MXPA96003062A - Generation of energy and generator, by means of non-harmonic fusion estimul - Google Patents

Abstract

A method for generating energy and a generator of energy by non-harmonic stimulated fusion medium of isotopes of hydrogen adsorbed on metal, comprising a step of charging on a metal core (1), an amount of hydrogen isotopes H and D a heating step, in which the core (1) is heated (9) to a temperature higher than the Debye temperature of the material that makes up the core, a starting step, in which a vibratory effort is produced a rise time of less than 0.1 second, which activates a nuclear fusion of the hydrogen isotopes, a stationary step during which the heat produced by the nuclear fusion reaction H + D that occurs in the core (1) because a coherent multimodal system of stationary oscillations remains constant

Description

GENERATION OF ENERGY AND GENERATOR. THROUGH NON HARMONIC FUSION STIMULATED FIELD OF THE INVENTION The present invention relates to the field of energy production by means of nuclear fusion and, more precisely, it relates to a method for generating energy by means of the non-harmonic, stimulated fusion of hydrogen glycopes adsorbed on a crystalline network . Additionally, the invention refers to a "generated"? of energy that carries out said procedure.

DESCRIPTION OF THE PREVIOUS TECHNIQUE The problem of obtaining energy has led to ls? industry and the research Jaboratorics increasingly, a source During the studies on nuclear fusion, an applicant, for that purpose, has devised a "device for the start-up and control of the process of energy production, obtained by means of the Excitation of vibrations of the crystalline lattice of a p-athecia 1 containing deutecium ", descited in the Italian patent application No. SI / 92 / A / 000002. The procedure on which the operation of the device is based comprises a step for the precession of an electrode composed of a metallic material formed either by a single metal or by an alloy of metal components, capable of receiving deutecia, and having a precise crystal structure, for example, isam? trica. Said electrode preparation step first comprises an operation to degas the electrode in order to clean its crystal structure. Subsequently, a certain amount of jjjßutecio (D) is left inside the crystalline network of the electrode at a previously established temperature and pressure. Then, when the proportion of the number gives deuterium atoms with respect to the metal atoms (D / Me) exceeds the minimum limit of 0.7, a D + D fusion reaction is activated between the deuterium atoms adsorbed in the crystal lattice. , after the application of an alteration that puts the consecutive network plans to vibrate in push-racció. They are provided to remove the thermal energy generated by the fusion. However, the device and method illustrated above present considerable difficulties when actually implemented. In the first place, the use of deuterium is expensive, in the case of the industrial application of the device. Additionally, the start or start step of the reaction is barely controllable or repeatable. In fact, in many cases, the amount of energy obtained has been different from the expected one, based on the energy values at a D + D reaction and, in any case, it has not been c > - under identical initial conditions of preparation and startup.

BRIEF DESCRIPTION OF THE INVENTION Rather, it is an object of the present invention to provide a method for the generation of energy, which is capable of lagging a fusion of isotopes of hydrogen adsoebids to metal, and which can be reproduced cheaply, at an industrial level, as well It can be activated and stopped easily. It is a further object of the present invention to provide an energy generator that activates the above-mentioned process. These and other objects are achieved by means of the present invention, wherein the process of gere is characterized by the fact that it comprises: a step of charging a metallic nucleus, a quantity of isotopes H and D of hydrogen, which are adsorbed on the crystal lattice of the nucleus; - a heating step, in which said core loaded with the isotopes of hydrogen is heated up to a temperature higher than the minimum temperature corresponding to the constant temperature of Debye for the material that the said core rings; a step of starting or starting, in which a vibratory e -.FWVcuuev is produced that activates a nuclear fusion reaction of said hydrogen isotopes; - a stationary step, during which it is possible to exchange the heat produced by the nuclear fusion reaction H + D, which occurs in the nucleus, due to a sustained continuation of a coherent multimodal system of stationary oscillations. A step is also provided to stop the reaction in case it is necessary to interrupt it, as a means of producing an additional vibratory effort, which disrupts said coherent multimodal system of statistical oscillations. The minimum temperature that, necessarily, must be exceeded in the heating step, is the constant of Debye and that, for many of the usable metals, is indicated in the square I. So that there is a greater probability of success in the In this reaction, said minimum temperature must be exceeded by at least one DT comprised between several gcadas and several tens of degrees, according to the type of material in which the active core is formed. The Debye constant, in any case, can be calculated analytically, given that it is equal to h / * n, _. , where h is Planc's constant, K, Boltsmann's constant and n ^;, a typical frequency of each material (for more details, see Charles Kittel, Introduct ion to Solid State Fhysics, John Uilley S Sons, New Y ^). The type of hydrogen to be adsorbed in the core is preferably natural hydrogen or, in other words, having a ratio between the D and H isotopes of about 1 / 6,000. However, it is possible to obtain the reaction also with deuterium-depleted or deuterated enriched natural hydrogen, where, in every house, there is a ratio of isotopes D to H greater than 1 / SO, 000 and, of pre-presence, comprised between 1 and / 10,000 and 1 / 1,000. The novel feature of the generator is that it is provided with a reactor comprising: an active core, on which natural hydrogen is adsorbed, possibly enriched with deuterium; - a generation chamber containing the active core; - a temperature to heat a thermal carrier fluid; - a dome for the collection of the thermal carrier fluid; - a plurality of tubes, in which the fluid flows from the prechamber to the collection dome, crossing said generation chamber.

