Patent Publication Number: US-2022219977-A1

Title: Method of and apparatus for plasma reaction

Description:
TECHNICAL FIELD 
     This invention relates to a method of and an apparatus for separating nucleons from atomic nuclei of gases such as nitrogen, carbon dioxide, etc. 
     BACKGROUND OF THE TECHNOLOGY 
     The inventor of this application has been developing a method of taking hydrogen out of water, in which a reaction agent is supplied into a sealed vessel as a reactor made of stainless steel, and the reactor is heated at a temperature of 500° C. to 600° C. The reaction agent comprises sodium hydroxide or potassium hydroxide and is heated so as to disperse the fine particles of the reaction agent into a reaction cylinder so that the particles collide with the molecules of water to separate hydrogen from oxygen. 
     PRIOR ART 
     Patent Literature 
     
         
         Patent Literature 1: Japanese Patent No. 6034550 
         Patent Literature 2: Japanese Patent No. 6005331 
       
    
     SUMMARY OF THE INVENTION 
     Subject to be Solved by the Invention 
     In the above patent publications  1  and  2 , hydrogen can be separated from water, gaseous oxygen is not discharged together with hydrogen, but remained in a reactor as oxide. Further, hydrogen comes out more than the amount of hydrogen included in water supplied thereinto. However, the reasons for these phenomena are not disclosed. 
     And, sodium hydroxide (NaOH) or potassium hydroxide (KOH) is used as catalyst or reaction agent which includes the ingredient of oxygen. Therefore, at the step of preparation of the reactor, even if the reactor is heated after it is made a vacuum, a little oxide is remained in the reactor to decrease a reaction efficiency and the life span of reaction. In addition, the principles of reaction are not explained efficiently, and there is a problem when it is practically used. 
     Means for Solving the Subject 
     The subject of this invention is solved by a method having the steps of: ejecting the first electromagnetic waves with a plurality of different frequencies by heating a reactor wall made of material having heat resistance and conductivity; supplying amplification material for amplifying the energy of the first electromagnetic waves into the reactor; vaporizing the amplification material under the cooperative influence of the first electromagnetic waves with the amplification material itself which is then changed into fine particles; ionizing the fine particles to form a plasma apace; radiating the first electromagnetic waves to the fine particles to emit the second electromagnetic waves having amplified energy; and separating nucleons of a gaseous element under the cooperative action of the second electromagnetic waves with gas fed into the reactor to be treated therein. 
     Further, the reactor is made of stainless steel or iron, and the amplification material comprises at least one of alkaline metals such as lithium, sodium or potassium or the fluoride of those elements. 
     As the gas to be treated, nitrogen, carbon dioxide, argon and stream (deuterium and tritium) are preferably supplied thereinto. 
     Furthermore, as the amplification material, sodium or potassium with stainless powder or zinc powder is preferable. 
     Further, a portion of the reactor for accommodating the amplification material is heated at a temperature of 400° C. to 600° C., and, further, the plasma space is preferably maintained in a state of air-cooling to keep it at a temperature of 200° C. to 300° C. 
     An apparatus for plasma reaction of this invention comprises: a reactor made of material having heat resistance, corrosion resistance and conductivity and emitting the first electromagnetic waves with a plurality of frequencies from a reactor wall to be heated; amplification material made of at least one kind of alkaline metals which are accommodated in the reactor to amplify the energy of the first electromagnetic waves by the interaction between the amplification material and the first electromagnetic waves to emit the second electromagnetic waves; and a heating device for heating the reactor to vaporize the amplification material and to emit the first electromagnetic waves from a reactor wall thereby to form a plasma space, nucleons being separated from the nuclei of the atoms in gas supplied into the reactor to be treated. 
     Further, the reactor is made of stainless steel or iron material, and the amplification material preferably comprises at least one kind of alkaline metals with stainless steel powder, iron powder or zinc powder. 
     Furthermore, the heating device preferably has an inner heating cylinder disposed in the reactor, and hydrogen produced in the reactor is fed into a burner in the inner heating cylinder to heat it. 
     Furthermore, the reactor has a air-cooled portion and a heated portion, and the plasma is formed corresponding to the air-cooled portion. 
     Furthermore, a carbon layer is attached to the inner wall of the reactor. 
