Nuclear fusion reactor with one reactor chamber

Abstract

The invention is a fusion reactor. It consists of a fusion chamber containing two fluid accelerators. The fluid accelerators are designed to produce a fusion-capable, incompressible liquid in the form of very small microdroplets, which are generated in pairs and collide with each other at a collision point. The microdroplets are sent towards each other at a collision point at approximately 50-100 km / s. Due to the very high speed of the microdroplets, nuclear fusion occurs at the collision point, releasing energy that accelerates the components of the microdroplet in all directions and also impacts the following microdroplets, leading to additional nuclear fusion reactions there. The molecules / atoms of the liquid are additionally aligned by electric fields directly at the collision point, optimally aligning them for nuclear fusion of the deuterium atoms.An electromagnetic coil focuses the structure and shape of the electrically charged micro-droplets more closely together at the meeting point, thus increasing the number of atoms that fuse together.

Description

The invention is a nuclear fusion reactor designed for almost any energy output power. Above all, it is also optimally suitable for medium to low powers and thus for mobile purposes, in particular vehicles, as primary energy source.Nuclear reactors used for the power supply operate exclusively on the fission principle. In nuclear fission, heavy radioactive elements are split into lighter elements, thereby releasing energy which is converted to electrical current by means of energy converters, e.g., steam turbines. Unfortunately, in nuclear fission, not all of the potential of the radioactive material is used efficiently to generate current. Radioactive residues remain, which entail further problems. This radioactive residue (radioactive waste) must be safely stored because it emits dangerous radiation by itself. Unfortunately, quite much of it remains in the nuclear reactor, making disposal more complicated. This also shows how poor the efficiency of a nuclear reactor is. If all of the material were almost completely "burnt", such a reactor would still supply at least 90% more energy. The efficiency of the nuclear reactors is about 20%. While it is often stated that the efficiency is about 30-35%, unfortunately this is not true. However, this is hardly important because the nuclear "fuels" also deliver very much energy in this way. The radioactive waste presents a great environmental risk. However, the radioactive waste can still be used as a primary energy supplier by a special design of a novel reactor and can thus recover a part of the other missing 90%. After this, a smaller amount remained which would be radioactive, but still if one were to consider that they were radioactive residues which would otherwise have to be stored in a complicated manner.Research has been carried out in the field of fusion technology for several decades. Although great advances have been made, there has been no breakthrough in the laying of the energy balance in the positive range.As in numerous core processes found by particle accelerators and nuclear explosives, there is no doubt that the matter is energy. The description of the photon dual property of the photon is accepted by many researchers today. The theory implies that the photon is corpuscular and wave at the same time. As soon as the photon hits material (and the material consists of entangled photons, of course), it can also be caught in the entanglement and thereby enlarge the chunk extremely little, but nevertheless somewhat (photon absorption). However, it can also spin out another photon (photon emission).In each type of material itself, much, enormous energy is inserted. Whether sand, rocks, wood, water, metal, air, soil, each of these materials contains extremely high energy. However, this does not mean (only) the chemical energy. Actually, all the matter is energy. Matter is a very stable form of the extremely highly concentrated energy. The energy in the form of photons that are strongly concentrated can form stable structures and keep the photons trapped there. If these structures are destroyed, the energy is released in photon form. There are numerous ways of relieving energy of the matter or of starting these transformations. The most common and simplest methods are chemical in nature. In such processes, combustible matter will simply enter into chemical reaction and build up or dissolve new chemical compounds. The widely used method of releasing energy is, for example, to combine the material with oxygen or to oxidize / combust it. However, this supplies only a very small proportion of the energy which would actually be available, on the other hand the initial energy for starting the process is relatively low. Moreover, this method only relates to combustible substances which form a fraction of the total matter present, for example, on the surface of the earth.Instead, energy can be obtained or released by nuclear reactions. The nuclear energy recovery methods available to us are nuclear fission and nuclear fusion. There is a third option for annihilation, which, however, is very difficult to implement because it presupposes antimatèism, which does not occur in our own nature and can be produced artificially only with extremely high energy expenditure. In the collision between an atomic group of antimaté and analogous matter, both atomic groups are completely converted into energy and radiated away from the point of collision with speed of light in photon state in all directions.Initiating core splitting is nowadays relatively easily feasible in technical terms. It is implemented in commercial core reactors and used for broad power supply. Radioactive elements are enriched until they are suitable for optimum nuclear reaction. The radioactive material is introduced in the form of elongated rods into a reactor filled with heavy water. Because the core fiber would lead to an atomic explosion in an uncontrolled manner, cadmium grids or rods (or boric acid dissolved in the heavy water) are placed between the cleavable radioactive material. The cadmium or graphite lattice or rods determine the power of the energy release or the rate at which the fission proceeds. The higher or lower the energy release, the depth to which they are introduced between the uranium (or plutonium) rods. Each time an atom is cleaved, it releases a neutron which in turn destabilizes one of the atoms in the vicinity by penetrating into its core. The cadmium rods are capable of absorbing free neutrons and thus control the fission processes quite well. Nuclear reactors with graphite as moderator are no longer used because they are not as easy to control. If the cooling fails in the reactor, a core melt can very quickly come about. In the case of a rumen, the rise in core reaction and thus also the temperature can take place in a lightning manner and quickly become out of control. It may increase by thousand times within one millisecond, which may lead to a violent explosion and thus to contamination of the environment.Unfortunately, during nuclear fission reactions, the radioactive "fuel" is not completely cleaved. Thus, radioactive residues still remain radiating hundreds, thousands or a few even millions of years. If one completely cleaved the radioactive material, the efficiency of a nuclear reactor would be significantly higher and less radioactive waste would remain. However, the construction of the nuclear reactors can be varied to minimize waste products. Alternatively, one can build new, special reactors which use the radioactive waste product of a conventional reactor and continue to produce power therefrom. A completely different construction and specific alloys as neutron exciters with a resonator unit can further make the use of conventional radioactive fuels useful. The performance of such a special extra reactor which uses only the radioactive wastes for power generation would be almost the same as that of the conventional reactor which generates the radioactive waste product! However, a detailed description of such a particular reactor is not the subject of this invention herein.A better efficiency in pointo energy yield would actually have to be achieved by the fusion reactors. Generally known and already present fusion reactors are built into various designs. Toroidal reactors and Tokamak machines are relatively known, for example. Unfortunately, however, such reactors have been still in the experimental phase for decades or are used as research reactors and, according to experts, are always constantly about "30 years" removed before commercial use, no matter how far one proposes in the direction.While in a hydrogen bomb nuclear fusion works smoothly, the continuous, controlled yield of energy in nuclear fusion reactors presents many problems, the solution of which makes the process very expensive and thus still unattractive to the industry. The fusion reactors require a great deal of starting energy, which must be provided for the first time. In addition, present reactors cannot then run permanently or the processes come to a standstill there rather quickly and the energy yield is thus relatively low. By investating some MW energy in the startup phase and then running the process for only a few seconds or, at best, a few minutes, with only fractions of the invested energy recovered, this is not a commercially interesting efficiency achieved thereby. For such purposes, the reactor must be capable of delivering energy permanently and not be in active operation for only a few minutes or only seconds every few idle hours or even days. Present-day fusion reactors usually unfortunately have a negative energy balance: more energy is injected in a clean manner than is obtained by the process. It is similar to a car with an internal combustion engine that requires the electric starter every few dozen seconds to start the engine for a few seconds. The car battery would then be quickly empty because the work of the internal combustion engine would not be sufficient to recharge it via the alternator.Nuclear fusion is an energy-supplying process which has been in the sun and in stars for billion years. The fusion process takes place at extremely high temperatures at which the material is in the fourth aggregate state, the so-called plasma. A plasma consists of atomic nuclei (ions) and electrons which are no longer bound to each other.Fusion reactions take place at about 15 million degrees inside the sun. Under the boundary conditions on the earth, the plasma is confined by strong magnetic fields at temperatures above 100 million degrees and at extremely low density (about 250,000 times thinner than the earth's atmosphere). What the earth attempts to achieve the magnetic fields is not necessary on the stars. There, the plasma is very strongly compressed by the large star mass that is not present or by gravitational forces acting on this mass. The highly heated plasma causing the fusion is mainly located in a sheath, depending on the size of the star, more or less near the core of the star. The fusion does not take place in the core of the star, as previously assumed, but in a sheathing which is located between the core and the surface. If fusion were to take place only in the nucleus, then all the stars would be similarly large and there would be no very large or small stars. Each star has its nuclear fusion cladding at a different distance from the star center. The sheathing arises where there is the balance between pressure and temperature that is necessary for the hydrogen fusion. Further sheathings, which are arranged concentrically deeper, fuse other materials and elements. In the core of the star, the pressure is so high that the material is very strongly compacted, wherein the atomic structure integrity is also no longer ensured. The neutrons that are to maintain the fusion in progress are decelerated much too quickly and bound prematurely to heavy atomic structures. The situation is different in the star shell layer which is more or less remote from the core. The distance from the star core is determined by the size and mass of the star. In any event, the fusion shell of a star is very hot and relatively thin, which also ensures very long "burning". The fusion shell does not always remain of the same size. It changes its size and shape with the aging process of the star, and may become unstable. It also plays a major role in Supernova explosion. First, if the star becomes unstable, this jacket will break itself and the layers above it will break. Because the jacket also spreads inwardly during the explosion, it compresses the material of the star in the direction of the core. Therefore, after a Supernova explosion, much smaller remains from the star. Firstly, the material is broken away over the jacket and secondly the material beneath it is largely compressed by the increase in pressure.As for the fusion, on the earth, the situation looks different. Here, engineers and researchers are attempting to melt the light cores (preferably hydrogen isotopes) by strongly heating and confinement of the magnetic field. A number of fusion reactions between light cores are conceivable. In the first generation of future fusion power reactors, the deuterium-tritium reaction will be used, which offers a comparatively high fusion power density: the nucleus of the heavy hydrogen deuterium (one proton, one neutron) fused with the nucleus of the supergravity hydrogen tritium (one proton, two neutrons) to the helium-4 nucleus, the so-called particle (two protons, two neutrons) with emission of a neutron. In this process, about four times as much energy per nucleon is released as in the cleavage of a uranium nucleus. 80% of this energy is bound to the neutron, which can freely leave the magnetic cage as neutral particle. Braking down the neutrons in the structural material and in the cladding of the plasma chamber, the so-called blanket, produces heat which is converted into electricity via a conventional steam circuit. The particle transfers kinetic energy by interaction with plasma particles and thus contributes to heating up the plasma. Under certain physical conditions, this heating alone is sufficient to maintain the plasma at operating temperature. This operating state is called "ignition".There are numerous methods that are promising to level the pathway for nuclear fusion and its commercial utility. Some publications which are available for generality are described or entered here:The IEC (Inertial Electrostatic Confinement Pressure) method summarizes the highly-modern development of electrostatic confinement inertial engines (IEC), which is divided into two parallel development lines: the IEC plasma source and the corresponding electromagnetic nozzle (EMN). Both lines of development begin with the establishment of theory and modeling and develop further for design implementation and experimental verification.The IEC discharge model illuminates a new perspective on the IEC discharge physics and the effects of the respective critical parameters that determine the design of the IEC plasma source. Experimental verification of theory is demonstrated by optical emission spectroscopy and the collision radiation model. The results provide conclusive evidence for the formation of a spherical bilayer within the IEC plasma source, which is the key to establishing the IEC discharge theory proposed in this work. This work constitutes a comprehensive study on the magnetohydrodynamic theory for assessing the plasma acceleration in the magnet nozzle. Nevertheless, the result shows a limitation in performance of the magnet nozzle. An innovative invention is proposed to overcome the limitation known as EMN. Detailed descriptions of EMN and its functional principle are summarized in this work, including its effects on plasma confinement, acceleration, and detachment. Testing of plasma plume characteristics with various plasma diagnostic tools further demonstrates EMN functionality and represents the first ECT prototype for which a proof-of-concept exists in the literature.Another nuclear fusion method is based on electrostatic inertial confinement. Electrostatic confinement (IEC) refers to methods that attempt to generate a high density, high ion energy plasma alone or primarily with the aid of an electric field. IEC assemblies are built with the aim of achieving fusion reactions between atomic nuclei of hydrogen isotopes (deuterium or deuterium and tritium). The apparatuses are also called Farnsworth-Hirsch-Fusor or Hirsch-Meeks-Fusor according to their developers. The polywell array is also a related concept. Because such devices release neutrons in the hydrogen fusion reactions, the electrostatic inertial confinement can be used as a basis for a neutron source. Unfortunately, the concept is not suitable for generating energy because of a negative energy balance. The concept of electrostatic inertial confinement for achieving nuclear fusion is based on deuterium and / or tritium ions being held in a small spatial range by an electric field and being bombarded from the outside with further, energy-rich ions of the same type(s). Thus, unlike nuclear fusion reactors with magnetic confinement, the energy at impact is not given by the temperature of the plasma, but higher ion energies can be used (by means of high acceleration voltages). This makes the coulomb barrier easier to overcome at the impact, so that the probability of the fusion reaction at the impact increases. Because the identically charged ions tend to scatter behavior, the frequency of the fusion reactions, which would be sufficient for net energy generation, is relatively low and thus a positive energy balance cannot be achieved with this method.Early work on this technique was done by Philo Farnsworth on television tube observations. The original designs in the early 1960s were based on cylindrical arrays of electrodes. The fuel for nuclear fusion, i.e. deuterium, was accelerated from ion sources in the direction of the inner reaction zone; here, ions of the fuel should be held by electrostatic forces. Farnsworth for this purpose predicted the term inertial electrostatic confinement (german: "electrostatic inertial confinement"). However, this technique has nothing to do with the inertial confinement in terms of inertial fusion.Further developments were made by Robert L. Hirsch. In the late 1960s, he built a large apparatus with six ion sources and a high voltage supply of up to 150 kV. With this apparatus, nearly 108fusion events per second were achieved with deuterium. Additionally, Hirsch proposed a design without an ion gun. A high voltage is applied between two concentric spherical electrode grids located in a larger container filled with deuterium under low pressure. The glow discharge igniting by the high voltage generates the desired deuterium ions by electron impact. In the early 1980's, it was possible to demonstrate in various experiments that in such an arrangement a potential minimum is formed within the inner, spherical grid electrode. However, no increased ion density at this potential was observed by closer investigations. Fusion in the laboratory is possible with moderate temporal and financial expenditure! The simplicity behind it is shown by the fusor devices. For fusion, heavy hydrogen is required, which must first be ionized with sufficient high voltage. This is done by glow discharge at the electrodes. Electron blasts break the hydrogen molecule into two individual atoms, after which the electron is separated from the body. The bare hydrogen nuclei remain, which are called deuterons in the case of heavy hydrogen. By sufficient energy, two deuterons can overcome their mutual repulsion and come so close that the strong interaction takes effect. The two deuterons fuse and emit the energy which is thereby produced in the form of neutrons. The reaction with the largest effective cross section has the deuterium-tritium reaction, but it is not the dominant reaction in the fusor, since only deuterium is used primarily as working gas (4He=He-4): D+T ->4He+1n+17,588MeVThe actual reaction which already starts at about 15 keV is the deuterium-deuterium reaction. It can proceed in two ways: D + D -> 3He + 1n + 3.268MeV D + D -> 3H + 1p + 4.03MeVIn a fusor, hazardous tritium is also additionally produced, but only in very small quantities. In addition, it reacts immediately via the D-T reaction to helium-4, producing very high-energy neutrons. Calculations predict that the boron densities and ion beam parameters achieved in the experiment would have to result in a fusion rate of around 100 billions per second when firing all three high energy emitters simultaneously. The fusion rate in the proton-proton reaction is proportional to the 4th power of the temperature. Thus, an increase in temperature by 5% causes an increase in the release of energy of 22%.A deuterium and a tritium atomic nucleus fuse to a helium nucleus to release a fast neutron. In nuclear fusion, atomic nuclei fuse to a new nucleus. Many nuclear reactions of this type release energy. Thus, the energy radiated by the sun also originates from nuclear fusion processes. In order for the fusion reaction to occur between two atomic nuclei, they must come very close to each other, to about 2.5 Femtometers. This is opposed by the Coulomb force (electrical repulsion), which has to be overcome with great energy expenditure (e.g. high temperature). The fusion reactions suitable for industrial energy generation are well known from investigations using particle accelerators. However, accelerator experiments use much more energy for the overall operation of the apparatus than the reaction then releases because the accompanying elements and the equipment consume too much energy. The electromagnets, their control and the cooling devices therefor are proper current reducers. Above all, the working and energy efficiency is not at all given thereby. A giant electromagnet with a mass of more than 12,000 kg, fully energized and having built up its maximum magnetic field, consumes almost the same amount of energy, regardless of whether it accelerates a group of only 4 or a group of two billions of ions simultaneously. A net energy gain, i.e. the operation of a power plant, is not possible in this way.In order that a nuclear fusion corresponding to the Eeinstein formula E=mc 2 can convert material into energy, the mass of the two fusing nuclei together must be greater than the mass of the nuclei and particles formed. This mass difference is converted into energy. The mass difference is particularly large if helium-4 forms from isotopes of hydrogen. In these, the electrical repulsion to be overcome before the fusion is also the smallest, because they each carry only a single elemental charge. A mixture of equal proportions of deuterium (D) and tritium (T) is therefore provided as the fusion fuel:Another method of releasing energy from nuclear fusion is fusion with magnetic plasma confinement. The most prospective concepts for fusion reactors heretofore provide for a deuterium-tritium plasma to be enclosed in an annular magnetic field and heated to a sufficient temperature. In order to achieve a net energy gain in this way, the plasma volume must be sufficiently large. To start the process, the well evacuated reaction vessel many cubic metres is charged with a few grams of deuterium-tritium (1:1) gas mixture. The gas density then corresponds to a fine to high vacuum. The gas is brought into the plasma state by heating and further heated. After reaching the target temperature-in the innermost region of the plasma around 150 million Kelvin-the plasma exerts a pressure of only a few bar. Against this pressure, the magnetic field must hold the particles together. Contact with the vessel wall must be prevented, since otherwise the plasma would cool immediately.Fusion reactions take place at a temperature of about 150 million Kelvin and a particle density of about 10 2° / m 3. The energy released thereby distributes itself as kinetic energy in a ratio of 1:4 to the alpha particles formed (He-4 nuclei) and free neutrons (source: https: / / pure.mpg.de / rest / items / item_2482728 / component / file_2482739 / content). The energy of the alpha particles is further dissipated by shocks in the plasma and contributes to its further heating. At a sufficient core reaction rate (number of reactions per time interval), this energy may be sufficient to maintain the plasma temperature without further external heating: the plasma then has "ignited" and "burns" by itself. This occurs if, at a given temperature, the triple product of the particle density, temperature and a time constant determined by the unavoidable heat losses, the energy confinement time, exceeds a certain minimum value according to the Lawson criterion.For an energy-supplying reactor, however, this point does not have to be reached. Even at somewhat lower temperatures and with constant additional heating, sufficient fusion reactions take place (so-called fusion with net energy gain without reaching the Lawson criterion). The additional heating even offers a justified possibility (in addition to the fuel replenishment) of controlling the reaction rate, i.e. the reactor output. The plasma state reached must be maintained permanently by replenishing new fuel corresponding to the consumption and discharging the helium produced-the result of the fusion, the "ash". The released neutrons leave the plasma; their momentum, four fifths of the fusion energy, is available for use.An energy gain has been achieved only very briefly in experiments on JET and TFTR (Princeton, USA), but not yet in the many other experiments, since the plasma vessels of the existing test installations are too small for this purpose, as a result of which the plasma cools down too much. In the Tokamak ITER, which is therefore larger, a permanently "burning" fusion is to be realized with a permanent additional heating. Even later installations such as DEMO are likely to be designed more so that a weak additional heating of, for example, a few percent of the fusion power remains necessary in order to retain an additional possibility for control.By increasing density and temperature, the performance produced by fusion reactions increases. However, it is not possible to swing to excessively high temperatures, since the energy loss of the plasma due to transport processes also increases with temperature.Various methods have been developed for heating the plasma to above 100 million Kelvin. All particles in the plasma move at very high speed according to the respective temperature (deuterium nuclei at 100 million Kelvin have an average speed of approximately 1000 km / s). The heating power increases the temperature and compensates for the losses due mainly to turbulent and neoclassic transport (caused by collisions of the particles with one another) and also due to bremsstrahlung. One possibility for heating up the plasma is electrical heating: the plasma is an electrical conductor and can be heated by means of an induced electrical current. In this case, the plasma becomes a secondary coil of a transformer. However, the conductivity of the plasma increases with increasing temperature, so that the electrical resistance, starting from about 20-30 million Kelvin or 2 keV, is no longer sufficient to heat the plasma more strongly. In the Tokamak reactors, the current through the central solenoid is continuously increased for electrical heating.In many reactors, microwaves are used to excite the ions and electrons in the plasma at their resonant frequencies and thus transfer energy into the plasma. These methods of heating are called Ion Cyclotron Resonance Heating (ICRH), Electron Cyclotron Resonance Heating (ECRH) and Lower Hybrid Resonance Heating (LHRH).Heating of the plasma can also be achieved by neutral particle injection. When injecting fast neutral atoms into the plasma (neutral beam injection, NBl), the kinetic energy of these atoms, which are immediately ionized in the plasma, is transferred to the plasma by collisions, as a result of which the plasma heats up.Another plasma heating method is magnetic compression. The plasma can be heated like a gas by rapid (adiabatic) compression. An additional advantage of this method is that the plasma density is increased at the same time. Magnetic fields generated by only variable current solenoids are suitable for pressurizing the plasma together. The magnetic field must hold the plasma together against its pressure so that it does not contact the vessel wall, because otherwise the fusion processes are abruptly interrupted. Both concepts for magnetic confinement, tokamak and stellarator, use a toroidal, twisted magnetic field for this purpose. Tokamaks produce the twisting of the field by inducing an electric current in the plasma, stellarators do this by a special, complicated shaping of their magnet coils.The magnetic field is generated with large coils. Their shape and arrangement determine the shape of the plasma; the current intensity in the coils determines the strength of the magnetic field and thus the possible size of the plasma, the particle density and the pressure. In a reactor (or in experiments where the plasma is confined for longer) the coils must be superconducting: the current flowing in normally conducting coils produces heat due to the electrical resistance to be overcome. Such coils could no longer be effectively cooled over a longer operating period, whereby the temperature would rise and the coil would be destroyed. Superconducting coils, on the other hand, do not have a resistance and therefore the current does not produce any heat in them which has to be dissipated.Tokamak is the most advanced concept followed internationally with ITER. However, at least in its original operating mode with a purely inductively generated plasma current, it has the disadvantage that the operation is not possible continuously, but only in pulses, that is to say with regular short interruptions.Deuterium and / or tritium is used as fuel for the fusion reactors. Single reactors also use boron isotopes for this purpose. While deuterium is present in the water of the earth in just unexpillable amounts (2.5·1013 t), tritium can be produced in the amounts required for a fusion reactor practically only by "incubations" of lithium-6 in the plant itself.The irdic occurrence of lithium is estimated to be more than 29 million tons. Only the isotope 6Li occurring with a natural fraction of 7.5% serves for tritium breeding. From this proportional supply of about 2 million t of lithium-6, according to the above formula, theoretically about 1 million t of tritium can be obtained. In practice, enriched lithium with a lithium-6 content of 30-60% is to be used. The technically usable lithium occurrence is therefore computationally sufficient to cover the energy requirement of mankind for thousands of years.A shortage due to the lithium requirement