BRIEF DESCRIPTION OF THE DRAWINGS Other characteristics and advantages of the method and the generator according to the present invention will become evident in the following description of some of its possible modalities, given as examples or non-limiting, with reference to the attached drawings, in which: Figure 1 shows a longitudinal sectional view of a first embodiment of the generator according to the invention. Figure 2 is a longitudinal sectional view of a second embodiment of the generator according to the present invention. The following table I indicates the Debye constant for various metals and alloys: TABLE I Al? + 2ß ° Mg 405 ° Ta 250 ° K Be il60 ° Mo 440 ° Sn 1 5 ° K Cd 209 ° K Ni 440 «K Ti 42A ° K Ei 11 &K ° 320 ° K! 405 ° Cr 610 ° Pd 374 ° K? N 300 ° K 344.5 ° K Pu 340 ° K Li 335 ° K Ge 370 ° K Rh 47 &K ° D 325 ° K Au 162.4 ° K Yes 640 ° K Zr 292 ° K In J.11 ° K Ag 226.2 ° K Hf 252 ° K Fe 464 ° K Na 15 & ° Sb 199 ° K Con ntan 3 £ 4- ° K Monel 374 ° Clunil 465 ° K DESCRIPTION OF THE PREFERRED MODALITIES With reference to the Figure 1, a generator to drive the cruedo process with the invention comprises a generation chamber 2, crossed by a bait of copper tubes, which extend between two flanges 10, welded to a sapactadgca cover 11, which defines externally the chamber 2. The tubes 5 cross the flanges 10 and communicate with a chamber 3, comprising an annular sleeve 3a, delimited by * Vfaf cylindrical shell 13 with entries 3b. Additionally, the tubes 5 communicate with a collection dome 4, which communicates by means of nozzles with flanges 14, can means for heat exchange and with a circulation pump, which are not shown. The chamber 2 communicates, through axial ducts 6, that cross the dome 10, on the one hand, with the prechamber 3 and on the other side with a gas tank and an air pump, not damaged, by means of connections of a known type, located externally with respect to the hull 13. The ducts 6 are suitable for feeding hydrogen or other gases in the chamber 2. On the tubes 3 an active metallic core 1 of a thickness of several millimeters is electroshocked. An electric coil 9 is wound around the sopsrtadar hull 11, for example, immersed in a ceramic matrix. The fluid coming from the inlets 3b and crossing the bait of tubes 5, is pre-heated in the jacket 3a and removes the ca-xar generated in the core 1 during a non-harmonic fusion reaction of the hydrogen isotopes, whose Start or start will be described later. With reference to Figure 2, another embodiment of the generator according to the invention comprises an active core 1 having the shape of a cylindrical rod inserted in chamber 2, contained in a heating cylinder 20, in which an electric winding is submerged 9. fl - A shirt 15, formed by a sapactadar shell 11 and a cylindrical helmet 13, allows the passage of a thermal carrier fluid, which enters through an inlet 22 and leaves from an outlet 23, after having traveled axially the hull 11. The gas present in the chamber 2 is controlled by the average chamber 24 which communicates with a gas tank and with an air pump, not shown, by means of connections of a known type. The core 1 is in contact with an electrode 25, capable of transmitting an impulse of a model-type, to activate the harmonic fusion reaction of the hydrogen isotopes, such as will now be detected. In both generators of Figures 1 and 2, the windings 9 have a multiple function since, in addition to generating a magnetic field, necessary for the adsorption of hydrogen by the core, they also have the function of heating the chamber of the thermal carrier fluid, as well as the function of starting or starting the reaction, for example, by means of an electric jiulso with an effect -r-aynett.estrictDr. The core 1, in the first house shown (figure 1), is a metallic layer, for example, a multiple layer of nickel and chromium, alternating, while in the second house (figure 2), it is a cylindrical metallic bar, for example, nickel-chromium steel. The core 1, preferably, has a homogeneous surface, and as far as possible, without faults or defects. In the crystalline network of the nucleus 1, by means of known techniques, the adsorption of hydrogena is forced which has a ratio of isotopes D to isotopes H of about 1 / 6,000. The percentage of deuterium D with respect to hydrogen H may also be greater than that indicated, even though, with a D / H ratio greater than 1 / 1,000, there may be no economic advantage in exploiting the reaction, due to current costs of deutecia, as well as the difficulty in interrupting the reaction with a normal detention operation, as will be described later. 