DE102024003673A1 - Nuclear fusion reactor with one reactor chamber - Google Patents

Abstract

The invention is a fusion reactor and can solve energy problems. The reactor could be particularly important for the automotive industry because it can be used as a primary energy source. It enables the advancement of electromobility and could be installed in any vehicle. The reactor consists of a fusion chamber containing two fluid accelerators designed to send a fusion-capable, incompressible liquid in the form of very small microdroplets, generated in pairs, to a collision point. The microdroplets are forced into collision at approximately 50–200 km/s. Due to the very high speed of the microdroplets, partial 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. The molecules/atoms of the liquid are also optimally aligned by electric fields for nuclear fusion of the deuterium atoms directly at the collision point.

Description

The invention is a nuclear fusion reactor that is highly scalable and designed for any desired energy output. Above all, it is also ideally suited for medium to low power levels, making it ideal for mobile applications, especially vehicles as a primary energy source.

Energy demand is constantly rising and is an ever-growing problem for humanity. Unfortunately, our energy resources are limited. Fossil fuels will run out in a few centuries, and their consumption is no longer appropriate. The resulting emissions are enormous and harm our atmosphere. Solar energy is a good alternative, but this is a temporary solution that serves more as a supplement to existing resources. Solar panels may seem sensible, but unfortunately they are not the best energy solution. The more surface area is covered with solar panels, the less space is available for plants and animals. Furthermore, at some point the energy generated will no longer be sufficient to meet total demand. Other environmentally friendly methods, such as wind farms, while acceptable for now, will also be outdated in the future. Wind turbines, if installed in excessive numbers, also have a negative impact on the climate because they interfere with the natural movement of atmospheric air masses. The Earth's natural air movements are part of a global system whose components have been optimally consolidated and harmonized over millions of years. Any intervention in such system components results in a "readjustment" of the system and a new adaptation that may no longer be suitable for us humans.

Other approaches are often pursued to solve energy problems. Many are on the right track, but some are also misguided, such as the absurd assumption that a PPM-1 system could work. Substantial financial investments are currently being made in a PPM-1 system that aims to harness the buoyancy of containers/barrels filled with water in two columns to generate energy.

This construction uses two tall towers filled with water, which support each other to push the floating containers (cylindrical containers) through a lock in the lower section of the towers and allow them to rise. However, an expert will immediately notice that the water masses in the towers are continuously moved with a high expenditure of energy. Each time a container is pushed in, the lock is flooded with water, which causes the water level in the tower to drop accordingly. When the container is pushed in, this water mass must be returned to the tower together with the container, which must be achieved against the enormously high pressure of the water column in the lower section of the tower. This alternates the water level in the tower (dropping at the bottom when the lock is opened and rising by exactly the volume of the container when the container is pushed in). Moving this large quantity of water up and down requires an expenditure of energy. The energy expenditure is greater than the energy gained from the buoyancy of the container. This rather expensive construction therefore always creates an uncompensable energy loss with each container insertion process, which makes energy generation impossible.

Nuclear reactors used to generate electricity operate exclusively on the principle of nuclear fission. During nuclear fission, heavy, radioactive elements are split into lighter elements, releasing energy that is then converted into electrical current with the help of energy converters such as steam turbines. Unfortunately, during nuclear fission, the full potential of the radioactive material is not used efficiently to generate electricity. Radioactive residues remain, which cause further problems. This radioactive residue (radioactive waste) must be safely stored because it emits dangerous radiation. Unfortunately, quite a lot of it remains in the nuclear reactor, which complicates disposal. This also shows how poorly efficient a nuclear reactor is. If all of the material were almost completely "burned," such a reactor would produce at least 90% more energy. The efficiency of nuclear reactors is around 20%. It's often claimed that they operate at an efficiency of around 30-35%, but unfortunately, that's not entirely true. This is hardly significant, however, because nuclear "fuels" produce a great deal of energy anyway. Radioactive waste poses a major environmental risk. However, by designing a new type of reactor, the radioactive waste can still be used as a primary energy source, thus recovering part of the remaining 90%. After that, a smaller amount would still be radioactive, but at least it's worth considering that this is radioactive waste that would otherwise have required complex storage.

Research in the field of fusion technology has been ongoing for several decades. While significant progress has been made, there has yet to be a breakthrough in shifting the energy balance into positive territory.

As has been demonstrated in numerous experiments and nuclear reaction processes observed in particle accelerators and nuclear explosions, there is no doubt that matter is made up of energy. The dual nature of the photon is now accepted by many scientists. The theory states that the photon is both corpuscular and wave. As soon as the photon hits matter (and matter is made up of entangled photons), it can be trapped in the entanglement, thereby slightly enlarging the "clump" (photon absorption). However, it can also eject another photon (photon emission) if it brings with it enough energy or, with a lot of luck, the "angle of impact" is right.

Every type of matter itself contains a huge amount of energy. Whether it's sand, rock, wood, water, metal, air, or earth, each of these materials contains an extremely high amount of energy. However, this doesn't just mean chemical energy. Actually, all matter is made of energy. Matter is a very stable and consolidated form of extremely concentrated energy. Energy in the form of highly focused photons can form stable structures and hold the photons captive there. If these structures are destroyed, the energy is released in photon form. There are numerous ways to extract energy from matter or to initiate these transformations. The most common and simplest methods are chemical in nature. In such processes, combustible matter will simply enter into a chemical reaction and form new chemical compounds or break them down. A widespread method of releasing energy is, for example, to combine matter with oxygen, or to oxidize/burn it. However, this only provides a very small portion of the energy that would actually be available, and the initial energy required to initiate the process is relatively low. Furthermore, this method only works with oxygen-combinable/combustible materials, which constitute a fraction of the total matter found on the Earth's surface, for example.

Rather, energy can be generated or released through nuclear reactions. The methods available to us for generating nuclear energy are nuclear fission and nuclear fusion. There is a third option, annihilation, which, however, is very difficult to implement because it requires antimatter, which does not occur naturally and can only be artificially produced with extremely high energy expenditure. During annihilation, or a collision between a group of atoms made of antimatter and analogous matter, both groups of atoms are completely converted into energy and radiated away from the collision point in all directions at the speed of light in the photon state.

Initiating nuclear fission is technically relatively easy these days. It is implemented in commercial nuclear reactors and widely used for electricity generation. Radioactive elements are enriched until they are suitable for an optimal nuclear reaction. The radioactive material is introduced in the form of elongated rods into a reactor filled with heavy water. Because uncontrolled nuclear fission would lead to an atomic explosion, critical masses are avoided and cadmium lattices or rods (or boric acid dissolved in the heavy water) are placed between the fissile radioactive material. The cadmium or graphite lattices or rods determine the power of the energy release, or the speed at which nuclear fission occurs. The higher or lower the energy release depends on how far they are inserted between the uranium (or plutonium) rods. Every time an atom splits, it releases a neutron, which in turn destabilizes one of the neighboring atoms by penetrating its nucleus. The cadmium rods are able to absorb free neutrons and thus control the nuclear fission processes quite well. Nuclear reactors with graphite as a moderator are no longer used because they are not as easy to control. If the cooling system in the reactor fails, a nuclear meltdown can occur very quickly. In the event of a malfunction, the nuclear reaction and thus the temperature can increase rapidly and quickly spiral out of control. It can increase thousands of times within a millisecond, which can lead to a violent explosion and thus contamination of the surrounding area.

Unfortunately, during nuclear fission reactions, the radioactive "fuel" is not completely split. This leaves behind radioactive residues that continue to emit radiation for hundreds, thousands, or even millions of years. If the radioactive material were completely fissioned, the efficiency of a nuclear reactor would be significantly higher, and less radioactive waste would be left behind. However, the design of nuclear reactors can be modified to minimize waste products. Alternatively, new, specialized reactors can be built that utilize the radioactive waste product of a conventional reactor and continue to produce electricity from it. A completely different design and special alloys such as a neutron exciter with a resonator unit can continue to make the use of conventional radioactive fuels useful. The performance of such a special extra reactor, which uses only the radioactive waste to generate electricity, would be almost the same as that of the conventional reactor, which produces the radioactive waste product! Another reactor would be designed in the form of a hybrid reactor, which uses the radioactive fuel in multiple stages, so that relatively little waste remains at the end. The structure of such a reactor is relatively simple in its core principle, but the accompanying components and safety concepts complicate things enormously. It is nevertheless worthwhile to build such reactors because their efficiency is at least twice as high as that of conventional ones. However, a detailed description of such a specific reactor is not the subject of this invention.

Fusion reactors should actually achieve optimal efficiency in terms of energy yield. Commonly known and existing fusion reactors are built in various designs. Toroidal reactors and tokamaks, for example, are relatively well-known. However, such reactors have unfortunately remained in the experimental phase for decades or are used as research reactors and, according to experts, are always about 30 years away from commercial use, no matter how far one advances in this direction.

While nuclear fusion works flawlessly in a hydrogen bomb, the continuous, controlled energy yield in nuclear fusion reactors is associated with many problems, the solution to which makes the process very expensive and thus unattractive for industry. Fusion reactors require a large amount of start-up energy, which must first be provided. In addition, today's reactors cannot run continuously or the processes there come to a standstill quite quickly, resulting in a relatively low energy yield. If you invest several megawatts of energy in the start-up phase and then the process only runs for a few seconds, or at best a few minutes, with only a fraction of the invested energy being recovered, the efficiency achieved is not a commercially interesting one. For such purposes, the reactor must be able to supply energy continuously and not be in active operation for only a few minutes or seconds every few hours or even days. Unfortunately, today's fusion reactors usually have a negative energy balance: more energy is put in than is gained by the process. It's comparable to a car with an internal combustion engine that needs the electric starter every few dozen seconds to get the engine running for a few seconds. The car battery would then quickly run out because the work of the internal combustion engine wouldn't be enough to recharge it via the alternator. Nuclear fusion is an energy-producing process that has been taking place in the sun and stars for billions of years. The fusion process takes place at extraordinarily high temperatures, at which matter is in its fourth state of matter, known as plasma. Plasma consists of atomic nuclei (ions) and electrons that are no longer bound to one another.

