 130 have progressively higher frequencies (compared to major wave 110 ).
- Other minor waves of even higher frequency may modulate major wave 110 , but are not shown for clarity.
- This new principle of waves waving demonstrates that wave frequency and wave intensity (amplitude squared) are simultaneous and continuous.
- the two different kinds of energy i.e., energy carried by the waves that is proportional to their frequency, and energy proportional to their intensity are also simultaneous and continuous.
- Energy therefore is waves waving, or “wave/energy.”
- the pattern of pulses applied to the electrodes of the cell is derived from super-looping wave activity.
- Electrolyte 11 may be any suitable liquid electrolyte, such as heavy water, light water, molten metals, etc.
- electrolyte 11 may, for example, be heavy water which is rendered electrically conductive by a suitable salt dissolved therein.
- an anode-cathode electrode pair formed by a cathode 12 and an anode 13 .
- Cathode 12 and anode 13 may be made of any suitable metal such as palladium, platinum, titanium, nickel, etc.
- cathode 12 may, for example, be a strip of palladium and anode 13 may, for example, be a coil of platinum.
- Anode coil 13 surrounds the strip of palladium metal so that the electrodes are bridged by the conductive electrolyte 11 and a voltage impressed across the electrodes causes a current to flow therebetween.
- a d-c voltage source 14 is provided whose output is applied across the electrodes 12 and 13 of the cell through an electronic modulator 14 whose operation is controlled by a programmed computer 16 , whereby the modulator yields voltage pulses whose amplitude and duration as well as the duration of the intervals between pulses are determined by the program.
- the maximum amplitude of the pulses corresponds to the full output of the d-c source 14 .
- the maximum amplitude of the pulses will be 45 VDC, and the amplitudes of pulses having a lesser amplitude will be more or less below 45 VDC, depending on the program.
- Computer 16 is programmed to activate electronic modulator 15 so as to yield a train of pulse packets, each packet being formed by a cluster of pulses that assume the pattern shown in FIG. 3.
- the first packet in the train, Packet I is composed of five pulses P 1 to P 5 which progressively vary in amplitude, pulse P 1 being of the lowest amplitude and pulse P 5 being of the highest amplitude.
- the respective durations of pulses P 1 to P 5 vary progressively, so that pulse P 1 is of the shortest duration and pulse P 5 is of the longest duration.
- the intervals A between successive pulses in the cluster forming the packet vary progressively in duration.
- the first interval between pulses P 4 and P 5 is shortest in duration, and the last interval between pulses P 4 and P 5 is longest in duration.
- the packets are shown as being composed of five pulses, in practice they may have a fewer or a greater number of pulses.
- the duration of a packet may in practice be about thirty seconds, and the intervals between successive packets may be in a range of two to five seconds.
- the second packet in the train, Packet II is also composed of five pulses P 6 to P 10 , but their amplitudes and durations, and the intervals between pulses are the reverse of those in the pulse cluster of Packet I.
- pulse P 6 is of the greatest amplitude and that of P 10 of the lowest amplitude.
- the third packet in the train, Packet III is formed of a cluster of five pulses P 11 to P 15 whose amplitudes and durations, and the intervals between pulses correspond to those in Packet I.
- the intervals between successive packets in the train have a duration B that changes from packet to packet.
- the varying amplitudes of the pulses in the successive packets conform to the amplitude envelope of a major wave W 1 .
- the varying durations of the pulses in the packets conform to the amplitude envelope of a minor wave W 2 whose frequency differs from that of major wave W 1 .
- the varying durations of the intervals between the pulses in a packet conforms to the amplitude envelope of still another minor wave W 3 of different frequency.
- the varying durations of the intervals between successive packets in the train are in accordance with the amplitude envelope of yet another minor wave W 4 of different frequency.
- a second modulator 20 may be implemented in order to measure the resistivity of cathode 12 .
- second modulator 20 may generate an AC current and pass the AC current through cathode 12 .
- This AC current is preferably at a different frequency than the pulses produced by electronic modulator 15 . In this way, no substantial interference exists between the pulses produced by modulator 15 and the current produced by second modulator 20 .
- the current provided by modulator 20 may be used to measure the resistivity of cathode 12 .
- This measurement may be obtained by passing an AC current, which may be substantially constant—i.e., the amplitude of the peaks and valleys of the current and the frequency of the current are substantially constant—, through cathode 12 while measuring the voltage potential across the cathode.
- the known resistivity change may then be used to indicate the level of ion packing of the cathode. As described above, ion packing may be a necessary precursor for the success of low energy nuclear reactions in a cell according to the invention.
- minor waves W 2 , W 3 and W 4 superimposed on wave W 1 are shown. Further for clarity, the amplitudes and frequencies of superlooping minor waves W 2 , W 3 , and W 4 , relative to each other and relative to major wave W 1 , are not drawn to scale. In fact the maximum amplitude of the minor waves may be proportional to the instantaneous amplitude of the major wave. Thus, minor waves W 2 and W 3 (which are located at about the peak amplitude of major wave W 1 ) are likely to have much larger maximum amplitudes than the maximum amplitude of minor wave W 4 (which is located at about the bottom of a valley in wave W 1 ).