1) FL STEP TO LOAD Among the known techniques for charging hydrogen into the active core, so that the isotopes of hydrogen are chemically adsorbed in the crystal lattice, are the following: electrolytic adsorption - immersion of the core in a gaseous environment containing typhrofenium, at a temperature and a previously established pressure; - Core immersion in solutions of HCl, H O ^, H-j.S0t <; - immersion of the core in galvanic baths containing, for example, NH3, when the core constituent is deposited on a support composed of a material such as Cu or ceramic. Some materials require the application of a magnetic field that has a greater intensity than the field of, usually of more than 0.1 Tesla. In the houses of the generators described above, the magnetic field is produced by the winding 9. The absolute pressure of the hydrogen inside the generation chamber must be maintained at values preferably between 1 and 1,000 millibars and, in each case, less than 4 bars, more to which the adsorption is no longer carried out, unless it is at high pressures (more than 50 bars). The chemical adsorption of the isotopes of hydrogen in the metal of the nucleus causes the dissociation of the molecules of Ha »and D-j. and the creation, within the crystal structure of the nucleus, of covalent bonds (hydrides) between the H and D atoms and the metal. The electrostatic repulsion between the hydrogen atoms is discriminated by the excess of negative charge created by the free electrons of the metal. Therefore, the decrease in electrostatic repulsion due to the unions, allows the united atoms to approach each other more intimately than is normally possible with free atoms under identical conditions. When the overcrowding of the H and D isotopes adsorbed on the metal in the above-mentioned ratio, it is sufficiently high, for example, with a numerical proportion of hydrogen isotopes to metal tats of more than 0.3, a reticular shaking vibration. , but created, can make the systems Me + H and D + Me approach between JH, so that the atoms of H and D are at a distance less than that in which the nuclear force comes into play. 2) THE WARMING STEP In accordance with the invention, only when the temperature of the active core 1 rises to a value higher than the Debye constant of the material making up the core, (the valares of many metals of which, are enlisted in the When it is possible to carry out the start or start of the fusion reaction satisfactorily, it is possible to carry out the fusion reaction. In fact, only above this temperature the number of non-harmonic oscillations of the crystal lattice, in which hydrogen is adsorbed, becomes greater than the number of harmonic oscillations, with the consequent increase in the probability that vibrational wave vectors are added together. However, it is necessary that, in order for the reaction to be successfully activated, the Debye constant should be exceeded by several degrees a? Jf2-ti s tens of degrees, in accordance with the metal used for the core, so that allow the "population" of the non-harmonic ila ions to surpass the harmonic oscillations sufficiently. The heating pass can be carried out by any known system, for example, by thermoelectric heating, oxidation of fuels or other chemical exoenergy reactions; recombination of ions to polyatomic molecules, laser impulses and immersion in 3) STARTING OR STARTING PASS At the tips of the nucleus in which the hydrogen has been adsorbed, a, in other words, in the vicinity of the outer surface of the core, an oscillation of the ejection of the network can successfully cause two isotopes to occur. Hydrogen, respectively hydrogen H and deuterium D, approach each other more intimately than the critical distance to which, as previously described, nuclear forces come into play. In accordance with the invention it is possible, under the conditions described above and only under these conditions, to activate the localized nuclear reaction described above, which produces an effort in the active nucleus capable of producing the coherent addition of a large number of wave vectors, In this way, a gigantic localized vibratory impulse, a z-layer to excite the crystalline lattice in which the hydrogen isotopes are adsorbed, has been measured. The localized volume variations due to the expansion of the active surface of the nucleus, and san 20 times greater than those measured in the non-active portion of the nucleus. Each H + D fusion produces aHe, releasing 5.5 MeV, which is enough energy to completely vaporize the area surrounding the tip where the reaction has occurred. In that house, the complete H + D reaction would be H + D =: aHe + g of 5.5 MeV. However, in this case, photons g and other particles are not released from the nucleus, since the duration of the covalent hydrogen-metal bonds is of the order of 10-: LS at 10-i * seconds, while the time of nuclear interaction is of the order of 10-; L < a a. 10 -5 * - seconds. As a result, the energy released from the fusion can be dissipated through the network without the emission of particles or photons g. (See Max Born, Ata ic Lysi s.ed. Blacky and Son, Glasgow, A. F. Davydov, Theory of