In the interior of the sun, fusion reactions occur at approximately 15 million degrees. Under the boundary conditions on Earth, the plasma is confined by strong magnetic fields at temperatures of over 100 million degrees and at extremely low density (approximately 250,000 times thinner than Earth's atmosphere). What the magnetic fields try to achieve on Earth is not necessary on stars. There, the plasma is strongly compressed by the unimaginably large mass of the star and the gravitational forces acting on this mass. The highly heated plasma that causes fusion is located primarily in a shell, more or less near the star's core, depending on the size of the star. Fusion does not occur in the star's core, as previously assumed, but in a shell located between the core and the surface. If fusion only took place in the core, all stars would be similar in size, and there would be no very large or small stars. Every star has its nuclear fusion shell at a different distance from the star's center. The mantle forms where the balance between pressure and temperature necessary for hydrogen fusion exists. Additional mantles, arranged concentrically at lower levels, fuse other materials and elements. In the core of the star, the pressure is so high that the matter is very dense, and the atomic structural integrity is no longer guaranteed. The neutrons that are supposed to drive fusion are slowed down far too quickly and prematurely bound into heavy atomic structures. The situation is different in the stellar mantle layer, which is more or less distant from the core. The distance from the stellar core is determined by the size and mass of the star. In any case, the fusion mantle of a star is very hot and relatively thin, which also ensures a very long "burn." The fusion mantle does not always remain the same size. It changes its size and shape as the star ages and can become unstable. It also plays a major role in supernova explosions. When a star becomes unstable, the first thing that will happen is that mantle and the layers above it explode. Because the mantle expands inward during the explosion, it compresses the star's material toward the core. This is why much smaller remnants of the star remain after a supernova explosion. First, the material above the mantle is blown away and secondly the underlying material is largely compressed by the increase in pressure.

As far as fusion is concerned, the situation on Earth is different. Here, engineers and scientists are attempting to melt light nuclei (preferably hydrogen isotopes) by intense heating and confining them in a magnetic field. A number of fusion reactions between light nuclei are conceivable. The first generation of future fusion reactors will use the deuterium-tritium reaction, which offers a comparatively high fusion power density: the nucleus of heavy hydrogen deuterium (one proton, one neutron) fuses with the nucleus of superheavy hydrogen tritium (one proton, two neutrons) to form the helium-4 nucleus, the so-called -particle (two protons, two neutrons), emitting a neutron. This releases approximately four times as much energy per nucleon as in the fission of a uranium nucleus. 80% of this energy is bound to the neutron, which, as a neutral particle, can escape the magnetic cage unhindered. The deceleration of neutrons in the structural material and in the plasma chamber's cladding, the so-called blanket, generates heat, which is converted into electricity via a conventional steam cycle. The particles transfer kinetic energy through interaction with plasma particles, thus contributing to the heating of the plasma. Under certain physical conditions, this heating alone is sufficient to keep the plasma at operating temperature. This operating state is called "ignition."

• Die IECT-Methode (Inertial Electrostatic Confinement Thruster) fasst die hochmoderne Entwicklung von Trägheitstriebwerken mit elektrostatischem Einschluss (IEC) zusammen, die in zwei parallele Entwicklungslinien unterteilt wird: die IEC-Plasmaquelle und die entsprechende elektromagnetische Düse (EMN). Beide Entwicklungslinien beginnen mit der Etablierung der Theorie und Modellierung und entwickeln sich weiter zur Entwurfsumsetzung und experimentellen Verifizierung.

There are numerous promising methods for paving the way for nuclear fusion and its commercial application. Here are some publications described or listed that are publicly available:

• The IECT (Inertial Electrostatic Confinement Thruster) method encompasses the state-of-the-art development of electrostatic confinement (IEC) inertial thrusters, which is divided into two parallel development lines: the IEC plasma source and the corresponding electromagnetic nozzle (EMN). Both development lines begin with the establishment of theory and modeling and progress to design implementation and experimental verification.

The IEC discharge model sheds light on a new perspective on IEC discharge physics and the impact of the respective critical parameters that govern the design of the IEC plasma source. Experimental verification of the theory is demonstrated using optical emission spectroscopy and the collision radiation model. The results provide conclusive evidence for the formation of a spherical double layer within the IEC plasma source, which is key to establishing the IEC discharge theory proposed in this work. This work presents a comprehensive study of the magnetohydrodynamic theory for evaluating plasma acceleration in the magnetic nozzle. Nevertheless, the result reveals a performance limitation of the magnetic nozzle. An innovative invention is proposed to overcome this limitation, known as EMN. This work summarizes detailed descriptions of EMN and its working principle, including its effects on plasma confinement, acceleration, and separation. The investigation of the plasma plume properties with various plasma diagnostic tools further proves the EMN functionality and represents the first IECT prototype for which a proof-of-concept is available in the literature.

Another nuclear fusion method is based on inertial electrostatic confinement (IEC). Electrostatic inertial confinement (IEC) refers to processes that attempt to generate a high-density plasma with high ion energy, either alone or primarily with the aid of an electric field. IEC devices are constructed with the goal of achieving fusion reactions between atomic nuclei of hydrogen isotopes (deuterium or deuterium and tritium). These devices are also called Farnsworth-Hirsch fusors or Hirsch-Meeks fusors after their developers. The polywell device is also a related concept. Because such devices release neutrons during hydrogen fusion reactions, electrostatic inertial confinement can be used as the basis for a neutron source. Unfortunately, this concept is unsuitable for power generation due to its negative energy balance. The concept of electrostatic inertial confinement for achieving nuclear fusion is based on the fact that deuterium and/or tritium ions are held in a small spatial region by an electric field and bombarded from the outside with other, high-energy ions of the same type(s). In contrast to nuclear fusion reactors with magnetic confinement, the energy during the collision is not determined by the temperature of the plasma; rather, higher ion energies can be used (by means of high accelerating voltages). This makes it easier to overcome the Coulomb barrier during the collision, thus increasing the probability of a fusion reaction occurring during the collision. Because the like-charged ions tend to exhibit scattering behavior, the frequency of fusion reactions sufficient for net energy production is relatively low, and thus a positive energy balance cannot be achieved with this process.

Early work on this technique was done by Philo Farnsworth based on observations of television tubes. The original designs in the early 1960s were based on cylindrical arrays of electrodes.

The fuel for nuclear fusion, deuterium, was accelerated from ion sources toward the inner reaction zone, where the fuel ions were to be held by electrostatic forces. Farnsworth coined the term inertial electrostatic confinement for this. However, this technique has nothing to do with inertial confinement in the sense of inertial fusion.

Further developments were made by Robert L. Hirsch. In the late 1960s, he built a large device with six ion sources and a high-voltage supply of up to 150 kV. With this device, nearly 108 fusion events per second were achieved with deuterium. Hirsch also proposed a setup without an ion gun. In this setup, a high voltage is applied between two concentric spherical electrode grids located in a larger container filled with deuterium at low pressure. The glow discharge ignited by the high voltage generates the desired deuterium ions through electron impact. In the early 1980s, various experiments demonstrated that in such an arrangement, a potential minimum forms within the inner, spherical grid electrode. However, closer investigations could not detect an increased ion density at this potential. Fusion in the laboratory is possible with moderate time and financial investment! The Fusor devices demonstrate the simplicity behind it. Fusion requires heavy hydrogen, which must first be ionized using a sufficiently high voltage. This occurs via a glow discharge at the electrodes. Electron collisions split the hydrogen molecule into two individual atoms, after which the electron is separated from the core. What remains are the bare hydrogen nuclei, which in heavy hydrogen are called deuterons. With sufficient energy, two deuterons can overcome their mutual repulsion and come close enough for the strong interaction to take effect. The two deuterons fuse, and the resulting energy is released in the form of neutrons. The reaction with the largest cross section is the deuterium-tritium reaction, but it is not the dominant reaction in the fusion reactor, since only deuterium is used as the primary working gas (4He = helium-4): $$\text{D}+\text{T}\to 4\text{He}+1\text{n}+\mathrm{17,588}\text{MeV}$$

$$\text{D}+\text{D}\to 3\text{H}+1\text{p}+\mathrm{4,03}\text{MeV}$$

The actual reaction, which begins at about 15 keV, is the deuterium-deuterium reaction. It can proceed in two ways: $$\text{D}+\text{D}\to 3\text{He}+1\text{n}+\mathrm{3,268}\text{MeV}$$

$$\text{D}+\text{D}\to 3\text{H}+1\text{p}+\mathrm{4,03}\text{MeV}$$

In a fusor, dangerous tritium is also produced, albeit in very small quantities. It also reacts immediately via the D-T reaction to form helium-4, generating very high-energy neutrons. Calculations predict that the boron densities and ion beam parameters achieved in the experiment should result in a fusion rate of around 100 billion per second if all three high-energy emitters are fired simultaneously. The fusion rate in the proton-proton reaction is proportional to the fourth power of the temperature. Therefore, a 5% increase in temperature results in a 22% increase in energy release.

