EP1638681A1

EP1638681A1 - Methdo and equipment for treating harmful gases

Info

Publication number: EP1638681A1
Application number: EP03748154A
Authority: EP
Inventors: Seppo Konkola; Robert Schiewe
Original assignee: Konkola Seppo
Current assignee: Konkola Seppo
Priority date: 2002-10-02
Filing date: 2003-10-02
Publication date: 2006-03-29
Also published as: WO2004030806A1; AU2003267467A1; NO20024750D0

Abstract

The present invention relates to a method and equipment for converting molecular gases, like carbon dioxide or oxides of nitrogen into a atomic form, carbon, oxygen or nitrogen, by using a rotating gas plasma reactor. The gases to be treated are fed to the reactor and treated to open the molecular bind between the atoms to release the atoms as pure atomic gases. After that the different types of atomic gases are separated into their own discharge channels for making pure atomic gases.

Description

Method and equipment for treating harmful gases

BACKGROUND OF THE INVENTION

The present invention relates to a method and equipment for treating harmful gases. At the same time the invention also relates to generation of charged gases and generation of glowing charged gases and plasma and production of circulating ball from those gases inside a chamber and the chambers and jets and nozzles to make this.

There is considerable interest in different branches of industries to use some reliable and effective methods to clean industrial gases like gases which contain CO₂ and other similar harmful ingredients. And this is done even more easily than producing energy from atomic gases, because when on molecule bind atom is ionized this means by curtain enough long right vibration level that the molecules chemical bind is lose and the molecule dissociates. This happens when non elastic scattering between electrons and molecules makes several electrons to more loosely bound stage, this charges atom, molecule or ion. The electron can also divide from atom or from molecule bind atom or from ion. And that means that atom or molecule bind atom is ionized. Atom or molecule bind atom is positive ion and usually charged.

When molecule bind atom is ionized this might mean the dividing the chemical bind of the molecules and the molecules dissociate. In some cases those by interaction processes off coming electrons have so much moving energy that they by interactions produce new ions.

The amount of non elastic scattering in molecule gases between electrons and molecules and its effect is much bigger than in atomic gases.

This is because molecule gases do have vibration rotation continuum which exists on infrared area. And because of those vibration continuums the beginning energy to non elastic scattering is much lower what is needed to ionize atom.

When the energy level inside chamber circulating gases grows also by interactions between particles produced photon's energy grows over the most tight bind K electrons binding energy, then there begins Compton's phenomenon, which is photons non elastic scattering from electrons, become more and more important interaction. When on scattering between photon and electron, the electrons binding energy's meaning is very small comparing to the photons energy, is the electron on this interaction a free particle. This happens usually in all circumstances in where the Compton phenomenon is the prevail interaction.

When radiation intrude into gaseous materials several different interactions do happen between the radiation and the particles, after which the situation and energy level of the gas material changes and also the behavior of the radiation changes. Therefore the ionization of the gases circulating inside the chamber to higher energy level is made step by step giving the needed time to all interaction and scattering processes to be in balance with the ionization and energy output. In this way all the different processes happening inside the circulating gases are on safe level.

The above referred interactions are physical phenomenon and there is also produced by recombination processes such new materials whose behavior must be known before putting them happening inside chamber. Those interaction processes are scattering processes between radiation and particles and scattering phenomenon between radiation and atoms and molecules and electrons in gases. There are also interactions between particles, atoms, molecules, ions and electrons and other charged particles in charged gases. This means that everything depends on the gas pressure, electromagnetic energy level, static electric level and electric tension level. The gases are on higher energy levels and they have faster vibration speeds, this means that the gases are in half ether energy levels where the Kundalin electric current is becoming effective and this means that there are both electrons positive and negative taking in and losing electrons.

In the above situation much small currents flow between ions and this makes the electric energy level and electric tension much higher level than before. In the half ether level also the molecule dissociation and all other interactions and scattering phenomenon processes are much faster and much more effective and the energy produced must be taken out in an amount which guaranties that the balance between ionization and deionization will be kept. This is also controlled by the amount gases which are fed into the chamber and taken our from the chamber and by the speed and amount of the gases and by the pressure of the gases.

The particle possessing immediately ionizing radiation moves in gaseous materials little by little and causes many electromagnetic interaction phenomenon, whereby each interaction will slow little the speed of the particle, until the whole energy is released. The effect of the indirectly ionizing in gases is the secondary ionizing and charging effect of the radiation.

To the indirectly ionizing radiation belongs electromagnetic; in other words photon radiation, X ray radiation, gamma radiation, braking radiation, disappearing radiation and neutron radiation.

The photon electric phenomenon leaves atom charged ion, and by this energy liberating the atom radiated the photons energy by characteristic X ray radiation quantum or by auger electrons which don't usually get any further than neighbor atoms without absorb. Because all those photo electric products electrons and X ray quantum absorb usually very close their birth place.

Electromagnetic movements, charged nucleus are results of alfa and beta breaks which leave very often the daughter nucleus on charged level. Also the products of nuclear reactions are usually charged.