the atomic nucleus, ed. 7anichelli, Bologna, G. K. Weithaim, Massbauer Effect). In more detail, after having exceeded the Debye constant, the probability that the H + D reaction is activated is greater when the harmonic terms of the interatomic displacement become important, and this can only happen when the temperature is sufficiently high. that the Debye constant, at a characteristic temperature gta each material. Under these conditions, after the production of a sufficiently strong stimulus, by means of an external action, the J vibratory energy that crosses the crystalline network, instead of oscillating in a disorganized way, interacts coherently with the following conditions of the wave vectors, tangentially with respect to the surface of the active nucleus, and with consequent creation rie peaks of amplified energy, in particular points (sites). The wave trains that move on the active core of the nucleus, in addition to localized fusions, form a coherent multimodal system of seasonal oscillations within portions of the active material of the nucleus, thus causing a negative change in entropy and the consequent discharge of jig, which may be exploited by the generator according to the invention. Subsequently, the standing wave continues to remain half of the pump effect produced by the H + D actions. In fact, because the configuration of the network is altered by the localized vaporizations produced by the individual H + D mergers, displaced in said sites, the wave vectors are added again in other places, close to the previous ones, but in where the network is still intact, and activate other H + D reactions. With the repetition of the mergers, the core becomes a surface with a plurality of substantially equidistant entities, separated by network tracts still intact, and becomes smaller, co or localized. Another significant ribuon for the maintenance of the standing wave is provided by the interaction of the electrons with the network, especially in the presence of a variable electromagnetic field. In fact, each transition from one state of Fer i to another gives rise to the emission of a particle of a wave vector at a given frequency. (See Charles Kittel, Introduction to Solid State Physics-, Da n Willey & NY). The starting or starting step can be carried out by means of several known types of pulses, as long as the lifting time is less than 10 ~ A seconds. In those cases in which the active core is composed of pure metals or their compounds with other elements or substances, steels, stainless steels, alloys or metal systems of a multi-layer layer room, the starting step can be taken or start according to one of the following methods: - Method of thermal stress, obtained by means of pressure gradients: a polyatomic gas is inserted, such as H-2, Dj », HD, HT, Ca / H +, Ha, N ^, Gj. , etc., in the generation chamber, with a negative enthalpy difference of physical adsorption (DH) and a corresponding pressure gradient, comprised between i millibary and 4 bar. As is already known, the introduced gas generates thermal stress on the surface of the active core, due to a transient dissociation of the gas molecules and to the sudden, additional reaction that forms again. the molecules, and catalyzed by the surface of the nucleus itself. Said thermal stress causes the formation of reaction wave trains and the rapid start of the energy production process, by means of nuclear fusion between H and D, as described above. The modality of figure i is designed exactly for this type of start-up, in which ßBeroduce polyatomic gas through ducts 6, shown in figure 1. During the reaction, by means of the current flow through the d < avaf ada 9, placed all along the core 1, a constant magnetic field between 0 and 1.5 Tesla is maintained. - Metada with mechanical impulse: A mechanical impulse of torsion, traction or compression is applied to the ends of the active nucleus, with an intensity and a time of elevation, pac Kemplo, of 10"-1- second, sufficient to cause a structural deformation, which then activates the fusion process - Method with electrical restriction An electric impulse is applied to the ends of the active core with pica values and time of For example, 1.00 amperes for 30 nanoseconds, to cause a structural deformation that then activates the fusion process.The modality of Figure 2 is also designed for P starting type, in which the impulse is produced. vcit e alternano by an elecfcrada 25, connected to the active core 1 and fed by means of the cables 6. - Optaelectcónica method: A laser beam pulse of gcan power is introduced into the nucleus, po example of i MUÍ, and causes a shock wave and a thermal stress that, in turn, cause a sudden structural deformation that then activates the fusion process - Radio Frequency method: Impulse is applied of the active nucleus, which has a frequency corresponding to the resonant frequency of the