- the maximum amplitude of minor waves W 2 and W 3 at the peak of the major wave may even be comparable to the peak amplitude of major wave W 1 , i.e., the minor waves may have the same intensity as the major waves as shown in FIG. 1.
- Other illustrative examples of superlooping minor waves within major waves and their frequency and amplitude distribution are provided by the FIGS. shown in the Dardik article “The Great Law of the Universe” incorporated herein by reference.
- the pattern of the voltage pulses which constitute the train is governed by superlooping waves W 1 to W 4 and the current which flows between the electrodes immersed in the electrolyte is pulsed accordingly.
- the deuterium ions travel in clusters, each created by a packet of pulses, to produce a high intensity surge of deuterium ions that bombards the palladium electrode.
- the surges of deuterium ions which repeatedly bombard the palladium electrode give rise to a dense packing of these ions on the palladium and fuse thereon to produce heat.
- Pulse packets in the pulse train may be completely turned off during the relaxation periods corresponding to the downward phases.
- FIG. 4 illustrates a pulse pattern with pulses (e.g., packet P 2 , FIG. 3) completely switched off during the relaxation period.
- the program is developed from a formation of superlooping waves which are digitized so as to derive a pulse at the peak of each wave cycle.
- the aforementioned Dardik article illustrates various forms of superlooping waves.
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Abstract
A low energy nuclear reaction power generator provided with an electrolytic cell containing an electrically-conductive heavy or light water electrolyte in which is immersed an electrode pair whose anode is formed of platinum and whose cathode is formed of palladium. Applied across these electrodes is a train of voltage pulse packets, each comprised of a cluster of pulses. The amplitude and duration of each pulse in the packet, the duration of the intervals between pulses, and the duration of the intervals between successive packets in the train are in a predetermined pattern in accordance with superlooping waves in which each wave is modulated by waves of different frequency. Each packet of voltage pulses gives rise to a surge of current in the electrolyte which flows between the electrodes and causes the heavy or light water to decompose, oxygen being released at the platinum electrode while deuterium ions migrate toward the palladium electrode. The successive surges of ions produced by the train of pulse packets bombard the palladium electrode, to bring about dense ion packing which results in fusion and heat.
Description
- This application is a continuation of copending, commonly-assigned U.S. patent application Ser. No. 10/161,158, filed May 30, 2002, which claims the benefit of copending, commonly-assigned U.S. Provisional Patent Application No. 60/294,537, filed May 30, 2001. All of these prior applications are hereby incorporated by reference herein in their entireties.
- 1. Field of Invention
- This invention relates generally to the use of electrolytic cells for the creation of nuclear fusion and more particularly to a low energy nuclear reaction power generator that includes an electrolytic cell across whose anode and cathode electrodes electrical pulses are applied in a predetermined pattern conducive to fusion.
- 2. States of Prior Art
- The quest for nuclear fusion to provide an inexhaustible, non-polluting source of energy seeks to exploit the phenomena of nuclear physics. It is known that when two nuclei, for example, of deuterium (heavy hydrogen), fuse together, the combined mass of the fusion product is less, by a minute quantity, than the tiny mass of the original particles. The conversion of this tiny mass to a fusion product releases an incredible amount of energy. Energy, as expressed in the classic Einstein equation, is equal to mass multiplied by the square of the speed of light; hence the minute mass yields an enormous amount of energy.
- It was Edward Teller, the atomic physicist, who in 1942 when an atom bomb had yet to be built, advanced the proposition that is the bedrock of nuclear fusion. Teller theorized that if deuterium nuclei were plunged into the fiery furnace having a temperature of many million degrees Fahrenheit created by an atomic fission reaction, the colliding nuclei would fuse in this environment and thereby liberate an incredible amount of energy. With the hydrogen bomb, Teller's theory became a reality.
- Deuterons are positively charged particles and, therefore, repel each other. The closer deuterons approach each other, the stronger their repulsion and the greater the energy it takes to overcome this repulsion. When the force of the repulsion reaches its maximum value, it then creates what is known as the Coulomb barrier. It is only when this barrier is penetrated and the deuterons are brought to one ten-trillionth of a centimeter next to each other, that a strong nuclear force takes over and the particles then fuse. This is the same nuclear force that prevents nuclei which include positively-charged protons from flying apart. Fusion also occurs with tritium nuclei, for tritium is a heavy isotope of hydrogen, but its nucleus has a proton and two neutrons, whereas a deuterium nucleus has a proton and a single neutron.