     Furthermore, the heating device preferably has an inner heating cylinder, and a plurality of cylindrical cassettes including the amplification material therein are disposed between the inner heating cylinder and the main body of the reactor to form paths for the gas to be treated. 
     Effect of the Invention 
     A sealed reaction cylinder (reactor) without the inflow of air (oxygen) is made of iron or stainless steel material (austenite crystal structure including nickel is preferable), and an energy amplification material is supplied into the inside of the reactor to amplify the energy of electromagnetic waves emitted from the wall of the reactor, and, further, the energy amplification material comprises alkaline metal or alkaline fluoride. When the reactor is heated at a temperature above 400° C., metal crystal lattices in the wall of the reactor oscillate, and electrons also oscillate to generate electromagnetic waves having wave lengths peculiar to the metal. Interaction between the electromagnetic waves and the amplification material partially occurs to generate a high temperature portion thereby to vaporize the amplification material, so that light fine particles are dispersed in the reactor. These fine particles have the same function as that of generating energized laser beams and interact with the electromagnetic waves emitted from the reactor wall to induce-emit the energized second electromagnetic waves. 
     When gases such as nitrogen, carbon dioxide, etc. are fed into the reactor to be close to the fine particles, the second electromagnetic waves enter the nuclei of the atoms of the gas to interact with gluons which are one kind of gauge elementary particles and are the source of nuclear force thereby to obstruct or recover instantly the exchange of color charge because both of the electromagnetic waves and gluons are wave motion. 
     In this manner, the nuclear force between a proton and a proton, between a proton and a neutron and between a neutron and a neutron is cut at a certain possibility or percentage, and especially in the case that the nuclear force between a proton and a proton is cut, the proton coming out of a nucleus with a repulsive force on the basis of an electromagnetic force to form a hydrogen gas atom by uniting with an electron. 
     Since the reactor is made a vacuum at its preparation step, there is no oxygen ingredient not to form an oxide layer in the reactor at all which has a fear to absorb the first electromagnetic waves emitted by a heat lattice oscillation on the reactor wall. On the basis of “law of conservation of energy” with respect to elementary particles, the theoretical energy level of the first electromagnetic waves is not limited for an extremely short time in spite of the level of a theoretical energy of a heat oscillation. That is, its energy level has a possibility to go up to a level more than the level on the basis of the heat oscillation. Further, there may be a certain possibility that the energy of the second electromagnetic waves is higher than a theoretical value produced by a reaction between the first electromagnetic waves and the amplification material, and the second electromagnetic waves cut the nuclear force instantly (e.g., time of 10 −10   second) to separate nucleons from a nucleus. Accordingly, protons and neutrons are separated from carbon dioxide in which molecules move freely to make it harmless and to prevent the global warming. In addition, tritium water generated in an atomic reactor can be made harmless by removing neutrons from protons in a nucleus. Further, as hydrogen is produced from nitrogen, a hydrogen electric power generation is possible all over the world (especially on desserts), and burning of hydrogen can produce electric power and water to contribute to afforestation of desert. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1  shows a schematic view of a hydrogen electric power system including a hydrogen generating apparatus (reactor) of this invention. 
         FIG. 2  shows a partial perspective view of an amplification material casing disposed in the reactor. 
         FIG. 3  shows a cross-sectional view along a line 
         FIG. 4  shows a structural view of a reactor which is one of other embodiments of this invention. 
         FIG. 5  shows a structural view of the reactor which is one of other embodiments of this invention. 
         FIG. 6  shows a partial cross-sectional view which is one of other embodiments of this invention. 
         FIG. 7  shows a cross-sectional view of the reactor shown in  FIG. 6 . 
         FIG. 8  shows a perspective view of a cassette cylinder accommodating nuclear reaction material. 
         FIG. 9  shows a cross-sectional view of the cassette cylinder shown in  FIG. 8 . 
         FIG. 10  shows a longitudinal-sectional view of a reactor for explaining a principle of this invention. 
         FIG. 11  shows a perspective view of a metal crystal lattice structure. 
         FIG. 12  shows a partial cross-sectional view which is one of other embodiments of this invention. 
         FIG. 13  shows an enlarged sectional view of the bottom portion of the reactor. 
         FIG. 14  shows an operational view for explaining a plasma space of the reactor. 