A deuterium and a tritium atomic nucleus fuse to form a helium nucleus, releasing a fast neutron. In nuclear fusion, atomic nuclei fuse to form a new nucleus. Many nuclear reactions of this type release energy. The energy radiated by the sun also comes from nuclear fusion processes. For a fusion reaction to occur between two atomic nuclei, they must come very close to each other, within approximately 2.5 femtometers. This is counteracted by the Coulomb force (electrical repulsion), which must be overcome with a great expenditure of energy (e.g., high temperature). Fusion reactions suitable for technical energy production are well known from studies using particle accelerators. However, in accelerator experiments, much more energy is expended for the overall operation of the apparatus than the reaction actually releases, because the accompanying elements and equipment consume too much energy. The electromagnets, their control systems, and the associated cooling devices are real energy wasters. Above all, labor and energy efficiency are not guaranteed. A giant electromagnet with a mass of more than 12,000 kg, fully energized and at its maximum magnetic field, consumes virtually the same amount of energy whether accelerating a group of just four or a group of two billion ions simultaneously. A net energy gain, i.e., the operation of a power plant, is not possible in this way.

• Eine weitere Methode, um Energie aus dem Kernfusion frei zusetzen ist die Fusion mit magnetischem Plasmaeinschluss. Die bisher aussichtsreichsten Konzepte für Fusionsreaktoren sehen vor, ein Deuterium-Tritium-Plasma in einem ringförmigen Magnetfeld einzuschließen und auf hinreichende Temperatur zu erhitzen. Um auf diese Weise einen Netto-Energiegewinn zu erreichen, muss das Plasmavolumen ausreichend groß sein. Um den Prozess in Gang zu bringen, werden in das viele Kubikmeter große, gut evakuierte Reaktionsgefäß einige Gramm eines Deuterium-Tritium-Gasgemischs (1:1) eingelassen. Die Gasdichte entspricht dann einem Fein- bis Hochvakuum. Das Gas wird durch Aufheizen in den Plasmazustand gebracht und weiter erhitzt. Das Plasma übt nach Erreichen der Zieltemperatur - im innersten Bereich des Plasmas rund 150 Millionen Kelvin - einen Druck von lediglich einigen Bar aus. Gegen diesen Druck muss das Magnetfeld die Teilchen zusammenhalten. Eine Berührung mit der Gefäßwand muss verhindert werden, da das Plasma sonst sofort auskühlen würde.

In order for nuclear fusion to convert matter into energy according to Einstein's formula E = mc ² , the mass of the two fusion nuclei together must be greater than the Mass of the resulting nuclei and particles. This mass difference is converted into energy. The mass difference is particularly large when helium-4 is formed from hydrogen isotopes. In these cases, the electrical repulsion that must be overcome before fusion is the smallest because they each carry only a single elementary charge. Therefore, a mixture of equal parts of deuterium (D) and tritium (T) is planned as the fusion fuel:

• Another method for releasing energy from nuclear fusion is fusion with magnetic plasma confinement. The most promising concepts for fusion reactors to date involve confining a deuterium-tritium plasma in a ring-shaped magnetic field and heating it to a sufficient temperature. To achieve a net energy gain in this way, the plasma volume must be sufficiently large. To initiate the process, a few grams of a deuterium-tritium gas mixture (1:1) are introduced into the well-evacuated reaction vessel, which is several cubic meters in size. The gas density then corresponds to a medium to high vacuum. The gas is heated to the plasma state and further heated. Once the target temperature is reached—around 150 million Kelvin in the innermost region of the plasma—the plasma exerts a pressure of only a few bars. The magnetic field must hold the particles together against this pressure. Contact with the vessel wall must be prevented, as otherwise the plasma would cool immediately.

• https://pure.mpg.de/rest/items/item_2482728/component/file_2482739/content ). Die Energie der Alphateilchen verteilt sich weiter durch Stöße im Plasma und trägt zu seiner weiteren Heizung bei. Bei genügender Kernreaktionsrate (Anzahl der Reaktionen pro Zeitintervall) kann diese Energie ausreichen, um die Plasmatemperatur ohne weitere äußere Heizung aufrechtzuerhalten: Das Plasma hat dann „gezündet“ und „brennt“ von selbst. Dies tritt ein, wenn bei gegebener Temperatur das Tripelprodukt aus Teilchendichte, Temperatur und einer durch die unvermeidlichen Wärmeverluste bestimmten Zeitkonstanten, der Energieeinschlusszeit, gemäß dem Lawson-Kriterium einen bestimmten Mindestwert übersteigt.

Fusion reactions occur at a temperature of approximately 150 million Kelvin and a particle density of approximately 10 ^2° / m ³ . The energy released is distributed as kinetic energy in a ratio of 1:4 between the formed alpha particles (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 distributed through collisions in the plasma and contributes to its further heating. If the nuclear reaction rate (number of reactions per time interval) is sufficient, this energy can be sufficient to maintain the plasma temperature without further external heating: the plasma has then "ignited" and "burns" on its own. This occurs when, at a given temperature, the triple product of 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.

However, this point need not be reached for an energy-producing reactor. Even at somewhat lower temperatures and constant auxiliary heating, sufficient fusion reactions occur (so-called fusion with net energy gain without reaching the Lawson criterion). The auxiliary heating even offers a welcome opportunity (in addition to fuel refilling) to control the reaction rate, i.e., the reactor power. The achieved plasma state must be permanently maintained by adding new fuel as needed and removing the resulting helium—the result of fusion, the "ash." The released neutrons leave the plasma; their kinetic energy, four-fifths of the fusion energy, is available for use.

So far, energy gains have only been achieved for a very short time in experiments at JET and TFTR (Princeton, USA), but not in many other experiments. The plasma vessels of the existing experimental facilities are too small, causing the plasma to cool too much. In the larger ITER tokamak, a permanently "burning" fusion process is planned with continuous auxiliary heating. Even later facilities such as DEMO will likely be designed in such a way that a weak auxiliary heating of, say, a few percent of the fusion power remains necessary to maintain an additional control option.

Increasing density and temperature increases the power produced by fusion reactions. However, escalating to excessively high temperatures is not possible, as the energy loss of the plasma through transport processes also increases with temperature.

Various methods have been developed for heating the plasma to temperatures above 100 million Kelvin. All particles in the plasma move at very high speeds, depending on the respective temperature (deuterium nuclei at 100 million Kelvin have an average speed of about 1000 km/s). The heating power increases the temperature and compensates for losses due primarily to turbulent and neoclassical transport (caused by collisions between particles), as well as bremsstrahlung. One possibility for heating the plasma is electrical heating: Plasma is an electrical conductor and can be heated using an induced electric current. In this process, the plasma becomes a secondary coil of a transformer. However, the conductivity of the plasma increases with rising temperature, so that above about 20-30 million Kelvin or 2 keV, the electrical resistance is no longer sufficient to heat the plasma much more. In tokamak reactors, the current through the central solenoid is continuously increased for electrical heating.

Many reactors use microwaves to excite the ions and electrons in the plasma at their resonant frequencies, thus transferring energy into the plasma. These heating methods are called Ion Cyclotron Resonance Heating (ICRH), Electron Cyclotron Resonance Heating (ECRH), and Lower Hybrid Resonance Heating (LHRH).

Heating the plasma can also be achieved by neutral beam injection (NBI). When fast neutral atoms are injected into the plasma (neutral beam injection, NBI), the kinetic energy of these atoms, which are immediately ionized in the plasma, is transferred to the plasma through collisions, causing it to heat 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 it simultaneously increases the plasma density. Only magnetic fields generated by magnetic coils with variable current are suitable for compressing the plasma.

The magnetic field must hold the plasma together against its pressure so that it doesn't touch the vessel wall, otherwise the fusion processes would be abruptly interrupted. Both concepts for magnetic confinement, the tokamak and the stellarator, use a toroidal, twisted magnetic field. Tokamaks generate the twisted field by inducing an electric current in the plasma, while stellarators achieve this through a special, complex shape of their magnetic coils.

The magnetic field is generated using large coils. Their shape and arrangement determine the shape of the plasma; the current in the coils determines the strength of the magnetic field and thus the potential size of the plasma, the particle density, and the pressure. In a reactor (or in experiments where the plasma is confined for a longer period of time), the coils must be superconducting: The current flowing through normally conducting coils generates heat due to the electrical resistance that must be overcome. Such coils could no longer be effectively cooled over extended periods of operation, causing the temperature to rise and the coil to be destroyed. Superconducting coils, on the other hand, have no resistance, which is why the current in them does not generate any heat that needs to be dissipated.

A generator developed at the Karlsruhe Research Center, a so-called gyrotron, can heat the plasma of a future fusion power plant to 100 million degrees Celsius. This temperature must be reached in a tokamak reactor to fuse hydrogen isotopes into helium and thus harness the sun's energy source for technical purposes. The Research Center's Institute for High-Power Pulsed and Microwave Technology has developed a microwave generator that delivers an output power of 3 megawatts.

The European fusion experiment JET and the international ITER project are based on the so-called tokamak principle. The WENDELSTEIN 7-X fusion experiment in Greifswald is based on the stellarator principle, which is being driven forward at the European level primarily by the Max Planck Institute for Plasma Physics in Garching. The advantage of a stellarator is that energy generation can occur continuously for at least several dozen minutes, whereas a tokamak requires regular short interruptions in operation. This advantage is achieved through a more complex geometry of the confining magnetic field.

In both of these concepts, a powerful heating system is required to generate the necessary temperatures of 110 million degrees Celsius in the plasma. At these temperatures, the plasma can "ignite" and the fusion of hydrogen isotopes into helium can begin. The heating phase can last approximately 60 to 100 seconds.

The tokamak is the most advanced concept, and is being pursued internationally with ITER. However, at least in its original mode of operation with a purely inductively generated plasma flow, it has the disadvantage that it cannot operate continuously, but only in pulsed mode, i.e., with regular short interruptions.