hydrogen isotope spins or to the plasma frequency of the free electrons of the crystal lattice. - Ultrasonic vibration meter The active nucleus is contained in a resonant cavity. An energy pulse of ultrasonic vibrations is applied to the active core, which has an intensity and duration (pac example, 10 ~ 'L seconds) It is necessary to cause the fusion reaction. In houses in which the material that focuses the active nucleus is of a type, such as a crystal, which is subject to the piezoelectric effect, the start-up step can be activated by means of a reverse-effect method, which sends At the ends of the metallic core pulses of alternating voltage with a frequency equal to the metal resonance of the nucleus can peak values (eg, more than 5 kV) sufficient to cause a structural deformation, the iñ If you activate then the fusion process. The mode of mode 2 is also designed for this type of starting, in which the alternate voltage pulse is produced by the electrode 25 connected to the active core 1 and is fed by means of the cables &; . Finally, if the material that forms the active nucleus is of a ferromagnetic type, the start-up step can be activated by means of a magnetostrictive step that consists of the production, along the metallic core, of a magnetic field with peak values. above the intensity of the magnetic saturation and with a rise time of less than 10 ~ A seconds. This type of starting can be carried out both with the generator of FIG. 1 and with that of FIG. 2, by applying an electromagnetic pulse through the winding 9. 4) HEAT EXCHANGE STEP After start-up, the reaction is maintained in stationary conditions, exchanging heat by means of a fluid thermal carrier, which is circulated in the bait of tubes crossing the generation chamber of FIG. 1, or through the jacket. of Figure 2. The heat removal does not exceed a level that causes the temperature of the active core to fall below the Debye constant, in which case a slow stop of the reaction would occur. With regard to the thermal energy that can be formed active core rail an active can be in the form of a bar, a sheet, separate and / or tangled wires, free or compressed dust, can a without binder. For example, in the generation chamber 2 of figure 1, the active nucleus can be composed, instead of a metal deposited on the tubes 5, of a plurality of bars placed at various points of the chamber itself. Alternatively, the chamber 2 can be filled with metallic powder. W Clearly, the temperature of nucleus 1 that harbors the reaction must remain well below the transition temperature, above which the lattice loses its crystalline properties and passes into an amorphous state, comparable to the vitreous state; and this happens at temperatures that are lower than the melting temperature of each metal. In such conditions, in fact, the nucleus would have a response to the oscillations completely different from the field that ßfeurre when the state is crystalline, because the preferential direction in which the wave vectors are added, would disappear, without Absolutely no chance of having the reaction described in the above. It is also necessary that the temperature of sustained operation, at which the core is located, does not approach particular critical temperatures, which are well known for each metal and identifiable from experimentally obtained adsorption diagrams, to which the hydrogen-progressive ejection of the network occurs, ) THE DETENTION STEP The reaction can be interrupted by stopping the coherent multimodal system of stationary oscillations simply by producing another vibratory effort that disorganizes the system by means of a localized, positive, entropy production. For example, this can be achieved by creating a forced vacuum in the generation chamber (absolute pressure less than 0.1 million pounds) and introducing a gas cylinder with a positive DH dissociation, for example, -? . Due to the impact with the active surface, the molecules are dissociated and a rapid elimination of the energy of the network occurs, with consequent negative temperature. The sudden decrease in temperature causes the disorganization of the active sites and the arrest of the nuclear reaction between the hydrogen isotopes. Alternatively, even if the pressure of the gas within the generation chamber is left unchanged, it is sufficient to exchange thermal cooling of the core to the point where the core itself carries below the Debye constant. Heat exchange, for example, can be achieved by circulating a fluid at a temperature below the Debye constant in the shed of tubes crossing the generation chamber. In order to provide an even more detailed description of the production according to the present invention, several practical examples related to the application of the aforementioned raisins to an active metallic core whose crystalline network has adsorbed a given amount of natural hydrogen.