         FIG. 15  shows a view for explaining a relation between an electromagnetic force and a nuclear force both of which operate among nucleons. 
         FIG. 16  shows a view for explaining separating operation of nitrogen in a reaction space. 
         FIG. 17  shows a sectional view of a lateral type of reactor which is one of other embodiments. 
         FIG. 18  shows an explanatory view of reactors disposed in parallel. 
         FIG. 19  shows an explanatory view with respect to a largeness of energy of the second electromagnetic waves, which is one of other embodiments of this invention. 
     
    
    
     EMBODIMENT OF THE INVENTION 
     The embodiments of this invention will now be explained with reference to the drawings. 
     In  FIG. 10 , a plasma reaction apparatus M of this invention has a cylindrical reactor  70  which is made of iron or stainless steel. In the stainless steel, SUS  304 ,  310  or  316  of austenite crystal structure is preferably used because it has a good heat resistance, an anticorrosion and a conductivity. Iron can be used in a state wherein oxygen can be completely prevented from flowing into the reactor. A carbon layer  71  is formed on the inner wall of the reactor  70  for the prevention of oxidation and for the emission of electromagnetic waves (cavity radiation). 
     The lower half circumferential portion is surrounded by a platelike heating device (heater)  72  which can heat the reactor  70  at a temperature of 400° C. to 700° C. A supplying pipe  73  is provided on the upper surface of the reactor  70  to supply gas thereinto, and extends into a plasma space  74  formed at the upper half portion of the reactor  70  so as to open to the space  74 . And a discharging pipe  75  is also provided on the upper surface of the reactor  70  to discharge the gas produced in the plasma space  74 . An emitting supplementary body  76  is disposed at the bottom portion of the reactor  70  and has a plurality of emitting plates  80 ,  80  . . .  80  to increase electromagnetic emitting area, and, further, amplification material for amplifying the energy of the electromagnetic waves is accommodated together with the body  76 . The emitting supplementary body  76  is made of the same material as the reactor  70 . Instead, powder of the same material, e.g., iron or stainless steel powder of approximately  70 pm can be used. 
     As the amplification material  77 , at least one of alkaline metals (lithium 7), sodium (Na) and potassium (K) can be used. Instead, fluoride (LiF, NaF, KF) of alkaline metals can be used. In the case that stainless, iron or zinc powder is added to those alkaline metals, a reaction efficiency increases. 
     Each electromagnetic amplification material has one electron on the outermost shell and is chemically active. If it is heated, electrons on inner shells easily jump up to one of outer shells. Further, these metal elements and those fluorides have relatively low melting points (Li:180° C., Na:98° C., K:64° C., Lif:460° C.) so that they are easily changed into liquid by heating them. For example, if the amplification materials are heated at a temperature above 400° C., they go up to a high temperature by their energy amplification function and by molecular heat oscillation to produce fine particles which are dispersed to fill the plasma space  74  therewith. 
     On the contrary, the metal material in the wall of the reactor has, as shown in  FIG. 11 , a crystal lattice  80  which comprises each element  81 . 
     Such a lattice structure emits electromagnetic waves having characteristic frequencies with respect to the lattice. This electromagnetic waves correspond to a cavity radiation in the reactor, and as shown in  FIG. 12 , are emitted so as to have different strengths in correspondence to a temperature. That is, the strength (number of photons) of the electromagnetic waves become larger as the temperature of the reactor goes up, and their peaks move in a direction where their frequencies become large. The frequencies of the electromagnetic waves emitted at a certain temperature are numberless from a small number of frequency to a large number thereof. The energy by (h: plank constant; v: frequency) of electromagnetic waves is not successive and is quantumized to change in a jumping manner. 
     In the case that sodium (Na) is used as amplification material, sodium is melted and liquidized at a temperature below 100° C., and, as shown in  FIG. 13 , goes slightly up along the surface of an emittance plate  75  by a surface tension. The crystal lattice of the amplification material oscillates fiercely and partially by being heated at a temperature of 300° C. to 400° C. through a cooperative reaction between the electromagnetic waves and the sodium Na. 