of other industries is counteracted by the isotope composition not being relevant for them and thus remaining available for them over 90% of the lithium. Even in a scenario with a greatly increasing lithium demand by massive expansion of the electromobility, only the lithium resources which can be depleted at present lithium prices and technologies are exhausted up to 2050.Tritium is radioactive, with a half-life of 12.32 years. However, it emits only beta radiation with low maximum energy and without accompanying gamma radiation. In the radioactivity inventory of a fusion reactor which has been in operation for some time, tritium will only be a relatively small contribution. The tritium necessary to start fusion reactors could be readily recovered in conventional fission reactors. In particular, tritium is produced as a by-product in heavy water reactors in an amount of about 1 kg per 5 GWa of electrical energy generated. For continuous operation of fusion power plants, however, these only sources available up to now would by far not supply enough tritium, which results in the need to herb tritium in the reactor. A fusion power plant with 1 GW electrical power would require approximately 225 kg tritium annually.The largest plants today worldwide according to the Tokamak principle are the joint eruopean torus (JET) in Culham / Great Britain and ITER (International Thermonuclear Experimental Reactor) in France, which has been built since 2007 and is completed approximately May 2035. The general aim is the experimental confirmation of the theory of nuclear fusion and the feasibility of generating energy from the fusion reaction. JET has been in operation since 1983 and is today capable of producing a power of 17 MW for a short time, which corresponds to about 70% of the power applied for heating the plasma. Unfortunately, it does not provide a positive energy balance.Parallel to the tokamak, which releases energy in long pulses, the "stellarator" line is developed further, which enables continuous plasma operation. Under the guidance of the Max-Plank Institution for plasma physics, the Stellarator plant Kendelstein 7X was set up in Griffswald. This system has a very complicated electromagnet arrangement and field geometry. However, it is promising and experimental operation shows that it is functioning. Some success messages have been published.The nuclear fusion is based on a reaction between two hydrogen isotopes, e.g. deuterium and tritium: 2H+3H=4He2+n. In this reaction, energy is released from Albert Einstein according to the law for the mass defect. To start the fusion of the hydrogen cores into helium cores, the hydrogen gas will be heated to a temperature above 100 million degrees Celsius (200 million degrees have already been reached). For comparison: the sun has a temperature of 5500 DEG C. on its surface and about 15,000,000 DEG C. in its interior, a so-called plasma, a mixture of free hydrogen ions and free electrons, is thereby produced.In a fusion reactor, plasmas are used in very small amounts, which consist of only 1 g of hydrogen ions. The thermal energy of the hot 1g hydrogen plasma is sufficient to heat and melt 100 kg of steel to 2000°C.In order to be able to operate at these high temperatures, the plasmas and their thermal radiation are captured in vacuum with magnetic fields whose strength exceeds 100,000 times the earth's magnetic field. The extremely high temperature is necessary to compensate for the very low ion density (about 10 high 14 ions / cm 3).In most techniques, energetic neutrons occur. Since they cannot be forced by magnets onto a defined path, they strike the material surrounding the plasma and are responsible for its radiation. However, they are used to produce the tritium most frequently required with lithium.In principle, a distinction can be made between some techniques of nuclear fusion: induced inertial fusion, fusion with magnetic inclusion, cold nuclear fusion, lattice-inclusion fusion, projectile fusion and fusion from particle accelerator technology.The method of creating the magnetic confinement fusion is used in many fusion reactors and is carried out in closed vacuum chambers. The gas, consisting of hydrogen, deuterium or tritium or combinations of these substances, is heated in this chamber to 50 to 400 million degrees and is then present as a plasma, i.e. the gas is completely ionized. Magnetic fields force the plasma onto a path that prevents the plasma from contacting the wall. Contact would cool the plasma momentarily and fusion would be interrupted. At high temperature, the thermonuclear firing finally occurs.Generally, magnetic confinement has the following problems: The difficulties of plasma confinement and impurities cause energy losses. Neutron bombardment causes the reactor material to become radioactive. The extreme conditions lead to high material fatigue and thus to high costs. Large amounts of energy stored in the magnetic fields and radioactive inventory represent a potential hazard. The high energy requirement during operation due to the required heating and magnets (about 300 MW, which corresponds to the consumption of a medium city) does not justifies repetitions of such tests.In the case of magnetic confinement, it is also necessary to distinguish at least three reactor types: actuators, tokamak and mirror machines.actuatorsHere, the reactor vessel is, similar to the Tokamak, an annular tube, i.e. a torus. The plasma flows in a circle here, wherein it is twisted by suitable magnetic fields in itself in order to minimize radiation losses. These additional magnetic fields complicate the technique of the reactor. Nor is the desired degree of inclusion achieved at present, which corresponds to the product from pressure times time. However, the actuator is very interesting for the construction of an energy-supplying reactor because it is suitable for continuous operation.- TokamakTokamak is an abbreviation for the Russian designation of toroidal chamber in the magnetic field. Tokamak is a torus in which the plasma flows in a circle. A current is induced in the plasma via external coils, similar to a transformer. This current minimizes the radiation losses, so that no magnetic field is necessary for twisting the plasma. In addition, the current in the plasma is a heating method. The conditions for self-sustaining thermonuclear burning have been closest to the tokamaks up to now, but this is perhaps also due to the fact that the most intensive research is being carried out here. The main disadvantage of tokamak is that it is not suitable for continuous operation, but must regularly be recharged again with plasma, which also makes an extreme load on the plant.mirror machinesThe reactor vessel forms a straight tube. At the ends, the plasma is reflected by corresponding magnetic fields in its direction of flow. Reflection at the end results in increased energy losses.However, there are also numerous other techniques for operating core fusion.MIGMA conceptIn the MIGMA method, particles (e.g., deuterons and trions) are repeatedly collided and fused from a particle accelerator. With this concept, a fusion between protons and the boron-11 isotope is also possible. Four high-energy alpha particles (4He2+) are formed. The particular point of this approach is that no radioactive and toxic tritium is required and no neutrons are produced which are responsible for the undesired radioactivity. The main problem with this technique is, according to KfK, the energy losses of the particles due to the synchrotron radiation which is produced. Unfortunately, this is ignored worldwide by some physicists for genialized technology. In spite of a reasonable initial result, not enough conveying means are provided for further development in the 70 years. This could be because this reaction does not produce high-energy neutrons, which lead to the very interesting by-product, the cleavable material.induced inertial fusionA mixture of deuterium and tritium is surrounded by a small spherical shell. These 1 mm spheres (pellets) are shot in vacuo with a high-energy laser or a light or heavy ion beam. In the impact thus produced, the hydrogen mixture is compressed to fifty-fourth its volume. The extreme heating causes the fusing plasma to form. Simulations have shown that the thermonuclear energy output is typically one hundred times the laser energy. The main problem is the construction of the required short wavelength high energy lasers or accelerators. Furthermore, high-energy neutrons are also produced here. The construction of an energy-saving reactor which would ignite, for example, ten pellets per second would be conceivable.Cold Nuclear Fusion (or Low Energy Fusion)The reaction was predicted from theoretical considerations already in the forty years by F. Frank and Andrej D. Sacharov and 10 years later experimentally "detected" by an accident of Luis W. Alvarez. In cold nuclear fusion or else myon-catalyzed cold nuclear fusion, the high temperatures and huge experimental setups can be bypassed. The cold nuclear fusion takes place at temperatures from 13 to over 1000 Kelvin in solid, liquid or gaseous media. The reaction can be carried out in a simple tritium and deuterium filled chamber. For this purpose, negative myones are allowed to penetrate into the chamber. The myones form tight bonds between the hydrogen molecules by particular impact processes. The thus myonically bound nuclei fuse and release energy in the form of heat. The myones are released again and can catalyze further fusions under certain conditions. Myones can be produced artificially with the aid of particle accelerators. In order for a myone to catalyze multiple nuclear fusions, high energies are necessary for its production. Where theory is stated. However, a practical implementation has not yet been successfully accomplished to date and there are at least no economically functioning reactors.The chemists Martin Fleischmann and Stanley Pons have also dealt with cold fusion and, in the context of a press conference, stated on 23.03.1989 that they have constructed a cold fusion reactor and tested it successfully. However, this technical wound was not confirmed. The two chemists could also not detect any excess heat in the reactor built before production. The cold fusion is currently only of interest for basic research. To date, there has been no reproducible test arrangement with a positive energy balance.In nuclear fusion, there has been the great technical challenge to overcome up to now, namely the energy balance. Unfortunately, more energy is required to allow the reaction to proceed than energy is later released.In South France, the largest fusion reactor of the world, the ITER, is formed. Here, the Tokamak technology is applied. The start-up should be about 2055. It is a giant construction project which is extremely expensive. Above all, the economics are fragile. ITER is not used for energy production and is not a prototype fusion reactor either. Rather, it is an experimental project intended to provide knowledge of future prototypes and batch reactors.There are increased considerations and numerous experimental attempts to start fusion with significantly less energy. The precursors present the advantages: secure, smaller and more stable reactors. Such processes and reactors are often called cold fusion machines or cold fusion reactors. As already described, special catalysts are used there which are intended to allow a fusion of deuterium and tritium (both hydrogen isotopes). Unfortunately, despite efforts (and some mis-interpretations such as that by Fleischmann and Pons) by world-wide trained researchers, no single truly functioning reactor has yet been produced. Also, reproduction of the results has not been successfully accomplished. Unfortunately, the problem is the theoretical approaches and the execution methods. Despite sometimes remarkable performance and catalytic effects of the catalysts, it is not so easy to bypass the necessary starting energy required for nuclear fusion. Nevertheless, cold fusion with the correct equipment and accurate adjustment of the components could also work. However, other materials and a completely different construction than those used in test plants are necessary for this purpose.Numerous attempts to produce sonoluminescence into a liquid (e.g. water or acetone) with the aid of ultrasound are also known. These processes are already known from the beginning of the 20th century. Ultrasonic waves can actually produce cavitation bubbles in liquid which then collapse quite quickly and thereby emit light flashes. These light flashes can be observed directly or recorded by high speed cameras. The bubbles, which are about 0.2 mm in size, collapse at a rate of about 30 m / s. There are numerous instructions to be able to produce a type of sonofusion by such methods. Unfortunately, there are no scientific evidence for this.To build a fusion reactor that operates in controlled form and supplies more energy than it consumes is an important task today of researchers.US NAVY also makes attempts in the direction. A patent, rather utopic and abstractly formulated, in which nothing was almost explained appeared in 2019 by their scientist, shows that they are interested in the thing. However, the patent document does not yet provide any evidence of how to build such a functioning fusion reactor, just as the other publications, such as the anti-gravity drive to be coupled to the fusion reactor, which is also abstractly and schutarchically formulated, rather giving rise to the impression that authors have made an attempt there without actually understanding this technology to copy and legally protect foreign, extra-ground technology by means of a fragile, deficient interactivity attempt with a substance that might have explained this, unfortunately already left this world. Nevertheless, this work should already be remarkable. Specifically, it is a series of patents filed by the Dr. Salvatore C.P. aeronautical engineer working for the Naval Air Warfare Center Aircraft Division (NAWCAD), a technology and development unit of the US-Navy, and apparently specialized for electromagnetic drives and the research of superconductors. The published patents are descriptions of a "high frequency gravitational wave generator" (US10322827B2); a "room temperature functioning superconductor" (US20190058105A1); an enormous powerful and asteroidal repulsion "electromagnetic 'force field' generator" (US10135366B2); and not least a "aircraft to be driven by a mass inertia reducing device" (US10144532B2) and to be capable of quite surprising and exotic maneuvers at extreme speeds both in the air and undersea but also in space. Another publication, US20190348597A1 (piezoelectrically induced high temperature superconductor) describes an invention which is a high temperature superconductor made of a wire consisting of an insulator core and a metal coating. The metal coating is disposed around the insulator core and the metal coating is deposited on the core. When a pulsed current flows through the wire. Also described is a plasma compression fusion apparatus (US20190295733A1) comprising a hollow channel and at least one pair of opposing counter-rotating dynamic fuses. The hollow channel includes a vacuum chamber disposed within the hollow channel. Each dynamic fuse has a plurality of apertures and an outer surface which is electrically charged.In order to initiate fusion processes, ideas have been made for decades ago to fire with ultrafast projectiles onto targets filled with deuterium and tritium. For some years, such projectiles have been used which impact a target at high speed. In recent years, disk collision attempts have been made to accelerate to up to about 6 km / s by gas pressure tubes or guns striking a cube-shaped target of about 1 cm edge length, each having two chambers enclosed with deuterium and tritium. A collision compresses the gases into a hot plasma, causing the atoms to partially fuse. In the first experiments, about 50 neutrons were generated per shot. If one were to optimize the shape of the target and the targets were no longer cube-shaped, but rather a pyramidal construction with 16 edges and a ratio of 1:1.24, in which one would incorporate a 4-chamber construction with a 103° arrangement in pairs, the neutron emission can be significantly increased.US20190295733A1 (plasma compression fusion device) describes a fusion reactor in which a concentrated plasma bubble surrounded by strong electromagnets is generated. The electromagnets rotate in order to be able to generate a stable field.EP 0438724B1 describes a nuclear fusion reactor having a reaction zone, magnetic flux lines surrounding a magnetic field with the reaction zone, which lines are convexly curved.DE 102012025244A1 describes a fusion reactor in which petawatt laser devices are used to generate laser pulses of picoseconds on solid-state dense nuclear fuel, wherein lateral reaction losses are avoided by spherical geometry of the irradiated laser pulses.DE 3913503A1 describes a method for carrying out a warm nuclear fusion, wherein catalytic elements are to be used to reach a nuclear melt.DE 102007022302B4 describes a method for accelerating solid bodies with the aim of bringing about a fusion reaction. Here, a plurality of radiation sources are used, each of which contains an energy beam on a solid body made of fusion material, which is then explosively vaporized and its parts are thereby accelerated.Unfortunately, the prior art does not present a solution for a fusion reactor that is to provide a positive energy balance.The Lawrence Livermore National Laboratory has recently published some success reports. In the experiments, as is customary in research, only the energy balance of the plasma itself was given. In this case, it is not taken into account how much current has flowed into the lasers, for example, that is to say the overall balance. For future power generation, it is decisive that the overall balance of the fusion is positive. Unfortunately, in the case of fusion reactors known to date, the overall balance has not long been positive.In the NIF experiment, the 200 lasers had a small fuel chamber containing minute amounts of hydrogen heated to more than three million degrees. As indicated, the plant required 300 megajoules of energy to deliver two megajoules of laser energy producing three megajoules of fusion yield. The fact that a total of several hundred megajoules of energy had to be inserted into the system only had to be inserted into the system, is therefore the hook on the success report. For power generation, at least twice the total amount of energy invested would have to be generated. In addition, the Lawrence Livermore National Laboratory achieves such attempts in principle about once a day. A fusion power plant to generate enough power would have to do ten times per second. Calculations would indicate that a larger scale laser system is able to achieve a hundreds of megajoules yield. However, such lasers do not yet exist at all and the energy consumption remains relatively high in this case.US 6919698 B2 describes an electrostatic liquid accelerator and a method for controlling a liquid flow. The electrostatic liquid accelerator includes a first number of corona electrodes and a second number of accelerating electrodes spaced from and parallel to adjacent corona electrodes. An electric power source is connected to supply an operating voltage to the corona and acceleration electrodes to generate a high intensity electric field in an inter-electrode space between the corona electrodes and the acceleration electrodes. The accelerating electrodes may be made of a high electrical resistance material, each of the electrodes having a perpendicular length and height dimension oriented transverse to a desired fluid flow direction and a width dimension oriented parallel to the desired fluid flow direction. A length of the electrodes in a direction transverse to a desired fluid flow direction is greater than a width of the electrodes parallel to the fluid flow direction, and the width of the electrodes is at least ten times a height of the electrodes in a transverse direction to both the desired fluid flow direction and the length.It is known in the art that various methods can be used to accelerate small amounts of liquid. One of these is also the electrospray ionization method. Here, a probe and electrostatic charge are used for acceleration. The probe is located midway between the two turbo-heaters, which are disposed at a 45 degree angle on either side of the probe. The combination of spray and heated dry gas from the turbo-heaters is sprayed at a 90 degree angle onto the opening of the curtain plate. Only compounds ionizing in the liquid solvent can be generated in the ion source as gas phase ions. The efficiency and velocity of ion generation depends on the solvate energies of the specific ions. Ions with low solvate energies are more likely to evaporate more readily than ions with higher solvate energies. The interaction of IonSpray Voltage (Analyst software), IonSpray Voltage Floating (Analyst TF software) or Spray Voltage (SCIEX OS) and turbo-heaters help bundle the jet and increase the rate of drop evaporation, resulting in a stronger ion signal. The heated gas increases the efficiency of ion evaporation, thereby increasing sensitivity and improving the ability to process larger volume streams of liquid samples. A high velocity stream of atomizing gas pushes droplets from the liquid sample flow into the inlet of the IonSpray Voltage or Spray Voltage. The variable high voltage applied to the atomizer causes the ion source to deliver a net charge to each drop. This charge assists in droplet dispersion. Ions of single polarity are preferentially drawn into the droplets by the high voltage when separated from the liquid stream. Nevertheless, this separation is incomplete and each droplet still contains many ions of both polarities. Ions of one polarity are predominant in each droplet and the difference between the number of positively or negatively charged ions gives the net charge. Only the excess ions of the predominant polarity are available for ion evaporation and only a fraction thereof actually evaporates. Droplets contain ions of both polarities, one polarity predominant. As the solvent evaporates, the electric field increases and the ions move to the surface. At some critical field value, the ions are emitted from the droplets. A nonvolatile residue remains as a dry particle. When the droplet contains excess ions and sufficient solvent evaporates from the droplet, a critical field is reached at which ions are emitted from the surface. Finally, all of the solvent is evaporated from the droplet and a dry particle of nonvolatiles of the sample solution remains.Unfortunately, despite intensive research and numerous experiments, it has not been possible to achieve a positive energy-total balance by nuclear fusion. This is not necessarily due to the fusion process itself, but rather to the technical components connected to the core reactor, which additionally consume energy and thus weaken the overall balance. Laser inertial fusion is considered promising by many researchers. A team of the Lawrence Livermore National Laboratory was given its own information to obtain more energy in a laser fusion experiment than was inserted previously. The fusion reaction produced 3.15 megajoules of energy while the lasers pumped 2.05 megajoules of energy into the target with the fuel. About four percent of the fusion fuel has been consumed. However, the entire plant (among other things the laser devices and the accompanying components) has consumed an almost hundred times energy, which has completely nullified the overall balance. During the demonstration of the results, the research team numbered the amount of energy consumed by the laser to ignite the fusion to around 300 megajoules (MJ). The energy of the laser light was 2.05 MJ, about 3.15 MJ was released during fusion, which would mean an energy gain of 153% when 100% was used. However, these are the pure energy ratios between laser energy and the fusion energy ratio. The system has consumed 300MJ! Thus, unfortunately, only 1% "energy gain" was ultimately opposed to 99% energy loss.The invention set out in claims 1 to 129 is based on the problem of providing a compact and widely scalable nuclear fusion reactor which is capable of carrying out nuclear fusion processes.This problem is solved by the features set out in claims 1 to 129.The invention achieves a cost-effective solution also for mobility purposes.Advantages of this reactor are:it provides a unique method for releasing nuclear fusion energy,it can be constructed very compact and small, therefore also suitable for vehicles,cost-effective construction,almost infinite energy source,secure operation.Exemplary embodiments are further explained with reference to FIGS. 1 to 36. The following are shown: FIG. 1 shows an exemplary embodiment of the fusion reactor with fluid jet formation on a common / straight line, FIG. 2 shows a variant with the slightly angled axes of the two fluid jet formations, FIG. 3 shows the single high pressure chamber construction of the reactor with lightning-like pulsating pressure values, FIG. 4 shows the two high-pressure chamber construction, FIG. 5 shows a further exemplary embodiment, wherein the discharge of the microdroplets takes place in a dot-line or dash-line manner in the overall shape of a very thin fluid jet, FIG. 6 shows an exemplary embodiment with additionally an electron beam generator (electron source) which directs an electron beam directly onto the collision point, FIG. 7 shows a further embodiment of this reactor with, in addition to hydrogen isotopes, also the element boron being used for the fusion, FIG. 8 shows the laser beam sources for additional acceleration of the micro drops, FIG. 9 shows an embodiment in which the piezoelectric elements are each installed in the high-pressure chambers, which are hollow-cylindrical in a block of a solid construction, FIG. 10 shows a high-pressure chamber with an inner diameter of 12 mm and a length of 2 mm, in which a piezoelectric element is installed directly opposite the nozzle and immersed in the chamber in the fluid, FIG. 11 shows a further exemplary embodiment with piezoelectric elements in the form of a disk and angled axes of movement of the micro-droplets, FIG. 12 shows an exemplary embodiment, wherein an electrical accelerator, which accelerates the two microdroplet beams relative to one another by electrical discharge, is additionally installed, FIG. 13 shows a further exemplary embodiment, wherein the microdroplets are only a fraction of a picoliter or at most a few picoliters in size, FIG. 14 shows an embodiment with fluid jet formations crossing one another, FIG. 15 shows the device provided with two ring electrodes, each of which is under high voltage from two separate voltage sources, FIG. 16 shows a fusion reactor with voltage collectors for direct energy output for end consumers, FIG. 17 shows a reactor in which the fluid consists of water (or heavy water), FIG. 18 shows an excitation of the liquid itself, which experiences an increase in volume of the orientation of the water or deuterium oxide molecules by electric fields, FIGS. 19 and 20 show an orientation of the water molecules which takes place by strongly concentrated microwave radiation from microwave sources and exact oscillation phase arrangement, FIG. 21 shows an exemplary embodiment, wherein the high-pressure chambers each have an inner volume that is so small that they can only accommodate one microdroplet at a time, FIG. 22 shows an embodiment in which electromagnets or strong permanent magnets are used to uniformly arrange and orient the water molecules, FIG. 23 shows a fusion reactor with a capillary high-pressure chamber, FIG. 24 shows the arrangement of the molecules when rotating on the electric field generated by microwaves, FIG. 25 shows the embodiments with electrostatic fields and microwave radiation in the longitudinal axis of the capillary high-pressure chambers, FIG. 26 shows an embodiment, wherein D 2 O cooled to 11.2° C. is used for fusion purposes, FIG. 27 shows the orientation of the D 2 O molecules in the electric field immediately before the collision of the micro-droplets, FIG. 28 shows the embodiment with the electrostatic running field, FIG. 29 shows an embodiment in which a single high-pressure chamber and a microwave radiator are used as fluid accelerators by excitation of the dipole molecules and a resulting fluid volume increase, FIG. 30 shows an embodiment with a femto laser, FIG. 31 shows the formation of the two fusion points, FIG. 32 shows the flow blocking function by micro-Tesla valves, FIG. 33 illustrates the use of laser sources for micro-expansion of the liquid into the high pressure chamber or outside, FIG. 34 shows a construction in which the distance between the nozzles can be made variable, FIG. 35 shows a further construction in which the collision angle of the micro-droplets flying on one another can be made variable, FIG. 36 shows the formation of standing waves in the chambers.This is a fusion reactor 1, which is designed as a primary energy source and would be suitable for supplying power to households, industry, or also for mobile purposes, e.g. vehicles. For the fusion processes, micro-droplets 2 made of fusible, incompressible material (fluid / liquid) are here accelerated strongly and brought into collision with one another. The micro-quantities in the form of micro-droplets of incompressible liquid accelerated against one another are here extremely small (about 100 picoliters) and are accelerated by pressure generators. Creating a fluid jet formation consisting of microdroplets or microquantities of incompressible fusible fluid arranged in one or more rows in the jet direction can substantially optimize the fusion processes. Here, several hundreds to hundreds of thousands of micro-quantities / micro-drops are generated per second from two nozzles (3 and 4 or high-pressure lamp openings 84) directed against one another and are accelerated toward a collision point against one another at more than 50 km / s. Because no continuous fluid jet is delivered here, but only formations of portioned micro-quantities in the form of micro-droplets in the picoliter volume which are separate from one another, the acceleration is somewhat more effective than in the case of the reactors with fluid jet production. The load on the construction is kept within limits and the "recharging" also works more optimally here. Because the mass of the micro drops with a volume of about 100 picoliters, which consist of liquid deuterium, is about 16 nanograms, an acceleration of this micro mass to 50 km / s requires an energy of 0.02 J (similarly large, as would be required, for example, with an acceleration of 160 g to 0.5 m / s), which can also be provided with a not excessively great technical outlay.The effort to realize fusion processes is currently the fusion technique in which the fusion of deuterium atoms with one another or a mixture of deuterium+tritium atoms takes place. This produces a helium core and a neutron becomes free and large amounts of usable energy. Alternatively, boron atoms can also be used for nuclear fusion. A variant described here additionally uses boron atoms which are intended to fuse with deuterium, but when using boron, a significantly higher kinetic energy of the microdroplets in which boron atoms are also present in addition to liquid deuterium is required (about 200 km / s). Nuclear fusion provides enormous energy. Only 1 g of hydrogen would replace drin, about 10,000 liters of oil (i.e. 1:10,000,000) when all atoms are completely fused in the nucleus. 