EXAMPLE 1 On a rod of 90 mm long, with a diameter of 5 mm, made of a metallic material (Clunil) formed by isamét rich crystals that have nickel and chromium atoms in equal number and alternating, was made to be assigned natural hydrogen (D / H = 1 / 6,000) after the introduction of H_¡. at a pressure of 500 millibars and a temperature of 220 ° C, with contemporary immersion in a magnetic field of 1 Tesla, 5ß held by means of coil 9, wound around the nucleus itself. The generator used was the one illustrated in figure 1, with a bale of tubes 5 na coated with metallic layer. Then the chamber containing the bar was gradually brought to a temperature of 20 ° above the Debye constant, which for the Clunil is 192 ° C. The start or start with the thermoelectric method occurred (by means of a thermal impulse produced by a fjl.so of current that passes through the winding 9), with the leo inserted at all times in the aforementioned magnetic field and submerged in hydrogen natural, at a pressure of 500 million pounds. More precisely, the start was obtained with an impulse intensity of 1,000 A and a lifting time of 30 nanoseconds. During the course of the reaction, a total net heat of 1.29 MJ was taken for a period of 5 days, after which the reaction was stopped with an arrest achieved by - introduction of Ha, after having temporarily caused a vacuum (0.1 mbar). While the reaction was stopped, it was observed that radioactive isotopes were detected during the course of the transient, which is believed to be due to the impact on the nuclei adjacent to the H, D, 3He nuclei that were accelerated by the energy of photons g ( 5.5 MeV) produced by the last H + D reactions and transferred to the network to activate other amino acids.

EXAMPLE 2 On a 200 mm long nickel rod, with a diameter of 3 mm, the adsorption of natural hydrogen (D / H = 1 / 6,000) was forced with the immersion mode in a gaseous environment at a critical temperature of 19 °. C and the contemporary application of a magnetic field of 1 Tesla, obtained by means of the i 9 coiled around the nucleus. The ger-t-rador used was the one illustrated in figure 2. Then the chamber containing the bar was brought to a temperature 20 ° poc above the Debye constant, which for nickel, is 167 ° C. The start-up occurred with the electric narrowing method or, in other words, by applying an electrode to the core through which an impulse of a piezoelectric nature was transmitted. More precisely, the ranque was obtained with a pulse of at least 10 kV and a rise time of 0.1 seconds. During the reaction, a total net average heat of 4.74 MJ per day was separated for a period of 31 days, after which the reaction was stopped with a slow stop.

EXAMPLE 3 On a rod 90 mm long, with a diameter of 5 mm, made of AISI 316 steel, which had been tempered at 400 ° C to eliminate internal stresses, natural hydrogen adsorption was forced (D / H = about 1 / 6,000), with the method of immersion in an acid solution, and then so much immersion in a gaseous environment at the absolute pressure of 600 mbar, bed the application of a magnetic field of 1 Tesla, obtained by means of coil 9, wound around of the nucleus.