     As a result, it is vaporized to produce fine particles which are dispersed in the plasma space  74 . In these fine particles, as shown in  FIG. 14 , one electron e −  on the outermost shell is sprung out through an ionization reaction to form a plasma atmosphere in which on NaT ion and the e −  are mixed with each other. This reaction happens even in the case of Li or K. At the same time, metal sodium ions in the plasma atmosphere is excited to emit the second electromagnetic waves which are, as shown in  FIG. 14 , reflected on a carbon layer as a reactor wall so as to be amplified by a cooperative reaction with the amplification material through the same function as a laser beam amplification function for increasing the number of the photons of laser beam. The amplified second electromagnetic waves react with gases (N 2 gas, CO 2 gas, helium gas, argon gas, tritium steam, normal steam) supplied into the reactor to separate nucleons from each nucleus. The upper half portion of the reactor  70  is opened to the atmosphere so as to be air-cooled. An air-cooling changes the energy amplification function of the plasma space. The plasma space  74  must be maintained, e.g., at a temperature of 200° C. to 400° C. In order to produce a lot of fine particles of the amplification material at the bottom portion of the reactor, the bottom portion is preferably maintained at a temperature above 400° C. so that there is a difference in temperature between the fine particle emitting portion and the plasma space. That is, the lower half portion of the reactor  70  forms a heating portion and its upper half portion forms an air-cooling portion so that the air-cooling portion corresponds to the plasma space  74 . 
     As mentioned above, in order to separate protons or neutrons from a nucleon, energy above the nuclear force (corresponding to binding energy) of a nucleus must be given to each nucleon. With respect to the generations of the first and second electromagnetic waves, as shown in  FIG. 12 , some electromagnetic waves of high frequencies (oscillations) are emitted by the cavity radiation. Furthermore, according to the “uncertainly principle”, the product of energy and time (period) makes a value above the Plank constant (ΔEΔt≥h). For example, in the instant period of 1/one billion second (10 −6   second), “the principle of energy reservation” is not adapted, so that an extremely large energy occurs at a certain probability. To be concrete, the nuclear force among nucleons of the nucleus of a nitrogen atom is 6 to 7 MeV which correspond to a wave motion energy of y ray with a frequency above 10 20 , and the second electromagnetic waves with such a wave notion energy react on the wave motion of gluons as elementary particles to cut instantly the nuclear force thereby to separate protons and neutrons from a nucleus. In the nucleus, protons and neutrons move on each orbit while they are oscillating, and the distances between them are changing. Especially, when a heating energy is given to them, they oscillate furiously to obtain kinetic energies, respectively (½ mv 2 ). When the nuclear force between two portions is cut, the protons are, as shown in  FIG. 15 , sprung away from each other by an electromagnetic repulsive force therebetween. At this time, in the case that each proton is united with an electron, an atom of hydrogen with a constant volume is formed. On the contrary, when nuclear forces (between a proton and a neutron, between tow neutrons) are cut to separate each neutron from a nucleus, each neutron has only a kinetic energy without an electromagnetic force. Therefore, its separating force is small in comparison with that of two protons, so that each neutron floats in the reactor without moving fast, and may be sometimes captured in the reactor wall. Each neutron changes to a proton after a predetermined time through a β-decay. Namely in the plasma space, an amplified energy is generated at a certain probability without abiding by the energy reservation principle, so that the temperature of the plasma space is remarkably raised. This results in that the nucleons are separated from each other to generate instantly an endothermic reaction. Such an endothermic reaction has been certified at several times by a thermometer. The range of temperature above 250° C. drops instantly even during heating the reactor. With respect to exothermic reaction, it was observed that some stainless steel powders of 1 mmp(diameter) as amplification material are completely vaporized to disappear in the reactor. This mean the raise of temperature above 3000° C., and, further, an amorphous crystal structure was found on the reactor wall. Therefore, the temperature of the reactor wall drops steeply from an extremely high temperature to an extremely low temperature. 