1 liter of oil provides 11 kWh of energy. One gram of fuel could thus generate 90,000 kilowatts hours of energy in a power plant - the combustion heat of 11 tons of coal. The fusion fuels are inexpensive and more or less uniformly distributed on the earth. The greatest problem with nuclear fusion is the Coulomb forces which prevent the ions from approaching to a very short distance, where the nuclear forces act and the nuclei are "stuck" together.The fusion reactor described here can overcome the Coulomb forces in a targeted manner and thus with a somewhat lower energy consumption than in plasma reactor types in order to operate the nuclear fusion, because here the atomic groups arranged close to one another are shot onto one another. In addition, neutral atoms or even differently charged ions are here incident on one another, so that there are no electrical repulsion forces or even attraction forces present at least in the atomic region precisely at the collision point. However, this changes as soon as the collision in the core / proton range is imminent. Advantages over projectile inertial fusion technology are provided here because not projectiles but rather liquid jet formations from portioned micro-liquid quantities or micro-droplets are shot against one another, which can be generated one after the other for any length of time at very short time intervals. The invention here also has an advantage over liquid jet bombardment fusion reactors because it is possible to generate a continuous or impulse fluid jet from liquid deuterium and tritium, in this case individual portioned micro-quantities or micro-drops which are separated from one another and are sent away from one another are generated. The nuclear reactor, which uses micro-droplets instead of fluid jets, is somewhat more suitable for operating the nuclear fusion because the micro-droplets can be accelerated significantly higher without having to accept material fatigue of the construction of the reactor. The reactor design based on this technology differs significantly from fluid jet fusion reactors because instead of fluid jets, nano targets of micro drops of picoliter size (about 100 pl) are sent with respect to one another at an extremely high speed, which can be set from low to very high. Because here instead of fluid jets, extremely small, individually generated microdroplets are sent against each other to the point of collision comparable to the microdroplets from inkjet printers (but much faster), the pressure in the high-pressure chamber can be brought into effect largely by the mass inertia of the solid wall. Thus, this type of reactor is longer lived than the fusion reactors in which fluid jets are sent to the collision point.The fluid accelerators used here fundamentally use two principles to accelerate the micro-droplets: a pressure generation with the aid of electrically rapidly deformable materials / elements which displace the liquid into the high-pressure chamber or expand rapidly and very slightly by excitation of the fluid / the liquid itself. The devices equipped with fluid accelerators that seek internal liquid excitation to increase volume generate the compressive force directly into the liquid by simultaneous and equal molecular dipole vector alignment in the liquid itself to ultrafast and slightly expand the total volume of the liquid. For our purposes we need to increase a volume of a total 2 ml volume of liquid into the high pressure chamber by only about 200pl, which means a volume increase of 0.00001%. With 20 ml of liquid entering the high pressure chamber, the ratio would even decrease to 0.000001%. However, this volume increase must take place very quickly, within 0.01 ns-0.1 ns, which also works in the devices and methods described below. The construction and material of the high pressure chamber perfectly withstand the compressive force generated by an increase in volume of the liquid drin within 0.01-0.1 ns 0.00001%. Not because the material of the high-pressure chamber walls is so stable, but rather by the mass inertia of the massive (several cm to dozen cm thick walls) high-pressure chamber walls. The volume increase takes only 0.01-0.1 ns and the mass inertia plays a decisive role for the stability of the construction. Although nano-vibrations are generated within the mass structure of the high-pressure chamber walls, they are absorbed by the massive construction.It is known that kinetic energy, if high enough, can cause nuclear fusion between two atoms. Fine measurements make it possible to establish that this process sometimes occurs in nature. In asteroidal collision in worldall when they collide with each other at high speed, flash-like gamma emissions are sometimes detected. Gama radiation is a safe indication that there has been nuclear fusion (sometimes even only nuclear fusion) at the point of collision between the two asteroids. The emission takes a very short time (a few nanoseconds) and therefore this can only be detected when remote measurement equipment is directed. The craters of meteorite impacts on moons or celestial bodies without atmosphere are sometimes slightly larger than would have occurred solely by the kinetic energy. This means that upon impact, nuclear energy was additionally released (mostly by nuclear fusion). The atomic structure and the molecules located on the front surface of the asteroid which comes into collision with the surface of the other will automatically trigger a nuclear fusion of the material located there upon an impact of 40-100 km / s if there water molecules, ice, hydrogen or boron bound in the rock are to be located. In the first nanoseconds of the impact, there is fusion of hydrogen which is directly at the point of collision. Depending on the size of the asteroids colliding with each other, a layer consisting of a few millimeters thick of the surface material of the asteroid may partially fuse. If the asteroid is 1000m or greater, then even underlying layers sufficient to a few dozen cm in depth are certainly involved in the nuclear fusion processes. It goes without saying that not the entire mass of the surface layers comes to fusion, because there is a large amount of material there which can only be fused with one another with difficulty, but traces of material are also present in this case which, owing to the kinetic impact energy of both asteroids, can also fuse. The energy content is very low compared with the kinetic energy of the asteroids, but can still be recorded with fine measuring instruments. Almost any frontal or angular collision between fast asteroids or meteorites leads to a small amount of nuclear fusion of the elements at the point of collision, which are located on the surface and slightly lower at the point of impact. The frontal collisions of the meteories or compact pieces of rock in general, which strike each other at dozen km / s, in this case generates not only a very bright flash light, but also UV and gamma emission. In particular, the gamma emission is an indicator that nuclear fusion has taken place. In addition, after a collision of two pieces of rock, it is generally also possible to detect the generation and release of helium nuclei with fine detectors. The meteorites entering our atmosphere at 35 km / s (or faster) also collide, among others, with water microdroplets (known to consist of oxygen and hydrogen) and free hydrogen atoms of the atmosphere. As a result of the enormous kinetic energy, some of the atoms are brought to nuclear fusion. Micro-explosions are generated from nuclear fusion processes which have destructive effect on the incoming rock chunk. These micro-explosions flash the surface and more and more quickly destroy the structure of the meteorites, which in effect, in addition to the rapid penetration of the air flow and heating by friction and air compression in the inner structure, also leads to their explosion in the atmosphere (if they are not too great). Being large and compact enough to reach the planetary surface, the fusion processes bring up to surface with and upon collision with the planetary crust, they again and boost nuclear fusion processes, but depending on the material supply of the rock, if it contains radioactive material, also bring about nuclear fishion. With nuclear energy release or fusion energy release, one can also explain the crater size in foreign planets, which otherwise would be made somewhat smaller if the fusion energy were absent and if alone the effect of the kinetic energy were involved.The fusion processes can be found not only outside the earth in the stars in space, but to a small extent also here on the earth in nature. Fusion processes can be registered in the case of intense lightning strikes by sensitive apparatus. Lightning strikes accelerate ions at up to 5-10% of the C velocity (C=300,000 km / s) and in some cases cause nuclear fusion. It is known that flash discharges in a gas (also in the natural or atmosphere) lead to ion movement. Atmospheric lightning on the earth or on other planets has the effect that during the discharge, some of the particles are accelerated so much that nuclear fusion can occur. Fine measurements show that in the case of flash discharges, sometimes a gamma radiation or a gamma emission is released. The ions are strongly accelerated by high voltage discharges. Although the speed which a flash discharge can achieve is lower than the speed of light, it can reach up to 70% of the speed of light (C). If one takes into account the material (or ions) that is set in motion very quickly in this ion channel, one can envisage that very high amounts of energy can be released there during a fusion process. Almost every time a natural flash discharge occurs, there is slight nuclear fusion of the light elements. However, in a flash discharge, as occurs in nature, only very few atoms or ions will collide with one another to such an extent and optimally that this leads to a fusion. In addition, the fusible elements are present in the atmosphere only in very low concentration. Often, the nuclear fusion processes are difficult to detect there with our technical possibilities. However, nuclear fusion also takes place there. If one is well upgraded with equipment, invested enough time for weathering and makes measurements, one can occasionally also measure and detect gamma emission in lightning strikes. Helium nuclei can also be detected in this case. These are indicators that fusion processes take place there. Thus, the nuclear fusion occurs not only in the stars and sun, but also outside in cosmos and on the earth, and which would be much more often thought of.The explanation of why so much energy can be released in the core fusion is in the nature of the atoms and the matter in general. Although the material consists of atoms, they are almost completely empty. A tiny nucleus of nuclei is located near the center, enveloped by a comparatively very large mist of rapidly circulating electrons, which indicate the circumference of the atom. The space therebetween is empty and is determined only by fields. Likewise, the nucleons and also the electron itself are not solid "articles". Although the electron is referred to as a punctiform, structureless elementary character, it also has an internal structure. Because it is so small, unlike the atomic core, it is almost inderuptable. Although the electron acts hard, for example in contrast to protons or neutrons, it also has a "spongy" construction, wherein it is somewhat harder than its "shell" in the center. An electron can also be destroyed or newly created. An example of this is the fractional quantum Hall effect. A strong magnetic field causes the electrons in some two-dimensional materials to behave as if they split into three (or more) new particles (anodes). However, with another technique, an actual splitting of the electron is possible. The complete electron consists of photons only entangled in each other. These photons are even trapped in one another there, although they always "rub" past one another in the smallest space at the speed of light. These entanglements can only occur when multiple photons of high energy come extremely close to each other or collide with each other linearly or at certain angles. In the reverse manner, the electron can also be knitted out in individual photons. Because these photons at speed of light still travel in the complicated paths, they impart a mass to the material. Photons get a mass or weigh "heavy" only when they fly at C-speed. Based on the data of the COBE satellite which provides the most accurate measurement of the spectrum of the Kosmic background radiation to date, researchers have the result that the lifetime of photons with an assumed mass of 2×10 54 kilograms must be at least three years. Because they have a mass (given as about 2×10 -54 Kg, but in reality is still less, about 3.4×10 -55 Kg) as they move, they interact with gravitates in the gravitational field and thereby get a weight, so that the light is attracted by the gravitational field of the star when it passes a star, and light diffraction thereby takes place (although it does not have to match, it can also be clarified woundable with the relativeistic spatial curvature... ). Diffraction can be calculated very accurately using simple physics (without considering curvature in space). They do not possess a rest mass (Higgs-Boson theory Ade). In a free nature, photon entanglements no longer occur, but already in large stars, because the photon density is enormous there. Black holes can generate not only particles but also atomic nuclei and electrons from the energy (photons). It has been previously considered that the light beams, when they cross each other or are emitted against each other, do not interact therebetween. Although not yet measurable with conventional methods, there is also an interaction between intersecting light beams! However, the light beam is extremely "sparsely populated", so that only a few of the photons "collide" with one another. Only when the radiation density and photon density are extremely high will the interactions become noticeable and measurable. With high-energy laser beams and strong focusing, the photons can be brought so close to one another or to collision that they become entangled with and within one another in a "slight" number and are caught by themselves. Thus, it is possible to "produce" full electrons (although it does decay from the point of view of quantum theory, it is also possible in other variants-for example half-electrons or quarter-electrons-even detected a few weeks ago). Similarly, the entire material is constructed in worldall from interdigitated photons. When these entanglements are caused, a giant amount of photons is released which is perceptible as energy. In the case of hydrogen nuclear fusion, approximately 4% of the mass is knitted out and an enormous photon concentration is thus released as radiation in all directions (which inflates spherically at the speed of light). This is the energy coming from nuclear fusion. In addition, the neutrons in the vicinity are blasted with photons and thus "saturated" and shifted away. In this case, they receive an enormous thrust force due to photons flying away, which thrust force is released as thermal energy during braking. The enormous high nuclear fusion energy comes from the photons which are already in the material or form the material. These photons then travel straight in all directions, always with the tendency to increase the distances between adjacent photons. This light energy, which consists of the 40 g knitted out (de-knitted / material-unknitting) material of a 1 kg hydrogen mass, is the flash, which from a hydrogen bomb first impinges on the environment. Practically all the environment is struck with a more expanding spherical envelope of 40 g of pure photon mass consisting of material in photon form accelerated at the speed of light. This 40 g photon mass is practically the knitted material, which in this case has "moved up", broken down into photons (the so-called mass defect) and floats at speed of light from the starting point. 40 g of pure photons mean an enormous radiation energy power, which has a destructive effect on the material in the path and is thereby released. The corpuscular radiation which additionally arises in this case receives its kinetic energy from the massively floating photons. Similar fusion processes occur all the time in world space, so photons from infinite stars have been moving away for billions of years. However, the photon is also not quite long-lived. A photon actually lives only about 3 years, but because of time dilation it may exist for a significantly longer time. In the relative theory, however, the C constant is not completely correctly implemented. On the contrary, C would have to be used to denote the gravitational field expansion speed, which although only very slightly higher than the speed of light in vacuum, nevertheless has a femto difference. This explains why a photon becomes 'tired' after approximately 13.8 billion years and is no longer visible. This also explains why we are not seeing any stars that are further away than 13.8 Farards of light years. And this does not only occur on our earth in all celestial directions, but the same is also observed from a planet that is 13.8 billion years of light we are removing. The residents there also see a ball around their planets with a 27.6 billion years of light in the center of which they are themselves located and who may know that the universum need not necessarily expand. This "invisibility" has little to do with the expansion of the universum and only quite nothing with the hypothetical dark matter. There are also in far-away regions in the all, stars and galaxias, which are not zubasing from us but on us, but which are also not seen! One only needs to consider from the point of view two reference systems of a star in 10 and again one in 20 billion years of light, then one becomes transparent, which takes place in the University and how it is actually done with the inflation. Also from these two stars everything flies spherically away, but a part of these "spherical shells" flies towards us, which absolutely does not fit Doppler effect observations!In order to be able to understand the nuclear fusion processes, an insight into the matter itself is required. The knitting out (unknitting) of the material is symbolically seen, as in a very rapidly rotating wheel which separates itself into individual parts by centrifugal force, each part flying apart or also analogously to a knitted glove (or a wool ball) in which the thread is drawn out. The faster the thread is drawn out, the smaller the glove becomes, but until the glove completely disappears, a thread having a length of several hundreds of meters is drawn out.The reactor of the invention utilizes the energy release fusion processes which are distributed by cold incompressible fluid jet formations (liquid in microdroplets which are individually accelerated) of fusible material which here consist of single microdroplets delivered in a pulsed manner in succession from two nozzles. The kinetic energy is extremely high and a collision of two micro-droplets has the effect of overcoming the Coulomb forces between colliding atoms contained therein, which leads to nuclear fusion. The liquid jet formations or the micro-droplets there are cold, but on collision they heat up extremely strongly and lightning-like. Once nuclear fusion occurs, heating rises to over tens to hundreds of million °C, flashing, with strongly ionized particles flying ultrafast away from the collision point in all directions. Such particles are struck by the following microdroplets if they are delivered at a correspondingly high repetition rate, so that at the moment of collision of the first microdroplet, the second one is already sent away and flies into the bombardment field of the particles which are flying apart after the nuclear fusion process. The repetition rate and the pauses between the delivery of two micro-droplets also determine the efficiency of the reactor. An optimal energy balance is always a rapidly repeated microdroplet delivery in which, as soon as two microdroplets come into collision, a few subsequent microdroplets are already sent out, so that the subsequent microdroplet comes close to it to approximately 28 μm and as far as possible involves a good yield of the flying particles from the colliding microdroplets. The flying particles, partly consisting of hydrogen ions / deuterium ions, are en route at about 500-30,000 km / s and significantly optimize nuclear fusion in the subsequent micro-droplets. This enables subsequent nuclear fusion processes even with significantly less pressure into the high-pressure chamber. The first drop must be accelerated strongly in order to "ignite" the fusion, while the following ones can also be moderately en route (with only a few km / s or even less) as long as they arrive row by row at the collision point. It is important to choose the flight speed of the subsequent microdroplets such that, when they are struck by the particles originating from the merging microdroplets, they also reach the collision point at the same time, so that the nuclear fusion does not take place far from the collision point, but rather as directly as possible there, because otherwise instead of one nuclear fusion point two points are produced which travel further and further in the nozzle direction. It is therefore important to increase the speed of the microdroplets to such an extent that they actually come to nuclear fusion at the intended collision point. This can also be achieved by increasing the repetition rate for generating the micro-droplets. As the number of micro-droplets travelling in the fundus formation to the collision point is increased, they always shield each other, and the subsequent micro-droplets are temporarily shielded from the intermediate ones, so that the high-energy particles do not directly hit them. Thus, the nuclear fusion processes decelerate somewhat in the subsequent micro-drops until they actually reach the calculated or intended collision point.This reactor can be constructed so as to be readily scalable for any performance. An application is also provided optimally for low to medium power, so that it is also suitable for mobile purposes (vehicles of all kinds). The nuclear fusion can be effected on a large scale or else on a mini-scale. For such purposes, micro-droplets are spun against one another in rows in the form of two very thin fluid jets (5 and 6 - fluid jet from micro-droplet formation) of fusible material and are thus caused to collide.The micro drops are accelerated by piezo actuators 7 or magnetostriction drive or plasma micro-explosions by pressure and additionally electrically from the nozzles. It is advantageous that the micro drops are charged, but not so far that all atoms are ionized. The electrical charge collects predominantly on the surface of the microdroplet and thereby forms a type of "electrostatic outer casing" 8. This fluid jet formation is not a continuous fluid jet, but rather a series of microdroplets which are delivered one after the other and do not contact each other. On a high speed camera, this microdroplet fluid jet formation would not look truly like a jet, but like small spots coming from both nozzles rapidly in succession and meeting each other at a point of collision. The fluid jet formations thus look like an extremely thin, dotted or dashed line, the distances of which are very large or somewhat smaller depending on the setting of the repetition rate for the generation of the micro-droplets. With long pauses between them (in the microsecond or even millisecond range), only one microdrop / point is seen on the recording, which point leads to the point of collision with the microdrop from the other nozzle. And only milliseconds later is the next point asserted. The collision of two micro-droplets over two fluid jet formations occurs linearly (straight 180°) on the same fluid jet formation axis 8 or at a very wide angle 10, almost linearly with respect to one another (about 176°-179°). These two "dotted lines" consist of micro-droplets 2, i.e. meet on the same axis or cross at a wide angle (e.g. 176°-179°). The point of collision 11 is exactly between both nozzles shooting these fluid jet formations against each other. In the case of fluid jet formations situated exactly on one line / axis, it is important to dispense the micro drops simultaneously, because otherwise, depending on which of the micro drops in which fluid jet formation first emerges from the nozzle, the point of collision with the other micro drop which comes out of the other nozzle shifts and it can happen that one micro drop no longer strikes the other drop at all, but directly strikes the liquid which is still located opposite it in the nozzle opening 12. Therefore, it is important to launch all of the two fluid jet formations simultaneously (FIG. 1 ). The variant with the slightly angled axes 9 of the two fluid jet formations (FIG. 2 ) does not have the problem, because the fluid jet formations (5 and 6) only cross one another there, but here at a low repetition rate fewer micro drops can meet (with present-day technology, the hit rate would be at a few percent below 176° fluid jet formation cross angle). The larger the crossing angle 10, the better the hit rate and it increases abruptly the closer the angle approaches 180°. At a wide angle of almost 180° (e.g. 179.998°), the collisions are still almost to be considered as in direct frontal hitting. As long as the fusible fluid (incompressible) is in the high pressure chamber, high pressure technology accelerates and exits the nozzles. Immediately thereafter or already in the nozzle, the micro-droplets are electrically charged and then further accelerated by electric fields and electrodes. The micro drops consist of a plurality of atomic groups 13 which are fusible in the event of a collision. Because the majority of the atoms in micro-droplets are neutral, no electrical repulsion forces are produced until their cores come very close to each other. When the microdroplets collide from two nozzles, in many cases a leverage effect between atomic groups also occurs, in which some atomic groups are greatly braked and the other, directly adjacent atomic groups benefit therefrom by additionally having this kinetic energy transferred (leverage effect), so that it is faster than the travel speed of the microdroplet as a whole. Such additionally accelerated atoms lead to increased fusion when they meet.In conventional fusion reactors, ions which are charged equally are predominantly used to effect nuclear fusion with each other. However, extremely high temperatures and long-term plasma confinement by magnetic fields are required for this purpose, so that the ions come close to one another and in particular often enough for them to be able to fuse. The greatest challenge there is the extremely thin plasma, which is almost like a high vacuum. There is an extremely low probability that two particles collide with each other.However, the invention does not use a plasma in large volumes, as occurs for example in the Tokamak reactors (a few m 3), but rather the kinetic energy of liquid micro drops (micro droplets) which are accelerated towards one another at high speed to a collision point. The advantages are here significantly greater compared to Tokamak technology. The material which is fused here is not almost vacuum-like thin like to Tokamak plasma, but rather very dense compared thereto. The fusible material is here in the form of two fluid jets, which do not consist of a continuous fluid flow, but of finely metered microdroplets, each of which is equipped with approximately 100 picoliter of material (fluid / liquid). And these paired drops of about 100 picoliter each are accelerated against each other over a very short distance (mm to several cm), so that they collide exactly with each other in the middle of a reactor chamber. The Coulomb forces which prevent fusion of the core are here substantially weakened in the invention up to a very short distance between two atoms, because the two groups of atoms which meet each other are not charged identically, but are charged electrically neutrally or even differently. While one microdroplet having one atomic group is positively charged, the other group which leads to the collision point is negatively charged. Thus, here, attractive electrical forces occur rather than repulsive forces, which is not the case in the conventional fusion reactors and the ions located therein. The acceleration of the electrically charged micro drops is also effected by two ring electrodes (15 and 16) which are connected to one another by an insulator ring 14 and which attract the micro drops respectively from the nozzles (3, 4-A and B) to which they are directed. The microdroplets attracted by the ring electrodes are additionally accelerated by a nozzle electrode (17 and 18), which are constructed, for example, in the shape of a disk or funnel, and the collision is found at the center of the ring electrode opening 19. The ring electrodes are positioned in the way with their openings 19 in the middle so that all the attractive force acts on a virtual line (fluid jet formation axis) 9 connecting the two nozzles together. It is very important that the two micro-droplets are sent simultaneously from the nozzles, so that they also meet at the center of the circle formed by ring electrodes. The micro-droplets / micro-droplets are accelerated up to the center point of the described circle of the ring electrodes, after which no longer (if the collision point is exceeded, rather braked). The microdroplets must therefore meet as close to each other as possible or exactly at the midpoint / collision point 11 because if they meet on one of the sides beforehand, then one of the microdroplets is decelerated by the electric field on the other side. The microdroplets are optimally struck exactly at the center of the circle belonging to the insulator between the two electrodes. There, the two electrostatic fields of the two ring electrodes are substantially neutralized. However, the insulator ring is very thin and this