- Thermonuclear fusion will occur when deuterons are combined at a high enough density and a high enough temperature for a time period sufficient to effect fusion. The center of the sun affords conditions conducive to thermonuclear fusion, for this fiery center is subjected to enormous gravitational forces and is at a temperature of about 10 million degrees Fahrenheit. On earth, the gravitational forces are much weaker and it therefore takes a much higher temperature, in the order of 100 million degrees Fahrenheit, to produce a deuterium-tritium (D-T) fusion reaction. The D-T thermonuclear reaction is the one currently being pursued, for it yields more energy than D-D fusion.
- Following Teller's invention of the hydrogen bomb, billions of dollars have been spent over the last 40 years toward contriving devices adapted to force heavy hydrogen nuclei to fuse together under controlled conditions and thereby liberate more energy than was expended to confine and heat the nuclei. One such device of enormous size is known as a Tokomak within whose toroidal interior powerful magnetic fields confine and squeeze hot plasma, causing deuterium and tritium ions to fuse together.
- Hot fusion overcomes the Coulomb barrier by ripping off atoms from the two heavy forms of hydrogen at extremely high temperatures to create a cloud of ions or plasma. Huge magnets produce the magnetic fields to hold the plasma together for a time sufficient for some of the nuclei to crash into each other and fuse. This thermonuclear fusion reaction produces tritium and helium nuclei as well as a shower of neutrons and gamma radiation.
- In a super-giant laser fusion generator, laser beams bombard a deuterium-tritium fuel pellet, causing its outer layer to vaporize and dissipate outwardly from the pellet. The resultant reaction force implodes the fuel to effect fusion. Yet despite the multi-billion dollar investments made in developing thermonuclear fusion reactors to produce energy, no such generator is at present a practical reality, and whether it ever will be, cannot be forecast. Other technologically simpler and less expensive techniques for fusing nuclei are desirable.
- In the past decade or so, electrochemical techniques have been investigated as a possible technique for fusing nuclei for power generation. The investigations typically utilize an electrolytic cell whose electrolyte is heavy water that is water in which deuterium takes the place of ordinary hydrogen. The heavy water is rendered electrically conductive by a salt dissolved therein; i.e., lithium deuterhydroxide. Immersed in this electrolyte is an anode-cathode electrode pair composed of a strip of metal (such as palladium) surrounded by a coil of similar or another metal (such as platinum wire).
- When a d-c voltage is impressed across these electrodes, the resultant current flow in the heavy water causes it to decompose into its constituent elements. As a consequence, oxygen is released as a gas at the platinum electrode, while deuterium ions migrate toward the palladium electrode. The buildup of a large concentration of these ions in the palladium metal is thought to initiate a low energy nuclear reaction. The energy released by such an low energy reaction could be captured by the atomic lattice of the electrode and show up as heat.
- In 1989, Martin Fleischmann and Stanley Pons, on observing excess heat generation in an electrochemical cell, claimed they had observed evidence of room temperature fusion of deuterium ions. It is now generally understood that their observations were not that of deuterium-deuterium fusion but of some other phenomena. Further electrochemistry studies by E. Storms, G. H. Miley and others, suggest that the phenomena involved is an anomalous nuclear process in the solid electrode. The excess heat generation may be attributed to the fusion of hydrogen or isotopic hydrogen nuclei with the nuclei of the solid electrode material rather than of the fusion of hydrogenic nuclei themselves. The amount of excess heat generated appears to depend on the nature of the voltage applied to the electrodes and on whether the resultant current flowing through the electrolyte is steady or pulsed.
- In any case, present day electrochemical cells do not generate enough excess heat to be commercially viable power sources. Further improvements in electrochemical cell design and methods of operation are desirable.
- The main object of this invention is to provide a low energy nuclear reaction power generator that includes a cell having a pair of electrodes immersed in an electrically-conductive heavy or light water electrolyte, to which electrodes electrical pulses are applied which are in a predetermined pattern.
- The significant feature of the present invention which distinguishes it from a prior cell in which the current through the electrolyte is pulsed, is that in a cell in accordance with the invention, pulsing takes place in a pulse pattern that is highly conducive to fusion.
- More specifically, an object of this invention is to provide a low energy nuclear reaction power generator that yields far more energy in the form of heat than is applied to the cell in the form of electricity.
- Briefly stated, these objects are attained in a low energy nuclear reaction power generator provided with an electrolytic cell containing an electrically-conductive electrolyte in which is immersed a metallic electrode pair whose anode and cathode are formed of platinum, palladium, titanium, nickel or any other suitable metal. The electrolyte may be any suitable fluid such as light water, heavy water, and liquid metals, etc. or may also be a suitable solid material—e.g., a semiconductor. Applied across these electrodes is a train of voltage pulse packets, each comprised of a cluster of pulses.
- The amplitude and duration of each pulse in the packet, the duration of the intervals between pulses, and the duration of the intervals between successive packets in the train are in a predetermined pattern in accordance with superlooping waves in which each wave is modulated by waves of different frequency. Each packet of voltage pulses gives rise to a surge of current in the electrolyte which flows between the electrodes and causes the electrolyte (e.g., heavy or light water) to decompose, oxygen being released, for example, at the platinum electrode while hydrogen (or isotopic hydrogen, e.g., deuterium) ions migrate toward, for example, the palladium electrode. The successive surges of ions produced by the train of pulse packets bombard the metallic electrode to bring about dense ion packing. The dense ion packing preferably causes fusion which results in the generation of energy in the form of heat. The energy generated in the heat is greater than the energy of the voltage pulses applied to the electrodes.