Deuterium and/or tritium are used as fuel for fusion reactors. Some reactors also use boron isotopes. While deuterium is present in Earth's water in virtually inexhaustible quantities (2.5 1013 t), tritium in the quantities required for a fusion reactor can practically only be produced by "breeding" it from lithium-6 in the plant itself.

The earth's lithium reserves are estimated at more than 29 million t. Only the isotope 6Li, which naturally occurs at 7.5%, is used for tritium breeding. From this proportionate reserve of approximately 2 million t of lithium-6, approximately 1 million t of tritium can theoretically be extracted according to the above formula. In practice, enriched lithium with a lithium-6 content of 30-60% is to be used. The technically usable lithium reserves is therefore mathematically sufficient to cover the energy needs of humanity for thousands of years.

A shortage due to lithium demand from other industries is counteracted by the fact that the isotopic composition plays no role for these industries, meaning that more than 90% of the lithium remains available. Even in a scenario with sharply increasing lithium demand due to the massive expansion of electromobility, only those lithium resources that can be mined at current lithium prices and technologies will be depleted by 2050.

Tritium is radioactive with a half-life of 12.32 years. However, it only emits beta radiation with a low maximum energy and no accompanying gamma radiation. Tritium will only make a relatively small contribution to the radioactivity inventory of a fusion reactor that has been in operation for some time. The tritium required to start fusion reactors could easily be obtained in conventional nuclear fission reactors. In particular, heavy water reactors produce tritium as a byproduct in quantities of around 1 kg per 5 GWa of electrical energy generated. However, these currently only available sources would not provide nearly enough tritium for the continuous operation of fusion power plants, which makes it necessary to breed tritium in the reactor. A fusion power plant with 1 GW of electrical output would require approximately 225 kg of tritium annually.

The world’s largest facilities based on the Tokamak principle are the Joint European Torus (JET) in Culham / Great Britain and ITER (International Thermonuclear Experimental Reactor) in France, which has been in operation since 2007 It will be built and completed around May 2035. The general goal is to experimentally confirm the theory of nuclear fusion and the feasibility of generating energy from the fusion reaction. JET has been in operation since 1983 and is currently capable of generating 17 MW of power for short periods, which corresponds to approximately 70% of the power required to heat the plasma. Unfortunately, however, it does not achieve a positive energy balance.

In parallel with the tokamak, which releases energy in long pulses, the "stellarator" line, which enables continuous plasma operation, is being further developed. The Wendelstein 7X stellarator facility was built in Greifswald under the leadership of the Max Planck Institute for Plasma Physics. This facility features a very complex electromagnet arrangement and field geometry. However, it is promising, and experimental operation shows that it works. Several success stories have been published.

Nuclear fusion is based on a reaction between two hydrogen isotopes, e.g., deuterium and tritium: 2H + 3H = 4He2 + n. According to Albert Einstein's law of mass defect, this reaction releases energy. To initiate the fusion of hydrogen nuclei into helium nuclei, the hydrogen gas must be heated to a temperature of over 100 million degrees Celsius (200 million degrees Celsius has already been reached). For comparison, the sun's surface temperature is 5500 °C and its interior is approximately 15,000,000 °C. This creates a so-called plasma, a mixture of free hydrogen ions and free electrons.

A fusion reactor works with very small plasmas, consisting of only 1g 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.

To operate at these high temperatures, the plasmas and their thermal radiation are trapped in a vacuum using magnetic fields 100,000 times stronger than the Earth's magnetic field. The extremely high temperature is necessary to compensate for the very low ion density (approximately 10 to the power of 14 ions/cm ³ ).

Most techniques involve high-energy neutrons. Since they cannot be forced into a defined trajectory by magnets, they strike the material surrounding the plasma and cause its radiation. However, they are used to produce tritium, which is the most commonly used element, with lithium.

In principle, one can distinguish between several techniques of nuclear fusion: induced inertial fusion, magnetic confinement fusion, cold nuclear fusion, lattice confinement fusion, projectile fusion and fusion from particle accelerator technology.

The method for generating fusion with magnetic confinement 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 between 50 and 400 million degrees Celsius and then exists as a plasma, meaning the gas is fully ionized. Magnetic fields force the plasma into a path that prevents it from touching the wall. Contact would instantly cool the plasma, interrupting fusion. At high temperatures, thermonuclear burning ultimately occurs.

In general, magnetic confinement presents the following problems: Energy losses due to the difficulties of plasma confinement and impurities. Neutron bombardment renders the reactor material radioactive. The extreme conditions lead to severe material fatigue and thus to high costs. Large amounts of energy stored in the magnetic fields and radioactive inventory pose a potential hazard. The high energy consumption during operation due to the required heating and magnets (approximately 300 MW, equivalent to the consumption of a medium-sized city) does not even justify repeating such experiments.

When it comes to magnetic confinement, it is still necessary to distinguish at least three types of reactors: stellerators, tokamaks and mirror machines.

- Stellerators

Here, the reactor vessel is a ring-shaped tube, similar to a tokamak. The plasma flows in a circle, twisted by suitable magnetic fields to minimize radiation losses. These additional magnetic fields complicate the reactor's technology. Furthermore, the desired degree of confinement, which corresponds to the product of pressure times time, is currently not achieved. However, the stellerator is very interesting for the design of an energy-producing reactor because it is suitable for continuous operation.

- Tokamak

Tokamak is an abbreviation for the Russian term for toroidal chamber in a magnetic field. A 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 radiation losses, so that no magnetic field is needed to twist the plasma. In addition, the current in the plasma represents a heating method. Tokamaks have so far come closest to the conditions for self-sustaining thermonuclear burning, which may also be due to the fact that the most intensive research is being conducted here. The main disadvantage of the tokamak is that it is not suitable for continuous operation and must be regularly recharged with plasma, which also places an extreme strain on the facility.

- Mirror machines

The reactor vessel forms a straight tube. At the ends, the plasma is reflected in its flow direction by corresponding magnetic fields. Reflection at the ends results in increased energy losses.

But there are also numerous other techniques for nuclear fusion.

- MIGMA concept

In the MIGMA process, particles (e.g., deuterons and trions) from a particle accelerator are repeatedly collided and fused. This concept also enables fusion between protons and the boron-11 isotope. Four high-energy alpha particles (4He2+) are created. The special feature of this approach is that no radioactive and toxic tritium is required, and no neutrons are produced, which are responsible for unwanted radioactivity. According to the KfK, the main problem with this technology is the energy loss of the particles due to the resulting synchrotron radiation. Unfortunately, this technology, considered ingenious by some physicists, is ignored worldwide. Despite considerable initial successes over the past 70 years, insufficient funding has been made available for further development. The reason for this could be that this reaction does not produce high-energy neutrons, which lead to the very interesting byproduct: fissile material.

- Induced inertial fusion

A mixture of deuterium and tritium is surrounded by a small spherical shell. These 1mm-sized pellets are bombarded in a vacuum with a high-energy laser or a light or heavy ion beam. The resulting implosion compresses the hydrogen mixture to one-fiftieth of its volume. The extreme heating creates the fusing plasma. 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-wave, high-energy lasers or accelerators. Furthermore, high-energy neutrons are also generated here. The construction of an energy-generating reactor that could ignite, for example, ten pellets per second is conceivable.

- Cold nuclear fusion (or low energy fusion)

The reaction was already described in the 1940s by F. Frank and Andrei D. Sakharov and 10 years later by chance by Luis W. Alvarez experimentally demonstrated that cold nuclear fusion With muon-catalyzed cold nuclear fusion, the high temperatures and huge experimental setups can be avoided. 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 chamber filled with tritium and deuterium. For this purpose, negative muons are allowed to enter the chamber. The muons create close bonds between the hydrogen molecules through special collision processes. The nuclei thus bound by muons fuse, and energy is released in the form of heat. The muons are released again in the process and can, under certain conditions, catalyze further fusion. Muons can be produced artificially with the help of particle accelerators. In order for a muon to catalyze multiple nuclear fusion reactions, high energies are required for its production. That's the theory, but to date it has not been successfully implemented in practice, and at least there are no economically viable reactors.

With cold fusion, the Chemists Martin Fleischmann and Stanley Pons and on 23.03.1989 announced at a press conference that they had built and successfully tested a cold fusion reactor. However, this technical marvel has not been confirmed. The two chemists were also unable to demonstrate any excess heat in the reactor they built in front of witnesses. Cold fusion is currently of interest only for basic research. To date, there is no reproducible experimental setup with a positive energy balance.

The major technical challenge to overcome in nuclear fusion so far is the energy balance. Unfortunately, more energy is required to run the reaction than is subsequently released.

The world's largest fusion reactor, ITER, is currently being built in southern France. It will use tokamak technology. Commissioning is scheduled for around 2045. It is a gigantic construction project that is extremely expensive. Above all, its economic viability is questionable. ITER will not be used for energy production, nor is it a prototype of a fusion reactor. Rather, it is an experimental project intended to provide knowledge for future prototypes and series-production reactors.

There are increasing considerations and numerous experimental attempts to start fusion with significantly less energy. Proponents point to the advantages: safer, smaller, and more stable reactors. Such processes and reactors are often called cold fusion machines or cold fusion reactors. As already described, they use special catalysts that are intended to enable the fusion of deuterium and tritium (both hydrogen isotopes). However, despite the efforts (and some misinterpretations, such as those of Fleischmann and Pons) of dedicated scientists around the world, not a single truly functioning reactor has yet been built. Reproducing the results has also not been successfully achieved. The problem unfortunately lies in the theoretical approaches and implementation methods. Despite sometimes remarkable performance and the great catalytic effects of the catalysts, it is not so easy to avoid the necessary start-up energy required for nuclear fusion. Nevertheless, cold fusion could also work with the right equipment and precise adjustment of the components. However, this requires different materials and a completely different construction than those previously used in test facilities.