The charge energy can be released in many different ways. The nucleus radiates particles; protons or neutrons or alfa or beta particles. The nucleus may divide (fission) or electromagnetic radiation may be formed. The nucleus charge is released step by step, so that each step leads the nucleus to a more stabile level. In the same way it is possible to begin several other different kind of radiation phenomenon.

Each ionization phenomenon ends so that a pair of positive and negative ions is formed. After scattering electrons have about five times longer ways comparing to heavier particles.

In atomic gases where the energy of the electrons is smaller than atoms spark energy, elastic scattering is the most usual mechanism to transfer energy between electrons and atoms. When on this like gases by gas in flow directs outsider electric field which speeds up electrons. So those electrons can not release they from electric field getting energy. Therefore they kinetic energy sets on higher level which may have higher than the heavier particles energy.

Between interactions by charged particles the effects depends on the ionization level of the gases.

Inside ionized gases the charged particles are in continuous interaction between other charged particles by Coulomb field. In the interactions the power is repulsive or attractive depending on the charges of those particles.

In air one particle has an infinite effect area.

However, inside ionized gases other nearby charged particles change the situation so that the energy fields of other charged particles modify the field of other particles so that the effect of the energy field of charged particles is reaching only the energy field of the nearest charged particles.

The interactions between charged particles are two or more times bigger than electron atom scattering. By charged particles the Coulomb potential effective area is larger than by atoms electron has.

By non elastic scattering there is more energy movement between particles what it is by elastic scattering, because by non elastic scattering part of movement energy is turned to ionization and charge energy.

Non elastic scattering might cause ionization, and more ionization happens by higher energy levels.

If other from scattering particles is already ionized before scattering, so the ionization energy can move to the other particle, this is called super elastic scattering.

If ionized atom scatters with other elements atom, which has lower ionization energy level, so this scattering might cause this other atom ionization, this happens specially in meta stabile levels 10 -3 also atom might then get ionized easier by electron scattering.

The amount of non elastic scattering in molecule gases between electrons and molecules is much bigger than in atomic gases.

Inside charged ionized gases photons penetrate much deeper than any other particles.

Charged ionized particle moves inside gases so long than its kinetic energy is bigger than the average particle's kinetic energy inside gases where its moves.

There is much free loose electrons in air gases and more than 10000 positive or negative ions inside each cubic inch, if not then the cars ignition plug don't work.

Those de ionization processes are recombination process in where positive ion and electron combine and they neutralize each others. Diffusion processes carry away charged particles from gases.

Forming negative ions doesn't change the charges amount, but effects to the amount of gases ability to bigger or smaller electric flow.

By recombination liberates energy, which amount is ionization energy's and kinetics energy's sum.

Photons movement speed is always the speed of light. And photon does not have mass but it has kinetic energy.

The interaction between photon and particles means either photons born emission or photons disappearing absorption or scattering.

By physics ways energy and movement energy can be changed between scattering photons and heavier particles. Those emitted photons also disappear very easily from gases.

Inside chambers photon energy's amount is much bigger if chambers have reflecting walls.

The electron's speed inside charged gases is 100 - 1000 times faster than ion's speed. Because electron's smaller mass they acceleration speed is much faster than ion's acceleration speed. And therefor electrons by elastic scattering loses only very little they energy. Also electrons free distance is longer.

By big electric charges in ionized gases begins photons, which born when charged gases dissociate they ionization energy or by ions recombination, begin to ionize gas molecules. Also many atomic gas molecules by form positive ions begins to separate electrons and when those forming electron ion pairs amount is big enough then inside gases exist continuous its self over keeping current.

When the ionized gases electric charge amount comes even bigger then the dependency to primary ionization is gone, and there is continuous electric current inside gases which can be controlled by non electric filling gases which are mixed in such amount with inside chamber circulating gases that the inside gases being electric current is on control. This information here is for the user of this equipment to make easier to understand and find out right ionization processes to clean molecule gases.

SUMMARY OF THE INVENTION

The gases generated by accordance by the present invention, are acceleration ionized by pressing them through ionization nozzles by high speed to make molecule gases to such high infrared rotation and vibration ionization energy level in where molecule gases have rotation and vibration continuum and they have low beginning energy to non elastic ionization to the energy and vibration level in where they dissociate so that the chemical bind which keeps molecule together is broken and the molecule dissociates.