Then he took the camera that contained the bar to p Jo * r above the Debye constant and, precisely, to 314 ° C. Start-up was obtained both with the thermoelectric method co or by the thermal stress method due to gas recovery. During the reaction, a net total of heat was extracted, on average, of 2.64 MJ per day, during a period of 34 days, cies.-pué5 from which the reaction was stopped with a slow stop, obtained by cooling below the critical temperature » EXAMPLE 4 In a generator co or the one illustrated in the figure 1, comprising a generation chamber traversed with a bait of tubes made of copper, a layer of 2 mm of pure nickel was applied electrolytically on each tube, and it was made that? natural hydrogen (D / H = about 1 / 6,000) was adsorbed, lfi n the method of immersion in gaseous environment, at the absolute pressure of 600 mbar and with contemporary application of a magnetic field of 1 Tesla, obtained by means of a coil wound around the core and immersed in a ceramic matrix. Then he took the camera containing the tube strip to a temperature of 210 ° C, 57 ° above the Debye constant. The starting point was obtained with the magnetast icter other words, applying an electromagnetic impulse to the nucleus, by means of the winding 9. More specifically, the start was obtained with an impulse of O.d Tesla and a rise time of 0.1 second. During the reaction, by means of the fluid thermal carrier that crosses the strip of tubes, a net total of heat was extracted, on average, of 4.9 MJ per day, during a period of 6 days; after which the reaction was stopped with a slow stop, obtained by cooling well below the critical temperature. The industrial applicability of the generation process * and the generator that drives the process, therefore, is evident, given that they allow the production of energy in the form of heat, by means of nuclear fusion at limited temperatures, without the emission of radioactive particles or other dangerous particles, and for extended periods. The materials used for both the active core and the rest of the generator are low-cost and, in this way, provide considerable possibilities for economic exploitation. In those cases where the active core of a material having a higher Debye constant, such as silicon (64-0 ° K), is focwn, the temperature at which the thermal biointeception takes place is greater than in the examples described above. Therefore, it is possible to directly exploit the energy acquired by the poctac tecic fluid, which crosses the generator, for example, to move turbine blades or for similar applications.The reaction of: 3He, as a product of the reaction, is also industrially exploitable, given the current high cost of this gas. *

Claims (1)

NOVELTY of the INVENTION CLAIMS

1- Process for the generation of energy by means of the non-harmonic, stimulated fusion of hydrogen isotopes adsorbed on a metallic core, characterized in that it comprises: a step of charging on said metallic core, a number of hydrogen isotopes H and D, which are adsorbed in the crystal lattice of the nucleus; a heating step in which the core charged with the isotopes of hydrogen ee heats up to a temperature above a minimum temperature corresponding to the constant Debye temperature of the material making up the core; a step of starting to start the nucleus, where a vibratory effort with a rise time of less than 0.1 second is activated, which activates a nuclear fusion of the hydrogen isotopes; a stationary pass, during which the heat produced by the nuclear fusion reaction H + D, which occurs in the nucleus, is exchanged, because a coherent multimodal system of stationary oscillations is maintained. 2. Method according to claim 1, further characterized in that during the passage of l & It is necessary to over-pass the minimum temperature which corresponds to the Debye constant at least in a DT between several degrees and several tens of degrees, depending on the type of material of which the active core is formed » 3. Method of compliance with claim 1, further characterized in that during the charging step, the heating pass, the start-up step and the stationary pass ee applies to the core a magnetic field having an intensity ≤ 0.1 Tesla. . 4. Method according to claim 1, further characterized in that during the step of charging isotopes of hydrogen that are made to be adsorbed in the core have a ratio of isotopes D to isotopes H greater than l / ñ0, O0. 5. Process according to claim 1, further characterized in that during the step of charging * -3β isotopes of hydrogen that are made to be adsorbed on the core they have a ratio of D isotopes to isotopes H comprised between 1 / 10,000 and 1 / 1,000. 6. Producer according to claim 1, further characterized in that during the step of charging isotopes of hydrogen that are made to be adsorbed on the nucleus have a ratio of D isotopes to H isotopes of about 1 / 6,000 (hydrogen natural). 7. Procedure according to claim I-Ar. 1, further characterized in that, at the end of the loading step, the overcrowding of the H and D atoms adsorbed on the metal exceeds a numerical ratio of isotopes from hydrogen to metal atoms of 0.3. S. - Method according to claim 1, further characterized in that after the stationary step a stop step of the fusion reaction is provided, provided on cooling the core below the minimum temperature. 9.- Performed in accordance with claim 1, further characterized in that after the stationary step a step of stopping the fusion reaction is provided by the production of an additional vibratory effort, which disrupts the coherent multirodal system of stationary oscillations. . 10. Method according to claim 9, further characterized in that the step of stopping before the introduction, after having temporarily caused a vacuum, of a polyatomic gas inside a chamber containing the active nucleus, which causes said additional vibratory effort. 