There have also been numerous attempts to generate sonoluminescence in a liquid (e.g., water or acetone) using ultrasound. These processes have been known since the early 20th century. Ultrasound can actually create cavitation bubbles in liquid, which then collapse quite quickly, emitting flashes of light. These flashes of light can be observed directly or recorded by high-speed cameras. The approximately 0.2 mm-sized bubbles collapse at a speed of approximately 30 m/s. There are numerous claims that such processes can produce a type of sonofusion. Unfortunately, there is no scientific evidence for this.

Building a fusion reactor that operates in a controlled manner and produces more energy than it consumes is an important task for scientists and researchers today.

The US Navy is also conducting experiments in this direction. A patent published by their scientists in 2019, albeit rather utopian and abstractly worded, in which almost nothing was explained, shows that they are interested in the matter. However, the patent document does not yet provide any clues as to how to build such a functioning fusion reactor, just like the other publications, such as the anti-gravity drive that is supposed to be coupled with the fusion reactor, which is also formulated in an abstract and schematic manner, creating the impression that the authors, without truly understanding this technology, attempted to copy and legally protect a strange, extraterrestrial technology, based on a fragmented, inadequate attempt at interactivity with a being that which has unfortunately already left this world. Nevertheless, this work is certainly remarkable. Specifically, it concerns a series of patents filed by the aeronautical engineer Dr. Salvatore CP, who works for the Naval Air Warfare Center Aircraft Division (NAWCAD), a technology and development unit of the US Navy, and apparently specializes in electromagnetic propulsion and superconductor research. The published patents are descriptions of a "high-frequency gravitational wave generator" ( US10322827B2 ); a superconductor that functions at room temperatures ( US20190058105A1 ); an enormously powerful and asteroid-defending "electromagnetic 'force field'generator" ( US10135366B2 ) and last but not least a “vehicle or aircraft driven by a device that reduces the mass inertia” ( US10144532B2 ) and is said to be capable of amazing and exotic maneuvers at extreme speeds both in the air and underwater – and even in space. Another publication, US US20190348597A1 (Piezoelectrically induced high-temperature superconductor) describes an invention which is a high-temperature superconductor consisting of a wire consisting of an insulator core and a metal coating. The metal coating is arranged around the insulator core and the metal coating is deposited on the core. When a pulsed current flows through the wire. Also a plasma compression fusion device (US US20190295733A1 ) comprising a hollow channel and at least one pair of opposing, counter-rotating dynamic fusors is described. The hollow channel includes a vacuum chamber disposed within the hollow channel. Each dynamic fusor has a plurality of openings and an outer surface that is electrically charged.

To initiate fusion processes, ideas were put forward decades ago to fire ultrafast projectiles at targets filled with deuterium and tritium. Such projectiles, which impact a target at high speed, have been used for several years. In recent years, experiments have involved collisions between discs accelerated to speeds of up to approximately 6 km/s through gas-pressure tubes or cannons. These discs impact a cube-shaped target with an edge length of approximately 1 cm, each containing two chambers containing deuterium and tritium. The collision compresses the gases into a hot plasma, which partially fuses the atoms. In the first experiments, approximately 50 neutrons were generated per shot. If the shape of the target were to be optimized and the targets would no longer be cube-shaped, but rather a pyramidal construction with 16 edges and a ratio of 1:1.24, in which a 4-chamber construction with a pairwise 103° arrangement would be installed, the neutron emission could be significantly increased.

US20190295733A1 (Plasma Compression Fusion Device) describes a fusion reactor in which a concentrated plasma bubble is created, surrounded by powerful electromagnets. The electromagnets rotate to create a stable field.

EP 0438724B1 describes a nuclear fusion reactor with a reaction zone, a magnetic field with convexly curved magnetic flux lines surrounding the reaction zone.

DE 102012025244A1 describes a fusion reactor in which petawatt laser devices are used to fire solid-state dense nuclear fuel using picosecond laser pulses, whereby lateral reaction losses are avoided by the spherical geometry of the applied laser pulses.

DE 3913503A1 describes a process for carrying out warm nuclear fusion, using catalytic elements to achieve core meltdown.

DE 102007022302B4 Describes a process for accelerating solids with the goal of inducing a fusion reaction. It uses multiple beam generators, each of which directs an energy beam at a solid made of fusion material, which then vaporizes explosively, accelerating its components.

Unfortunately, the current state of the art does not present a solution for a fusion reactor that would provide a positive energy balance.

The Lawrence Livermore National Laboratory recently published several success stories. As is common practice in research, the experiments only reported the energy balance of the plasma itself. This does not take into account the amount of electricity flowing into the lasers, for example, i.e., the overall balance. For future power generation, it is crucial that the overall balance of fusion is positive. Unfortunately, in current fusion reactors, the overall balance is still far from positive.

In the NIF experiment, the 200 lasers heated a small fuel chamber containing tiny amounts of hydrogen to more than three million degrees Celsius. The facility reportedly required 300 megajoules of energy to power two megajoules of lasers. to deliver energy that produced a fusion yield of three megajoules. The fact that several hundred megajoules of energy had to be put into the system first is the catch to this success. To generate electricity, at least twice the total amount of energy invested would be required. In addition, the Lawrence Livermore National Laboratory can generally conduct such experiments about once a day. A fusion power plant would have to do this ten times per second to generate enough electricity. Calculations would indicate that with a larger-scale laser system, it is possible to achieve a yield of hundreds of megajoules. However, such lasers do not yet exist, and their energy consumption remains relatively high.

The patent US 6919698 B2 describes an electrostatic fluid accelerator and a method for controlling fluid flow. The electrostatic fluid accelerator comprises a first plurality of corona electrodes and a second plurality of accelerating electrodes spaced apart from and arranged parallel to adjacent corona electrodes. An electrical power source is connected to supply an operating voltage to the corona and accelerating electrodes to generate a high-intensity electric field in an interelectrode space between the corona electrodes and the accelerating electrodes. The accelerating electrodes may be made of a high-resistivity material, with each of the electrodes having a mutually 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 direction transverse to both the desired fluid flow direction and the length.

It is known from the prior art that various methods can be used to accelerate small amounts of liquid. One of these is the electrospray ionization method. This method uses a probe and electrostatic charge for acceleration. The probe is located centrally between two turbo heaters arranged 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 that ionize in the liquid solvent can be generated as gas-phase ions in the ion source. The efficiency and rate of ion generation depend on the solvation energies of the specific ions. Ions with low solvation energies are more likely to evaporate more easily than ions with higher solvation energies. The interaction of IonSpray Voltage (Analyst software), IonSpray Voltage Floating (Analyst TF software), or Spray voltage (SCIEX OS) and the turbo heaters helps focus the beam and increase the rate of droplet evaporation, resulting in a stronger ion signal. The heated gas increases the efficiency of ion evaporation, increasing sensitivity and improving the ability to handle larger volume flows of liquid samples. A high-velocity stream of nebulizer gas pushes droplets from the liquid sample flow into the inlet of the IonSpray Voltage or Spray voltage. Due to the variable high voltage applied to the nebulizer, the ion source imparts a net charge to each droplet. This charge promotes droplet dispersion. Ions of single polarity are preferentially drawn into the droplets by the high voltage when they are separated from the liquid stream. However, this separation is incomplete, and each droplet still contains many ions of both polarities. Ions of one polarity predominate in each droplet, and the difference between the number of positively and negatively charged ions determines the net charge. Only excess ions of the predominant polarity are available for ion evaporation, and only a fraction of these actually evaporate. Droplets contain ions of both polarities, with one polarity predominating. As the solvent evaporates, the electric field increases, and the ions move to the surface. At a certain critical field value, the ions are released from the droplets, leaving a non-volatile residue as a dry particle. When the droplet contains excess ions and enough solvent evaporates from the droplet, a critical field is reached at which ions are emitted from the surface. Eventually, all of the solvent is evaporated from the droplet, leaving a dry particle composed of non-volatile components of the sample solution.

Despite intensive research and numerous experiments, it has unfortunately not yet been possible to achieve a positive overall energy balance through nuclear fusion. This is not necessarily due to the fusion process itself, but rather to the technical components associated with the nuclear reactor, which consume additional energy and thus weaken the overall balance. Many scientists consider laser inertial fusion to be a much more A team from the Lawrence Livermore National Laboratory claims to have succeeded in extracting more energy from a laser fusion experiment than was previously put in. The fusion reaction produced 3.15 megajoules of energy, while the laser pumped 2.05 megajoules of energy into the target containing the fuel. This consumed around four percent of the fusion fuel. However, the entire facility (including the laser devices and accompanying components) consumed almost 100 times more energy, which completely negated the overall balance. During the presentation of the results, the research team estimated the amount of energy absorbed by the laser to ignite the fusion at around 300 megajoules (MJ). The energy of the laser light was 2.05 MJ, while around 3.15 MJ was released during the fusion, which would represent an energy gain of 153% if the experiment were used at 100%. But these are the pure energy ratios between laser energy and fusion energy yield. The entire process consumed 300 MJ! Thus, unfortunately, in the end, only 1% "energy gain" was offset by a 99% energy loss.

The invention specified in patent claims 1 to 203 is based on the problem of creating a compact and widely scalable nuclear fusion reactor that is capable of carrying out nuclear fusion processes.

This problem is solved by the features listed in patent claims 1 to 203.

The invention provides a cost-effective solution for mobility purposes.