Inside the chamber rotating glowing gas mass temperature is kept also in such level what is needed to over keep inside circulating molecule gases rotation and vibrating continuum on level. In where they ionization energy level is low so that by non elastic scattering and by Compton scattering and other scattering phenomenon ionizes those CO₂ molecules so that they dissociate. The temperature inside circulating gas mass is also kept in so high level, in where they also have thermal diffusion and or ambi polar ( both pole) diffusion on so effective level in where ionization and dissociation phenomenon are so fast that from molecules separated atoms are not ionized. That is therefore that by thermal diffusion and ambi polar diffusion dissociated charged particles can be separated away from gas mass by different diffusion processes. Before also atomic gases begin ionize and coming charge, and diffusion separating comes more difficult. Are other molecule gases by lower ionization energy level by non elastic scattering by so high energy level in where they dissociate, and are ionized so that their chemical bind is off and their charged particles can be separated by diffusion processes. CO₂ containing molecules dissociates. C0₂ molecules have low dissociating energy level and they are usually well dissociated by chamber temperatures over 1000 Fahrenheit (540 Celsius) degrees. So that by ionization of the combustion products occurs C0₂ = C + O₂, and NOx = N₂ + 0₂ at temperatures over 1000 Fahrenheit (540 Celsius) degrees. The temperature might be higher depending on how fast is gases in coming and through flowing through the chamber. Also the temperature might be higher depending on how dissociated atoms and other particles are used after they chemical bind is off.

After ionized molecules chemical bind is off those charged particles may have separated by diffusion processes and that must be done before separated atomic gases and other not yet charged particles are ionized and when this is done well its means curtain temperature in gas mass.

When separated particles are recombined to other non harmful molecules with other ways than they were before ionizing and dissociating. And this recombining can be done for producing energy by this recombining or producing can be done for getting new gaseous materials from separated particles. And recombining can be done, by mixing new gaseous particles together recombined particles, for producing new wanted gaseous or chemical materials.

And this recombining might have been done in continuous processes, by using several chambers which are connected so together by pipes, or holes if chambers are placed side by side.

If there is in same cleaned gas mass several different molecule gases to be ionized so that they chemical bind is off. This can have been done also so that there is several chambers connected together by pipes or if chamber are side by side they can be connected by holes. And holes and pipes can have either + or - charge to separate different charged gases coming in. The gas income in other chamber, can be done also so that gases are separated from others, by placing the out coming gas pipe so that from circulating gas mass by vortex separated gases are taken from place where right kind gases are get to the other chamber. This therefore that different molecule gases have they own different rotation vibration continuums energy level in where they ionization energy is low. And if there is in same cleaned gas mass several different molecule gases to be separated, to make this work well the process needs own chamber in where is going continuous ionization process by needed high level temperatures to ionize and separate inside this chamber circulating molecule gases. This process can be done so many times than needed to clean those gases to less harmful gases. And there is also produced energy by this processes by recombination processes.

By recombination processes positive ion and electron combine and by this there is released the energy amount which is ionization energy's and electron's kinetics energy sum. There is much of this energy because through ionization nozzles in chamber pressed gases, lose much electrons when they are pressed through ionization nozzles. This produces also many negative ions and because higher loose electron amount and bigger negative ion amount there is well high electric flow in chamber and high static electric tension and energy level inside chamber. Those electric tension level and static electric energy level inside chamber circulating gas mass are over kept by continuous gas flow inside chamber through nozzles.

When through nozzles inside chamber coming gas flow mixes with inside chamber circulating gas mass this speeds up and accelerates loose electrons between interaction scattering so that electrons energy level goes on higher energy level. If those electrons don't release they higher energy by scattering those electrons kinetic energy stays on higher energy level and they are much more effective by scattering phenomenon processes. And this happens by this ionization nozzles equip chambers all the time. And this makes this molecule gases ionization and dissociation so easily by this method.

This method pictured here is sheep scaled down method from U.S. Pat. No.

5,541 ,385 and from NO patent applications 20021548, 20021895 and 20024248. By this way used chambers are developed for cleaning by industrial and power plant and by other factories produced harmful gases by sheep ways and more easily controlled ways than by those patent and by those patent applications. By which inside circulating gas mass ionization level is much higher and in where energy is produced by ionizing gases so high energy level in where atomic size is larger so that not only the electrons have larger circulating radius also the atoms nucleus has spread on larger area. This like atom is lighter and releases some of its atomic binding energy by different radiation and by electromagnetic forces.

In those cases there is very high energy level inside chamber circulating gases and they need much more expensive equipment to control and over keep this process. What is happening inside those chamber circulating gases you can see by looking those patent which is all ready public and patent applications when they come public.

There is however one easily controlled method used in those patent and patent applications which we can take to use with this patent application.

And this method is to acceleration ionize normal air gases so high electromagnetic energy level and so fast vibration level in where the air begins to burn by flame. Like seen by pictures No. 1 , 2, 4, 5, 6 and 7. This is done by pressing air gases together burning gases by higher speed over 1000 m/s inside pipe like chamber through ionization nozzles. Inside pipe like chamber radiation can not disappear, and it ionizes air gases to the higher energy level and to faster vibration speed level in where they atomic size also nucleus spreads on larger area and this releases some of those gases atomic binding energy to make higher energy level inside pipe like chamber and this energy can also after testing that its safe so after that this level energy and burning air gases can be directed circulate around inside round chambers and use them to produce more effective interaction processes to clean molecule and other harmful gases.