- It should be noted that the dense ion packing may substantially increase the resistivity—i.e., the measure of a material's ability to oppose the flow of an electric current—of the metallic electrode by introducing hydrogen, or other, ions to the structure of the metal. This resistivity preferably can be measured in real-time by passing a current through the metallic electrode and measuring the change in current over time. The measured current over time is an indication of the change in resistivity, and, hence, the level of ion packing of the metallic electrode over time. Thus, a real time indicator of the ion packing may then be realized by continually passing a current through the metallic electrode and measuring the current.
- For a better understanding of the invention as well as other objects and features thereof, reference is made to the following detailed description to be read in conjunction with the annexed drawings wherein:
- FIG. 1 schematically illustrates superlooping wave phenomena;
- FIG. 2 schematically illustrates a low energy nuclear reaction electrolytic cell in accordance with the invention;
- FIG. 3 illustrates the pattern of electrical pulses applied to the electrodes of the cell; and
- FIG. 4 illustrates the pattern of electrical pulses applied to the electrodes of the cell with pulse packets switched off during relaxation periods.
- Superlooping:
- The present invention represents a significant advance beyond the discovery at the Los Alamos National Laboratory that a greater production of excess heat is obtained in an electrochemical cell by pulsing the current flowing through the cell. In the present invention, applied to the electrodes of the cell are voltage pulses to produce a pulsed current flow in the cell. However, these pulses are not of constant amplitude and duration but are in a pattern in which the amplitude and duration of the pulses and the intervals therebetween are modulated to give rise to a dense packing, for example, of deuterium ions in the palladium electrode that promotes a fusion reaction.
- This pulse pattern is in accordance with superlooping activity as set forth in the theory advanced in the Irving I. Dardik article “The Great Law of the Universe” that appeared in the March/April 1994 issue of the “Cycles” Journal. This article is incorporated herein by reference.
- As pointed out in the Dardik article, it is generally accepted in science that all things in nature are composed of atoms that move around in perpetual motion, the atoms attracting each other when they are a little distance apart and repelling upon being squeezed into one another. In contradistinction, the Dardik hypothesis is that all things in the universe are composed of waves that wave, this activity being referred to as “superlooping.” Superlooping gives rise to and is matter in motion; i.e., both change simultaneously to define matter-space-time.
- Thus in nature, changes in the frequency and amplitude of a wave are not independent and different from one another, but are concurrently one and the same, representing two different hierarchical levels simultaneously. Any increase in wave frequency at the same time creates a new wave pattern, for all waves incorporate therein smaller waves and varying frequencies, and one cannot exist without the other.
- Every wave necessarily incorporates smaller waves, and is contained by larger waves. Thus each high-amplitude low-frequency major wave is modulated by many higher frequency low-amplitude minor waves. Superlooping is an ongoing process of waves waving within one another.
- FIG. 1 (adapted from the illustrations in the Dardik article) schematically illustrates superlooping wave phenomena. FIG. 1 depicts low-frequency
major wave 110 modulated, for example, byminor waves major wave 110, but are not shown for clarity. - This new principle of waves waving demonstrates that wave frequency and wave intensity (amplitude squared) are simultaneous and continuous. The two different kinds of energy, i.e., energy carried by the waves that is proportional to their frequency, and energy proportional to their intensity are also simultaneous and continuous. Energy therefore is waves waving, or “wave/energy.” In a low energy nuclear reaction power generator in accordance with the invention, the pattern of pulses applied to the electrodes of the cell is derived from super-looping wave activity.
- The Low Energy Nuclear Reaction Power Generator:
- Referring now to FIG. 2, there is shown one preferable embodiment of a low energy nuclear reaction power generator in accordance with the invention provided with an electrolyte cell having a
vessel 10.Vessel 10 containselectrolyte 11.Electrolyte 11 may be any suitable liquid electrolyte, such as heavy water, light water, molten metals, etc. For purposes of illustration,electrolyte 11 may, for example, be heavy water which is rendered electrically conductive by a suitable salt dissolved therein. - Immersed in the electrolyte is an anode-cathode electrode pair formed by a
cathode 12 and ananode 13.Cathode 12 andanode 13 may be made of any suitable metal such as palladium, platinum, titanium, nickel, etc. For purposes of illustration,cathode 12 may, for example, be a strip of palladium andanode 13 may, for example, be a coil of platinum.Anode coil 13 surrounds the strip of palladium metal so that the electrodes are bridged by theconductive electrolyte 11 and a voltage impressed across the electrodes causes a current to flow therebetween. - Connected across the electrodes of the electrochemical cell is a low-voltage battery, resulting in a steady current flowing through the heavy or light water electrolyte, causing it to decompose, so that oxygen gas is liberated at the platinum anode electrode while hydrogenic ions migrate toward the palladium cathode electrode and accumulate thereon.