• - er bietet eine einzigartige Methode, um Kernfusions-Energie freizusetzen,
• - er kann sehr kompakt und klein gebaut werden, daher auch für Fahrzeuge geeignet,
• - kostengünstige Bauart,
• - fast unendliche Energiequelle,
• - sichere Arbeitsweise.

Advantages of this reactor are:

• - it offers a unique method to release nuclear fusion energy,
• - it can be built very compact and small, therefore also suitable for vehicles,
• - cost-effective design,
• - almost infinite source of energy,
• - safe working practices.

Examples of implementation are shown on the 1 to 64 explained further.

• 1 ein Ausführungsbeispiel des Fusion-Reaktors mit Fluidstrahlen-Formation auf einer gemeinsamen / geraden Linie,
• 2 eine Variante mit den leicht abgewinkelten Achsen der beiden Fluidstrahl-Formationen,
• 3 die Ein-Hochdruckkammer-Konstruktion des Reaktors mit blitzartig pulsierende Druck-Werte,
• 4 die Zwei-Hochdruckkammer-Konstruktion,
• 5 ein weiteres Ausführungsbeispiel, wobei die Abgabe der Mikrotröpfe punkt- oder strich-linienförmig in Gesamt-Gestalt eines sehr dünnen Fluidstrahls erfolgt,
• 6 ein Ausführungsbeispiel mit zusätzlich einem Elektronen-Strahlen-Geber (Elektronenquelle), der einen Elektronenstrahl direkt auf dem Kollisionspunkt richtet,
• 7 eine weitere Ausführung dieses Reaktors mit zusätzlich zu Wasserstoff-Isotopen, auch das Element Bor für die Fusion verwendet wird,
• 8 die Laserstrahlenquellen für eine zusätzliche Beschleunigung der Mikro-Tropfen,
• 9 ein Ausführungsbeispiel, bei der die Piezoelemente jeweils in den Hochdruckkammern, die hohl-zylinderförmig in einem Block aus einer massiven Bauweise bestehen, eingebaut sind,
• 10 eine Hochdruckkammer mit einem Innen-Durchmesser von 12mm und einer Länge von 2mm, in der ein Piezoelement direkt gegenüber der Düse drin in die Kammer in dem Fluid eingetaucht, eingebaut ist,
• 11 ein weiteres Ausführungsbeispiel mit Piezoelemente in Form einer Scheibe und Abgewinkelte Bewegungs-Achsen der Mikro-Tröpfen,
• 12 ein Ausführungsbeispiel, wobei zusätzlich ein elektrischer Beschleuniger, der durch elektrische Entladung die beiden Mikro-Tropfen-Strahlen gegeneinander beschleunigt, eingebaut ist,
• 13 ein weiteres Ausführungsbeispiel, wobei die Mikrotropfen lediglich einen Bruchteil eines Pikoliters oder höchstens ein paar Pikoliter groß sind,
• 14 ein Ausführungsbeispiel mit einander kreuzenden Fluidstrahlen-Formationen,
• 15 die Vorrichtung mit zwei Ring-Elektroden versehen, die jeweils unter Hochspannung aus zwei getrennten Spannungsquellen stehen,
• 16 einen Fusionsreaktor mit Spannungskollektoren für direkte EnergieAbgabe für Endverbraucher,
• 17 einen Reaktor, in dem das Fluid aus Wasser (oder schwerem Wasser) besteht,
• 18 eine Anregung der Flüssigkeit selbst, die eine Volumenzunahme durch Orientierung der Wasser- oder Deuterium-Oxyd-Moleküle durch elektrische Felder, erfährt,
• 19 und 20 zeigen eine Orientierung der Wassermoleküle, die durch stark gebündelte Mikrowellenstrahlung aus Mikrowellen-Quellen und genaue SchwingPhasen-Anordnung erfolgt,
• 21 ein Ausführungsbeispiel, wobei die Hochdruckkammern je ein so kleines Innenvolumen haben, dass sie lediglich jeweils einen Mikro-Tropfen aufnehmen können,
• 22 ein Ausführungsbeispiel, bei dem Elektromagneten oder starke Dauermagneten verwendet werden, um die Wassermoleküle einheitlich anzuordnen und zu orientieren,
• 23 einen Fusionsreaktor mit Kapillar-Hochdruckkammer,
• 24 die Anordnung der Moleküle beim Drehen auf dem elektrischen Feld, das durch Mikrowellen generiert wird,
• 25 die Ausführungen mit elektrostatische Felder und Mikrowellenstrahlung in Längsachse der Kapillar-Hochdruckkammern,
• 26 ein Ausführungsbeispiel, wobei D²O auf 11,2°C gekühlt für Fusionszwecke verwendet wird,
• 27 die Orientierung der D²O Moleküle im elektrischen Feld unmittelbar vor der Kollision der Mikro-Tröpfen,
• 28 die Ausführung mit dem elektrostatischen Lauf-Feld,
• 29 eine Ausführung, wobei eine einzige Hochdruckkammer und ein Mikrowellenstrahler als Fluidbeschleuniger durch Anregung der Dipol-Moleküle und eine daraus resultierende Fluid-Volumenzunahme benutzt wird,
• 30 ein Ausführungsbeispiel mit einem Femto-Laser,
• 31 die Entstehung der beiden Fusionspunkte,
• 32 die Fließ-Sperr-Funktion durch Mikro-Tesla-Ventile,
• 33 die Verwendung von Laserquellen für eine Mikro-Ausdehnung der Flüssigkeit in die Hochdruckkammer oder außerhalb,
• 34 eine Konstruktion, bei der die Distanz zwischen den Düsen variabel gestaltet werden kann,
• 35 eine weitere Konstruktion, bei der der Kollisions-Winkel der auf einander fliegenden Mikro-Tropfen variabel gestaltet werden kann,
• 36 die Bildung der Stehwellen in den Kammern,
• 37 ein Ausführungsbeispiel mit Block-Einheiten,
• 38 eine Variante mit in Kugeln eingebauten Kapillar-Hochdruckkammern,
• 39, 40 und 41 weitere Ausführungsbeispiele des Reaktors, wobei die Abschuss-Röhre (Kapillar-Hochdruckkammer) jeweils in massiven Kugeln oder Vollzylindern mittig eingebaut sind,
• 42 die Darstellung der Beschleunigung-Vorgang der fusionsfähigen Dipol-Moleküle,
• 43 die zusätzliche Beschleunigung der Mikro-Tropfen durch elektrische Felder,
• 44 eine weitere Ausführungsmöglichkeit des Reaktors mit zwei Kapillar-Hochdruckkammer mit je einer Länge von 50mm und perpendikular zu Längsachsen-Anordnung der Hochdruck-Kapillare abgegebene Mikrowellen
• 45 eine Ausführung mit zwei kreuzende Mikro-Tropfen-Formationen, die unter einem Winkel (geringfügig kleiner als 180°) einander kreuzen und ein zusätzliches,
• elektrisches Beschleunigungs-System für die Mikro-Tropfen,
• 46 und 47 die abwechselnden Stromentladungen mit sehr hohe Repetitionsrate und dabei die elektrisch beschleunigten Mikrotropfen,
• 48 eine Ausführung, wobei Mikro-Spiegel-Chips für die Ablenkung der Mikrowellen auf das fusionsfähige Fluid verwendet werden,
• 49 eine Ausführung mit einer Laserstrahlen-Quelle, deren Laserstrahlen eine Dipol-Molekül-Drehung bewirken,
• 50 ein Ausführungsbeispiel, wobei die stark gebündelte Mikrowellenstrahlung nicht perpendikular, sondern etwas schräg auf die Kapillar-Hochdruckkammer trifft und die Dipol-Moleküle zu synchronen Rotation bringt,
• 51 eine Möglichkeit, wobei statt elektrische Felder, die Magnetfelder eine synchrone Dipol-Molekülen-Orientierung bewirken,
• 52 die spiralförmig gebauten Kapillar-Hochdruckkammer,
• 53 die Konusförmigen Kapillar-Hochdruckkammer,
• 54 ein weiteres Ausführungsbeispiel, wobei nur einer Kapillar-Hochdruckkammer eingebaut ist und mit Mikro-Tropfen auf einer stehenden Masse aus fusionsfähigem Fluid geschossen wird,
• 55 eine weitere Ausführung, wobei hier die Mikro-Tropfen aus der Kapillar-Hochdruckkammer auf frei fallenden Flüssig-Tropfen schießen,
• 56 eine Ausführung, bei der ein quer zu der Schuss-Linie der Mikro-Tropfen abgegebener Dauer-Flüssigkeitsstrahl, durch beschleunigte Mikro-Tropfen beschossen wird,
• 57 eine Variante, bei der die Targets aus Eiskügelchen bestehen, die aus einem fusionsfähigen Material bestehen,
• 58 eine Variante, bei der die Beschleunigung und Generierung der Mikro-Tropfen durch Rotation der Dipol-Moleküle, zusätzlich durch synchrone Schwingungen des Materials der Hochdruckkapillar-Kammern begleitet wird,
• 59 ein Ausführungsbeispiel, wobei die Schwingungserzeugung der Material-Konstruktion der Hochdruck-Kapillarkammer durch externe Hilfsmittel, wie Ultraschall-Quellen unterstützt wird.
• 60 eine Variante, die eine oder mehrere zusätzliche Kammer aufweist, die die Materialkonstruktion durch eigene Schwingungen stabilisieren,
• 61 eine Variante, bei der reines Wasser als „Antriebselement“ für die Beschleunigung anderer Atome (z.B. Bor-Atome) und Kernfusionsvorgänge benutzt werden kann,
• 62 eine Makrodarstellung des Mikrotropfens sowie deren „Ummantelung“ und „Kern“,
• 63 ein Ausführungsbeispiel mit nur einer Kapillar-Hochdruckkammer und einen schnell fließenden Flüssigkeitsstrahl,
• 64 ein Ausführungsbeispiel mit einem Femto-Laser-Gerät.