If there is more money to use for this harmful gases cleaning then it can be made by the way like is pictured by those patent and patent applications. They are capable to produce all kinds charged particles, or those chambers in those patents are equipped with such equipment that they can handle such high electromagnetic energy levels and faster gases vibration levels that most all kind of charged particles can be produced and handled inside those chambers.

There is possible with this ionization nozzles to produce by high speed gas flows most all kind of charged particles which in curtain amount can be used inside among chambers circulating gas mass to ionize and dissociate those gas combinations being cleaned. Therefore the methods to produce charged particles are mentioned here.

PRODUCTION OF CHARGED PARTICLES IN GASES.

PRODUCTION OF NEGATIVE IONS. PRODUCTION ELECTRONS +

POSITIVE IONS Radioactive attachment Chemical and nuclear processes Ion pair production Excited atoms

Associative attachment Thermal ionization

Dissociative attachment Radiation

Positive ion collision

Electron collision

More from used equipment and how different gas particles are separated from each others by description of figs.

IONIZATION

Of the gas combinations and molecule gases must occur CO₂ to dissociate to C + O₂ by temperatures higher than 1000° F = (540° C). And NO x to dissociate to N₂ + O₂ by temperatures higher than 1000° F = (540° C). And similarly all other similar gases and gas combinations and molecule gases.

COOLING SEPARATED IONS AND MOLECULE IONS AND ATOMIC GASES.

Cooling is made by pressing gases through coolers in where temperature is taken to use, or by electric separators to separate cool and heat from each others and pressing after that heat particle gases through coolers in where heat is taken to use.

The ions are also cooled by allowing them combine with same type of gases, and slow their speed and vortex circulation in such level inside pipes were carbon atoms precipitate out of the gases at temperatures below 1000° Fahrenheit ( 540° Celsius) and separating from gases or pressing gases through water scrubber in speed in where carbon atoms stays in water. By this methods begins different type gases separating in chamber in where they are ionized and taken out from different places the chamber depending on they charge and weight. The separating continues in Figs No. 1 incoming pipe No. 70. By vortex made by sideways being gas incoming pipes No. 85 and 86. The separating continues by series three magnets, No. 87, 88 and 89 placed on walls, the amount of magnets varies depending on use. The vortex circulation of the gas flow begins to separate the through passing gases so that heavier particles goes on outer surface of the chamber and lighter particles goes to the center of the chamber. The magnets continue the separating so that through magnetic field flowing gases the heavier particles move to the exterior of the chamber and lighter move to inner section of the chamber.

If there is separated differently charged particles then is used by both magnetic pole energies on different walls to pull those particles away from each others.

When gases flow comes to bigger chamber No. 72 it flows through fourth magnet No. 71 and its magnet field and after that gases are separated in Fig. No. 2. Which is cross-section of Figs 3 chamber. There are multiple chambers in where gases are separated, the gas flows speed and temperature must be in curtain level that separating goes well. By Fig 2 the lightest particles goes in No. 77 center chamber and next lightest particles goes in No. 76 Chamber, and medium light particles goes in No. 75 chamber, and medium particles goes in No. 74 chamber, and medium heavy particles goes in chamber No. 73 and heavy particles goes in chamber no. 72. The separating chamber No. 72 is seen by sideways taken cross-section in Fig No. 3. There is seen separated particles out coming. The chamber temperature is kept in such level that separating continues and chamber doesn't rust. Each chamber discharge has a throttle valve to limit the flow according to the desired particle size and distribution.

SEPARATION THE DISSOCIATED PARTICLES

Ionized particles are passed through magnetic field after beginning cooling spin. The magnetic field will deflect the lighter ions and charged particles toward the inner chamber. Allowing the heavier particles and ions and molecule ions to move to exterior of the chamber. Beside this is used the centrifugal separation

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a side cross section of a pipe through which the gas and particles are coming in;

FIG. 2. Shows cross section of the chamber according to Fig. 3;

F I G. 3 shows a side cross section of chamber no 72 of FIG. 2; , and multiple different collecting chambers no. 72, 73, 74, 75, 76 and 77, for different heavy particles, there is seen the gas incoming chamber no. 70 and the wall magnet no. 71 and the exhaust pipes no. 78, 79, 80, 81 , 82 and 83 and they ventilators no. 84.

FIG. 4 shows from above a cross section from an ionization chamber;

FIG. 5 shows a cross section of the chamber of Fig. 4;

FIG. 6 is a cross section of a different chamber;

F IG. 7 shows an enlarged discharge duct no. 7a of FIG. 4; FIG. 8 shows a cross section from top of an oval chamber;

FIG. 9 is a cross section of the chamber of FIG. 8;

FIG. 10 shows a side view of a multi chamber system;

FIG. 11 shows a cross section of a back wall of FIG. (23) 10;

FIG. 12 shows a side cross section from multi chamber system which has four chambers;

FIG. 13 shows a side view of a multi chamber system which has three inner chambers;

FIG. 14 shows side view of a multi chamber system which has a second inner chamber after the first;