11. - Method according to claim 1, further characterized in that the stopping step occurs by means of a thermal stress obtained by introducing within a chamber containing the nucleus a polyatomic gas with a pressure gradient comprised between i ilibary and 4 bar . £ Sk J2.- Compliance procedure n claims 10 and 11, characterized further because the polyatomic gas comprises H2, T) .-, HD, HT, Cz t, NHa, N. ^,, O-j, or a mixture of days or more of them. 13. Method according to claim 1, further characterized in that the starting step occurs by a mechanical torsion, compression traction applied to the ends of the active core, with a rise time of less than 10 ~ A seconds. Mff 14. - Method according to claim 1, further characterized in that the step of starting occurs by electrical strenght obtained by means of an electric current pulse applied to the active core. 15. Process according to claim 1, further characterized in that the start step occurs by pulses of a laser beam, which is incised on the core. 16.- Pracedimienta in accordance with the claim- "I", further characterized in that the starting step occurs poc radio frequency pulses applied to the active core, which have a frequency that corresponds to the resonance frequency of the spins of the hydrogenated isotopes. 17. Progressing according to claim 1, further characterized in that the start step occurs by radio frequency pulses applied to the active core, which have a frequency that corresponds to the plasma of the free electrons of the core network. - Method according to claim 1, further characterized in that the start step occurs by pulses of ultrasonic vibrations applied to the active core; the latter being contained in a resonant cavity. 19.- Proceeding in accordance with claim 1, further characterized because the start-up step occurs - inverse piezoelectric effect, when sending to the ends of a metallic core impulses of alternating voltage with a frequency equal to the mechanical resonance of the nucleus. 20. Proof of confrmidad with claim 1, further characterized by the occurrence of the starter pass by magnetaest ictac effecta, through the production, along the metallic core, of a magnetic field with peak values above the intensity of magnetic saturation and with a rise time of less than 10-A seconds. - »21. Proof of conformity n l to claim 1, also characterized because the charge passes occurs by electrolytic means. 22. Method according to claim 1, further characterized in that the step of charging occurs medium immersion of the nucleus in a gaseous environment containing hydrogen. 23.- Procedure according to the claim- ?? 1, characterized in that the loading step occurs by means of immersion of the core in solutions of HCl-HCl or 24. - Conformity procedure with claim 1, characterized in that the charging step occurs by means of immersion of the core in galvanic baths containing standard NH 5 deposited the metal constituting the core on a support composed of Cu or ceramics. 25. A generator of energy poc means of harmonic fusion, stimulated, of isotopes of hydrogen, adsorbed on metal, characterized in that it comprises: an active metallic core, on which isotopes of hydrogen are adsorbed, a generation chamber containing the active core, heat exchange means, placed inside or around the generating chamber, and in which a thermal carrier fluid flows; A means for initiating a harmonic fusion reaction of the hydrogen isotopes adsorbed on the core 26.- Generator in accordance with the claim 25, further characterized in that the active core has the shape of a bar inserted in the generation chamber. 2.7. - Generator in accordance with the claim 25, further characterized in that the means for initiating the reaction comprises an electric coil immersed in a ceramic matrix and wrapped therein by a support hull defining the generation chamber. 2 .- generator of deformation with claim 27, further characterized in that the generation chamber is crossed by a bait of tubes that extend between two flanges welded to the splitter helmet; crossing the pipe gutter said flanges and communicating with a prechamber comprising an annular jacket delimited by a cylindrical helmet; also communicating said bait of tubes with a collection dome connected with means for external exchange of ^ Lar and with a circulation pump of a thermal carrier fluid. 29.- Generated in accordance with the claim 27 and? Ñ, further characterized in that the metallic active core is electrolytically deposited on the bait of tubes. 30.- Confidence generator with the claim 27 to 29, further characterized in that the generating chamber communicates, by means of axial ducts crossing the damp, in a _sfdo and with the prechamber on the other side, with a gas tank and a suitable air pump to feed hydrogen or other ga-e- into the generation chamber, creating thermal stress and starting or starting the reaction. 31.- Generator in accordance with the claim 25 and 26, further characterized in that the generation chamber is contained in a heating cylinder ep which is submerged in an electric winding; a sleeve being provided around the cylinder which is formed by a cylindrical supporting hull, and which allows the passage of the ico fluid; communicating the generation chamber, through a dome camera, with a gas tank and with an air pump; the nucleus being in contact with a suitable electrode to transmit an impulse to start or start the reaction. 32. Conformance generator cn claim 25, further characterized in that the core is a layer of metal deposited electolytically on a Cu or magnetic support 33. Generator according to claim 25, further characterized because the core It is a metallic powder present in the generation chamber. 34.- Generator in accordance with the rei indication 25, further characterized in that the means for initiating or starting the reaction comprise a piezoelectric electrode fixed to the nucleus. P