They show:

• 1 an embodiment of the fusion reactor with fluid jet formation on a common / straight line,
• 2 a variant with the slightly angled axes of the two fluid jet formations,
• 3 the single-high-pressure chamber design of the reactor with lightning-like pulsating pressure values,
• 4 the two-high-pressure chamber design,
• 5 a further embodiment, wherein the microdroplets are emitted in dot-like or dashed lines in the overall form of a very thin fluid jet,
• 6 an embodiment with an additional electron beam generator (electron source) that directs an electron beam directly onto the collision point,
• 7 another version of this reactor with, in addition to hydrogen isotopes, the element boron is also used for fusion,
• 8 the laser beam sources for additional acceleration of the micro-droplets,
• 9 an embodiment in which the piezo elements are each installed in the high-pressure chambers, which are hollow-cylindrical in a block of solid construction,
• 10 a high-pressure chamber with an inner diameter of 12mm and a length of 2mm, in which a piezo element is installed directly opposite the nozzle and immersed in the fluid inside the chamber,
• 11 another embodiment with piezo elements in the form of a disc and angled movement axes of the micro-droplets,
• 12 an embodiment in which an electrical accelerator is additionally installed, which accelerates the two micro-droplet jets against each other by means of electrical discharge,
• 13 another embodiment, wherein the microdroplets are only a fraction of a picoliter or at most a few picoliters in size,
• 14 an embodiment with intersecting fluid jet formations,
• 15 the device is provided with two ring electrodes, each of which is under high voltage from two separate voltage sources,
• 16 a fusion reactor with voltage collectors for direct energy delivery to end users,
• 17 a reactor in which the fluid consists of water (or heavy water),
• 18 an excitation of the liquid itself, which causes an increase in volume by orientation of the Water or deuterium oxide molecules by electric fields,
• 19 and 20 show an orientation of the water molecules, which is achieved by highly focused microwave radiation from microwave sources and precise oscillation phase arrangement,
• 21 an embodiment in which the high-pressure chambers each have such a small internal volume that they can only hold one micro-droplet each,
• 22 an embodiment in which electromagnets or strong permanent magnets are used to arrange and orient the water molecules uniformly,
• 23 a fusion reactor with a capillary high-pressure chamber,
• 24 the arrangement of the molecules when rotating on the electric field generated by microwaves,
• 25 the versions with electrostatic fields and microwave radiation in the longitudinal axis of the capillary high-pressure chambers,
• 26 an embodiment in which D ² O cooled to 11.2°C is used for fusion purposes,
• 27 the orientation of the D ² O molecules in the electric field immediately before the collision of the micro-droplets,
• 28 the version with the electrostatic running field,
• 29 an embodiment in which a single high-pressure chamber and a microwave emitter are used as a fluid accelerator by exciting the dipole molecules and a resulting fluid volume increase,
• 30 an embodiment with a femto laser,
• 31 the formation of the two fusion points,
• 32 the flow-lock function through micro-Tesla valves,
• 33 the use of laser sources for micro-expansion of the fluid into or outside the high-pressure chamber,
• 34 a design in which the distance between the nozzles can be varied,
• 35 another construction in which the collision angle of the micro-droplets flying towards each other can be varied,
• 36 the formation of standing waves in the chambers,
• 37 an embodiment with block units,
• 38 a variant with capillary high-pressure chambers built into spheres,
• 39 , 40 and 41 further embodiments of the reactor, where the launch tube (capillary high-pressure chamber) is installed centrally in solid spheres or solid cylinders,
• 42 the representation of the acceleration process of the fusion-capable dipole molecules,
• 43 the additional acceleration of the micro-droplets by electric fields,
• 44 Another design option for the reactor with two capillary high-pressure chambers, each with a length of 50 mm and microwaves emitted perpendicular to the longitudinal axis of the high-pressure capillary
• 45 a design with two crossing micro-drop formations that cross each other at an angle (slightly less than 180°) and an additional,
• electrical acceleration system for the micro-droplets,
• 46 and 47 the alternating current discharges with very high repetition rate and the electrically accelerated microdroplets,
• 48 an embodiment in which micro-mirror chips are used to deflect the microwaves onto the fusible fluid,
• 49 a version with a laser beam source whose laser beams cause a dipole molecule rotation,
• 50 an embodiment in which the highly focused microwave radiation does not hit the capillary high-pressure chamber perpendicularly, but at a slight angle, causing the dipole molecules to rotate synchronously,
• 51 a possibility where instead of electric fields, magnetic fields cause a synchronous dipole molecule orientation,
• 52 the spiral-shaped capillary high-pressure chamber,
• 53 the conical capillary high-pressure chamber,
• 54 another embodiment, in which only one capillary high-pressure chamber is installed and micro-droplets are fired onto a standing mass of fusible fluid,
• 55 another version, where the micro-droplets from the capillary high-pressure chamber shoot onto freely falling liquid drops,
• 56 a design in which a continuous liquid jet emitted transversely to the line of fire of the micro-droplets is bombarded by accelerated micro-droplets,
• 57 a variant in which the targets consist of ice spheres made of a fusion-capable material,
• 58 a variant in which the acceleration and generation of the micro-droplets is accompanied by rotation of the dipole molecules, additionally by synchronous vibrations of the material of the high-pressure capillary chambers,
• 59 an embodiment in which the vibration generation of the material construction of the high-pressure capillary chamber is supported by external aids, such as ultrasound sources.
• 60 a variant that has one or more additional chambers that stabilize the material construction through their own vibrations,
• 61 a variant in which pure water can be used as a “propulsion element” for the acceleration of other atoms (e.g. boron atoms) and nuclear fusion processes,
• 62 a macro view of the microdroplet and its “shell” and “core”,
• 63 an embodiment with only one capillary high-pressure chamber and a fast-flowing liquid jet,
• 64 an embodiment with a femto laser device.

In the invention, the nuclear fusion of fusible elements is achieved through extremely high kinetics.

The fact is that colliding particles, atoms, molecules, or groups/formations of molecules, can, under certain circumstances, fuse. Many light elements can fuse together, releasing very high levels of energy. To achieve this, extremely high kinetic energies are required. Collisions with sufficiently high kinetic energy can force matter to undergo nuclear fusion. The colliding masses can be in the picogram (pg), nanogram, microgram, or even gram range. It is simply a matter of the technical feasibility of the acceleration devices that cause this matter to collide. Ions are the easiest to accelerate because they are electrically charged and can be accelerated very strongly by electric fields. However, ion acceleration also has some disadvantages. The colliding ions have the same electrical charge, and the closer they come to each other, the more intense the electrical repulsion forces become. This is why the ion beams are relatively sparsely populated. The situation is different when electrically neutral particles are sent to collide with each other. These can form larger clumps. To achieve nuclear fusion, these particles/groups/clumps would have to be sent against each other at a speed of at least 50 km/s. Although such accelerations are complex to achieve, there is still a way to do it. Projectile fusion, for example, proves that even masses in the gram range can be accelerated against a target. The advantage here is the larger number of particles that are accelerated at the same time. They are sent on a collision course in atomic or molecular form, not individually, but in groups consisting of millions or billions of them. 50 km/s is sufficient to cause nuclear fusion. Of course, only a very small number of atoms fuse with each other, but this is enough to release a huge amount of energy, also because a high repetition rate of collisions per second is feasible.

The rotation of dipole molecules can cause mass acceleration. Molecular dipoles and molecular acceleration of a fluid can be achieved using several existing techniques. Using IR femto-lasers to rotate dipole molecules is a promising approach. The challenge of accelerating a droplet to 100–200 km/s requires enormous energy and precise control.

• - Hochintensitätslaser: Diese können genutzt werden, um durch die Erzeugung von Plasma auf der Oberfläche eines Tropfens extrem hohe Drücke zu erzeugen. Ein starker Laser oder ein Teilchenstrahl wird durch ein Gas geschossen, um ein Plasma zu erzeugen.
• - Elektromagnetische Beschleunigung: Technologien, die ähnlich wie Railguns oder Coilguns funktionieren, könnten theoretisch verwendet werden, um kleine Flüssigkeitsmengen auf hohe Geschwindigkeiten zu beschleunigen.
• - Plasma-Beschleuniger: Diese Technologie nutzt Plasmawellen, um Teilchen auf extrem hohe Geschwindigkeiten zu bringen und könnten für Flüssigkeiten angepasst werden. Der Laser oder der Teilchenstrahl erzeugt im Plasma eine dichte Welle von Elektronen, die als Plasmawelle bezeichnet wird, die die Moleküle eines Mikrotropfens vorschieben kann und deren als Antrieb für starke Beschleunigung dienen. Die Mikrotropfen werden dabei in Plasma-Welle mitgezogen bzw. vorgeschoben. Die Moleküle können dabei auf sehr hohe Geschwindigkeiten gebracht werden. Plasma-Beschleuniger sind in erster Linie für die Beschleunigung von geladenen Teilchen (z.B. Elektronen) konzipiert. Die direkte Anwendung auf Flüssigkeiten ist etwas komplexer, weil Flüssigkeiten aus neutralen Molekülen bestehen und nicht ohne weiteres in einem elektrischen oder magnetischen Feld beschleunigt werden können wie geladene Teilchen. Allerdings könnten theoretisch ähnliche Prinzipien genutzt werden, um Flüssigkeits-Mikrotropfen in einem Plasmaumfeld zu manipulieren oder zu beschleunigen, indem sie indirekt durch die erzeugten Druckwellen oder Schockwellen beeinflusst werden.
• - Zuletzt eine Ultraschnelle Strömungsmechanik: Fortschritte in der Strömungsmechanik könnten neue Wege eröffnen, um Flüssigkeiten effizient und schnell zu beschleunigen.