FIG. 15 shows a side view of three chambers;

FIG. 16 shows a cross section of a chamber system, which has four ionization nozzles;

FIG. 17 shows from above a cross-section of the chamber of Fig 16;

FIG. 18 shows from above an inner chamber system different from the one shown in FIG. 16;

FIG. 19 shows a cross section of an inner chamber wall;

FIG. 20 shows a cross section of an inner wall which has ring form + and - high tension voltage surfaces;

FIG. 21 shows a side view of a friction nozzle; FIG. 22 shows a cross section of a friction ionization nozzle;

FIG. 23 shows an inner section of a friction nozzle;

FIG. 24 shows a front section of a round ball formed chamber;

FIG. 25 shows a front section of a chamber like in FIG. 24;

FIG. 26 shows a side view of a round ball formed chamber system;

FIG. 27 shows a front section of an oval formed chamber;

FIG. 28 shows from above a round ball formed chamber system;

FIG. 29 shows a cross section of the jets of FIG. 31 ;

FIG. 30 shows a side view of an adjustable jet;

FIG. 31 shows a side view of the jet of FIG. 29.

FIG. 1 shows a side cross-section of a gas and particles incoming pipe like chamber no. 70. It has three separate magnets no. 87, 88 and 89, and fourth magnet no. 71 in chamber no. 72 wall. There are the gas incoming pipes no. 85 and 86 and they are pressure control valves no. 90 to retain pressure in the ionizing chamber.

FIG. 2 shows a cross-section of the chamber according to Fig. 3. There is seen the multiple collecting chambers no. 72, 73, 74, 75, 76 and 77. There is seen also the wall magnet no. 71 and its electric cords no. 91 and exhaust pipes from each chamber no. 78, 79, 80, 81 , 82 and 83.

F I G. 3 shows aside cross-section of chamber no 72 of FIG. 2, and multiple different collecting chambers no. 72, 73, 74, 75, 76 and 77, for different heavy particles, there is seen the gas incoming chamber no. 70 and the wall magnet no. 71 and the exhaust pipes no. 78, 79, 80, 81 , 82 and 83 and they ventilators no. 84.

FIG. 4 shows from above a cross-section from ionization chamber no. 8 which has also all the equipment to take gases to half ether energy level, but which can be used by lower energy level by particle interactions and scattering processes described in this patent application. The chamber has transparent bulb no. 7b and insulation no. 8a over chamber wall. There is laser no. 1b and side magnets no. 6a and 6b and their cables, there are also magnets no. 35 on walls and ionization nozzles on pipes no. 7a, and exhaust pipes no. 7c and 7d to direct out differently charge gas particles to separate dissociated particles. There are ignition points no. 3a and 3b to ignite the electric arc. The discharge is directed into the duct no. 90 of FIG. 1.

FIG. 5 shows a cross-section of the chamber of Fig. 4 and there is seen the laser no. 1 b and side magnet 6b and wall magnet no 35 and exhaust pipe no. 7d with ventilation and the transparent bulb no 7b.

FIG. 6 shows a cross-section of chamber no. 14 on which other end to no. 7e is coming ionization nozzle This pipe like chamber is for producing half ether energy level gases inside the same and pressing them circulate inside a round chamber.

FIG. 7 shows an enlarged discharge duct no. 7a of FIG. 4 from top cross-section from chamber 14, there is seen the chamber to ionize from through nozzles coming gases to half ether energy level before putting them circulate inside round form chamber. There is seen the chamber inlet no.7e in where comes ionization nozzle.

FIG. 8 shows a cross-section from top of an oval chamber no 8, which has all the needed equipment to ionize gases to half ether energy level. There is laser no. 1b and gases incoming pipes with ionization nozzles no. 7a and 7f, transparent bulb or view port no. 7b and magnets on wall no. 35, and exhaust pipes 7d and 7e and side magnets 6a and 6b and ignition points no. 3a and 3b.

FIG. 9 shows a cross-section of the chamber of FIG. 8. There is seen the laser no. 1 b and chamber wall 8a and gases income jet 7b and exhaust outcome 7f and wall magnets no. 35 and transparent bulb no. 7b and side magnet 6b and ignition point 3b.

FIG. 10 shows a multi chamber system including several chambers over inner chamber and ionization nozzles on the other side. The first chamber is on the middle chamber and in the third chamber there are several nozzles on the same side than in the first chamber. Those several chambers are for producing opposite magnetic vector forces to ionize through passing air and flame gases. This chamber is connected to the gas incoming pipes no. 7a of the chamber of FIG. 4 and to the gas incoming pipes no. 7a and 7f of the chamber 8 of Fig no. 8.

FIG. 11 shows a cross-section of the back wall of FIG. (23) 10. The chamber system and air leading and other similar pipes are to be put ionization nozzles to this chamber wall. The other side of this chamber is connected to the incoming gas pipes no. 7a of the chamber of Fig. No. 4.