makes the neutral field region very short. Therefore, the microdroplets need only travel very short distances there (about 1 mm) without driving, predominantly due to the mass inertia and the attractive force of both microdroplets. The electric attractive force of the two micro-droplets always increases until the time of collision of the two micro-droplets because they are charged differently. The fusible atoms (deuterium or tritium atoms in the liquid state) constituting the microdroplets do not all fuse with each other. Although both colliding microdroplets are mutually electrically attracting, only about 3% thereof will actually also fuse with each other. Fusion takes place predominantly in the central region of the microdroplet. These atomic groups have the best chances to fuse because they are enveloped by the other atoms and a scattering effect (scattering effect) is rather unlikely because the escape possibilities are lower. In order to promote the fusion processes, one can help with laser beams or by a rapidly alternating electrical discharge directly in the drop rows. If an electrostatic flash discharge is alternately performed in one drop row and then another discharge is performed on the oncoming drop row, with a common ring electrode at the point of collision attracting the micro drops alternately from the nozzle to the left and then from the nozzle to the right to the midpoint / point of collision, the micro drops can be accelerated additionally. The discharge and the attractive force can take place here alternately at a high pulse rate frequency or also simultaneously / simultaneously. With simultaneous attractive force, the two micro drops are attracted from the nozzles by the centrally located two ring electrodes with the insulator ring therebetween. The discharge also takes place simultaneously in such a way that a circuit is respectively closed through the ring electrode, the nozzle on the same side as the ring electrode and the ion channel (current discharge channel) 20 to be generated from the microdroplet jet.The system includes numerous components. Important are the pressure generators forming the fluid accelerators 21, nozzles, the annular electrodes in the middle, high-voltage sources 22, etc. Two fluid accelerators with piezoelectric drive elements 7 are installed in each case in a high-pressure chamber (24 and 25), which each bring about a pulse-like hydraulic pressure on the fluid and a generation of the micro drops from the nozzles. Two micro-drops are generated from the two nozzles and simultaneously leave them. The micro-droplets are shot against each other at high speed. The pressure from the piezoelectric elements (45) is not sufficient to accelerate them sufficiently strongly with respect to one another. Although piezoelectric technology can accelerate them directly to a few 100 m / s, they cannot be so far that the collision energy is sufficient for fusion. Nevertheless, by means of a transmission of pressure force in the small-dimensioned high-pressure chamber, a 100 picoliter drop can be accelerated very strongly. For the duration of 0.1 ns, pressure values above 1.5 Calif. can be generated without the high-pressure chamber design suffering! It is not the very stable high pressure chamber design that holds them together, but rather the mass inertia of the massive high pressure chamber walls 26. In order to generate a deuterium jet at a speed of 50 km / s via a 0.01 mm nozzle opening, one would bum pressure values at about 13 MPa, which can also be achieved with the piezoelectric elements very short (0.1 ns) and with extremely small fluid quantities (picoliter range).Although the nuclear fusion processes are pulsed / "digital", the reactor here supplies energy almost continuously and almost uniformly as long as the microdroplets are generated and launched onto each other at a constant repetition rate. Depending on the desired output power, hundreds of thousands to tens of millions of microdroplets per second can be caused to collide. The drop size also does not necessarily have to be 100 pl. It can also be only 1 picoliter in size.The reactor would generate a lot of energy if the entire mass of colliding micro-droplets were to fuse. However, since only about 3% of the mass of colliding micro-droplets leads to nuclear fusion, the efficiency of this reactor is about 3%. This means that here only 3% of the mass of the fuel is fused upon each microdrop collision. This manko is compensated relatively well by high repetition rate of the colliding micro-droplets. In addition, the fuel is not lost, but is collected and provided in the reactor again in microdroplet form for collision. The micro-droplets are thereby discharged in about 100 picoliter volumes. Each microdroplet consisting of liquid deuterium weighs about 16 ng. Accelerating this micromass to 50 km / s requires an energy of 0.02J (similarly large as would be required e.g. when accelerating from 160g to 0.5m / s). If two such droplets with a total of 200 picoliters meet each other and thereby fuse only 6 picoliters, approximately one nanogram of deuterium mass (169 kg / m 3 in the liquid state) will come to fuse and release an energy which is equalized with the combustion of approximately 0.01 g of oil, which provides approximately 420J of energy (1 kg of oil provides approximately 42MJ). This means that the reactor would ideally operate with an energy balance of about 21,000 / 1. The energy invested for reactor operation would, in this case, release 21,000 times higher amounts of energy. It goes without saying that a lot of energy is lost due to conversions and the accompanying components also consume current, but finally at least one energy excess which is at least about 800:1 still remains in the positive balance. By means of a widely adjustable repetition rate of the microdroplet generation (from 1 to 50,000 pieces / second), the energy released can be very well controlled in the process. Thus, the thermal energy can be released from 0.01 ml to 500 ml of oil combustion / second, which would last mean about 1800 liters of oil combustion per hour. The 1800 liters of oil supply about 16 h of energy. By increasing the repetition rate of microdroplet generation, the fusion performance can be further increased, but this would involve high wear for the fusion reactor design and could mean rapid wear thereof. An energy release would be optimal, which can also be well dissipated, so that the reactor integrity is maintained in the long term. In addition, it is also possible to install a plurality of reactor chambers which run in parallel or one behind the other during operation.The reactor utilizes the kinetic energy of the fluid droplets that collide with each other. The acceleration takes place initially by hydraulic pressure, which is generated with the aid of a fluid accelerator, such as piezoelectric elements (or magnetostrictive elements coupled to micro-hydraulic translators) and then, during the transition into two fluid jet formations, which consist of micro-drop rows, which are each discharged from the two nozzles, additionally electrostatically accelerated or, in the case of dipole molecules, at least optimally rotated / oriented in such a way that they collide against one another with the hydrogen / deuterium atoms (in the case of heavy water) toward the front.In the high-pressure chambers, which can take up relatively little contents (depending on the reactor size and output, about 0.01-150 cm 3), the fusible liquid is injected as far as possible in an incompressible state (e.g. deuterium at the very low temperature). Depending on the technique used, it is possible to build only one high-pressure chamber with two nozzles directed towards one another, or two separate high-pressure chambers, in which, however, the high pressure is generated simultaneously. There, in the high pressure chamber drin, an electrically stretchable member capable of electrically changing its dimension or deforming is installed. This property is possessed by numerous technical elements, for example the piezoelectric elements or magnetostrictive elements. The magnetostrictive elements are slower, therefore they require a micro-hydraulic translator that converts the slow vibrational energy into kinetic energy for fast fluid jets. This can be made quite simple. This would suffice if the pressure area (pressure area) of a magnetoactive element into the high pressure chamber is about 2800 m times larger than the area of the circle having the diameter of the drop. The oscillating / piezoelectric element is installed in a recessed location in the reactor chamber wall and expands there in a pulsating manner. The element thus reduces the volume into the high-pressure chamber in a lightning-like and pulsating manner to a minimum, and that by about 220 picoliter in the case of a single high-pressure chamber design (FIG. 3 ) or 120 picoliter in the case of a two high-pressure chamber design (FIG. 4 ). As a result, the fluid capable of fusion is displaced slightly from the high-pressure chamber, electrically controlled.Because the fluid in the high-pressure chamber is under high pressure, the space in front of the pressure surface of the piezoelectric element quickly fills up again with the fluid already during the pause times, while the piezoelectric element retracts. The high pressure chamber walls 26 are very stable and massive (e.g., made of stainless steel / titanium alloy and are a few tens of cm thick). The high pressure chamber, in which the fluid is injected from the reservoir tank 27, can be constructed in the shape of a ball or a hollow cylinder. The very small amount of fluid (a few ml or even less than 1 ml) that fits in is injected through a very thin capillary conduit 29 by an injector 28 and the high pressure chamber is filled therein fully. The capillary conduit may be closed by an electro-valve 62. The electro-valve may also be installed above the injector. A vacuum or high low pressure prevails in the high-pressure chamber and in the reactor chamber 23, when they are empty, so that the high-pressure chamber can be completely filled without problems. The fusible fluid Drin should be incompressible. The nozzle is very fine and in our embodiment is about 28.8μ in size in exit orifice (diameter) 12 and can deliver very small micro drops. However, it can also have other diameter sizes, such as, for example, approximately 0.07 mm-0.014 mm in nozzle diameter. An extreme high pressure is generated in the high-pressure chamber, which is of very small dimensions (a few cm 3 volume or even smaller), but this also only takes an extremely short duration (0.1 ns) when the piezoelectric element is pulsed at a frequency of 10 GHz, wherein two to four amplitude movements (2-5 μm) are performed. After this, a pause of 0.01 to 4.5 milliseconds occurs (depending on the setting for the output power requirement of the reactor), during which only after a few micro drops have been dispensed and the short line chamber 30 (about 1-2 mm long) leading to the nozzles slowly becomes empty does a refilling process take place by the "pushing" of the fluid in front of the pressure surface of the piezoelectric element. With the aid of the injectors, a small amount of liquid deuterium can be replenished, for example, every few seconds. The oscillation amplitude direction of the oscillation element 7 is arranged such that it pushes the fluid with the pressure surface in the nozzle direction and thereby accelerates the latter. The amplitude of 2-5 μm is very small, but is sufficient to displace two or four microdroplets of 100 picoliter each from the high-pressure chamber out of both nozzles. The line paths from the oscillating element to the two nozzles must be exactly the same length so that one microdroplet comes out of each nozzle simultaneously. The thrust force for the micro drops and their kinetic energy is determined by the size of the pressure surface 31 of the piezo actuators, similar to the hydraulic pressure in a working cylinder. With a print area 1000 times larger than the circle area with a drop diameter size, a 1000 higher kinetic energy is generated on the 100 picoliter drop. For larger fluid quantities (e.g., milliter range), this would fail because the fluid mass then provides significant resistance to such accelerations, but for picoliter quantities, this is quite irrelevant.It should be mentioned that the term "fluid jet formation" is intended merely to provide a better understanding of the operations and principle of this reactor. In reality, when viewed with a high speed camera, there is no fluid jet formation of microdroplets seen, but only a single, single dot (microdroplets) coming out of the nozzles. One microdroplet travels 50m per microsecond (at 50km / s). Thus, micro drops discharged from a nozzle "one behind the other" do not "see" each other at all. Only when the repetition rate becomes relatively high would they be submitted to each other to the extent that they actually form a fluid jet formation. If an extreme high pressure of this kind, which lasts only 0.1-0.2 nanoseconds, is generated every 4.5 milliseconds, approximately 220 pulses are generated per second and just as many microdroplets each having 2×100 pico litres of content are delivered to collision with one another. However, a repetition rate of 220 microdroplets per second is not optimal for the nuclear fusion energy balance. The microdroplets should be dispensed so often after one another that the subsequent microdroplets are always located close to a few millimeters or even up to fractions of a millimeter (approximately 100-800 μm) when the first microdroplets have reached the collision point. This is because of the possibility of utilizing the kinetic energy of the particles of the colliding microdroplet triggered by the nuclear fusion processes. Immediately after the nuclear fusion, atoms, ions and particles (all these are parts of the microdroplet) are accelerated from the microdroplet at a few hundreds to thousands km / s in all directions and also toward the rear. The closer the subsequent microdroplet is, the more such high velocity particles they meet. Per doubling of the distance to the collision point, the square of the number of particle hits with the microdroplet drops. Therefore, it is important to calculate or find out the optimum value for each reactor, which indicates how often and quickly the microdroplets must be generated in order to optimally maximize the nuclear fusion energy balance. This value is dependent on the nozzle distance from each other, the microdroplet size and its velocity.The extremely high pressure (a few to dozen mbars to even giga-bar) could destroy the high-pressure chamber, but does not do so because this pressure is again in the decomposition phase after 0.2 nanoseconds. The oscillation amplitude of the pulsating element is so small that this pressure alone offers the mass inertia of the material structure of the solid high-pressure chamber walls of the construction sufficient stability. However, the pressure is sufficient to accelerate two per 100 picoliter microdroplets (or even smaller) to a few dozens to 50 km / s (or even even faster, for smaller drops). In the case of oscillation elements with a larger oscillation amplitude (e.g. 50 μm) and 10 GHz frequency, speeds of up to 500 km / s would also be achieved, but the microdrop here should only be a few pico litres in size or even smaller. The 100 pico litres quantity passes through one nozzle, while the other nozzle which is opposed supplies once again as much. In order to avoid the scattering of the microdroplets by their own electric charge, they are selected to be extremely small and the distance up to the collision point is designed to be as short as (a few millimetres or at most a few cm). The micro-droplets do not have enough time to crack, as is the case, for example, with an electrosprayer, where the micro-droplets explode in shape due to the electrostatic field after they spray from the nozzle, because the molecules fly away from one another by the same electric charge. The microdroplets which are rapidly accelerated in this manner are no longer spherical, but rather look disc shaped with a small tip in the middle and a slight conical deformation tendency, forming a very small disc shaped edge at the back. The micro drops which are sent out of both nozzles in a row towards each other can move on the same axis line up to the point of collision or else strike each other under a slightly angled line. In this case, they would meet each other not on a line (180°) but at an angle of, for example, 176-179°. This would have the advantage that the micro-droplets which are not decelerated by collision or do not collide with each other do not strike the nozzle opposite, but they could strike a mass of liquid deuterium 32 which would be freely located in the reactor chamber, or uniformly radially distributed by a reactor chamber rotation and by centrifugal force to its hollow sphere wall 33, wherein the kinetic energy of the micro-droplets is either absorbed there or again partly leads to the fusion of the nucleus. However, because the micro-droplets shoot one upon another in a liquid-beam form in rows, the probability of them colliding with each other is very high despite a cross-path at 179° angle.Mathemic calculations and energy yield are determined as follows:1pl contains about 0.000 000 000 17g (0.17 nanogram) liquid state deuteriumHere, 200pl / second is consumed and the time is about 220 times / sliquid deuterium density is 169 kg / LThe ratio grams / volume is given as 1:6 for liquid deuterium1 g deuterium fusion energy provides equivalent to combustion of about 11,000 kg coal or 9,000 kg oilWhen about 2200 x 2 micro drops (100 picoliters each) are sent to collision in a medium-size reactor with a very short distance between its two nozzles, a mass of 0.44 microliters / second results, which means about 0.00007 g liquid deuterium per second, which are emitted against one another in the two fluid jets. For this, the equivalent to oil combustion is: 0.00007 x 9,000,000=0.63 Eq / s (fusion material), which means about 2,270 kg oil combustion energy / hour. This would be equivalent to 2270 oil combustion per hour, releasing about 25 MHh of energy. This energy would be possible if all atoms were to fuse into microdroplets. However, because only about 3% of this leads to fusion, the performance is 0.75 MHh. The energy expenditure for high-pressure generation, control, pumps, injectors, cooler systems and energy converter losses must be subtracted therefrom, which finally remains about 0.5 MHh. This is the energy that such a mini-reactor would provide. When the microdroplet repetition rate is increased or two fusion chambers driven in parallel are installed, the power can be increased as desired. 22,000 micro drops / second on each collision beam would deliver ten times energy, which would mean about 5MW. Considering that 1MHh can be powered to about 4000 homes, 5MHh will be sufficient for about 20,000 homes (a city). For the easier calculation of the released energy, it can be assumed that always two micro-droplets with a total of 200 picoliters, which meet one another and at the same time fuse together only 6 picoliters, bring about one nanogram of deuterium mass to fuse, releasing an energy which is equalized with the combustion of about 0.01 g of oil.The microdroplets with a volume of 100 pl liquid deuterium form per microdroplets which look like a sphere with a radius of approximately 0.0288 mm (28.8 μm) or like a disk with the same diameter. This is the microdroplet size which is accelerated here. The diameter of the nozzle should also be as large or slightly larger if microdroplets are to be produced in size. To achieve the speeds of 50 km / s per second, the pressure required for the liquid jet (liquid deuterium jet) is about 2Ar continuous, or pulsed, about 1.6 x 10 9 bar (about 1.6 gigabar). This is a very high pressure and could not be withstood by any material. However, as already described, something else still remains in play here, which resists the pressure: the mass inertia of the massive high-pressure chamber walls. Because the pressure is generated only for 0.1 ns and then it is immediately released, with the displacement being only 100 picoliters, no damage to the construction is expected.In order to optimize the fusion processes, there is the possibility of charging the microdroplet in such a way that it has a positively charged core and a negatively charged shell, both consisting of atomic / molecular groups (or vice versa). Here, first a microdroplet of a small group of molecules would have to be positively charged and immediately after it exits the nozzle would meet another microdroplet of a group of molecules negatively charged from another immediately adjacent nozzle shooting in the same direction and steering at a very narrow angle towards each other and then the travel would arrive together up to the meeting point with the oncoming fluid jet from two other opposing nozzles. In that case, the outer shell of the microdroplets would be negatively charged and could be attracted and accelerated by a positively charged electrode. Such a microdroplet can be charged electrostatically to a very great extent and it would not crack up in the process, but rather travel as compact microdroplets (almost like neutral drops). The same, charged only differently, occurs with the microdroplets from the opposing nozzles shooting against them also simultaneously. At the collision point, atomic groups which are charged differently meet. The "outer shell" 8 of a microdroplet is positively charged, while the other which is leading to the collision point is negatively charged. Thus, the two micro-drips attract each other.It should be mentioned that the reactor would also have to function with heavy water. Two jets of liquid consisting of heavy water, accelerated towards each other at 300 km / s each, would also lead to nuclear fusion of deuterium atoms although in molecular linkage.Likewise, a two-jet technique, one of which is heavy (D 2 O) and the other of which is super heavy water (T 2 O), would have to be able to function well. Although the repetition rate of the electrical pulses for the piezoelectric element is not very high (in our example approximately 2200 Hz), the deformation of the element takes place very quickly (10 GHz). Within 0.1 ns, one or more oscillations with an amplitude of 2-5 micrometers should take place. The area (pressure area) 31 of the element 7 on the expansion side 34, which is about 200 times larger than the circular area projection of the diameter of the nozzle or of the circular area which has the same diameter as the microdroplet, will cause a very rapid displacement of the fluid per pulse and thereby seek about 250 picoliter of ejection from the nozzles. About 50 picoliters of expansion are lost to microscopic levels of elasticity despite massive high pressure chamber walls and their inertia, although they seem macroscopically rigid and are constructed of massive stainless steel, while the remainder, about 200 picoliters of expansion volume and displacement, translates to the fluid. The high pressure chamber should be constructed in one piece and not welded together from several walls. The inflexibility of the chamber design is very important for achieving the high jet velocities. Due to the 200 picoliter displacement within 0.1 ns, an acceleration of the two per 100 picoliter microdroplets is achieved to a speed of 50 km / s each. Because their nozzles (also made of solid and hard material) are directed towards each other, at this speed the two micro-droplets meet each other. Because the two micro drops are electrified additionally and differently at the nozzle outlet 12 in each case, they are accordingly accelerated further toward one another by the two ring electrodes ( 15, 16) in order to collide at the collision point 11. Although it is a challenge to bring the two micro-droplets towards one another exactly and at the same time on the collision point, since these are much larger than e.g. single ions, optimal alignment is nevertheless technically feasible. In addition, the micro-droplets, due to their different electric charge and the increasing electrostatic attraction force towards each other, perform the last nano-course corrections themselves.The greatest risk of the micro-droplets being electrically charged is their jumping / explosion immediately after they have left the nozzles. The electrostatic fields can work against structural stability and force the atomic groups apart until the microdrop breaks. This effect occurs, for example, in the case of electric spray generators. While the microdroplets are to be broken there by electrostatic charging, this effect is undesirable and is to be avoided in our case. By the parabolic mirror shaped electrodes at each nozzle, the electrostatic fields are generated so that the microdroplets do not yet diverge as long as they are en route. However, in our short fluid jet path, this effect is virtually impossible. The path up to the collision point is very short and can be a few mm or even cm, wherein the time is no longer sufficient to break the microdroplet electrostatically. The electrostatic fields are built up concentrated along the flight path of the microdroplets and impart an additional thrust to them. The external electric field additionally has the effect that the coulomb forces in the microdroplets are largely suppressed, so that a cracking of the microdroplet is prevented even in the case of a longer path. Immediately before they reach the collision point (a few microns to collision), the electrostatic fields on the parabola electrodes are shut off extremely quickly to become neutral, which suddenly lacks an important stabilization component for the microdroplet due to lack of the external factor or electrostatic field. The microdroplet starts to destabilize itself, but it continues to fly at dozen km / s on the other microdroplet, also passing the same time. The two micro-droplets reach the collision point and, because they are charged differently, they increasingly attract one another. If a very short distance has arrived, their electrostatic charges are sufficient to cause them to crack, but the time is no longer. Although it may also happen in the case of strong electrostatic charge that they crack immediately before the physical collision with one another, the atomic groups formed thereby nevertheless collide with the groups from the oncoming microdroplets in a considerable number.The electric charge in the microdroplets and additional discharge between the nozzles and the respective surfaces on the facing ring electrode surfaces cause the microdroplets to become fast. In the collision, both microdroplets are additionally subjected to corona discharge and to nuclear fusion of a considerable number of atoms which are then simultaneously explosively decomposed in the atomic level and ionized particles. The two exploding microdroplets release atomic groups or ions which then strike the incoming subsequent microdroplets at high speed and in part continue to lead to core fusion. Although not all atomic groups or ions meet (only about 10-20% thereof), this is sufficient for usable fusion energy release. Thus, once the fusion is initiated in the reactor, further nuclear fusion reactions easily occur from the subsequently arriving micro-droplets, which then need not necessarily reach the exact point of collision to fuse.FIG. 5 shows a further exemplary embodiment. The dispensing of the microdroplets 2 takes place in a dot-line or dash-line manner in the overall shape of a very thin fluid jet ( 5, 6) each, the jet length of which is only a few centimeters or even millimeters. However, with a high repetition rate setting, the microdroplets are discharged for collision in rows, one after the other in a chain-like manner in a very high number. From 1 to about 2.2 million micro-droplets (or rather depending on the reactor control setting and energy requirement) per nozzle can be dispensed per second. The beam resulting therefrom is very thin and can be about 0.01113 mm in diameter. The nozzle also has this diameter. The circular area of a circle having the diameter is 0.01 μm 2. In order to realize the acceleration of the microdroplet, a part of the chamber (acceleration region) immediately before the nozzle region is with a diameter of approximately 0.0016 mm, which means a cross-sectional area of approximately 200 times greater (2 μm 2), than the cross-sectional area of the fluid jet (consisting of microdroplet rows). There, an end tip of the electrically deformable element is introduced and it brings about a fluid displacement by its expansion amplitude of only 25 nm, as a result of which two, per 100 picoliter micro drops can emerge from the nozzles at up to 50 km / s. Since the wall of the deformable element moving at a amplitude of 10 GHz and 2 to 5 μm generates an extremely high pressure for only 0.1 ns, the structural integrity of the chamber is maintained without problems, rather supported by its mass inertia of the construction / solid walls. The oscillating element is also not damaged as a result, because the expansion takes place at the atomic level and uniformly. In addition, electrostatic acceleration takes place here through the nozzle electrodes 17 and both ring electrodes (15, 16) in the middle.Depending on the reactor use, smaller powers or even powers can be generated. Smaller reactors, thus producing some MW of power, can serve as the motive power source for ships / container ships. Even smaller micro-fusion reactors (up to 100 KWh) would be well suited for both stationary and mobile purposes, for example, to propel vehicles.The variant from FIG. 6 additionally has an electron beam generator 35 (electron source), which directs an electron beam 36 directly onto the collision point 11. As a result of the electrical charging of the micro-droplets, these are cold-ionized, but nevertheless at least one of the fluid micro-droplets series is electrically neutralized by the electron beam 36 at the point of collision, such that they do not escape from one another but collide with one another. In the case of an electron excess on one of the two fluid rows, it will occur that the two mutually colliding micro drops are electrically attracted and thus promote nuclear fusion.FIG. 7 shows a further embodiment of this reactor. Here, in addition to hydrogen isotopes (D or T), the element boron 37 is used for fusion. In this case, two supply tanks (38 and 39) are installed, each of which is equipped with a volume of about 100-500 cm 3. In one, the hydrogen isotope (e.g., deuterium) 32 is attached in the liquid state, while the other is filled with water in which boron 37 is dissolved. Boron can also be introduced directly into the water in nanopowder form and can always be mixed through by a mixer 40 in the storage tank with water or heavy water in the storage tank. From the two tanks, minute quantities (e.g., 