- In a generator in accordance with the invention, a
d-c voltage source 14 is provided whose output is applied across theelectrodes electronic modulator 14 whose operation is controlled by a programmedcomputer 16, whereby the modulator yields voltage pulses whose amplitude and duration as well as the duration of the intervals between pulses are determined by the program. The maximum amplitude of the pulses corresponds to the full output of thed-c source 14. Thus if the source provides a 45 VDC output, the maximum amplitude of the pulses will be 45 VDC, and the amplitudes of pulses having a lesser amplitude will be more or less below 45 VDC, depending on the program. -
Computer 16 is programmed to activateelectronic modulator 15 so as to yield a train of pulse packets, each packet being formed by a cluster of pulses that assume the pattern shown in FIG. 3. Thus the first packet in the train, Packet I, is composed of five pulses P1 to P5 which progressively vary in amplitude, pulse P1 being of the lowest amplitude and pulse P5 being of the highest amplitude. The respective durations of pulses P1 to P5, vary progressively, so that pulse P1 is of the shortest duration and pulse P5 is of the longest duration. And the intervals A between successive pulses in the cluster forming the packet vary progressively in duration. Thus the first interval between pulses P4 and P5 is shortest in duration, and the last interval between pulses P4 and P5 is longest in duration. While the packets are shown as being composed of five pulses, in practice they may have a fewer or a greater number of pulses. The duration of a packet may in practice be about thirty seconds, and the intervals between successive packets may be in a range of two to five seconds. - The second packet in the train, Packet II, is also composed of five pulses P6 to P10, but their amplitudes and durations, and the intervals between pulses are the reverse of those in the pulse cluster of Packet I. Hence pulse P6 is of the greatest amplitude and that of P10 of the lowest amplitude.
- The third packet in the train, Packet III, is formed of a cluster of five pulses P11 to P15 whose amplitudes and durations, and the intervals between pulses correspond to those in Packet I. The intervals between successive packets in the train have a duration B that changes from packet to packet.
- The varying amplitudes of the pulses in the successive packets conform to the amplitude envelope of a major wave W1. The varying durations of the pulses in the packets conform to the amplitude envelope of a minor wave W2 whose frequency differs from that of major wave W1. The varying durations of the intervals between the pulses in a packet conforms to the amplitude envelope of still another minor wave W3 of different frequency. And the varying durations of the intervals between successive packets in the train are in accordance with the amplitude envelope of yet another minor wave W4 of different frequency.
- A
second modulator 20 may be implemented in order to measure the resistivity ofcathode 12. Preferably,second modulator 20 may generate an AC current and pass the AC current throughcathode 12. This AC current is preferably at a different frequency than the pulses produced byelectronic modulator 15. In this way, no substantial interference exists between the pulses produced bymodulator 15 and the current produced bysecond modulator 20. - In the proposed configuration shown in FIG. 3, the current provided by
modulator 20 may be used to measure the resistivity ofcathode 12. This measurement may be obtained by passing an AC current, which may be substantially constant—i.e., the amplitude of the peaks and valleys of the current and the frequency of the current are substantially constant—, throughcathode 12 while measuring the voltage potential across the cathode. The change in voltage potential reflects the change in resistivity based on the relationship V(voltage)=I(current)*R(resistance). The known resistivity change may then be used to indicate the level of ion packing of the cathode. As described above, ion packing may be a necessary precursor for the success of low energy nuclear reactions in a cell according to the invention. - It will be understood that in FIG. 3 for purposes of clarity only small portions of minor waves W2, W3 and W4 superimposed on wave W1 are shown. Further for clarity, the amplitudes and frequencies of superlooping minor waves W2, W3, and W4, relative to each other and relative to major wave W1, are not drawn to scale. In fact the maximum amplitude of the minor waves may be proportional to the instantaneous amplitude of the major wave. Thus, minor waves W2 and W3 (which are located at about the peak amplitude of major wave W1) are likely to have much larger maximum amplitudes than the maximum amplitude of minor wave W4 (which is located at about the bottom of a valley in wave W1). The maximum amplitude of minor waves W2 and W3 at the peak of the major wave may even be comparable to the peak amplitude of major wave W1, i.e., the minor waves may have the same intensity as the major waves as shown in FIG. 1. Other illustrative examples of superlooping minor waves within major waves and their frequency and amplitude distribution are provided by the FIGS. shown in the Dardik article “The Great Law of the Universe” incorporated herein by reference.
- With continued reference to FIG. 3, the pattern of the voltage pulses which constitute the train is governed by superlooping waves W1 to W4 and the current which flows between the electrodes immersed in the electrolyte is pulsed accordingly.