FIG. 12 shows a sideways cross-section of a multi chamber system which has four chambers after each other and gas directing wall between each chamber. This multi chamber system is connected to the gas incoming pipes no. 7a and 7f of the chamber 8 of Fig 8 and also to the gas incoming pipes 7a of the chamber of Fig. 4.

FIG. 13 shows a side view of a multi chamber system which has three inner chambers after each other and gas directing wall between each chamber and one chamber over all the inner chambers and all the inner chambers has same gas pressure adjustable pipe on the end the last inner chamber. This chamber is also connected to the gas incoming pipes of the chamber of FIG. no. 4 and of FIG. 8.

FIG. 14 shows a side view of a multi chamber system which has a second inner chamber after the first inner chamber and gas directing wall between chambers and gas ionized holes on it, both inner chambers direct some gas flows in outer chamber in where those ionized gases mixes together. This chamber is also connected to the gas incoming pipes of the ionization chambers of FIG. 4 and on FIG. 8.

FIG. 15 shows a side view of three chambers after each others and having a gas directing wall between each chamber and after gas directing wall there is a pipe inside the next chamber and friction holes are placed into this pipe for having bigger gas pressure and faster gas speed and bigger friction effect by friction holes. This chamber is also connected to the gas incoming pipes of the chambers of FIG. 4 and FIG. 8.

FIG. 16 shows a cross-section of a chamber system, which has four ionization nozzles and an inner chamber into which the ionized gases are coming from pipe and on the inner chamber wall there are many transparent bulbs for radiation ionization of the inner chamber gases. On the inner chamber wall there are, between the transparent bulbs, ionizing surfaces of high tension voltage and extra gas mixture leaders. On the surface of the outer chamber wall there are several pipes for leading gas in and out which can be connected to the pipes for leading gas in or out of the chambers of FIG. 4 and FIG. 8. The friction nozzles can be fastened into those pipes to ionize incoming gases. These chambers have four ionization nozzles and several pipes to direct in ionized gases sideways, and the purpose is by ionization inside among chambers high tension electromagnetic gases by the effect of Kundalin electricity and high tension static electricity ionization to change bigger amount gases, like molecule gases like CO₂ to other less harmful gases, by dissociating them so that atoms separate from the molecules and C0₂ dissociates to C + O₂, which products are not any more harmful.

FIG. 17 shows a longitudinal cross section from the chamber system of FIG. 16.

FIG. 18 shows a longitudinal cross section of an other type of an inner chamber system for the FIG. 16, which has high tension voltage ionizing surfaces on its inner wall and several pipes leading gas mixture in, on the sides.

FIG. 19 shows a cross section of an inner chamber wall which has + and - high tension voltage ionizing surfaces.

FIG. 20 shows a cross section of an inner wall which has ring form + and - high tension voltage surfaces.

FIG. 21 shows a side view of a friction nozzle with a small gas director.

FIG. 22 shows a cross section of a friction ionization nozzle.

FIG. 23 shows an inner section of a friction nozzle.

FIG. 24 shows a front section of a round ball, of achamber no. 8 for continuous air gas mixture ionization. There is a transparent bulb no. 7 and two jets 2a and 2b and in the center there is the laser la electrodes 3a and 3b on both sides and between those jets comes the electric arc which stops the laser b, in on the center point the discharge on side there are those big electromagnets no. 6a and 6b.

FIG. 25 shows a front section of a chamber like FIG. 24 which has one center laser and two scanning lasers 20a and 20b for ionizing the circulating plasma gases inside the chamber circulating gas mass.

FIG. 26 shows a side view of a round ball formed chamber system and there is the transparent bulb 7 and the big side magnet 6b and the electrode 3b and the center laser 1 b and the jet 2b and lasers beam.

FIG. 27 shows a front section of an oval chamber 8. This chamber has bigger inner section for radiation ionization by ionization reflecting back from the wall of the chamber. FIG. 28 shows from above a round ball formed chamber system which has gas circulation from chamber sides back to the nozzles and back in side the chamber through the nozzles. On the pipes in which the gases circulate back the nozzles are turbo and high tension ionizing jets. From each these round form chamber there is leaded gases back to the chamber 70 of FIG 1 to its gas incoming pipes no 85 and 86 and gas is taken from the round chamber 8 from its exhausts pipes 11a and 11 b or from similar pipes. This is made for separation of the dissociated particles, which are dissociated inside those round form chambers 8 in FIG. 8 and in FIG. 4 and inside chamber 8 in FIG. 24, 25, 26, 27 and 28.

FIG. 29 shows a cross section of the jets of FIG. 31 jets, including the main nozzle 2L and the back wall 2K and there 11 are in a ring several nozzles 2M which are not in this cross section, the main fire channel 2a and the ionization nozzles 2P on ring and the nozzles flame holes 2T, fuel pipes 2h and inside the nozzle ring there is fuel pipes 2y to the other nozzles, 2u is the jets frame and 2q is installation.

FIG. 30 shows a side view of a version which is adjustable in the longitudinal direction. The main fire channel is designated with 2a, the frame of a jet is 2U and 2q is installation.