0.1 cm 3) each are placed in one of the high pressure chambers. When the micro-droplets have arrived there, they are generated from both fusible materials, which are discharged at high speed with respect to one another at a point of collision into the center of the reactor chamber. Here too, depending on the repetition rate, short or long micro-drop rows consisting of individual drops are generated, which meet at approximately 50 km / s. Here, the energy can be directly absorbed from the ions generated by fusion at the collision point by voltage collectors (current collectors) 65 of grid electrodes and charged in an electric capacitor (FIG. 16 ). This current could be routed to end users through electrical control and distribution systems. Here, the design would be much simpler because no steam turbines or other thermal energy converters are required. The element boron can be "dissolved" in the heavy water or else be accelerated together with the heavy water mass in the form of nanospheres and collide against the pure deuterium jet at the collision point. Boron can also be introduced directly into the liquid deuterium in one of the high-pressure chambers and collide with one deuterium fluid jet against the other fluid jet. It is likewise possible for both beams which collide with one another to be enriched with boron atoms. In this case, although boron atoms would collide against each other, boron would also collide with deuterium atoms, which could lead to fusion.Similar accelerating techniques for the microdroplets are also observed in ink jet printers. These also produce microdroplets in picoliter range (between 3 and 40 picoliters). However, the micro-droplets only reach about 5-100 m / s there, because there is no longer any need for them. In addition, the oscillation frequencies of the piezoelectric elements are designed to be significantly lower (KHz range). Here, in the invention, 10 GHz piezoelectric elements are installed, which oscillate with a 2-5 μm amplitude, as a result of which the microdroplets can be accelerated to 20-50 km / s.The picoliter micro drops which are additionally electrically accelerated may be deflected by an electrostatic cumulation lens (ring electrode) or electromagnetic coil for a more accurate meeting point. Because the microdroplets of the two nozzles are each charged differently, they once again attract one another immediately before the collision, and thus they automatically perform auto-course corrections in the nanoscale (FIG. 5 ). One microdrop with a positive charge strikes the other, negatively charged microdrop. The micro-droplets are not completely ionized here, but are electrostatically charged and roughly comparable to particles in weathering clouds. For additional acceleration, laser acceleration methods can also be used because the micro-droplets can be accelerated very high, but they are somewhat more inefficient in terms of energy consumption. This requires two laser sources (41 and 42) which emit short but very intense pulses of bundled laser beams (FIG. 8). These laser sources are illuminated from behind the micro-droplets directly after they leave the nozzles and are pushed to the collision point in a contactless manner by photon energy. The laser beam sources can emit very short, extremely strong pulses and their laser beams 43 can also be directed into the nozzles. Because the two laser beams also strike each other and are emitted on the same optical axis, they would also strike the oncoming microdroplet, at the end. However, the laser beam diameter is so small that the beam is completely shaded / covered by the drop, and when the drop is "illuminated", the beam then diverges greatly. The two laser sources can also be switched on and off alternately (e.g. with a 100 GHz repetition rate). As a result, each drop alternately experiences a plurality of micro-shear pulses up to the collision point.Unlike a continuous fluid jet, the micro-drop jet formation (micro-drop chain) has numerous advantages. It can be accelerated much more quickly and the fusion reactions can proceed more continuously, because the pressure on microdroplets can be generated more easily by piezoelectric elements ( 7, 45). In addition, the high-pressure chamber is filled very efficiently by injecting small amounts of fluid during the pause times between two micro-drop discharges, so that the pressure pulse remains constant again and again.FIG. 9 shows an exemplary embodiment in which the piezoelectric elements 7 are each installed in the high-pressure chambers. The high-pressure chamber is here produced hollow-cylindrically in a block of a solid construction. A rear end is closed, while the front end is provided with a nozzle. The nozzle is also of very massive construction and has a diameter of only 0.03 mm. The high-pressure chamber can also be dimensioned approximately as large. A 20 mm long hollow cylinder high-pressure chamber with a diameter of 0.03 mm, into which a piezoelectric element rod in the form of a cylinder with a diameter of 0.02999 mm is inserted, can generate the 100 picoliter drops. Nevertheless, the high-pressure chamber can also be larger.In Fig. 10 a high pressure chamber with an inner diameter of 1.2 mm and a length of 0.2 mm (but can also have other dimensions, e.g. be built between 2 - 50 mm) is shown, in which a piezo element is installed immersed in the chamber in the fluid. The piezo element is installed in the high-pressure chamber wall 26 in a guide channel 44 or in a depression there. The pressure surface 31 at the free end of the element serves to push the fluid as it extends electrically.FIG. 11 shows a further exemplary embodiment. Here, the piezo element is constructed in the form of a disc 45. The piezo element here has a disc shape with a thickness of 0.02-0.3 mm and a diameter of less than 0.1 mm. The high pressure chamber has a hollow cylindrical shape provided with the nozzle at one end and closed at the other end where the piezoelectric element in a disc shape is installed on the high pressure chamber inner wall 26 opposite to the nozzle in a disc shaped depression 46, with the vibrating axis of the piezoelectric element facing the nozzle. Here, the axes of movement (108, 109) of the two fluid formations or of the micro-droplets from both nozzles are no longer on a line, but meet at a wide angle 107 (about 176°-179°). Although this requires precise timing in the firings of the micro drops, the micro drops, in the case of a technically induced "delay" of the activation of the opposing nozzles and of the fluid generator, do not strike technically sensitive reactor parts but a blank or the stationary fluid which protects the reactor walls, so that a longer-lived construction can be realized therewith.The variant from FIG. 12 additionally has an electrical accelerator which accelerates the two microdroplet beams relative to one another by electrical discharge. Ideally, an extremely small spot electrode would be placed exactly at the collision point of the two micro-drop beams, which electrode would be negatively charged, while the two micro-drop beams are positively charged. This electrode would attract the two beams, but it would itself be a major problem because it is in the way and would also be rapidly vaporized by the heat of the fusion processes. Help in this case can provide a virtual electrode 47 consisting of an ion beam 48. A voltage discharge is produced via the ion beam from a high-voltage source 49, which runs through the collision point transversely, perpendicular / at right angles to the axis 9 connecting the two microdroplet beams. Application of a voltage to this virtual electrode and the two nozzles causes an electric attractive force to the micro-droplets of the two micro-droplet beams. In order to optimize the fusion process, the charges of the electrode and of the nozzles can be selected in each case such that the two mutually colliding microdroplets are charged differently, so that they are electrically attracting one another during the collision. By means of a control, the discharge voltage can be generated very quickly alternately for each micro-drop beam, so that a discharge never takes place simultaneously over both beams.Alternatively, an acceleration of two microdroplets of equal charge which are intended to collide with one another is also an acceleration which, however, are neutralized by an electron beam immediately before or exactly at the collision point (FIG. 12 ). FIG. 13 shows a further exemplary embodiment, wherein the microdroplets are only a fraction of a picoliter or at most a few picoliters in size. However, the repetition rate of the microdroplet generation is about 100 times higher for this purpose. Due to the very low mass of the micro drops, laser acceleration methods can also be used here. Two laser sources (41, 42) will strike the micro-droplets 2 and push them against each other towards the collision point 11.FIGS. 14 and 15 show exemplary embodiments with mutually crossing fluid jet formations. Here, the intersection angle of the two fluid jet formations is about 178°. The microdroplet which does not hit the other continues to fly up to a fluid mass 50 of the fusible material which is standing in the reactor chamber 23 and can emit its kinetic energy there, which, however, rarely also leads to nuclear fusion. The fusion chamber can rotate completely by an electric motor 64, whereby the standing fluid mass can be distributed better onto the reactor chamber wall. For acceleration, additional electric fields may be established here by crossing ring electrodes or circuit closures between a virtual electrode at the point of collision and the nozzle electrodes, which alternately attract the crossing fluid jet formations. The two circuits (each between the nozzle and the virtual electrode) are always quickly alternately closed. Here, each microdroplet is in open positive communication with the ring electrode disposed at the nozzle, electrically connected by electrical leads (53 and 54). The high-voltage sources (55 and 56) and their controller 57 alternately each produce an electric discharge which accelerates the microdroplet above the collision point 11 from the nozzle to the ring electrode. When passing through the collision point, one microdroplet strikes the other at very high velocity, which partly leads to fusion. In Figure 15, this device is provided with two ring electrodes (51, 52), each under high voltage from two separate voltage sources (55, 56), each mounted on the other side of the point of collision with the centres (58, 59) of which the central orifices (60, 61) are installed in the way of the respective fluid jet formation of the opposing nozzle. Thereby, the micro-droplets arrayed in the fluid jet formations passing the collision point without collision will each pass per fluid jet formation through the respective central opening of the ring electrodes, each ring electrode being electrically coupled to the opposing nozzles (3, 4) or nozzle electrodes (17, 18). By control, rapidly alternating voltage discharge per fluid jet formation will take place between the ring electrode and the opposing nozzle or nozzle electrode through the fluid jet formation concerned. The direction of flow through the fluid jet formations is such that it accelerates the micro-droplets in each fluid jet formation towards the point of collision.Additionally, a small amount of liquid deuterium or other fusible material that captures the micro-droplets passing the collision point without collision may be placed in the reactor chamber to protect the reactor chamber wall 62 from premature erosion. It should be mentioned that when very small micro-droplets (about 0.7 picoliter or less) are used as fuel for the fusion processes, heavy water or even simple water 67 is also suitable (FIG. 17 ). The extremely small water micro-droplets are thereby accelerated extremely strongly to almost 1000 km / s and then brought into collision with each other. If here a terahez electric field (oscillation frequency of at least 1.1 THz) is allowed to flow to the microdroplets through two electrode pairs (73, 77) in each case, then free electrons will form in the waterdrop, which can be electrostatically influenced. It may be helpful to incorporate additional alignment electrodes 66 on both sides between the collision point and the nozzles that extremely quickly build up and break down electrostatic fields, whereby the water molecules 68 in the fluid jet formation orient themselves such that, in the event of a collision, the hydrogen atoms are oriented forward in the flight direction (FIG. 18 ). Because the water molecule is a dipole, it will orient itself in the electrostatic field. Electrical acceleration of the micro-droplets may also be considered, but is not necessarily required. The alignment electrodes 66 here only cause the water molecule to align in the electric field to "extend feet forward" or to arrange the two hydrogen atoms in the water molecule forward (Fig. 18). The use of the hydrogen atoms 69 as a crumple zone for the water molecules brings some advantages. The hydrogen atoms of two water molecules actually collide increasingly with one another and not with the oxygen atoms ( 70), which in the case are positioned at the rear in the flight direction. The alignment electrodes 66 are relatively small and effect water molecule dippol alignment throughout the fluid jet formation (on both sides of the point of collision) or at least on the last millimeters prior to collision for each microdroplet, separately on both sides, respectively, as viewed from the point of collision. Due to the positioning and dimensions of the alignment electrodes, the electrostatic fields are actually most acutely exactly where they are needed. However, the fields are no longer active directly at the collision point or neutralize each other. This is also necessary because otherwise the colliding molecules would be equally oriented and this would not bring any advantage because the hydrogen atoms of one molecule would be opposite the oxygen atom of the other molecule. However, since the alignment already takes place separately on both sides before the point of collision, in each case in the fluid jet formations, the molecules are rotated optimally for nuclear fusion of their hydrogen atoms. The oxygen atoms in each case at the "tail" of the molecules push the hydrogen atoms more strongly towards one another due to the inertia, which promotes the nuclear fusion processes.FIGS. 19 and 20 show an orientation of the water molecules 68, which is effected simply by strongly concentrated microwave radiation from a microwave source. The microwave beams 75 are split into two beams, out of phase, and strike the water molecules perpendicular to their axis of motion. The oscillation amplitudes and oscillation phases of the two microwave beams, by the precise adjustment of the distance of the microwave radiator, are selected such that the water molecules on both sides, as seen from the collision point, with their hydrogen atoms facing each other. For such specific alignment, it is even better to align a separate microwave source (73 and 74) for each fluid jet formation immediately prior to the point of collision. These two microwave beams are parallel to each other and are in the opposite phase to each other, so that they put the water molecules of both micro-droplets colliding with each other in simultaneous rotation and bring them into a rotational position precisely at the time of collision, so that the two hydrogen atoms of one molecule meet the two hydrogen atoms of the other molecule coming in the opposite direction. The microwaves will strike the microdroplets from a precisely calculated distance and with a certain oscillation phase. Because the microwaves can rotate the water molecules not only partially but completely, this effect is used to rotate and align the water molecules through just before the collision of two microdroplets so that they reach exactly the rotational position upon impact, moving with the hydrogen atoms directed forward. Because the atoms in the microdroplet are neutral, no significant repulsive forces are expected between both microdroplets at the point of collision. Although the water molecules are rotated, by accurately calculating the rotational position, the microwave radiation can be generated such that at the time of impact the molecules are actually aligned such that their hydrogen atoms are located in the front in the flight direction and thus both molecules collide with their hydrogen atoms. The last micrometers will pass the molecules without the influence of the microwaves because two microwave beams, one for a fluid beam formation, will not contact each other and form a "gap" therebetween. It is important that the hydrogen atoms of both molecule groups of both micro-droplets colliding with one another are oriented toward the point of collision with the hydrogen atoms toward the point of collision. Although the alignment fields of alignment electrodes are missing immediately before the collision point, the respective alignments of the molecules for this short distance remain on both sides as viewed from the collision point, nevertheless exist. The time would no longer be sufficient to assume a different orientation by itself for the water molecules. Depending on the distance from the nozzle to the collision point, the molecular alignment can begin immediately before the collision point or even earlier. The alignment is very important because in this case the collisions are not allowed to randomly, but rather are optimized in a controlled manner. This is evident directly in the energy release intensity of the fusion reactor. The energy intensity always increases with the increase in the degree of alignment of the molecules with the hydrogen atoms with respect to each other. In this way, the reactor performance can also be controlled. It should be noted that when water is used as the fusion fuel, it is cooled down to exactly 4°C, it is best suited for fusion purposes provided that the micro-droplets are accelerated to 500 km / s or higher (up to 1000 km / s). The micro-quantities (a few microliters) of water in a stably built high pressure chamber, which is very narrow and long like a capillary tube, micro-expansion of the water, cooled to 4°C, can be initiated by some methods to generate the two micro-droplets. Here, an electric field, microwave radiation or laser source is sufficient to slightly decrease the density of water to increase the volume, and that with an extremely high speed factor. The expansion is greatest in the longitudinal axis of the high-pressure chamber. Any density change which is so small results in a flow of liquid through the very narrow high-pressure chamber into the longitudinal axis of the high-pressure chamber as far as an outlet opening through which the microdroplet is then accelerated. Each reactor, depending on its performance, dimensions and nozzle arrangement, may require different parameters. Optimization of the technical parameters, nuclear fusion procedures and energy balance can be determined by accurate reactor specific calculations and additional empirical values. This is necessary because only then can the reactor be operated economically in an optimum manner. The total energy balance should be far above 800:1 with optimum setting of all parameters (from 8:1 a mini-fusion reactor and from 1.7:1 a large fusion reactor can be operated economically viable).The water molecule has an electric dipole moment due to the different electron density of the oxygen and hydrogen atoms. In liquid water, these molecular dipoles generate an electric field whose strength fluctuates on a femtosecond time scale (1 fs=10 -15 seconds) and reaches peak values even up to 300 MV / cm for a short time. In such electric fields, an electron will leave its bound state in the water molecule (H 2 O) and tunnel through an energy barrier into the surrounding liquid (quantum mechanical ionization process). However, the electron returns extremely quickly to its initial state because the fluctuating field does not have a preferred direction and the electron therefore cannot move away from the site of ionization. Because of the highly efficient charge recombination, the number of free electrons remains very low (less than one billionth of the number of water molecules). An external electric field in the frequency range of approximately 1.1 to 1.2 terahertz (1.1-1.2×10 12 Hz) generated via two electrode pairs (76, 77) or two radiation sources can increase the number of free electrons by a factor of 1000. The THz field has a maximum strength of 2.5 MV / cm, but it has a preferred spatial direction. Along this preferred direction, the electrons generated by the fluctuating field are accelerated and reach a kinetic energy of approximately 11 eV, which corresponds to the ionization energy of the water molecule. This suppresses charge recombination at the ionization site. The electrons travel distances many nanometers before being localized to another location in the liquid. This effect can be used here for our purposes by generating two THz electric fields on each fluid jet formation immediately after the micro-droplets leave the nozzles. The electrons in the micro-droplets would be partially unbonded and an electrical acceleration of the micro-droplets would be significantly more efficient 1000 times higher). This would mean that the micro-droplets could be accelerated at an exit velocity of only 1 km / s from the nozzle, up to 1000 km / s electrically on the way to the collision point. At this impact speed, the conventional water drops are very well fusible and an enormous amount of energy per micro-drop collision would be released at the collision point (FIG. 17 ).FIG. 21 shows an exemplary embodiment, wherein the high-pressure chambers each have an inner volume that is so small that they can only accommodate one microdroplet at a time. Fluid intake occurs during pause times between two microdroplet discharges by injectors 28 and their microcapillary conduits 29. Because the microcapillary channels or conduits 29 are much narrower than the nozzle orifice, the extremely high pressure, lasting only about 0.1ns, does not seriously impact the design and will also hardly flow liquid back in the injectors. This can also prevent special electro-valves 62. The important factor remains here, too, the mass inertia of the installed components. The micro-quantities / micro-droplets of liquid are accelerated towards each other at very high speed (50 km / s or more). Electromagnets 71 or possibly strong permanent magnets 72 can also be used for the dipole orientation of the water molecules. However, these fields would accompany the water molecules from the nozzle to the point of collision and arrange the molecules to rotate forwardly with the hydrogen atoms (69), fly in the direction of collision (Fig. 22).The fusion reactors described here are lighter, more compact and are intended to have a relatively good efficiency or a positive, commercially usable energy balance. By using micro-droplets instead of fluid jets, some advantages are achieved in optimizing the fusion processes. In contrast to the reactors which operate with mutually colliding fluid jets, there are severe differences here. The micro-droplets are pressed out here using a completely different technique and, because they are accelerated individually, the micro-droplet reactor designs can achieve significantly higher collision speeds and improved output energy control. In addition, significantly lower loads are generated on high-pressure chambers here than in the case of the fluid jet variants, which brings about a longer durability of the materials used for this purpose. The extremely small high pressure chambers, which in some embodiments have only 1-100 picoliters of volume, which have very thick, stable walls (a few cm or dozen cm wall thickness), can withstand very high pressure values (millions or even billion bars) because the pressure there takes only about 0.1 ns. Not the material thickness, but rather the mass inertia of the walls guarantees the stability of the construction. The pressure waves which are conducted within 0.1 ns into the chamber walls are completely absorbed by the mass inertia, so that no damage to the construction is to be expected. Above all, even the very low displacement of 1-100 picoliters, makes very much the construction to remain stable. The incorporation of hard materials is also necessary here so that no microcracks can arise. Nevertheless, the fluid jet fusion reactors have an advantage over the microdroplet variant. In fluid jet reactors with continuous fluid jets or fluid jet pulses, molecules / atoms which are constantly pushing towards the collision point are fed towards the collision point, which molecules / atoms exert an extremely high contact pressure on the front ones which have already arrived at the collision point (similar to a train which would travel against a rock wall, wherein the rear cars continue to push the lok with an ever increasing force due to the mass inertia), whereby a good energy balance is produced by nuclear fusion. In the microdroplet fusion technique, this approach is lacking, but this is compensated for by the substantially higher kinetic energy. A high repetition rate, wherein only 0.5 to 18 diameter lengths would be present between the individual droplets, would also allow here the "contact pressure force" (pressure) at the collision point to be increased.Interesting embodiments have also been shown in Figures 23 and 24. Here deuterium oxide 67 is used for the fusion. The heavy water molecule (deuterium oxide, D 2 O) 68 is a dipole, as is a water molecule. A dipole arises when the distribution of charge in a molecule is not symmetrical, resulting in positive and negative partial charge. In the case of heavy water, the two hydrogen atoms have a partially positive charge, while the deuterium atom (a heavy hydrogen isotope) has a partially negative charge. This results in a dipole moment in the molecule. This property is used to accelerate the micro-droplets. The fluid accelerator or micro-droplet acceleration system herein is comprised of a coherent microwave source 78 (e.g., MASER or GUNN element / GUNN diode) that emits coherent microwave radiation 79 in the fluid directly in the high pressure chambers or in the fluid conduits or nozzles and moves the fluid molecules therein for synchronous rotation. Because deuterium oxide molecules, like water, also have dipole properties, microwave beams can be caused to move or rotate. If all molecules are rotated synchronously by the coherent microwave radiation, then during each rotation there are two rotational positions where the molecular assembly causes greater expansion in one axis and also two positions where the fluid contracts most strongly on the same axis. The speed at which D 2 O molecules rotate in microwave radiation depends on various factors, such as the frequency of the microwaves and the temperature of the heavy water. The rotation of a D 2 O molecule can take place at a characteristic speed of several billion revolutions per second. This speed is referred to as the rotational frequency. At room temperature (about 25 degrees Celsius), the average frequency of rotation of a water molecule is about 10 billion to 100 billion revolutions per second. At higher temperatures, the rotational frequency increases as the kinetic energy of the molecules increases. It is important to note that the exact rotational speed is influenced by various factors and can vary slightly from molecule to molecule. Electrostatic expansion of water by electric fields is a phenomenon that does not occur at normal household levels and temperatures, but well in the micrometer or even nano range. Electrostatic expansion occurs when an electric field is applied to a liquid or gas and the charges within the liquid or gas are re-oriented or even displaced. This may result in expansion or contraction of the material. With respect to heavy water, electrostatic expansion can be observed when placed in a strong electric field. In the case of microwaves, such rapidly changing fields are generated. The electric field causes the heavy water molecules to alternately contract and push each other and thus cause electrostatic expansion and contraction of the heavy water. The heavy water itself serves as an actuator and also generates the driving force for accelerating the own substance or micro-drip itself. Heavy water molecules, because they are dipoles and have a positive and a negative charge, will be directed into an electric field which can result in an expansion of the heavy water in one direction. This effect is referred to as the dielectric polarization or orientation polarization. By the action of an external electric field, these dipoles are always better rectified the stronger this field is. As the frequency of the electric field increases, this polarization disappears first, but the frequency must be relatively high. In the orientation polarization, which is produced by the orientation (orientation) of permanent electrical dipoles, e.g. water, in an electric field, the heavy water can also expand and contract. Their thermal movement acts against this orientation of the dipoles. The orientation polarization is therefore dependent on the temperature (the higher the temperature, the lower the orientation polarization), which is described by the Debye equation, so the fluid temperature is to be kept low. If the direction of the electric field is reversed, the dipole molecules must re-align (relaxation process). Because of their relatively high inertia, they require a certain time for this (typical rotational time of a molecule in liquid 10 to 100 GHz). The heavy water has a microwave absorption maximum at about 18 GHz (for water it is about 22 GHz). At even higher frequencies, no orientation polarization can be observed any longer, but only shift polarization, and the Debye equation changes over to the Clausius-Mossotti equation. Electrical polarization is a physical quantity from electrodynamics that characterizes the strength of the electrical dipole moment in a dielectric material. In the case of non-conductive materials, too, a displacement of electrical charges takes place over short distances of the order of magnitude of an atomic distance by applying an external electric field. Dipole molecules can be permanently oriented with DC voltage. At very low frequencies (below 1000 Hz), ions may occasionally change place and remain there (dielectric absorption) even after the external field has been switched off. With increasing frequency, dipole molecules are excited to periodically flip at about 10 10 Hz-provided they are not retained by a crystal lattice. In this case, enormous friction losses occur between adjacent water molecules in the case of microwave radiation. At 10 12 Hz, the ions oscillate about their rest positions in the molecule. Because the deflections are limited to fractions