- Thus instead of a steady stream of deuterium ions migrating toward the palladium electrode, the deuterium ions travel in clusters, each created by a packet of pulses, to produce a high intensity surge of deuterium ions that bombards the palladium electrode. The surges of deuterium ions which repeatedly bombard the palladium electrode give rise to a dense packing of these ions on the palladium and fuse thereon to produce heat.
- Highly effective computer pulse pattern programs afford optimum results, resulting in the greatest amount of fusion heat at the palladium electrode. These can be determined empirically by modifying the program to find the most effective pattern.
- One example of the most effective pulse pattern is to incorporate a relaxation period corresponding to the downward phases of the major wave W1. Pulse packets in the pulse train may be completely turned off during the relaxation periods corresponding to the downward phases. FIG. 4 illustrates a pulse pattern with pulses (e.g., packet P2, FIG. 3) completely switched off during the relaxation period.
- The program is developed from a formation of superlooping waves which are digitized so as to derive a pulse at the peak of each wave cycle. The aforementioned Dardik article illustrates various forms of superlooping waves.
- While there has been shown a preferred embodiment of a low energy nuclear reaction power generator, it is to be understood that many changes may be made therein without departing from the spirit of the invention. Thus one may use a silicon instead of platinum wire. And the electrode pair may be formed by concentric tubes, rather than by a strip surrounded by a coil as illustrated in FIG. 2.
Claims (6)
1. A method for intensifying an interaction between a metal and at least one of deuterium and hydrogen, the metal and the at least one of deuterium and hydrogen being combined in a metal-gas system, the method comprising:
applying a train of energy packets to the metal-gas system, a cluster of intensified energy pulses being superimposed on each packet, to cause a correspondingly pulsed wave to impact the metal, each packet of pulses producing a surge of the at least one of deuterium and hydrogen to pack the metal, successive surges producing a dense packing of the at least one of deuterium and hydrogen on the metal; and
wherein each pulse in the cluster of pulses has an amplitude that is proportional to an instantaneous amplitude of a major wave associated with the train of energy packets, and wherein each pulse in the cluster of pulses has a frequency that is proportional to an instantaneous frequency of the major wave associated with the train of energy packets.
2. The method of claim 1 , wherein the amplitude and duration of each pulse in the packet, the duration of the intervals between these pulses and the duration of the intervals between successive packets in the train are in a predetermined pattern in accordance with superlooping waves in which each wave is modulated by waves of different frequencies.
3. The method of claim 2 , wherein said train of energy packets is produced by an energy source whose output is applied to the metal-gas system through an electronic modulator controlled by a computer which is programmed to produce energy pulses in said pattern.
4. A method for intensifying an interaction between a metal and at least one of deuterium and hydrogen, the metal and the at least one of deuterium and hydrogen being combined in a metal-gas system, the method comprising:
applying a train of energy packets to the metal-gas system, a cluster of intensified energy pulses being superimposed on each packet, to cause a correspondingly pulsed wave to impact the metal, each packet of pulses producing a surge of the at least one of deuterium and hydrogen to pack the metal, successive surges producing a dense packing of the at least one of deuterium and hydrogen on the metal; and
wherein each pulse in the cluster of pulses has an amplitude that is proportional to an instantaneous amplitude of a major wave associated with the train of energy packets, and wherein each pulse in the cluster of pulses has a frequency that is proportional to the instantaneous amplitude of the major wave associated with the train of energy packets.
5. The method of claim 4 , wherein the amplitude and duration of each pulse in the packet, the duration of the intervals between these pulses and the duration of the intervals between successive packets in the train are in a predetermined pattern in accordance with superlooping waves in which each wave is modulated by waves of different frequencies.
6. The method of claim 5 , wherein said train of energy packets is produced by an energy source whose output is applied to the metal-gas system through an electronic modulator controlled by a computer which is programmed to produce energy pulses in said pattern.