FIG. 31 shows a side view of the same jet which is as a cross section in FIG. 29. There are main nozzles 2L and 2M and on the back wall 2K there are the ionizing equipment 16a, 17a, 18a. Around the jet channel 2a there are nozzles 2R and ending in the channel 2a and fore them there are high tension ionizes around the channel wall and thereafter there are bigger nozzles 2P on ring, they flame hole fuel pipes 2h and fuel pipes inside the nozzle ring 2y and a frame 2U for the jet and the installations 2Q and 8a of the jet are on the wall of the round ball formed chamber 8.

Claims

1. A method ionizing gases to higher energy level by pressing them, by high speed through ionization nozzles to circulate inside chambers, first ionization is contact ionization which takes high speed gases to at once to half ether level, when gases are pressed through ionization nozzles, inside jets flame channel in where ionization continues and ionizes more gases by step by step by different accelerating ionization processes by interactions and by non elastic scattering and by Compton scattering and by other scattering phenomenon to higher energy levels, which continues when charged gases flow to circulate around in much bigger round form ionization and dissociation chamber, in where ionization processes like interactions and scattering phenomenon processes keeps on electric charge level and temperature on level that those molecule gases being cleaned are kept on energy level in where they rotation and vibrating continuum is on level where their ionization energy is low, and they are easily ionized to the level in where the chemical bind is off and molecule gases like CO₂ dissociates to C + 0₂ and NO _x dissociates to N₂ + 0₂ etc.

2. A method according to claim 1 , wherein different interaction scattering phenomenon are temperature inside circulating gas mass kept on such high level by non elastic scattering between electrons and molecules, so that there also exists thermal diffusion and ambi polar ( both pole) diffusion together recombination in where positive ions and electron combine and release energy so that thermal diffusion and ambi polar diffusion and other diffusions are so fast and effective level in where ionization and different dissociation phenomenon are so fast and on such energy level that from molecules separated atoms are not ionized, that's therefore that by thermal diffusion and by ambi polar diffusion and by other diffusion processes dissociated charged particles can be separated away from gas mass by different diffusion processes and by charged particles bulling magnetic forces in exhaust chambers, before also atomic gases begin ionize and coming charged, and diffusion separating comes difficult.

3. A method according to claim 1 or 2, wherein whereby in this method the used energy is taken partly from those through nozzles inside chambers by high speed pressed gases which come ionized to half ether energy level by contact ionization which releases ouch electrons off, when those ionized gases flow inside chamber and mixed with circulating charged chamber gases they direct continuous outside electric field in circulating charged gas mass, this accelerates and speed up big amount those electrons between scattering and this keeps those electrons kinetic energy on high level on where they interaction scattering are effective ionizing molecule gases n level in where the chemical bind is off and they dissociate, and this happens very effectively because this is made so that by dissociation released energy is from the dissociated particles and then it is the same energy which also binds particles together, it is the right form energy by right vibration level and speed, which helps much to ionize molecule gases like other gases too, when there is be cleaned other harmful particles, which need higher ionization level to dissociate, its is made by higher electric and electromagnetic and static electric tension levels, by higher gas speeds through nozzles and higher gas pressure inside chamber, and the electric and electromagnetic and radiation energy produced is used to further acceleration ionization to taken used gases to higher energy level and to higher and faster vibration level, and its works well because energy is taken from material it self.

4. A method according to any of preceding claims wherein the ionization and de ionization processes are kept on balance by ionized gas incoming in chamber and by dissociated gases out taking from chamber and by gas pressure and by electric charge and electromagnetic charge level in circulating gas mass, and by the amount of half ether level gases pressed through ionization nozzles in chamber, and this is controlled by through nozzles pressed gas flows speed, lower speed less half ether level gases, much half ether level gases inside chamber causes air gases to bum and this makes faster ionization, different ionization processes are kept on going by right energy level, like electron consent ration and recombination by which are also produced less harmful molecule gases and materials, like is made by negative ion forming which makes faster electric flows inside circulating gas mass and by ion pair production the ionization grows and by radiative, associative and dissociative attachment there are formed more charged particles like by chemical and nuclear processes and by thermal ionization, radiation, positive ion collision and electron collision, and by clustering by which is collected away harmful materials from gases, diffusion processes like thermal diffusion and ambi polar diffusion are used to separate harmful charged particles away from gases and but them through ionization nozzles to circulate to other chamber in where they by similar processes is produced specially to those material to make them less harmful materials, and this is done so many times than there are different molecule in gases which needs handling, this therefore that different molecule gases have they own rotation vibration continuums energy level in where they ionization energy is low, and they mighty need they own chamber to clean them, after separating particle gases can be recombined for less harmful form or other use, and this is done by separating dissociated particles and recombining them by mixing them together other recombined materials and gases by right temperature and by right energy and vibration speed, by recombination processes positive ion and electron combine and by this there is released the energy amount which is ionization's energy's and electron's kinetic energy sum, there is much of that energy because through ionization nozzles in chamber pressed gases lose much electrons, when they are pressed through ionization nozzles, this produces also negative ions and because high electron amount and high negative ion amount there is well high electric flow in chamber circulate gas mass and high static electric tension and high electromagnetic energy level inside chamber to make possible to ionize end dissociate most gas combinations, and if there is more power to needed then is whole inside chamber circulating gas mass energy level taken to half ether level in where there is all atomic particles atomic size spread on bigger area releasing some of they atomic binding energy and there are ionized and dissociated all kind of gases.