of an atomic diameter, the maximum possible polarization is quite small. In the heavy water molecules, the center of gravity of the positive and negative electric charges are clearly separated from each other. Therefore, these dipole molecules can be very well influenced in their directions by orientation polarization. The polarization vector direction and the extent are strongest there, with longer water molecule chain formation in the longitudinal direction of this chain. In our reactor this will be into the capillary conduit leading to the nozzle. In this case, a larger chamber (high-pressure chamber) is dispensed with. Thus, the capillary conduit is also a capillary high pressure chamber 80 at the same time. As a result of the heavy water molecule orientation, the volume on the fluid jet formation axis 9 (the virtual line connecting the two nozzles) is expanded and contracted in the nozzle direction at approximately 18 GHz. Each time during expansion, a microdroplet of about 1-100 picoliter is ejected through the nozzle. At the same time, the same also passes on the other side with the other nozzle. The two micro drops 2 meet at a collision point 11 approximately in the middle of the distance between the two nozzles into the reactor chamber, and the molecular bond is destroyed and the partial fusion between the deuterium atoms occurs. By this fluid accelerator, which consists of the capillary high-pressure chamber 80 and a microwave source 78, emits coherent microwave radiation in the fluid directly into the capillary high-pressure chamber 80 and brings the heavy water fluid molecules to rotate synchronously there, and thereby excites the fluid to expand and contract rotationally and thereby to the micro-expansion rotating vector, a sufficiently large expansion is excited in the fluid jet axis 9. Because the capillary high pressure chamber is several millimeters long, the longitudinal dimension will be most embossed, generating a fast moving microdrop from the nozzles each time in the jet direction. The longer the capillary that functions as a high pressure chamber, the higher the oscillation amplitude. Although it is a very narrow capillary high pressure chamber, it nevertheless has massive and stable walls that are as large as several dozen cm in size for larger reactors. The liquid can only be dispensed in microdroplet form through the open end 84 while the trailing end 83 of the capillary high pressure chamber is closed. The microwaves need not penetrate transversely to the capillary high pressure chamber longitudinal axis. They can also penetrate in the longitudinal axis direction. The coherent microwave radiation can enter the capillary high pressure chambers via the open entrances at an oblique angle or can be transmitted directly to the fluid through a stable ceramic wall 81 (FIG. 23 ). Here, no nozzles are installed either, because the micro drops flow out directly from the capillary high-pressure chamber.The fusion fuel can be replenished directly into the capillary (high-pressure capillary chamber). It can be injected directly through an injector via the nozzle orifice into the capillary chamber during pauses between two pulses each generating a micro-drop. Figure 24 shows the rotations of the deuterium oxide molecules and their orientation polarization. As a result of the microwave energy, these molecules are rotated synchronously at up to 18 GHz and the electric fields thereby come about in an attracting and a more intensive repulsive state, which slightly changes the distance between the molecules. The microwaves drive almost all molecules in the capillary high pressure chambers into synchronous rotation. An expanding force is generated rotating in all directions. However, due to coherence and polarization of the microwaves, the rotation of the molecules is designed to take place on a perpendicular to the line connecting the two capillary high pressure chambers. Although this does effect an expansion only on one plane, the expansion vector force always rotates, e.g. clockwise. Thus, the axis of rotation 85 of the molecules is perpendicular to the longitudinal axis 82 of the capillary high pressure chamber 80 and because all molecules are rotated synchronously, they will all simultaneously come closer together, often repel each other. The capillary high pressure chamber is narrow (diameter in the micrometer range). Although the length thereof is also very short, it is nevertheless a few millimeters (or shorter). However, the ratio between diameter and length of the capillary high-pressure chamber is about 1:5000 or more. Thus, an extension which is arranged transversely to the longitudinal axis 82 of the capillary high-pressure chamber is virtually meaningless compared to the extension in the longitudinal axis direction, which is 5000 to 120,000 times larger in this case. By chaining the molecules into the capillary high pressure chamber, the distance increase between the molecules sums as the vector expansion force rotates so far and comes to a position coincident with the longitudinal axis of the capillary high pressure chamber. Expansion is greatest here and this produces the enormous high pressure which accelerates the microdroplets towards one another. By longitudinally positioning the fluid mass and volume into the capillary high pressure chamber, the compressive force on the microdroplet is automatically and automatically generated by microwave energy. In this case, not the thermal energy is the external force for the enormous high pressure, but rather the alignment of the molecules in the specific phases. The molecular alignment acts almost as in the case of the piezoelectric elements a micro-expansion of the material (here liquid), which acts like an expanding chain in the longitudinal direction of the capillary high-pressure chamber. The microwave source must be quite intense because the radiation pulses are also extremely short. MASER or powerful GUNN elements can be used if their microwaves can be focused on very small areas. The microwave sources may also be installed at the closed end of the capillary high pressure chamber and deliver their beams into the liquid in the longitudinal axis direction 82 (Fig. 25).It should be noted that the picoliter microdroplets may also be generated by electrostatic fields when the liquid in the capillary high pressure chamber is extended into the longitudinal axis 82 by dielectric polarization or orientation polarization. This would require for each capillary high pressure chamber, one electrode 86 in each of the capillary high pressure chambers and another electrode 87 in the open end of the capillary high pressure chamber. A combined variant has been shown in FIG. 25, wherein electrostatic fields or microwaves are used for the expansion of the liquid. By applying a voltage between electrode 86 and 87, the liquid is extended "chain-like" for a short time in the longitudinal direction and thereby accelerates a microdroplet. The expansion will become more and more pronounced the further the molecules are in the direction of the open end into the capillary high-pressure chamber. Field build-up and degradation should be extremely fast (within 0.01-0.1 nanoseconds).Unfortunately, the reactor constructed in this manner can be immortalized after several days or weeks of continuous operation to the extent that it requires new replacement parts. The most stressed and wearable parts are the fluid accelerator and the nozzles, or the two capillary high-pressure chambers. There are, however, almost daily reports of new, better and long-lived materials which can also be used here.Carbon meta materials with Cu atoms doped in the crystal lattice can also be incorporated as acceleration actuators for the fluid accelerator. There has been a prototype for a few weeks capable of generating 0.8 μm amplitude oscillations with approximately 258 GHz. In this case, it could accelerate microdroplets to approximately 206.4 km / s. This is because the better durability of this material. Other meta-materials with independent regeneration properties are also optimally suitable for this reactor. Such meta-materials are ideally suited for the nozzles and for the capillary high pressure chamber because they oppose the erosion of the material by "self-healing" properties.The embodiment in FIG. 26 shows a simple, but nevertheless readily usable variant of the reactor. Here, the capillary high pressure chamber is filled with deuterium oxide (heavy water), the heavy water being cooled to a temperature which brings about its maximum density, and this is about 11.2°C. At this density, any specific change in the orientation of the dipole molecules can lead to a density variation of the total fluid mass into the high pressure chamber. This process can be used here for an extremely strong increase in pressure within 0.01-0.1 ns. The reactor has corresponding cooling systems. For this purpose, temperature-controlled and sensor-controlled Peltier elements 88, for example, are monitored by temperature sensors 89 and a controller 90 for this purpose. This allows a precise temperature of 11.2°C to be maintained in the high pressure capillary chamber and in the heavy water. Once the two microwave radiation pulses are respectively emitted in the heavy water in the capillary high pressure chambers, the heavy water is extended in all directions, but extension in the longitudinal axis is strongest because the molecular array is longest there. Also a temperature change of a few degrees causes the expansion of the liquid. This temperature difference can be achieved within 0.1 ns because the amount of liquid is in the picoliter range. Each expansion promotes the production of microdroplets which are then discharged at the open exit. A wetting layer 91 of water or heavy water protects the reactor wall construction from abrasive effect of the flying particles from the nuclear fusion point where the micro-droplets collide with each other. Two or more additionally installed alignment field electrodes 92 mounted on the microdroplet travel axis 93 and at the point of collision can favorably arrange the D 2 O molecules immediately before reaching the point of collision so that they actually collide with the deuterium atoms (FIG. 28 ). The alignment is performed separately and immediately before the collision for each micro-drop. To optimize alignment, a plurality of alignment field electrodes / cathodes 92 may be switched to generate a running electric field that is generated in synchronism with the movement of the microdroplets, which respectively travel from the exits of the capillary high pressure chambers toward the point of collision and which are seen on either side from the point of collision. It is sufficient if the micro drops pass the ring-inside region between the electrodes / ring cathodes in contactless fashion and are under a strong electric field before they reach the cathodes. Once the microdroplet has approached the cathode center to about 1.5 mm, the field is turned off and the next ring cathode (92,94), which is closer to the collision point, is turned on. In this manner, just before the microdroplet enters the center point 97 of the ring-shaped cathode 92, it is turned off, so that when the microdroplet comes behind the cathode, no disturbance of the molecular arrangement follows. Thus, the electric running field is generated which keeps the orientation of the molecules in the two micro-droplets further up to the collision point. The array arrangements of ring cathodes are designed so that the D 2 O molecules of each microdroplet align at the point of collision, with the oxygen atom being placed at the back. When using multiple ring cathodes, neither of which is intended to be in the point of collision, the point of collision is not under electric field.The molecular geometry of the D 2 O produces a negatively and positively charged region in the molecule. Such a molecular geometric state forms a dipole, which occurs with both H 2 O and D 2 O. When an electric field is now in the vicinity of a dipole, it is aligned, similar to the elementary magnets in a magnetic substance. In Fig. 27, the ring-type electrically negatively charged cathode 94 is disposed at the center at the point of collision, which is supplied with high voltage by a high voltage source 95 which then aligns the water molecules in the two micro-droplets, which flow toward the point of collision with each other, with the hydrogen atoms / deuterium atoms toward the point of collision. The two exits of the capillary high pressure chambers are each positively electrically charged (by electrodes 87 or anodes 96) and more draw the oxygen atoms toward them. For this purpose, the outputs can be used directly or extra incorporated anodes 96 can also be incorporated. In the variants that have nozzles, the material of the nozzles can be placed under tension, so that the micro-droplets can orient themselves thereon.Figure 29 illustrates the orientation of the dipole molecules by pulsed microwave radiation in a somewhat larger high pressure chamber 63. The incompressible liquid is irradiated by coherent microwaves 79 and the molecules therein are rotated. With each rotation, the total volume of liquid becomes extremely slightly larger (expanded) once and extremely slightly smaller (shrunk) once. The molecules are fully rotated once by a very short microwave pulse, having a maximum extension at a rotational position and a minimum extension at a position offset 180° therefrom. Thus, the liquid is given a maximum density and a lower density alternately, pulsating by the coherent microwave radiation. Decisive in this technique are the dimensions of the high-pressure chamber, the dimensions of which in the microwave radiation direction should be only about 12.5% or one eighth of the wavelength of the microwaves. The pulse duration is controlled by a controller which controls the microwave source 78. The liquid is hardly heated by the strong microwave pulse, but heating may also be helpful to promote expansion. When using heavy water, the temperature of the liquid should be about 11.2°C because then the density is highest (similar to the density nanomalie of the water, at which the density is highest at 4°C). In this case, any temperature change would also cause expansion. The expansion takes place identically in all directions throughout the liquid, but due to the geometric shape of the high-pressure chamber (long and extremely narrow), the expansion in the longitudinal axis of the high-pressure chamber is many times higher because the molecules, as in a chain, move one another in the longitudinal direction, this displacement increasing with the "chain length". As a result of the expansion, extremely small quantities of liquid flow out of the two inflow fluid channels / capillary channels ( 29, 98) in the form of micro-droplets 2 at a very high speed, which collide with one another. The orientation of the dipole molecules outside the capillary up to the collision point 11 takes place by the ring cathode 94.Any method that causes the dipole molecules to rotate can be used for expansion. However, the rotation of the molecules should take place completely simultaneously and the molecules must all have the same alignment. In addition, the energy for the rotation of the dipoles must be fully deployed within 0.01-0.1 ns. In addition to microwaves, dipole alignment can also be accomplished by laser beams. In this case, extremely short laser pulses must be emitted which can rotate the dipole molecules. Laser induced expansion allows the liquid to expand slightly within less than 0.1ns. It is also possible to influence the spin axis direction of the atoms by very strong magnetic field pulses. Due to the thermal energy of the cores at normal temperatures, the dipole moments are aligned almost completely isotropically. Here, the fact is used that the atomic nuclei of hydrogen (protons) have an intrinsic angular momentum (spin) and, linked thereto, a magnetic dipole moment. If such a core is placed in a static magnetic field, its energy is lowest if the magnetic dipole moment is aligned parallel to the field vector. Atomic cores are subjected to a torque that attempts to orient the direction of the magnetic moment in the direction of the magnetic field. Because of the inherent angular momentum of the atomic core and the maintenance of the angular momentum, this results in the precessional motion of the core. The precessional movement of the nuclear spins takes place with the Larmor frequency. It depends on the strength of the external magnetic field and on the core. For protons at 1 tesla, it is about 42.58 MHz. A high-frequency auxiliary field, which oscillates orthogonally to the static magnetic field in the transverse plane and whose frequency is resonant with the Larmor frequency, deflects the cores in phase-synchronous manner from their random, current position with respect to the static field. The magnetization is tilted from the direction of the static field, a transverse magnetization is produced which, with a correct duration of action of the alternating field, can be at most just equal to the original longitudinal magnetization (saturation). In this way, an overall volume increase into the high-pressure chamber can also be effected. For our purposes we need to increase a volume of a total 2ml volume of liquid into the high pressure chamber by only about 200pl, which means a volume increase of 0.00001%. For 20 ml of liquid, this would even decrease to 0.000001%.An extremely rapid expansion of the fluid, e.g. consisting of liquid deuterium or of heavy water, can be achieved very efficiently by laser technology. As numerous experiments can be found in some publications, for example under the name "The fastest water cooker of the world", show that it is possible to heat water to 100,000 degrees Celsius in 0.0000000000075 seconds-with a powerful X-ray laser. When water or heavy water is heated, the molecules move more and more vigorously. However, the heating with the laser works somewhat differently. At the U.S. SLAC National Accelerator Laboratory, the research team irradiated a jet of water with strong ultra-short x-rays. The beam carried the electrons from the water molecules, thus bringing the electric charges out of balance. The atoms are thereby repelled and begin to move very quickly. In less than 75 femtoseconds, the water reached more than 100,000 degrees Celsius in the test. Upon heating by the laser beams, the water was slightly expanded, but nevertheless retained the density of a liquid and this is a very important aspect demonstrating that nuclear fusion can also function by colliding micro-droplets of liquid deuterium or even deuterium oxide. The slight expansion of the liquid occurs extremely quickly and this is sufficient for us to generate the micro-droplets and let them collide against one another at high speed. From the experiments, the scientist wanted to learn more about water and its properties. This is because the water and also the heavy water behave atypically, due to its density anomaly (at 4° C., or 11.2° C., respectively).Particles can likewise be accelerated with lasers. For this purpose, laser physicists shoot with ultra-short, extremely strong laser pulses onto material, usually onto thin metal foils, and thereby generate a plasma in which the electrons are released from the atomic nucleus. The high energy of the laser pulse produces a strong, directed electromagnetic field which is capable of accelerating the protons. The same can be done with microdroplets. A variety of micro-droplets, arrayed in a beam formation, theoretically allow a high laser bombardment repetition rate of up to several million times per second and bombardment thereof can produce directed proton beams. FIG. 30 shows an exemplary embodiment, wherein a strong ultra-short pulse laser source 100 (femto pulse laser source) is used to heat the micro-droplets before, or directly at the collision point so strongly and within femtoseconds that they accelerate a part of the atoms extremely quickly towards one another and excite them to nuclear fusion. In this case, all the two micro-droplets are struck perpendicular to their movement axis 9 on a path about 1810 nm before the collision point by laser pulses 101 and these are brought to an enormous temperature. The two microdroplets react somewhat with delay, so that they each travel 905 nm as far as the collision point and break apart quite precisely in the collision point 11 (a few nanometers before), wherein their particles meet on an approximately 47° angle-wide circular sector. As a result of the enormous increase in the velocity of the particles there (atoms, ions), nuclear fusion and energy release increasingly occur.The energy released by nuclear fusion of micro-droplets can be captured in three forms: thermal energy, high energy light (gamma, X and UV radiation), and direct electrical energy from the ion charges captured by collectors. The thermal energy makes the greater part thereof. The light energy can also be converted into current in part by special solar cells 99, which are also used in UV laser technology Bere8ich. These solar cells are capable of capturing very intensive, high-energy light (even over the visible light spectrum) and converting it into current. Such solar cells are used for experimental purposes in laser energy transfer devices, wherein a laser (UV or blue) projects over several hundred meters its bundled beams onto a small solar cell, which then converts the light into current.The uniform core of all exemplary embodiments and of the patent claims specified in the application lies in the solution which, with the aid of micro drops which are generated as single drop emission not in liquid jet form but in portioned micro quantities, generates nuclear fusion processes by means of their collision and efficient alignment with the aid of electric fields. Single microdroplet emission has numerous advantages over nuclear fusion reactors using colliding fluid jets or the variants using hard projectiles and targets. The micro-droplets are significantly more efficient to accelerate than shooting fluid jets or projectiles onto targets. Although the liquid jet fusion reactors have the mass which is fully successful at the collision point because the liquid molecules always travel subsequently to the collision point and additionally exert a high pressure on the atoms already located at the collision point, the microdroplet technique spots at significantly higher speeds at the collision point (above 50 km / s), the longer-lived and simpler construction, the better scalability and the somewhat higher energy output efficiency.As mentioned, we have available numerous methods by which ultra high pressures on micro liquid quantities can be generated. The pressure values and a compression can be generated by deforming the walls and reducing the volume of the high-pressure chamber, by deforming an electrical element drin, or also by the "deformation" of the liquid. If the atoms or molecules migrate into the liquid, synchronously and in the same direction, the distance between the molecules can be slightly changed by their orientation vector. This occurs in a flashing manner upon application of a voltage, laser beam emission or microwave irradiation applied to the liquid. The pressure values are thereby enormous, but they are maintained extremely short (0.1ns), which is perfect for our purposes. The inertia of the solid walls in the high pressure chambers significantly helps maintain structural stability of the design.For fast successive micro-droplets delivered at a distance of about 1-200 times the micro-droplet diameter (assuming a spherical micro-droplet hypothetically) in a fluid jet formation, the rate of fusion and energy release increases dramatically. In this case, two fusion points (102 and 103) are produced which no longer coincide with the collision point 11 of the microdroplets 2. The two fusion points (102, 103) each move in the opposite direction from the collision point 11 and are slightly closer to the nozzles or high pressure chamber outlets. Therefore, only a high initial energy is required here, because once "ignited", the nuclear fusion almost runs through by itself (FIG. 31 ). It is only necessary to always supply micro drops in good time, which do not have to follow much too close and also not much too far behind one another. If they are much too close, then they ignite chain-like all micro-droplets that are on the axis of movement on the way to the collision point and the fusion points get much too close to nozzles. If they are far too far away, then the number of ultrafast particles is much too small (square fusion rate drop with distance). The optimal distances between subsequently emitted micro-droplets can be determined mathematically for each fusion reactor size and also by empirical values. The distances are reliably controlled by the electronic control, whereby these can be accurately controlled. At optimal intervals, the subsequent micro-droplets, by their inertia alone, also protect the nozzles and the outlets of the high-pressure capillary chambers from damage that the high-energy particles might cause. Finally, it is the interest of operators to implement long-lived design measures for such reactors.The high-pressure chambers or capillary high-pressure chambers can be filled with the fusion material or liquid 106 capable of fusion via microchannels (ultracapillary fluid lines) 98 arranged obliquely in the flow direction, which open into the chambers (21, 63) or capillary high-pressure chamber (80) at a very narrow angle (e.g. opening angle of 2°-10°). For a back flow function, micro-Tesla valves 105 can be incorporated. In Tesla valves, the double-sided permeability continues approximately up to a Reynolds number of 100 (Reynolds number is the size determined by the raw radius, the viscosity of the liquid and the flow rate). However, as the Reynolds number increases to over 200, the Tesla valve will abruptly become the fluid flow switch and direct it in one direction only. The value of 200 is here rapidly exceeded, especially by the flow speed. Moreover, only due to the very oblique angular position of the opening or opening angle 104, hardly any penetration occurs back into the inflow line (FIG. 32 ).Figure 33 illustrates an embodiment in which laser induced expansion of the fusible fluid is used. Strong laser pulses (IR or UV or X-ray laser beams 111) of extremely short duration (less than 0.1 ns) by IR or UV or X-ray laser sources 110 are emitted onto the liquid (fluid deuterium or heavy / super heavy water) and these are caused to expand by the same dipole orientation. The laser source may be an IR laser source, a UV or even X-ray laser source 110. Irradiation of the fusible liquid takes place either in the high pressure chamber / capillary high pressure chamber (63,80) or outside, directly in the micro-droplets 2 immediately before the collision point 11. When this occurs within the high pressure chamber, the pressure is generated there. However, because the expansion is very small and is only sufficient for the generation of a microdroplet, the extremely high pressure is generated only for 0.1 nanosecond and this can be accommodated by the inertia of the solid high pressure chamber walls, so that the construction does not fly apart. Between the strong repulsive force of particles at very small distances due to steric effects and the Coulomb force repulsive at medium distances, there is a primary minimum at distances in the range of the inverse Debye Hückel parameter. Here, van der Waals attractive force exceeds electrostatic repulsion. At greater distances, the surface charge results in electrostatic repulsion and, consequently, an energy barrier at intermediate inter-particle distances. The height of this barrier can be reduced by increasing the ionic strength of the medium, which can be achieved without problems by laser irradiation.It must be borne in mind in the invention that the microdroplet delivery only into the first path section is relatively compact. Thereafter, as the distance is removed, the shape of the microdroplets changes rapidly. Short paths from the generation of the micro drops to the collision point are therefore sought. The shorter the path, the better the efficiency. However, a much too short path may speed up the wear of the reactor components. Therefore, a trade-off in path length selection, which is dependent on reactor performance expectation, must be specifically calculated or found for each reactor.An embodiment in which the path from the point from where the micro-droplets leave the nozzle (or chamber exits) to the point of collision of the two micro-droplets is adjustable has been illustrated in Figure 34. Here, the two nozzles are not rigidly connected to one another in the entire construction, but are designed to be movable from and to one another. For this purpose, electrical actuators (actuators) 112 (linear actuators / actuators or locking systems) are used, which can make the distance between the two nozzles variable. Instead of electric actuators, manual adjusting devices can also be installed. With this construction, even the collision angle 113 can be adjusted at any time by additionally installed angle adjusting actuators 114 (FIG. 35 ). In this case, the structures in which the nozzles are located in each case are rotated slightly about a rotation axis 115 such that the collision angle ( 113) of 180° comes to a somewhat smaller value, for example 176°- 179°.Optimized design of the high pressure chambers / capillary chambers, selection of the frequency of the electromagnetic radiation source (microwave source or laser source), and installation of a mirror / reflector 117 on an inner wall of the chamber may promote the formation of standing waves 116 in the high pressure chambers that control synchronous rotation of the dipole molecules (FIG. 36 ). The entire chamber can function as a wave resonator and generate the super-high pressure values within 0.1 ns. This ultrafast micro-expansion generates the micro-droplets which fly on each other at over 50 km / s. Because the pressure values are reduced again extremely quickly in all variants, the mass inertia of the chamber walls will reliably prevent the construction from being destroyed.In the embodiment in which the laser radiation impinges on the micro-droplets outside the high-pressure chamber, the micro-droplets are caused to break up, the constituents of which then impinge on the micro-droplet located at the collision point, which micro-droplet was likewise broken up simultaneously. It is interesting that here the fusible liquid (e.g. liquid deuterium or heavy water) can be additionally mixed with conventional water. In the case of liquid deuterium, of course, the water should be injected in picoliter quantities within a few than 1 ns, otherwise it freezes. The water masses in the nanogram range bring their dipole properties with them and can cause an expansion of the entire