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US10/461,285 US20030213696A1 (en) | 2001-05-30 | 2003-06-13 | Pulsed electrolytic cell |
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US29453701P | 2001-05-30 | 2001-05-30 | |
US10/161,158 US20020179433A1 (en) | 2001-05-30 | 2002-05-30 | Pulsed electrolytic cell |
US10/461,285 US20030213696A1 (en) | 2001-05-30 | 2003-06-13 | Pulsed electrolytic cell |
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US10/161,158 Continuation US20020179433A1 (en) | 2001-05-30 | 2002-05-30 | Pulsed electrolytic cell |
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US12/398,052 Abandoned US20090166218A1 (en) | 2001-05-30 | 2009-03-04 | Pulsed electrolytic cell |
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EP (1) | EP1404897A4 (en) |
JP (2) | JP2004527661A (en) |
CN (1) | CN1273645C (en) |
CA (1) | CA2448661A1 (en) |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20070199820A1 (en) * | 2006-02-28 | 2007-08-30 | Hitachi, Ltd. | Oxygen sensor |
US8419919B1 (en) | 2007-03-14 | 2013-04-16 | Jwk International Corporation | System and method for generating particles |
Families Citing this family (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20080190780A1 (en) * | 2007-01-24 | 2008-08-14 | Treadstone Technologies, Inc. | Electrochemical processor for hydrogen processing and electrical power generation |
WO2012065825A2 (en) * | 2010-10-29 | 2012-05-24 | Em-Silicon Nano-Technologies, S.L. | Nanostructured semiconductor materials, method for the manufacture thereof and current pulse generator for carrying out said method |
WO2012166808A2 (en) * | 2011-06-01 | 2012-12-06 | Target Technology International, Ltd. | Nickel alloys for hydrogen storage and the generation of energy therefrom |
CZ307004B6 (en) * | 2016-03-08 | 2017-11-08 | Power Heat Energy S.R.O. | A method of producing thermal energy, a device for this purpose and systems of thermal generation |
CN107532310B (en) | 2016-03-25 | 2019-02-05 | 卡特国际有限责任公司 | Electromagnetic resonance equipment for molecular, atomic and chemical modification of water |
US20180277259A1 (en) * | 2017-03-27 | 2018-09-27 | Jerry I. Jacobson | Method and apparatus for controlled thermonuclear fusion power |
WO2018226903A1 (en) * | 2017-06-07 | 2018-12-13 | Industrial Heat, Llc | Dual laser electrolytic cell |
US11268202B2 (en) | 2019-02-13 | 2022-03-08 | Industrial Heat, Llc | Methods for enhanced electrolytic loading of hydrogen |
JP2021091930A (en) * | 2019-12-10 | 2021-06-17 | 中国電力株式会社 | Voltage application device, and electrolysis device comprising voltage application device |
DE102021200029A1 (en) * | 2020-01-10 | 2021-07-15 | Sms Group Gmbh | Process for the production of hydrogen and oxygen by means of an electrolyzer |
Citations (13)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4017008A (en) * | 1970-12-29 | 1977-04-12 | Eli Raitport | Spray container |
US4054502A (en) * | 1975-02-03 | 1977-10-18 | Societe De Recherches Techniques Et Industrielles | Quick start electrolysis apparatus |
US4316786A (en) * | 1980-09-19 | 1982-02-23 | The United States Of America As Represented By The United States Department Of Energy | Apparatus for electroplating particles of small dimension |
US4478689A (en) * | 1981-07-31 | 1984-10-23 | The Boeing Company | Automated alternating polarity direct current pulse electrolytic processing of metals |
US4963239A (en) * | 1988-01-29 | 1990-10-16 | Hitachi, Ltd. | Sputtering process and an apparatus for carrying out the same |
US4986887A (en) * | 1989-03-31 | 1991-01-22 | Sankar Das Gupta | Process and apparatus for generating high density hydrogen in a matrix |
US5037518A (en) * | 1989-09-08 | 1991-08-06 | Packard Instrument Company | Apparatus and method for generating hydrogen and oxygen by electrolytic dissociation of water |
US5411654A (en) * | 1993-07-02 | 1995-05-02 | Massachusetts Institute Of Technology | Method of maximizing anharmonic oscillations in deuterated alloys |
US5549812A (en) * | 1994-03-26 | 1996-08-27 | Wt Wassertechnologie Gmbh | Process and apparatus for processing industrial waste water by electrolysis |
US5567303A (en) * | 1989-08-04 | 1996-10-22 | Canon Kabushiki Kaisha | Hydrogen storing member and process for storing hydrogen into the hydrogen storing member |
US6221220B1 (en) * | 1997-12-30 | 2001-04-24 | Hans Buringer | Portable device for deionizing liquids |
US20010040935A1 (en) * | 1991-06-11 | 2001-11-15 | Case Leslie Catron | Commercial power production by catalytic fusion of deuterium gas |
US20030112916A1 (en) * | 2000-02-25 | 2003-06-19 | Keeney Franklin W. | Cold nuclear fusion under non-equilibrium conditions |
Family Cites Families (13)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE1489023A1 (en) * | 1964-08-12 | 1969-04-24 | Inst Plasmaphysik Gmbh | Method and arrangement for generating short neutron pulses with a high surface current density |