5. A method according to any of the preceding claims, wherein an atom which is part of a molecule is ionized breaking the chemical bind of the molecule and dissociating the molecule and whereby the formed particles possibly take part in interaction processes producing new ions.

6. A method according to any preceding claims wherein the generated gases are acceleration ionized by pressing them through ionization nozzles by high speed to make molecule gases to such high infrared rotation and vibration ionization energy level in where molecule gases have rotation and vibration continuum and they have low beginning energy to non elastic ionization to the energy and vibration level in where they dissociate so that the chemical bind which keeps molecule together is broken and the molecule dissociates.

7. A method according to any preceding claims wherein the temperature of the glowing gas mass rotating inside the chamber is kept also in such level what is needed to over keep inside circulating molecule gases rotation and vibrating continuum on level, in where their ionization energy level is low so that by non elastic scattering and by Compton scattering and other scattering phenomenon ionizes CO₂ molecules so that they dissociate.

8. A method according to any preceding claims wherein the temperature inside the circulating gas mass is also kept in so high level, in where they also have thermal diffusion and or ambi polar ( both pole) diffusion on so effective level in where ionization and dissociation phenomenon are so fast that the atoms separated from the molecules are not ionized.

9. A method according to any preceding claims wherein the charged particles that have been dissociated by thermal diffusion and ambi polar diffusion are separated away from gas mass by different diffusion processes before also atomic gases begin ionize and coming charge, and diffusion separating comes more difficult.

10. A method according to any preceding claims wherein C0₂ and/or NO_x containing molecules are treated to dissociate in the chamber temperatures over 1000° Fahrenheit (540° Celsius) degrees so that the gases will degrade to CO₂ = C + O₂, and NOx = N₂ + 0₂ .

11. A method according to any preceding claims wherein separated particles are recombined to other non harmful molecules in other ways than they were before ionizing and dissociating for producing energy by this recombining or for getting new gaseous materials from separated particles and/or new gaseous particles can be mixed together with the recombined particles for producing new wanted gaseous or chemical materials.

12. A method according to any preceding claims wherein the gas consists of several different molecule gases, ionization is effected by leading each of the different gases through their own ionization chamber, the chambers being connected together by pipes or holes having eventually different charges.

13. A method according to any preceding claims wherein, due to the fact that different molecule gases have they own different rotation vibration continuums energy level in where their ionization energy is low, several different molecule gases are separated from each other, each molecule gas is treated in its own chamber, where the gas is continuously ionized in the suitable high level temperature to ionize and separate the molecule gases circulating inside this chamber, the process being, when needed, repeatable.

14. A method according to any preceding claims wherein air gases are pressed together with burning gases by a speed over 1000 m/s inside a pipe like chamber through ionization nozzles, whereby the gases are ionized to a higher energy level and to a faster vibration speed level, where their atomic size and nucleus spread on larger area releasing some of the atomic binding energy of the gases to raise the energy level inside the pipe like chamber, burning air gases are directed to circulate around the round chambers and use them to produce more effective interaction processes to clean molecule and other harmful gases.

15. A method according to any preceding claims wherein the gases are cooled by pressing gases through coolers in where temperature is taken to use, or by electric separators to separate cool and heat from each others and pressing after that heat particle gases through coolers in where heat is taken to use.

16. A method for converting unwanted and harmful molecular form gases, like carbon dioxide and oxides of nitrogen into a less harmful or completely harmless form, which method consists of steps of;

- forming a rotating gas plasma in a reactor;

- ionizing the gases to be treated in an ionizing apparatus, - feeding the gases to be treated to the reactor for ionizing to a level where the molecular gases, like CO₂ and No_x are separated into atomic materials, like C, 0₂ and N₂, and

- when applicable, separating the different material flows from each other.

17. A method according to claim 16, wherein the gas to be treated is fed between the rotating gas plasma ball halves of opposite charges on opposite sides of the reactor.

18. Equipment for treating and separating unwanted and harmful molecular form gases, like carbon dioxide and oxides of nitrogen into a less harmful or completely harmless form consisting of, in addition to a gas plasma ball,

- chambers having magnets to have effect on the atomic materials while they are rotating in the chambers and

- inside each other located collecting tubes for receiving gases sorted in respect of their weight and/or charge and for discharging pure atomic materials from the equipment.

19. Equipment according to claim 18, including throttling means for restricting the gas flow and/or the pressure of the same in at least some of the channels for the incoming and outgoing gas flow.