     With reference to  FIG. 16 , the action of a nitrogen nucleus  90  supplied into the reactor  70  will now be explained. The nucleus  90  has seven protons P and seven neutrons n, and the amplified second electromagnetic waves generate a large energy (7 to 8 Mev) which makes seven protons P spring out of the nucleus  70  into the plasma space  74 . At this time, each proton springs out at a high speed by a repulsive force to have a large kinetic energy. However, in the case that the proton is reunited with an electron to form a hydrogen atom having a predetermined volume, the flying speed of its kinetic energy becomes small. Even if the proton collides with the reactor wall  70 a, it cannot be caught in the reactor wall because of a repulsive force from atoms of stainless steel in the reactor wall. In addition, when a nuclear force including seven neutrons is cut, the velocity of the kinetic energy (½ mv 2 ) of each neutron is smaller than that of each proton because of no repulsive force among them in an electromagnetic field. when each neutron collides with each particle (Nat, etc.) dispersed in the space, it loses the velocity of the kinetic energy. In this state, it is changed into a proton by a β-decay or it flies in the reactor without moving out of the reactor. In this manner, instant exothermic reaction and endothermic reaction are repeated by the generation of a high energy and the separation of protons from a nucleus. 
     In this invention, since the exothermic reaction balances with the endothermic reaction, the reactor can be operated safely. That is, if the separation of protons only occurs, a remarkable endothermic reaction only occurs so that the temperature of the reactor drops at the absolute temperature 0° to stop the reaction. If the exothermic reaction only occurs, the reactor wall is instantly melted to stop the reaction. In this invention, the probability of the endothermic reaction balances almost with that of exothermic reaction, and, however, it is preferable that the possibility of endothermic reaction is slightly larger than that of the exothermic reaction in view of safety of the reactor. In this manner, the two reactions continue safely, and there is little such a danger that neutrons jump out of the reactor. At the time of experiments, a device for measuring neutrons was always disposed near the reactor  70 , and, however, there was not fact that the device detected distinctly the neutrons. 
     The vertical type of reactor is operated as mentioned above, and a lateral type of reactor can be also operated in the same manner as shown in  FIG. 17 . A reactor  100  has a lateral cylindrical body  101  made of stainless steel or iron, and a carbon layer  102  is formed on the inner wall of the body  101 . At the left end portion of the body  101  is provided a gas supply pipe  103 , and at the right end portion thereof is provided a hydrogen discharging pipe  104 . A heating pipe  105  made of stainless steel (SUS  304 ) is extended in the central axis direction of the body  101  to the central portion of the body. 
     A heater  106  as an inner device is accommodated in the heating pipe  105  to heat the inside of the body  101 . In addition, the outer circumferential wall positioned at the left half portion of the body  101  is covered with a plate-like heater  107  as an outer heating device to form a heating portion. The right half portion of the body  101  is exposed to the atmosphere to be coaled to form a cooling portion which corresponds to a plasma space  108 . A case  109  for accommodating amplification material is mounted on the lower surface of the left half portion of the body  101 , and metal lithium, sodium, etc., as the amplification material re accommodated in the case  109 . In the case that the reactor  100  is heated by both heaters  106  and  107 , the fine particles of the amplification material are sufficiently dispersed to fill a plasma space therewith thereby to ensure a phase transition in the cooled reaction space. 
     The inventor of this invention has been making experiments for eleven years, and the kind of experiments and opinions on the basis of each experiment will now be explained. 
     1. An Experiment with Respect to the Kind of the Material of the Reactor 
     NaOH was conventionally used as the amplification material. The reactor can be made of ceramic, copper, nickel, iron or SUS 304 ,  310 ,  306 , SUS materials were preferable, and ceramic, copper or nickel material were not preferable to produce hardly hydrogen from water supplied into the reactor. In SUS materials, SUS 304  or  306  having a austenite crystal structure was preferable, and SUS material of ferrite crystal structure was inferior. Further, the reactor made of iron had a good reaction, and, however, the reaction did not continue for a long time. At first, NaOH was used as the amplification material, and alkaline metal itself without the ingredient of oxygen is used in view of the prevention of oxidation. 
     2. An Experiment with Respect to the Kind of the Amplification Material 
     At first, stainless steel piece (SUS 304 ) with sodium hydroxide (NaOH) or potassium hydroxide (KOH) were used to take hydrogen out of supplied water, and instead of these materials, sodium titanium oxide (KTiO 2 ) or potassium titanium oxide (NaTiO 2 ) was used to take hydrogen from water. On the contrary, a reactor of SUS 304  without the amplification material could produce a slight amount of hydrogen from water. However, the reactor had to be heated at a temperature above 650° C. in order to produce a sufficient amount of hydrogen. In addition, it was clearly confirmed that a reactor of SUS 304  accommodating only NaTiO 3  or KTiO 3  therein was simply heated at a temperature above 500° C., so that hydrogen continued to be produced for long hours (almost one week). The reactor was heated, before the experiment, at 600° C. for several hours to discharge outside hydrogen included in a reactor wall. In the case of sodium titanium oxide, a plasma atmosphere (Na + , Ti 3+ , O 2− , electron e − ) was formed over the surface of the amplification material by its heated oscillation to separate protons from at least one of these ions. There is a high possibility that hydrogen is produced from oxygen having the smallest bounding energy among these three ions. 