US4107008A (en) * | 1975-06-16 | 1978-08-15 | Beeston Company Limited | Electrolysis method for producing hydrogen and oxygen |
DK0463089T3 (en) * | 1989-03-13 | 1996-09-16 | Univ Utah Res Found | Method and apparatus for generating energy |
JPH02271290A (en) | 1989-04-13 | 1990-11-06 | Semiconductor Energy Lab Co Ltd | Electrochemical nuclear fusion |
AU2336192A (en) * | 1991-06-11 | 1993-01-12 | Electric Power Research Institute, Inc. | Apparatus for producing heat from deuterated palladium |
JPH054094U (en) * | 1991-07-05 | 1993-01-22 | 憲太郎 渕岡 | Nuclear fusion device |
JPH0527062A (en) * | 1991-07-23 | 1993-02-05 | Tanaka Kikinzoku Kogyo Kk | Generation of abnormal heat |
JPH06207993A (en) * | 1992-11-20 | 1994-07-26 | Tekunoba:Kk | Excess heat generating material, electrode for dissolving heavy water and its producing method, heavy water dissolving device, excess heat measuring device and excess heat utilizing device |
JPH0784076A (en) * | 1993-09-15 | 1995-03-31 | Hiroshi Kubota | Normal temperature fusion device |
JPH07146387A (en) * | 1993-11-25 | 1995-06-06 | Technova:Kk | Excess heat generating method by ac current heavy water electrolytic decomposition |
JPH08166478A (en) * | 1994-12-15 | 1996-06-25 | Mitsubishi Heavy Ind Ltd | High charging method for hydrogen in hydrogen storage alloy |
JPH1018070A (en) * | 1996-07-08 | 1998-01-20 | Technova:Kk | Method for stabilizing high hydrogen occlusion in palladium electrode |
US5840172A (en) * | 1997-03-25 | 1998-11-24 | Whatman Inc. | Direct current hydrogen generator, system and method |
-
2002
- 2002-05-30 WO PCT/US2002/017334 patent/WO2002097166A1/en active Application Filing
- 2002-05-30 CN CNB028142276A patent/CN1273645C/en not_active Expired - Fee Related
- 2002-05-30 CA CA002448661A patent/CA2448661A1/en not_active Abandoned
- 2002-05-30 EP EP02732005A patent/EP1404897A4/en not_active Withdrawn
- 2002-05-30 US US10/161,158 patent/US20020179433A1/en not_active Abandoned
- 2002-05-30 JP JP2003500323A patent/JP2004527661A/en active Pending
-
2003
- 2003-06-13 US US10/461,285 patent/US20030213696A1/en not_active Abandoned
-
2009
- 2009-03-04 US US12/398,052 patent/US20090166218A1/en not_active Abandoned
-
2010
- 2010-04-02 JP JP2010086572A patent/JP2010174379A/en active Pending
Patent Citations (13)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4017008A (en) * | 1970-12-29 | 1977-04-12 | Eli Raitport | Spray container |
US4054502A (en) * | 1975-02-03 | 1977-10-18 | Societe De Recherches Techniques Et Industrielles | Quick start electrolysis apparatus |
US4316786A (en) * | 1980-09-19 | 1982-02-23 | The United States Of America As Represented By The United States Department Of Energy | Apparatus for electroplating particles of small dimension |
US4478689A (en) * | 1981-07-31 | 1984-10-23 | The Boeing Company | Automated alternating polarity direct current pulse electrolytic processing of metals |
US4963239A (en) * | 1988-01-29 | 1990-10-16 | Hitachi, Ltd. | Sputtering process and an apparatus for carrying out the same |
US4986887A (en) * | 1989-03-31 | 1991-01-22 | Sankar Das Gupta | Process and apparatus for generating high density hydrogen in a matrix |
US5567303A (en) * | 1989-08-04 | 1996-10-22 | Canon Kabushiki Kaisha | Hydrogen storing member and process for storing hydrogen into the hydrogen storing member |
US5037518A (en) * | 1989-09-08 | 1991-08-06 | Packard Instrument Company | Apparatus and method for generating hydrogen and oxygen by electrolytic dissociation of water |
US20010040935A1 (en) * | 1991-06-11 | 2001-11-15 | Case Leslie Catron | Commercial power production by catalytic fusion of deuterium gas |
US5411654A (en) * | 1993-07-02 | 1995-05-02 | Massachusetts Institute Of Technology | Method of maximizing anharmonic oscillations in deuterated alloys |
US5549812A (en) * | 1994-03-26 | 1996-08-27 | Wt Wassertechnologie Gmbh | Process and apparatus for processing industrial waste water by electrolysis |
US6221220B1 (en) * | 1997-12-30 | 2001-04-24 | Hans Buringer | Portable device for deionizing liquids |
US20030112916A1 (en) * | 2000-02-25 | 2003-06-19 | Keeney Franklin W. | Cold nuclear fusion under non-equilibrium conditions |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20070199820A1 (en) * | 2006-02-28 | 2007-08-30 | Hitachi, Ltd. | Oxygen sensor |
US7704358B2 (en) * | 2006-02-28 | 2010-04-27 | Hitachi, Ltd. | Oxygen sensor |
US8419919B1 (en) | 2007-03-14 | 2013-04-16 | Jwk International Corporation | System and method for generating particles |
Also Published As
Publication number | Publication date |
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EP1404897A4 (en) | 2008-06-04 |
US20020179433A1 (en) | 2002-12-05 |
JP2010174379A (en) | 2010-08-12 |
WO2002097166A1 (en) | 2002-12-05 |
CN1529770A (en) | 2004-09-15 |
CA2448661A1 (en) | 2002-12-05 |
JP2004527661A (en) | 2004-09-09 |
US20090166218A1 (en) | 2009-07-02 |
CN1273645C (en) | 2006-09-06 |
EP1404897A1 (en) | 2004-04-07 |
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