fluid volume by means of ultra-short laser pulses, which can be used as a "propellant" for the acceleration of the micro drops to the collision point 11. The problem is not present with heavy water and the water is always in the liquid state. Heavy water also has dipole properties and thus dilution with water is not required.Unfortunately, once the micro-droplets leave the nozzles or outlets, due to the enormous high velocity, they do not retain their shape during flight to the collision point. The molecules or atoms in the fluid drop would thus not remain in a compact molecular / atomic formation, but they begin to scatter. However, due to the short distance they must travel, they do not have much time to achieve a nano-sputtering state. In addition, the molecular layers of the microdroplets that are in direct contact with the inner nozzle wall form a peripheral sliding film in the form of a "sliding shell" for the centrally located fluid masses and assist in the "compactness" of the microdroplet. This promotes nuclear fusion due to the extremely high kinetic energy and collision of two micro-droplets at the collision point.LIST OF REFERENCE CHARACTERS1 Fusion reactor 2 Micro-droplets / micro-droplets / micro-quantities of incompressible liquid / fluid 3 Nozzle A 4 Nozzle B 5 Fluid jet of micro-droplet formation / fluid jet formation A 6 Fluid jet of micro-droplet formation / fluid jet formation B 7 Piezo actuators / piezo drive elements / piezo element 8 Electrostatic "outer shell" 9 Fluid jet formation axis / virtual line / micro-droplet movement axis 10 Crossing angle, wide angle 11 Collision point, Center 12 nozzle orifice / nozzle orifice 13 atom groups 14 insulator ring 15 ring electrode A 16 ring electrode B 17 nozzle electrode A 18 nozzle electrode B 19 ring electrode orifice 20 ion channel (current discharge channel) 21 pressure generators, Fluid accelerators 22 High-voltage source 23 Reactor chamber 24 High-pressure chamber A 25 High-pressure chamber B 26 High-pressure chamber walls 27 Storage tank / storage tank 28 Injector 29 Capillary line / fluid line / inflow line or inflow channel 30 Short line chamber 31 Pressure surface 32 Liquid deuterium 33 Hollow sphere wall 34 Expansion side 35 Electron beam transmitter / electron emitter / electron source 36 Electron beam 37 Element boron 38 Storage tank A 39 Storage tank B 40 Mixer 41 Laser source A 42 Laser source B 43 Laser beams 44 Guide channel 45 Piezoelectric element in the form of a disk 46 Disk-shaped depression 47 Virtual electrode 48 Ion beam 49 High-voltage source 50 Stand Fluid mass 51 Crossing ring electrode A 52 Crossing ring electrode B 53 Line A 54 Line B 55 High voltage source A 56 High voltage source B 57 Controller 58 Center A 59 Center B 60 Center opening A 61 Center opening B 62 Electro valve 63 High pressure chamber / high pressure chamber 64 Electric motor 65 Voltage collectors 66 Additional electrodes / alignment electrodes 67 Water / heavy water 68 Water molecules / deuterium oxide molecules 69 Hydrogen atoms / deuterium atoms 70 Oxygen atoms 71 Electromagnets 72 Strong permanent magnets 73 Microwave source A 74 Microwave source B 75 Microwave beams 76 THz field electrode pair A 77 THz field electrode pair 78 Coherent microwave radiation source 79 Microwave radiation 80 Capillary high pressure chamber 81 Ceramic wall 82 Longitudinal axis of the capillary high pressure chamber / longitudinal axis line 83 Closed end of the capillary high pressure chamber 84 Open end of the capillary high pressure chamber / outlet of the capillary high pressure chamber 85 Axis of rotation of the molecules 86 Electrode into the capillary high pressure chamber 87 Electrode in the open end of the capillary high pressure chamber 88 Peltier element / cooling element 89 Sensor 90 Control for temperature compliance 91 Wetting layer (e.g. water or heavy water) 92 Alignment field electrodes / cathodes 93 Micro-drop travel axis 94 Ring electrode at the point of collision / cathode / ring cathode 95 High voltage generator / high voltage source for alignment the molecules 96 anode the open end of the capillary high-pressure chamber 97 center point of the annular cathode 98 capillary channels / inflow fluid channels 99 solar cell (for higher light energy / UV light) 100 ultra-short pulse laser source / femtolaser 101 laser pulse / femtolaser beam pulse 102 fusion point A 103 fusion point B 104 junction angle 105 micro-Tesla valves 106 fusible liquid 107 angle of the movement axes of the micro-droplets 108 movement axis A 109 movement axis B 110 IR or UV or X-ray laser source 111 IR or UV or X-ray laser beams 112 actuators (actuators) / linear actuators / actuators or locking system that makes the distance between the nozzles variable 113 collision angle 114 angle adjustment actuators / actuators or angle locking system that can adjust the collision angle 115 rotation axis of the structure 116 standing shaft 117 mirror / reflectorReferences included in the specificationThis list of documents cited by the applicant has been produced in an automated manner and is only included for the better information of the reader. The list is not part of the German patent application or utility model application. The DPMA does not take any adhesion for any faults or omissions.Patent Literature citedUS 10322827B2

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[0037] F. Frank and Andrej D. Sacharov predicted and 10 years later by an incidence of Luis

[0053] Chemker Martin Fleischmann and Stanley Pons and studied on 23.03.1989

[0054]

Claims

Nuclear fusion reactor with a reactor chamber, characterized in that it comprises at least - a storage tank (27) which is filled with a fusible liquid (106) or fusible fluid, - a high-pressure chamber (63), - a fluid line (29) and valve control which directs the liquid or the fluid into the high-pressure chamber in very small, portioned quantities, - at least two nozzles (3, 4) which are directed towards one another at a distance or almost touch one another or high-pressure chamber outputs which are installed in the reactor chamber (23), which are evacuated to a greater or lesser extent and in which micro-drip collisions take place, - a fluid accelerator (21) or a micro-liquid quantity acceleration system which consists of one or more fluid accelerators, which accelerate the fluid from the high-pressure chamber (63), pulse-wise in small portioned quantities, in the form of in each case two individual micro-quantities or micro-droplets (2) via the two nozzles (3, 4) or high-pressure chamber outputs directed towards one another, to a plurality of km / s simultaneously with one another over a short distance, - a controller (57) which controls the fluid accelerator (21) or the micro-liquid quantity acceleration system in such a way that it generates high pressure values in pulse-like fashion and the micro-quantities or micro-droplets are arranged in series in a row in an adjustable number per unit of time and waiting times between the generation of the individual or successively line-like, micro-quantities or micro-droplets (2) which move rapidly to a collision point (11), on in each case one fluid jet formation (5, 6 ) consisting of individual micro-droplets (2) separated from one another, of both nozzles (3, 4) or high-pressure chamber outlets simultaneously emerging and in the process the micro-quantities or micro-droplets (2) from one nozzle strike one another frontally at the collision point (11) for micro-quantities or micro-droplets of the other nozzle, - an energy dissipation system which dissipates the excess energy from the nuclear fusion processes.Nuclear fusion reactor with a reactor chamber according to Claim 1, characterized in that it comprises at least - a pair of electrodes consisting of two joined annular electrodes (15, 16) and an annular electrical insulator (14) installed therebetween, which are installed in the reactor chamber (23) as centrally as possible between the two nozzles (3, 4) or the high-pressure chamber outputs, - a high-voltage source which places the two electrodes (15, 16) under high voltage, - an galvanically separate or a further high-voltage source which is coupled via electrical lines in each case to the nozzles which electrically charge the small micro-droplets of the fluid from the two nozzles differently, the electrical polarity of which is selected such that the fluid droplets which are swept from the nozzles in the direction of the pair of electrodes, The method according to the invention is characterized in that the method according to the invention is characterized in that the method according to the invention is performed by the method according to the invention is performed by the method according to the invention in which the electrode pair is electrically attracted by the aligned nozzles on both sides, an electronic control which controls the two fluid accelerators simultaneously and charges the nozzles and the two ring surfaces of the electrode pair electrically via the high voltage sources such that the electrode pair electrically attracts the two micro drops which are discharged from the nozzles toward the center of the circle which the ring-shaped electrode pair simultaneously, an energy dissipation system which dissipates the excess energy from the reactor chamber to the outside directly as a current of charged particles, or is configured as a thermal dissipation system which is coupled to an energy conversion system which produces electric current.Nuclear fusion reactor with a reactor chamber according to claim 1 or 2, characterised in that the high-voltage sources are two separate sources (55, 56), the circuits of which form a closed circuit through a nozzle (3, 4) or nozzle electrode (17, 18) in each case, via the microdroplet row produced by the nozzle in the form of a microdroplet formation fluid jet (5, 6) up to the ring electrode surface (15, 16) applied to the respective nozzle.Nuclear fusion reactor comprising a reactor chamber according to any one of the preceding claims, characterized in that it comprises a controller generating, via the high-voltage sources, pulse voltages which are accordingly discharged in pulses on the microdroplet rows simultaneously or alternately one after the other.Nuclear fusion reactor with a reactor chamber according to any one of the preceding claims, characterised in that it is equipped with two separate storage tanks, one filled with hydrogen isotopes in the liquid state and the other with boron or boron isotopes (37) in the liquid state or dissolved in a liquid solution, from which jets of fluid directed towards each other, each consisting of a series of micro-droplets, emerge through the built-in nozzles.Nuclear fusion reactor with a reactor chamber according to one of Claims 1 to 4, characterized in that it is equipped with two separate storage tanks, one containing hydrogen isotopes in the liquid state and the other containing liquid deuterium or water or heavy water in which boron or boron isotopes are dissolved, from which mutually directed fluid jets, consisting of a row of microdroplets each, emerge through the incorporated nozzles.Nuclear fusion reactor with a reactor chamber according to any one of claims 1 to 4, characterised in that it is equipped with two separate storage tanks, one containing hydrogen isotopes in the liquid state and the other containing liquid deuterium or water containing a nanopowder additive of boron or boron isotopes from which mutually directed fluid jets, each consisting of a series of microdroplets, emerge through the built-in nozzles.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 1 to 4, characterized in that liquid deuterium, in which a nanopowder additive of boron or boron isotopes is present, is present in the high-pressure chamber, said additive being coupled to both nozzles directed towards one another, from which a fluid jet, each consisting of a row of microdroplets of liquid deuterium and boron atoms drin, emerges through the incorporated nozzles as far as the collision point.A nuclear fusion reactor comprising a reactor chamber according to any preceding claim, characterised in that the fluid is an incompressible liquid.Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fluid is mixed or provided with an electrolyte.Nuclear fusion reactor with a reactor chamber according to any one of the preceding claims, characterized in that the fluid consists of fusible matter bound in a liquid material with adsorptive storage properties, which are discharged in the form of microdroplets of fluid from two nozzles facing each other and collide with each other at a point of collision (11).Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it comprises at least two fluid accelerators which are installed in the high-pressure chambers in the immediate vicinity of the nozzles or the high-pressure chamber outlets, which generate a pressure in each case in an electrically and simultaneously controlled manner and in each case generate a pressure in the manner of pulses and in each case strike against one another via the two nozzles which collide with one another in the middle of the ring-electrode opening (19) of the electrode pair.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the number of micro-droplets and the pauses therebetween per unit time can be adjusted via the controller.Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the two fluid accelerators are each installed directly in or connected to the nozzles, which are controlled electrically and simultaneously, generate a pressure in each case in a pulsed manner and in each case shoot one or more micro drops against one another via the two nozzles, which micro drops collide with one another in the middle of the ring opening of the electrode pair.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the micro droplets from the respective nozzle are charged electrically differently and attract one another electrically immediately before and during the collision.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the paths of the two micro-droplets striking one another are located on a common line or movement axis (9).Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 1 to 15, characterized in that the paths of the two micro drops which meet one another are located on a line / movement axis (108, 109) in each case, which at one point intersect one another at a wide angle (107), slightly below 180°, and the micro drops collide with one another there (Figure 11).Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fluid accelerator or the microdroplet acceleration system consists of at least one or two micropump devices which have piezoelectric elements (7, 45) which accelerate the microdroplets towards one another at high pressure and high speed.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the micro-drop acceleration system or the fluid accelerators consist of at least two hollow-cylindrical or hollow-spherical high-pressure chambers, in each of which a piezoelectric element (7, 45) is installed, which is inserted in the direction of expansion, partially or completely into an inner wall depression (46) or inner wall channel of the high-pressure chamber, which is designed to match the shape of a piezoelectric element in which the piezoelectric element can change its dimension in an electrically controlled unimpeded manner, wherein the piezoelectric element is equipped at the free end with a straight pressure surface (31) and is arranged such that its direction of expansion lies on the same axis (9) as the fluid jet consisting of micro-drops (2) and emerging from the nozzle.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the high-pressure chamber has, in the nozzle region, a nozzle prechamber, into which the free end with the pressure surface of the piezoelectric element can penetrate during electrically controlled expansion and thereby generate a microdrop from the nozzle.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the high-pressure chamber is a hollow cylinder with small dimensions, in which a piezoelectric element (7, 45) can expand along the hollow cylinder and pushes the fusible fluid with its pressure surface (31) in the direction of the nozzle.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the piezo element is cylindrical or disc-shaped and is shaped into the high-pressure chamber in a manner similar to a piston in a piston pump or in a working cylinder.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that an inflow line or inflow channel (29, 98), by means of which a small quantity of fluid flows from the storage tank (27) at high pressure after each impulse surge through the piezoelectric element, opens into the high-pressure chamber.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the fluid accelerator is designed such that it generates pressure pulses, the generation of which can be controlled at 0.1 to 10 GHz.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the fluid accelerator is designed such that it or the incorporated piezo element can be actuated with a repetition rate of between 0.01 and 18 GHz.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the controller simultaneously conducts very short impulse currents to two fluid accelerators or piezoelectric elements.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the controller is adjustable in such a way that a break of at least 5 times the length of the pulse current duration is placed between two pulse currents for the pressure generation.A nuclear fusion reactor with a reactor chamber according to claim 26 or 27, characterized in that the number of pulses and their repetition rate are adjustable.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 18 to 28, characterized in that the piezo element with its freely movable end or its pressure surface (31) opens into a nozzle prechamber which is part of the high-pressure chamber and is coupled directly to the nozzle which has a larger diameter than the nozzle opening, the contact surface of the piezo element with the fluid being greater than the cross-sectional surface of the nozzle opening and the oscillation amplitude movement of which generates high-pressure pulses of short duration and with very high pressure values which accelerate micro-droplets from the nozzles with respect to one another at a speed which is higher by the factor of the surface conditions between the contact surface of the piezo element and the cross-sectional surface of the nozzle opening.Nuclear fusion reactor with a reactor chamber according to one of claims 18 to 29, characterised in that the piezo element is installed in a depression or a guide channel or a guide groove, wherein its end or contact surface applied to the fluid is freely movable or oscillatable.Nuclear fusion reactor with a reactor chamber according to any one of claims 18 to 30, characterised in that the high-pressure chamber has a hollow cylindrical shape provided with the nozzle at one end and closed at the other end, at which the piezo element is installed in the form of a disc on the high-pressure chamber inner wall opposite the nozzle in a disc-shaped depression, the oscillation axis of the piezo element pointing towards the nozzle (Fig. 11).Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fluid accelerator or the microdroplet acceleration system consists of at least two ignition devices which can be activated electrically simultaneously by the control system which accelerates the microdroplets relative to one another.Nuclear fusion reactor with a reactor chamber according to claim 32, characterised in that oxyhydrogen or silicon is incorporated as ignition material.Nuclear fusion reactor having a reactor chamber according to one of the preceding patent claims, characterized in that the micro droplets are integrated, additionally accelerated by electric fields from further electrodes into the fusion chamber.Nuclear fusion reactor with a reactor chamber according to any one of claims 1 to 17, characterised in that the fluid accelerators are installed in the high-pressure chambers and are components of the inner walls of the high-pressure chamber, which consist of pan-shaped or semi-spherical elements made of iron or another ferromagnetic material installed opposite discharge orifices that convey the fluid outwards in microdrop shape, which are electromagnetically accelerated with very small amplitude towards the discharge orifices, the fusible fluid being forced out or accelerated in the form of individual microdroplets from at least two nozzles colliding with each other.Nuclear fusion reactor with a reactor chamber according to any one of the preceding claims, characterized in that - one of the nozzles is charged electrically positively and correspondingly charges positively the micro-droplets emerging from this nozzle, - an annular surface of an annular pair of electrodes applied to this nozzle is charged electrically negatively, - the opposite nozzle is charged electrically negatively and correspondingly charges negatively the fluid droplets emerging from this nozzle, - an annular surface of the annular pair of electrodes applied to this nozzle is charged electrically positively.Nuclear fusion reactor with a reactor chamber according to any one of claims 2 to 36, characterised in that the high-voltage sources are controlled so as to supply the electrodes and the nozzles with impulse current alternately simultaneously or in pairs on each side of the point of collision.A nuclear fusion reactor with a reactor chamber according to any one of claims 2 to 37., characterized in that one of the high voltage sources is coupled to the two nozzles and the other high voltage source is coupled to the pair of electrodes.Nuclear fusion reactor with a reactor chamber according to any one of claims 2 to 38, characterised in that one of the high-voltage sources is coupled to one of the nozzles and to the electrode of the pair of electrodes applied to the nozzle, while the other high-voltage source is coupled to the electrode of the pair of electrodes and to the nozzle to which it is applied.A nuclear fusion reactor with a reactor chamber according to any of the preceding claims, characterized in that a further electronic controller, a high voltage source and a smaller double-ring electrode is installed with an insulator-ring therebetween in the middle where the micro-drop collision point is located, which generates lightning discharges between the nozzles and the respectively applied sides of the ring electrodes with a high impulse repetition rate, which closes two separate circuits via two lightning discharges on the fluid jets consisting of micro-drops.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the ion movement direction in the jets of individual micro-droplets is designed such that the micro-droplets are moved electrically from the respective nozzles in the direction of the collision point in the middle.Nuclear fusion reactor with a reactor chamber according to any one of the preceding claims, characterized in that a high voltage is applied which generates an electrical polarization which is always oriented such that - one of the nozzles is negatively charged, - the electrode applied to this nozzle is positively charged, - the electrode positioned on the rear side is negatively charged, - the nozzle opposite is positively charged.Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that a virtual point electrode, which is produced by at least one laser emitter and its ionizing laser beam focus, is generated in the microdroplet collision point.Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it is equipped with an electron emitter or an electron source (35) which emits an electron beam (36) into the reactor chamber (23) in a targeted manner on the microdrop collision point (11) or on one of the microdrop rows (5, 6) or fluid beams, said electron beam electrically neutralizing the positively charged ions in the collision point (11).Nuclear fusion reactor with a reactor chamber according to claim 44, characterised in that it is equipped with deflection coils or ring electromagnets (71) for controlling the spatial propagation or the geometric configuration of the electron beam.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the distance between the two nozzles is very small and is in the cm or mm range.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that a low pressure or high vacuum prevails in the reactor chamber.Nuclear fusion reactor comprising a reactor chamber according to any one of the preceding claims, characterized in that the nozzles are equipped with a disc-shaped electrode or a ring electrode, respectively, electrically coupled to the nozzle and electrically charged in the same way as the nozzle.Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the controller is designed to supply the electrodes and the nozzles simultaneously with pulse voltage via built-in high-voltage sources.Nuclear fusion reactor with a reactor chamber according to any one of claims 2 to 49, characterised in that the controller is designed to supply the electrodes and the nozzles with alternating voltage in simultaneous phases via built-in high voltage sources.Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the controller is designed to alternately supply the electrodes and the nozzles with pulsed voltage on each side via built-in high-voltage sources.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the fluid accelerators are equipped with electromagnetic or magnetostrictive or piezo-drive elements which bring about a pulse-like hydraulic pressure on the fluid and a generation of the micro drops from the nozzles.Nuclear fusion reactor with a reactor chamber according to any one of the preceding claims, characterized in that it is equipped with at least one ion lens which guides the electrically charged micro-droplets to the point of collision.Nuclear fusion reactor with a reactor chamber according to any one of claims 44 to 52, characterised in that it is equipped with deflection coils or electromagnets for controlling the spatial spread or geometry of the electron beam.Nuclear fusion reactor with a reactor chamber, characterized in that it comprises at least - a storage tank (27) filled with an incompressible fluid / liquid (106) made of fusible material, - two high-pressure chambers (24, 25, 63) of very stable construction and equipped with solid walls, each having a very small intake volume in the picoliter to nanoliter range or between 1 nm 3 and 1 μm 3 in which a respective microdrop of incompressible fusible liquid / fluid fits clean, - two nozzles (3, 4) directed towards one another, each coupled to the high-pressure chambers, - a capillary fluid line (29) with an injection device (28) and associated valve control, respectively, which conducts the fluid in the high-pressure chambers in very small portioned amounts and completely fills the same without any residue, - two fluid accelerators or micro-drop acceleration systems which are installed in the high-pressure chambers (24, 25, 63) and consist of one or more pressure generators which accelerate the fluid from the high-pressure chamber in small portioned amounts, in the form of in each case two micro-drops (2) or in each case one fluid jet formation (5, 6) consisting of individual micro-drops which are separated from one another, simultaneously with one another over a short distance from a collision point (11) via nozzles (3, 4) directed towards one another over a plurality of km / s, - two electrically expandable or deformable elements which are constituents of the fluid accelerators which are directly or indirectly in contact with the fluid and are in contact with the fluid by electrical voltage or electrical current, while the current supply can be rapidly deformed or can expand in one direction and thereby generate short pressure pulses on the fluid into the high-pressure chamber and respectively displace a micro-drop therefrom at high speed, a control system which controls the elements in the fluid accelerators in such a way that they generate high pressure values simultaneously and simultaneously emerge from both nozzles simultaneously the micro-drops with an adjustable number per unit time and waiting times between the generation of the individual micro-drops, aligned individually or successively in series, whereby the micro-drops of one nozzle strike one another frontally on micro-drops of the other nozzle in a collision point, an energy dissipation system, which derives the excess thermal or direct electrical energy from the nuclear fusion processes and electrical charges generated there by means of ionization processes.A nuclear fusion reactor comprising a reactor chamber, characterized in that it comprises at least - a storage tank (27) filled with an incompressible fluid of fusible material, - a stable high-pressure chamber (24, 25, 63), - two nozzles (3, 4) directed towards one another and coupled to the high-pressure chamber, - a capillary fluid line (29) having a valve control which directs the fluid into the high-pressure chamber in very small portioned quantities, - a fluid accelerator or microdropped acceleration system which is installed in the high-pressure chamber and consists of one or more pressure generators which direct the fluid from the high-pressure chamber in small portioned quantities, in the form of in each case two microdroplets (2) or in each case one fluid jet formation (5, 6) of individual portions, Micro-droplets which are separate from one another, comprising, via nozzles, simultaneously accelerate against one another from a short distance to a collision point over a plurality of km / s, - an electrically expandable or deformable element which is a constituent of the fluid accelerator and is directly or indirectly in contact with the fluid which is able to deform in a lightning-like manner or expand in one direction by means of electrical voltage or electrical current, while the power supply is able to expand in a lightning-like manner and thereby generate short pressure pulses on the fluid, - a controller which controls the element in the fluid accelerator in such a way that it generates high pressure values in a pulsing manner and the micro-droplets are aligned in a row in an adjustable number per unit time and waiting times between the generation of the individual micro-droplets, individually or in a row in a row in a row in a row in a row-like manner, In this case, the micro-droplets of one nozzle are simultaneously ejected from both nozzles and the micro-droplets of the other nozzle strike one another frontally at a collision point, an energy dissipation system which dissipates the excess energy from the fusion process.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the reactor chamber in which the microdroplet collision takes place is evacuated.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 55 to 57, characterized in that the electrically deformable element is a piezoelectric element or piezoelectric actuator (7, 45).Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the high-pressure chamber is constructed in the form of a hollow cylinder of very small dimensions and in that the electrically expandable or deformable element is installed, which generates a high pressure briefly into the high-pressure chamber and thus the microdroplet output through the two nozzles directed towards one another.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 55 to 59, characterized in that the electrically expandable or deformable element can be operated electrically with a high frequency up to a maximum of 18 GHz or with pulse currents with high repetition rates.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 55 to 60, characterized in that the repetition rates or the frequency can be adjusted.Nuclear fusion reactor with a reactor chamber according to any one of claims 55 to 61, characterised in that the electrically expandable or deformable element deforms with very small amplitudes less than 100 micrometres,Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that it is equipped with a capacitor-energy converter system which conducts the fusion energy via ionization of the fusion material after the fusion of the atoms directly into electric current as a power output in a current output.A nuclear fusion reactor comprising a reactor chamber according to any one of the preceding claims, characterized in that it is equipped with a high-resolution, high-speed camera built into the reactor chamber, by means of which the operations in the reactor can be monitored.A nuclear fusion reactor comprising a reactor chamber according to any preceding claim, characterised in that the storage tank (27) or tanks are at high pressure.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the high-pressure chamber is always under pressure which is lower than the pressure required for the production of the micro-droplets, independently of inactivity of the fluid accelerator.A nuclear fusion reactor comprising a reactor chamber according to any preceding claim, characterised in that it comprises an ion beam source which emits a sharp ion beam at right angles to a microdroplet movement axis at the point of collision.Nuclear fusion reactor with a reactor chamber according to claim 67, characterised in that the ion beam (48) is electrically connected as a virtual electrode (47) or serves as a virtual electrode.Nuclear fusion reactor with a reactor chamber according to claim 68, characterised in that a sharp and point-focused laser beam from a built-in laser beam source is provided as the virtual electrode, and in that the paths of the micro-droplets in a respective row in fluid jet formation collide crossing one another at the collision point at an angle slightly smaller than 180°.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that a high-voltage source is electrically coupled to the two nozzle electrodes via an electrical pole and to the ion beam via the other electrical pole via an additional electrode, and emits a voltage discharge between the ion beam and the nozzle electrodes via the ion beam as a virtual electrode, the polarity of which is designed for accelerating the micro drops from the two nozzles at a collision point.Fusion nuclear reactor comprising a reactor chamber according to any one of the preceding claims, characterised in that it comprises two annular electrodes (15, 16), each under high voltage from two separate voltage sources, each of which, on the other side of the point of collision with the centres of which the central orifices are in communication with the respective fluid jet formation of the nozzle facing it, whereby the micro-droplets aligned in the fluid jet formations passing the point of collision without collision pass, per fluid jet formation, through the respective central orifice of the annular electrodes, each annular electrode being electrically coupled to the nozzle or nozzle facing it, whereby a voltage discharge controlled by the control rapidly alternating per fluid jet formation takes place between the ring electrode and the nozzle or nozzle electrode opposite it through the fluid jet formation concerned, the current direction through the fluid jet formations being arranged to accelerate the micro-droplets into each fluid jet formation towards the point of collision.Nuclear fusion reactor comprising a reactor chamber according to any one of the preceding claims, characterized in that a small amount of liquid deuterium or other fusible material which captures the micro-droplets which pass the collision point without collision is filled into the reactor chamber.Nuclear fusion reactor comprising a reactor chamber according to any one of the preceding claims, characterized in that - the reactor chamber is shaped like a hollow sphere or hollow cylinder, - it is equipped with an electric drive which rotates it, - it is partially filled with a fluid capable of fusion, which is radially distributed by the centrifugal force to its hollow sphere wall on which the micro-droplets which have not collided with one another strike and whose kinetic energy is either absorbed or these again partially lead to the nuclear fusion with the fluid.Nuclear fusion reactor comprising a reactor chamber according to any one of the preceding claims, characterized in that it comprises, for additional acceleration of the micro-droplets, two laser sources directed towards each other and the collimated beams of which strike the micro-droplets from behind, immediately after emerging from the nozzle or already in the nozzle, and strike them up to the point of collision with laser beams.Nuclear fusion reactor with a reactor chamber according to claim 73 characterised in that it comprises a control which alternately switches on and off the laser sources at a very high repetition rate.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the repetition rate of the microdrop generation and its firing with respect to one another is so high that the subsequent microdroplet reaches between 3200 and 2 micrometers to the preceding microdroplet which collides with the other microdroplets at the collision point and begins to fuse at the time of the start of the fusion process.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the fluid is water or heavy or super heavy water.A nuclear fusion reactor having a reactor chamber according to claim 77, characterized in that the water is heavy or super heavy water.Nuclear fusion reactor with a reactor chamber according to claim 77 or 78, characterised in that it is equipped with electrostatic fields by additionally built-in electrodes which, while they travel in micro-droplets towards the point of collision, orient the hydrogen atoms forwards in the flight direction, the water molecules of both micro-droplets.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 77 to 79, characterized in that the water is equipped with a small amount as admixture of surfactants.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 77 to 80, characterized in that an additive which converts it into a current-conducting electrolyte is mixed with the water.A nuclear fusion reactor having a reactor chamber according to claim 81 characterised in that the additive is a salt, acid or base.Nuclear fusion reactor with a reactor chamber according to one of Claims 77 to 82, characterized in that it is equipped with electromagnetic or magnetic fields by additionally installed electromagnets (71) or strong permanent magnets (72) which, while they are still travelling in the micro-droplets in the direction of the point of collision, orient the water molecules of both micro-droplets in the forward direction of flight by the magnetic field with the hydrogen atoms.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 77 to 82, characterized in that it is equipped with electrostatic fields by electrodes installed in the reactor chamber, which electrodes orient the water molecules of both micro drops while they are still travelling in the micro drops in the direction of the point of collision, by the electric field, in each case orient the water molecules of both mutually colliding micro drops with the hydrogen atoms forwards in the flight direction.Nuclear fusion reactor with a reactor chamber according to any one of claims 77 to 84, characterised in that it is equipped with a microwave beam source which emits strongly concentrated microwave beams (75) having a beam width of at least two millimetres directly on the point of collision (11) of the micro-droplets (2) perpendicular to the axis of movement (9) of the micro-droplets which reaches the water molecules of both micro-droplets while these travel in micro-droplets to the point of collision, at least one millimetre before the collision, magnetic field generated by the microwaves, which sets the water molecules in synchronous rotation to such an extent that they align with the hydrogen atoms pointing forwards in the direction of the point of collision.A nuclear fusion reactor comprising a reactor chamber according to any one of claims 1 to 84, characterized in that it comprises two microwave beam sources (73, 74) radiating in parallel, one microwave beam highly concentrated, in phase facing relationship to each other, having a beam width of at least 500 μm on both sides immediately before the point of collision of the micro-droplets perpendicular to the axis of movement of the micro-droplets that reaches the fluid molecules or the water molecules of both micro-droplets colliding with each other while traveling in micro-droplets toward the point of collision, at least 500 μm before the point of collision, magnetic fields generated by the microwaves, each of which is in an amplitude and phase, such that they set the water molecules in rotation to such an extent that they are equipped with the hydrogen atoms pointing forward in the direction of the point of collision, thereby orienting themselves.Nuclear fusion reactor with a reactor chamber according to claim 86, characterised in that the two microwave beams which bring the water molecules of the two micro-droplets colliding with one another in the same direction of rotation and have an electronic control which aligns the water molecules of the two micro-droplets precisely with the point of collision with hydrogen atoms arranged in the flight direction in each case on the front side.Nuclear fusion reactor with a reactor chamber according to any one of the preceding claims, characterized in that the controller comprises an electronic adjustment circuit aiming at such a repetition rate and speed of the micro-droplets that provide a distance of at least half micro-droplet diameters between the micro-droplets successively dispensed.Nuclear fusion reactor comprising a reactor chamber according to any one of the preceding claims, characterized in that it is equipped with at least one electric field source or radiation source generating electric fields in the giga- to terakeratome range which act on the water droplets immediately after they have left the nozzles, thereby increasing the number of free electrons in the micro-droplets.A nuclear fusion reactor comprising a reactor chamber according to any preceding claim, characterised in that the fluid accelerator or micro-droplet acceleration system is supplied from a laser source or microwave beam source which emits coherent microwave radiation directly in the fluid in the high pressure chambers or in the fluid lines or in the nozzles and causes the fluid molecules to rotate synchronously there, thereby exciting the fluid to expand and contract rotationally and thereby excite a micro-expansion vector of the total fluid mass into the high pressure chambers which is highest once in the fluid beam axial direction and in the nozzle beam direction by the sum of all vectors of the fluid molecules and an elongated geometrical shape of the high pressure chamber or fluid lines respectively up to the outlet opening, each time, at least one fast moving micro drop each of the nozzles generating.Nuclear fusion reactor with a reactor chamber according to claim 90, characterised in that the high-pressure chamber is a capillary high-pressure chamber (80) in the form of a capillary fluid line, in which the coherent microwave radiation is emitted directly onto the fluid and which is coupled directly to the nozzle or is directed open simply in the direction of the point of collision without a nozzle.Nuclear fusion reactor with a reactor chamber according to any one of claims 1 to 89, characterised in that the fluid accelerator or the micro-drip acceleration system consists of carbon actuators which change their dimensions under electric voltage, which with a surface directly press out the incompressible, fusible fluid from the nozzles to the point of collision in micro-drip form.A nuclear fusion reactor comprising a reactor chamber, characterized in that it consists of at least - two high-pressure capillary chambers (80), the internal spaces of which are shaped as very narrow hollow cylinders or like the internal spaces of capillary tubes provided with solid, stable walls filled with small quantities of incompressible fusible liquid having dipole properties, each closed at one end and open at the other end and directed towards each other at a small distance from the open ends / exits linearly or on an array located on a longitudinal axis line (82) or slightly angled line, - microwave-permeable walls or partial walls which are components of the high-pressure capillary chambers which directly contact the liquid in the high-pressure capillary chambers, a coherent microwave radiation source (78) which emits its microwaves (79) in a bundled or parallel-radiating manner through the microwave-transmissive walls (81) of the two capillary high-pressure chambers (80) simultaneously onto the liquid located there, an electronic controller which controls the microwave source in such a way that it emits short, rapidly repeating, very intense microwave emission pulses into the liquid which expands and contracts the liquid in the capillary high-pressure chambers by orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions, whereby, in each case when the expansion direction matches the line or longitudinal axis line of the capillary high-pressure chamber, the pressure generated in the two capillary high-pressure chambers is reached, The method according to the invention is characterized in that the method is performed by the sum of all expansion vector directions of the fluid molecules located there, accelerates one micro-drop each, which collides with one another in the middle of the path on a micro-drop running axis and partly lead to nuclear fusion, a liquid injector (28) which, after each generation of micro-drops, consists of very small amounts of the liquid in both capillary high-pressure chambers via the same opening through which micro-drops are ejected or, through a separate channel each, injects these into the capillary high-pressure chambers, an energy dissipation system which dissipates the excess energy to the outside.A nuclear fusion reactor comprising a reactor chamber, characterized in that it comprises at least one fluid accelerator which causes excitation of the liquid itself for ultrafast and slight expansion, consisting of at least - two high-pressure capillary chambers (80), the interior of which is shaped as hollow cylinders or like the interior of capillary tubes provided with solid, stable walls filled with small quantities of incompressible fusible liquid having dipole properties, each closed at one end and open at the other end and directed towards each other at a small distance from the open ends linearly or on an array on a longitudinal axis line (82) or slightly angled line, - a coherent microwave radiation source (78), which emits their microwaves (79), bundled by the open ends in the longitudinal axis direction in the two capillary high-pressure chambers, simultaneously onto the liquid (32, 106) located there, - an electronic controller which controls the microwave beam source in such a way that it emits short, rapidly repeating, very intense microwave emission pulses into the liquid, which expands and contracts the liquid in the capillary high-pressure chambers by orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions, whereby, in each case when a match of the expansion direction with the longitudinal axis line of the capillary high-pressure chambers is reached, the pressure generated in the two capillary high-pressure chambers accelerates in each case one micro droplet which collides with one another in the middle of the section and lead in part to the fusion of the nucleus, a liquid injector (28) which injects very small amounts of the liquid in both high-pressure capillary chambers after each generation of micro drops via the same opening through which micro drops are ejected or through a separate channel (97) each, said liquid in the high-pressure capillary chambers, an energy dissipation system which dissipates the excess energy to the outside.A nuclear fusion reactor having a reactor chamber according to claim 93 or 94, characterized in that the microwave radiation is polarized on a plane which causes rotation of the liquid molecules about an axis perpendicular to the longitudinal axes of the capillary high pressure chambers.A nuclear fusion reactor comprising a reactor chamber, characterized in that it comprises at least one fluid accelerator which causes excitation of the liquid itself for ultrafast and slight expansion, consisting of at least - two high-pressure capillary chambers (80), the interior of which is in the form of capillary tubes or fine hollow cylinders, provided with solid, stable walls filled with small quantities of incompressible fusible liquid having dipole characteristics, each closed at one end (83) and open at the other end (84) and facing each other at a small distance from the open ends linearly or in an array on a longitudinal axis line (82) or slightly angled line, - two electrodes each installed at the closed end in the high-pressure capillary chambers, two further electrodes, each installed at the open end of the high-pressure capillary chambers, an electronic control system which, at both high-pressure capillary chambers, in pairs, places the electrode at the closed end and the electrode at the open end under high-voltage pulses generated at a high repetition rate which expands and contracts the liquid in the high-pressure capillary chambers by dielectric polarization or orientation polarization or displacement polarization of the dipole molecules, the entire liquid dimension in the high-pressure capillary chambers, as a result of which, in each case in the direction of expansion in the longitudinal axis direction of the high-pressure capillary chambers, the pressure generated in the two high-pressure capillary chambers accelerates a respective microdrop which collides with one another in the middle of the section and partly leads to nuclear fusion, a liquid injector, The high pressure capillary chambers may be operated by a very small quantity of liquid in both high pressure capillary chambers after several productions or after each production of micro drops via the same opening through which micro drops are ejected or injected through a separate channel into the high pressure capillary chambers, an energy dissipation system which dissipates the excess energy to the outside.A nuclear fusion reactor with a reactor chamber according to claim 96, characterized in that the controller is configured to break up and break down the high voltage pulses within less than 0.1 nanoseconds or at a frequency of several GHz.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 93 to 97, characterized in that the two high-pressure capillary chambers form elongate hollow cylinders, the longitudinal axes (82) of which are located on a line.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 93 to 98, characterized in that the liquid capable of fusion having dipole properties is deuterium oxide.A nuclear fusion reactor having a reactor chamber according to any one of claims 93 to 99, characterized in that the high pressure capillary chambers and the fusible deuterium oxide are cooled to 11.2°C by electric cooling elements, and the microwave radiation penetrates into the liquid transversely or along the longitudinal axis of the high pressure capillary chamber or at an angle between 0 - 90° to the longitudinal axis of the high pressure capillary chamber.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 93 to 100, characterized in that - the open outputs (84) of the high-pressure capillary chambers (80) are positively charged, - in the point of collision (11) of the two micro-droplets (2) there is installed an annular, electrically negatively charged electrode or cathode, perpendicular to the axis of movement of the micro-droplets, in the opening of which there is the point of collision, which electrically aligns the deuterium oxide molecules of both micro-droplets moving towards one another with the deuterium atoms pointing towards the point of collision.A nuclear fusion reactor comprising a reactor chamber, characterized in that it comprises at least one fluid accelerator which causes excitation of the liquid itself to expand its volume ultrafast and slightly, which is composed of at least - a high-pressure chamber (24, 25, 63) with solid, stable walls filled with small quantities of incompressible, fusible liquid with dipole properties, which is equipped with two capillary channels and their open outlets or nozzles (3, 4) respectively installed therein, from each of which the liquid can emerge in the form of micro-droplets (2) which are directed towards each other at a small distance on a longitudinal axis line (9) or slightly angled line, which collide with each other at a point of collision, - a source (78) of microwave radiation, emitting a coherent microwave radiation (79) into the high pressure chamber and the liquid therein, a ring cathode installed in the middle between the two outlets or nozzles (3, 4), in the ring opening of which the collision point (11) is located, two anodes installed in each case at the outlets of the capillary channels or integrated in the nozzles, a high voltage source coupled to the cathode and the anodes, an electronic controller which controls the microwave radiation source in a pulse-like manner and in the process expands and contracts the entire liquid dimension into the high pressure chamber by means of dielectric polarization or orientation polarization or displacement polarization of the dipole molecules, whereby the pressure generated in the high pressure chamber in each case expands and contracts an expansion direction in the longitudinal axis line of the capillary channels, The method of the invention is to accelerate a microdroplet of the liquid which collides with one another in the middle of the path in the collision point and partly lead to nuclear fusion, a liquid injector (28) which injects very small amounts of the liquid into the high-pressure chamber after a plurality of productions or after each production of microdroplets through a separate channel and injects these into the capillary high-pressure chambers, an energy dissipation system which dissipates the excess energy to the outside.Nuclear fusion reactor with a reactor chamber according to any one of claims 93 to 102, characterised in that it comprises a plurality of annular electrodes or cathodes arranged in a row in the micro-drop travel axis, which are alternately switched on and off rapidly generating electrostatic travel fields from the open exits of the high-pressure capillary chambers to the point of collision with the speed of movement of the micro-drops and synchronously with their position in the micro-drop travel axis only as long as the micro-drop has not yet entered the centre point of the annular cathode in its movement.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the reactor chamber inner walls are equipped with efficient solar cells (99) which convert the radiant energy released into the reactor chamber by nuclear fusion into current and make it available as current output for a consumer or for the reactor current demand and accompanying elements.Nuclear fusion reactor with a reactor chamber according to any one of the preceding claims, characterised in that it is equipped with reactor chamber nozzles wetting the inner walls of the reactor with a liquid intended to protect the walls of the reactor against fast flying particles against erosion.Nuclear fusion reactor with a reactor chamber according to any one of claims 93 to 105, characterised in that instead of or in addition to the microwave radiation source, at least one laser source which radiates on the fluid into the high-pressure chamber (63) or into the capillary high-pressure chamber (80) and which causes the dipole molecules to be oriented in the same and synchronous manner or causes the fluid to be heated very rapidly.A nuclear fusion reactor with a reactor chamber according to any one of claims 93 to 105, characterized in that instead of or in addition to the microwave beam source, an electromagnetic coil is incorporated for an equal orientation of the spin axes of the atoms of the dipole molecules.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 93 to 107, characterized in that the excited liquid expansion or a liquid volume increase takes place in a pulse-like manner by the control.A nuclear fusion reactor comprising a reactor chamber according to any one of claims 85 to 108, characterized in that the microwave radiation source emits microwave radiation polarized and coherent on a planeNuclear fusion reactor with a reactor chamber according to one of Claims 106 to 109, characterized in that the laser source (100) is installed outside the high-pressure chamber in each case hitting the colliding micro-droplets directly before or directly in the collision point and causing an ultrafast rapid heating or expansion of the fluid present therein.Nuclear fusion reactor with a reactor chamber according to any one of claims 93 to 110, characterised in that the laser source is a pulsed laser source or a femto laser source.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 93 to 111, characterized in that the laser beams (101) from the laser source strike the micro-droplets perpendicular to their movement axis (9).Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the axes of movement of the micro-droplets accelerated towards one another are located on a line or intersect one another at a point slightly angled.A nuclear fusion reactor comprising a reactor chamber according to any preceding claim, characterised in that the spacing of the counter-facing nozzles or the outlets of the open ends of the high pressure capillary chambers is very small or large depending on the reactor performance objectives.Nuclear fusion reactor with a reactor chamber according to any one of the preceding claims, characterized in that the volume of the micro-droplets is between 2 femto litres and 100 nano litres.Nuclear fusion reactor with a reactor chamber according to any one of the preceding claims, characterized in that the mass of the micro-droplets is between 2 pico-grams and 16 micro-grams.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that the high-pressure chamber or capillary high-pressure chamber is filled with fusion material by very thin inflow fluid channels or capillary channels which are arranged obliquely in the flow direction and open into the high-pressure chamber or capillary high-pressure chamber at a narrow angle.Nuclear fusion reactor with a reactor chamber according to one of the preceding patent claims, characterized in that Tesla valves (105) in micro format are installed in the inflow fluid channels or capillary channels.Nuclear fusion reactor with a reactor chamber according to any one of the preceding claims, characterized in that the controller is configured to control the generation of the micro-droplets, arranged one after the other in a movement axis, at a distance between 1 and 200 times the diameter of the micro-droplets.Nuclear fusion reactor comprising a reactor chamber according to any one of the preceding claims, characterized in that it is equipped with at least one powerful laser source emitting, on the fusible fluid, pulse-like laser beams which cause laser-induced expansion of the fluid in less than one nanosecond.Nuclear fusion reactor with a reactor chamber according to claim 120, characterized in that the laser source is an IR or UV or X-ray laser source (110).A nuclear fusion reactor comprising a reactor chamber according to claim 120 or 121 characterised in that the laser beams from the laser source within the high pressure chamber or capillary high pressure chamber irradiate the fluid.A nuclear fusion reactor comprising a reactor chamber according to claim 120 or 121 characterised in that the laser beams from the laser source irradiate the micro-droplets outside the high pressure chamber or capillary high pressure chamber while they are on the way to the collision point.A nuclear fusion reactor having a reactor chamber according to any preceding claim, characterized in that the fusible fluid or liquid additionally contains water or heavy water.A nuclear fusion reactor with a reactor chamber according to any of the preceding claims, characterized in that an actuator or locking system (112) is incorporated which can make the path length of the colliding micro-droplets variable from the position where they are generated to the collision point or make the distance between the nozzles (3, 4) or the chamber exits adjustable.Nuclear fusion reactor with a reactor chamber according to any one of claims 1 to 124, characterised in that it comprises a mechanism or a drive system which can make the distance between the nozzles (3, 4) or the chamber outlets where the micro-droplets are produced variable or shorten or lengthen them in an electrically controlled manner.Nuclear fusion reactor with a reactor chamber according to any of the preceding claims, characterized in that an actuator or angle locking system (114) is installed, which can make a collision angle (113) of the paths of the micro-droplets in the reactor chamber, from the point where they are generated to the collision point (11), variable in an electrically controlled manner.Nuclear fusion reactor with a reactor chamber according to one of Patent Claims 90 to 127 characterised in that a reflector or mirror (117) which can reflect incident microwaves or laser beams back is installed in the inner wall of the high-pressure chamber or in the capillary chamber.A nuclear fusion reactor having a reactor chamber according to any one of claims 90 to 128, characterized in that the laser source or microwave source is positioned at a distance and emits electromagnetic waves having a wavelength forming a standing wave (116) into the high pressure chamber or capillary chamber.

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