     3. An Experiment with Respect to the Condition of the Plasma Space in the Reactor 
     When Na was used as the amplification material and a kind of gas such as nitrogen or argon was fed into the reactor, a flame reaction of Na could be conspicuously observed. The flame reaction means that a lots of Na fine particles were flying in the plasma space of the reactor. When the reactor was disposed in an insulated state, it could be confirmed that there was a potential difference between an outer side surface, corresponding to the plasma space, of the reactor and the ground, and the reactor space was filled with electrons. Further, two reactors were, as shown in  FIG. 18 , disposed in parallel, and the plasma spaces  201 ,  201  were connected with each other through a pipe  202  which was provided with an insulator piece  203  at its center portion though which the plasma spaces were communicated with each other. In this case, it was confirmed that both reactors were electrically communicated with each other to generate a potential difference. Namely it is understood that the plasma space is formed with an ionized gas, and electrons fly in the space. In general, it is known that sodium has a function for amplification of electromagnetic waves. Accordingly, the plasma space has an amplification function for the electromagnetic waves. 
     4. An Experiment with Respect to the Optimum Position of the Plasma Space 
     In the case that, in a vertical type of reactor as shown in  FIG. 10 , the reactor accommodates Na and stainless steel powder (SUS 304 ; φ70 μ) as the amplification material, and the bottom surface and the half lower side surface of the reactor were covered with a platelike heater, the temperature of the gas discharging pipe  75  projecting upward from its upper surface dropped suddenly at its root portion which was air-cooled. Thus, it was observed that the temperature of an air-cooled portion changed largely. That is, a plasma reaction occurred at a predetermined range of temperature. In synthetic view of various experiments, it occurred almost at the range of 200° C. to 300° C., and it is understood that a plasma phase transition occurs at such a range of the temperature. At this range, sodium hydride (NaH) is formed on the inner surface of the reactor. Further, when the gas supplying pipe was extended to the bottom portion of the reactor to supply water of 2cc therein in one operation (normally 0.5cc) to cool the bottom portion of the reactor, a gas separation reaction occurred actively to generate a lot of gases of mass numbers of 15 to 24 before and after mass number  18  so that hydrogen was produced by approximately 5 times as much as normal amount. This reaction continued for more than 40 days and stopped after that. It is supposed that gases of mass numbers 15 to 24 belong to CH gases, and a huge amount of hydrogen came out of oxygen in water in addition to hydrogen in water. This reaction generated a lot of hydrogen in the following manner. First, the reactor wall was heated at a high temperature to emit the first electromagnetic waves, so that a lot of fine particles are generated from the amplification material attached on the reactor wall. In addition, a lot of steam cooling the plasma atmosphere to generate the phase transition (the change of condition of plasma), and, further, to energize the second electromagnetic waves, and furthermore to generate a lot of proton separations. 
     5. An Experiment with Respect to an Action of Nucleons at a Time of Reaction 
     In the case that sodium hydroxide and some stainless steel pieces were accommodated, as the amplification material, in a reactor made of stainless steel, and heavy water (D 2 O) was supplied thereinto while heating it by an inner heater, the heavy water was almost changed into H 2  gas so that D 2  gas disappeared. Analysis of a reactor wall piece showed that some isotopes had more neutrons than normal isotopes. Especially, the phenomenon was remarkable in the case of Fe isotopes. It seems that the neutrons were absorbed in each metal of the reactor. 
     In addition, in the case that tritium water (T 2 O) is supplied instead of D 2 O, tritium above 70 percent disappeared. This result proved to be true by measuring the amount of β-rays. It seems that neutrons were separated from nuclei also in this case. 
     6. An Experiment with Respect to the Energy of the Generated Electromagnetic Waves 
     As shown in  FIG. 19 , a reactor  300  has an inner pipe  302  and an outer pipe  302  with a large diameter, and sodium hydroxide and stainless pieces were accommodated in the inner pipe  302 , and, further, an electric heater  303  was disposed in the inner pipe  302  to heat its inside at a temperature of approximately 550° C. Argon gas was fed into a space  304  between the inner and outer pipes for insulation. Normal water was supplied in the inner pipe. In this experiment, the space  304  was maintained at a constant temperature, and, however, a certain gas in the space  304  was expanded for three days to increase its pressure to over 0.3 Mpa. According to a gas analysis, the argon gas was almost changed into hydrogen gas. It seems that the second electromagnetic waves in the inner pipe  302  passed through the pipe wall to change the argon gas into hydrogen or the first electromagnetic waves emitted from the outer surface of the inner pipe  302  changed the argon gas into hydrogen. According to an analysis of the ingredient of the inner pipe wall, a lot of fluorine was detected. There might be some nuclear transformation under the influence of the second electromagnetic waves. Accordingly, it is supposed that the second electromagnetic waves had instantly a frequency corresponding to X-ray or y-ray which has a strong penetration. On the basis of these teachings, a cassette type of reactor was invented as shown in  FIGS. 6 to 8  which are mentioned after. 
     Next, a hydrogen power generation system including a plasma reaction apparatus of this invention will now be explained. A hydrogen power generation system has, as shown in  FIG. 1 , a reactor  1  which is provided with a separation device  2  for separating nitrogen from oxygen in air. The separation device  2  has a known separation film. Nitrogen N 2  and oxygen O 2  separated from air are supplied to the reactor  1  through a path I 1  and a path  1   2 , respectively. The reactor  1  transforms a part (above 50%) of nitrogen into hydrogen (H 2 ), and the remaining nitrogen (N 2 ) and hydrogen are fed into a separation  3  for separating hydrogen from the remaining nitrogen. The separated nitrogen (N 2 ) is fed into the reactor  1  through a path I 4  to be transformed into hydrogen again, and the separated hydrogen (H 2 ) is fed through a path I 5  into the reactor  1  to be used as a combustion gas. 
     The reactor  1  has a main body  4  made of stainless steel (SUS 304 , 310 , 316 : austenite is preferable) in which the left end of an inner heating cylinder  5  for heating the inside of the body  4 , and the left end of the body  4  are supported by a fixing flame  6 . The heating cylinder  5  has a double-structure which comprises an outer cylinder  5   a  and an inner cylinder  5   b . A burner  7  is set on the side of the fixing flame  6  of the inner cylinder  5   b  which is open on the opposite side thereof (forward end), and the combustion gas from the burner  7  is turned back along the forward end surface (right end) of the closed outer cylinder  5   a  to be fed into a path  11  through a discharging space  8  formed between inner and outer cylinders  5   a  and  5   b . Hydrogen gas is supplied in the burner  7  through a path  9  of the fixing flame  6 , and oxygen gas is supplied therein through a path  10 , and both gases are burned by the burner  7  to produce steam of a high temperature which passes through the inner cylinder  5   b  and is returned back at its forward end to come to a path I 6  through the path  11 . The steam from the path I 7  rotates a steam turbine of a known power generation device  12  to generate electric power. After this, the steam is changed into water by a condenser  13  through a path I 7  to be stored in a water tank through a path I 8 . 
     A case  15  is accommodated at the lower portion of the body  4  of the reactor  1  as shown in  FIGS. 2 and 3  to hold amplification material R therein, and is in the shape of a gutter which is closed by end plates  15   a ,  15   a  at its both ends. Each end plate  15   a  has a semicircular hollow  15   b , at the upper end of the end plate  15   a , to be engaged with the heating cylinder  5 . A plurality of slide pieces  15   c ,  15   c  . . .  15   c  are formed on the outer wall surface of the case  15  so as to ensure that the case  15  can slide on the inner wall surface of the body  4 . The quality of the material of the case  15  is the same as that of the reactor  1 . 
     The heating cylinder  5  is made of heat resistance ceramic so that the outer lower surface of the outer cylinder  5   a  contacts directly with the amplification material R to heat it. 
     The amplification material R is changed into fine particles to form a plasma atmosphere which can produce H 2  gas from, e.g., carbon dioxide (CO 2 ), argon (Ar), oxygen (O 2 ), helium (He), etc., in the same manner. 
       FIG. 4  shows another embodiment of the reactor in which a supplementary electric heater  40  is mounted on the outer circumferential surface of a cylindrical main body  4  to supplement the heating of the heating cylinder  5  so that nitrogen gas fed into the main body  4  is heated from both sides of a main body wall and a heating cylinder wall to increase the number of fine particles and the energy of the first electromagnetic waves. In this case, lithium fluoride of 70% and be lithium fluoride of 30% are used as the amplification material forming a kind of molten salt which is circulated by a pump  41  through the main body, and chemical treatment device  42  disposed outside of the main body  4 , and the amplification material is newly supplied into the device  42  in response to the consumption of that. In the case that the molten salt includes nitride and carbide as impurities, the chemical treatment device  42  eliminates them from the molten salt thereby to be able to operate the reactor continuously for a long time. In addition, when radium or polonium both emitting a-ray is added, as additives, to the molten salt, the decay of nitrogen happens remarkably to increase the production of hydrogen. Further, a carbon layer  43  is formed on the inner surface of the main body  4  to prevent the inner surface of the stainless wall of the main body  4  from corroding, and a plasma space  49  is formed at the right half portion of the main body  4 . 
     Next, another embodiment is shown in  FIG. 5 . That is, the inner-heating cylinder  5  is removed from the main body  4  and the amplification material R is heated by a heating device  83  disposed outside. 
     Further, the amplification material R is ejected by an ejecting pipe  44  to increase a contact efficiency with nitrogen gas. In addition, the center portion of the main body  4  is heated by a hater  40 . 
     Next, an embodiment in which the amplification material is easily changeable by designing it in the form of cassette will be explained. 
     In  FIGS. 6 to 9 , on the basis of the teachings of the experiment in  FIG. 19 , a plurality of cylindrical slender cassette cylinders  50 ,  50  . . .  50  are detachably disposed between the outer circumferential surface and the inner wall of the main body  4  in a state where a gas passage  51  is formed between adjacent cassette cylinders  50 , each of which is exchangeable by forming an end plate  52  of the main body  4  in a detachable manner. 
     Each cassette cylinder  50  is made of stainless steel (SUS 310 , SUS 316 ), and the amplification material R is hermetically accommodated therein. 
     As the amplification material, powder of SUS, Fe or Zn is preferably added to Na, K or Li of alkaline metal. Instead of each alkaline metal, NaH (sodium hydride) can be used. A carbon layer  62  is formed on the inner wall of the cassette cylinder  50 , while the powder of radium or polonium emitting a-waves is applied to the outer circumferential surface thereof with a binder or the powder is thermally sprayed thereby to form a a-wave layer  60 . And a similar a-wave layer  61  is formed also on the outer circumferential surface of the heating cylinder 
     A vacuum is formed in the cassette cylinder  50  by a vacuum pump  63  ( FIG. 9 ) to prevent an oxidation reaction therein. When the cassette cylinder  50  is heated at a temperature above 500° C., it emits the first electromagnetic waves which are amplified to generate the second electromagnetic waves which include partially waves of high frequencies so as to pass through a stainless steel wall. Further, these a-wave layers  60 ,  61  emit a-waves into the main body  4 . The second electromagnetic waves spring out electrons in a nitrogen atom to ionize the atom and to cut the nuclear force of a nucleus. The a-waves increase the above function. 
     Utilization Possibility in the Field of Industry 
     According to this invention, an electric power generation can be done from air without discharging carbon dioxide in addition to the production of water. Accordingly, the electric power generation can be done all over the world, and this invention is the most optimum means for afforestation of dessert due to the production of water. Further, conventional fuels can be used because carbon dioxide discharged on the earth can be changed into hydrogen. 
     Explanation of Numerals 
     
         
           1 ,  7  . . . reactor 
           4  . . . main body 
           5  . . . hating cylinder 
           43  . . . carbon layer 
           50  . . . cassette cylinder 
           60 ,  61  . . . a-wave layer 
           71  . . . carbon layer 
           72  . . . heater 
           74  . . . plasma space 
           76  . . . emission supplementary body 
           77  . . . electromagnetic amplification material