To accelerate a droplet to extremely high speeds, the following technologies could also be helpful:

• - High-intensity lasers: These can be used to generate extremely high pressures by creating plasma on the surface of a droplet. A powerful laser or particle beam is fired through a gas to create a plasma.
• - Electromagnetic acceleration: Technologies that work similarly to railguns or coilguns could theoretically be used to accelerate small amounts of liquid to high speeds.
• - Plasma accelerators: This technology uses plasma waves to accelerate particles to extremely high speeds and could be adapted for liquids. The laser or particle beam creates a dense wave of electrons in the plasma, known as plasma. A plasma wave is a device that can propel the molecules of a microdroplet forward and serve as a propulsion system for strong acceleration. The microdroplets are pulled along or pushed forward in the plasma wave. The molecules can be accelerated to very high speeds. Plasma accelerators are primarily designed for the acceleration of charged particles (e.g. electrons). The direct application to liquids is somewhat more complex because liquids consist of neutral molecules and cannot be easily accelerated in an electric or magnetic field like charged particles. However, similar principles could theoretically be used to manipulate or accelerate liquid microdroplets in a plasma environment by indirectly influencing them through the generated pressure waves or shock waves.
• - Finally, ultrafast fluid mechanics: Advances in fluid mechanics could open up new ways to accelerate fluids efficiently and quickly.

The invention relates to a fusion reactor 1 designed as a primary energy source and suitable for powering households, industry, or even mobile applications, e.g., vehicles. For the fusion processes, microdroplets 2 of fusible, incompressible material (fluid) are strongly accelerated and brought into collision. The micro-quantities accelerated against each other in the form of micro-droplets of incompressible liquid are extremely small (approximately 100 picoliters) and are accelerated by pressure generators. The generation of a fluid jet formation consisting of microdroplets or micro-quantities of incompressible, fusible liquid arranged in one or more rows in the jet direction (like strings of pearls) can largely optimize the fusion processes. The liquid does not have to be completely fusion-capable. It is sufficient if fusion-capable elements are integrated or present in their molecules (e.g., hydrogen atoms or deuterium/tritium together with other chemical elements, such as oxygen, etc.). Several hundred to hundreds of thousands of micro-quantities/micro-droplets are generated per second from two opposing nozzles (3 and 4 or high-pressure chamber openings 84) and accelerated to a collision point at over 50 km/s. Because no continuous fluid jet is emitted here, but rather only formations of portioned micro-quantities in the form of separate micro-droplets in picoliter volume, the acceleration is somewhat more effective than in reactors with fluid jet generation. The load on the structure is kept within limits, and the "recharging" also works more optimally here. Because the mass of the micro-droplets with a volume of approximately 100 picoliters, which consists of liquid deuterium, is approximately 16 nanograms, accelerating this micro-mass to 50 km/s requires a Energy of 0.02J (similar to what would be required, for example, for acceleration from 160g to 0.5m/s), which can also be provided with a not too great energy expenditure.

The aim of achieving fusion processes currently favors fusion technology, in which deuterium atoms or a mix of deuterium and tritium atoms fuse. This creates a helium nucleus, releases a neutron, and releases large amounts of usable energy. Alternatively, boron atoms can also be used for nuclear fusion. One variant described here also uses boron atoms, which are intended to fuse with deuterium. However, the use of boron requires a significantly higher kinetic energy of the microdroplets, which contain boron atoms in addition to liquid deuterium (approx. 200 km/s). Nuclear fusion produces an enormous amount of energy. Just 1g of hydrogen would replace approximately 10,000 liters of oil (i.e., 1:10,000,000) if all atoms in it undergo complete nuclear fusion. 1 liter of oil produces 11 kWh of energy. One gram of fuel could thus generate 90,000 kilowatt-hours of energy in a power plant—the equivalent of the combustion heat of 11 tons of coal. Fusion fuels are very cheap and more or less evenly distributed across the Earth. The biggest problem with nuclear fusion is the Coulomb force, which prevents the ions from approaching within very short distances, where the nuclear forces act and "glue" the nucleons together. However, with sufficiently high kinetic energy, this barrier can be overcome.

The fusion reactor described here can overcome the Coulomb forces in a targeted manner and thus with somewhat less energy expenditure than plasma reactors to drive nuclear fusion, because it involves closely spaced groups of atoms (from the picogram to microgram range) being fired at each other. In addition, neutral atoms or even differently charged ions are firing at each other, so that at the point of collision, at least at the atomic level, no electrical repulsion forces are present (in the best case, attractive forces even arise). This changes, however, as soon as the collision advances to the nuclear/proton range. Advantages over projectile inertial fusion technology exist here because it is not projectiles, but rather liquid-jet formations made up of portioned micro-quantities of liquid or micro-droplets that are fired at each other. Any number of which can be generated one after the other in very short time intervals. The invention here also has an advantage over liquid jet bombardment fusion reactors because instead of generating a continuous or pulsed fluid jet of liquid deuterium and tritium, individual, portioned, separate micro-quantities or micro-droplets are generated and fired against each other. The nuclear reactor that uses micro-droplets instead of fluid jets is somewhat better suited to nuclear fusion because the micro-droplets can be accelerated to significantly higher speeds without having to accept material fatigue of the reactor structure. In addition, the resonant vibrations of the material can be used to optimize the structural stability of the high-pressure chamber. With phase-inverted vibrations directed against the vibration amplitudes of the high-pressure chamber walls, which are generated during pressure generation by rotating the dipole molecules, the stability can be significantly increased.

The reactor design based on this technology differs significantly from fluid jet nuclear fusion reactors because, instead of fluid jets, "nano-projectiles" that also serve as targets are used. Micro-droplets in picoliter size (approx. 100 pl) are fired against each other at extremely high speeds with a repetition rate that can be adjusted from low to very high. Because, instead of fluid jets, extremely small, individually generated micro-droplets, comparable to the micro-droplets from inkjet printers (albeit much faster), are fired against each other to the collision point, the pressure in the high-pressure chamber can be largely controlled by the inertia of the solid wall. There is also an important factor that utilizes inertia to protect the structure: the micro-droplet generation gives the chamber's construction material some time to "regenerate," or deformation oscillations occur in the chamber material, which provide positive support for the generation of the next micro-droplets. Every mass has a vibrational resonance that depends on the material construction, the material used, and the mass of the construction. This resonance frequency can be used constructively by using the vibration amplitudes to balance the forces and counterforces during microdroplet generation. The vibrational resonance of the high-pressure chamber can be calculated mathematically or simply determined empirically, which is specific to each construction type. If the microdroplets are launched at the exact moment when the construction contracts (after it has expanded slightly during the first microdroplet generation), the stability of the reactor is at its highest. Ultrasonic generators can also be used to introduce ultrasonic or sonic vibrations into the reactor structure that are synchronized with the vibration phases generated by microdroplet generation. This makes this type of reactor more durable than nuclear fusion reactors, which use fluid jets to project fluids to the collision point. Of course, the chamber in which the collision takes place is either airless or evacuated, or there is a very low pressure there.

The fluid accelerators used here essentially utilize two principles to accelerate the micro-droplets: pressure generation using electrically rapidly deformable materials/elements that displace the fluid into the high-pressure chamber, or by stimulating the fluid/liquid itself to expand quickly and very slightly. Devices equipped with fluid accelerators that aim for internal fluid stimulation to increase volume generate the pressure force directly within the fluid through a simultaneous and equal molecular dipole vector alignment within the fluid itself, resulting in an ultra-rapid and slight expansion of the fluid's total volume. In the versions with expansion elements, these are immersed in the fluid and generate a pressure pulse on all sides of the fluid for an extremely short time. The expansion of the expansion elements is also very slight and is stimulated electrically, by electromagnetic/electrostatic fields, or by microwaves. For our purposes, we need a volume increase of only approximately 200 pl of a 2 ml total volume of liquid in the high-pressure chamber or in a capillary high-pressure chamber, which corresponds to a volume increase of 0.00001%. With 20 ml of liquid in the high-pressure chamber, the ratio would even drop to 0.000001%. However, this volume increase must occur very quickly, within 0.01 ns - 0.1 ns, which also works with the devices and methods described below. The design and material of the high-pressure chamber/capillary high-pressure chamber perfectly withstands the pressure force generated by a 0.00001% volume increase of the liquid within 0.01 - 0.1 ns. This is not because the material of the high-pressure chamber/capillary high-pressure chamber walls is so stable, but rather due to the inertia of the massive high-pressure chamber walls (a few cm to dozens of cm thick). The volume increase takes only 0.01 - 0.1 ns, and the inertia of the walls plays a crucial role in the stability of the structure. Although nano-vibrations occur within the mass structure of the high-pressure chamber walls, they are suppressed by the massive The design and inertia of the structure are quickly absorbed or smoothed out.

It is known that high enough kinetic energy can cause nuclear fusion between two atoms. Through careful measurements, it can be determined that this process also sometimes occurs in nature. When asteroids collide in space at high speed, flashes of gamma radiation are often detected. Gamma radiation is a reliable indication that nuclear fusion, or sometimes even nuclear fission, of a very small mass has occurred at the collision point between the two asteroids. The emission lasts only very briefly (a few nanoseconds) and can therefore only be detected if measuring instruments are aimed at it from a distance. Craters from meteorite impacts on moons or celestial bodies without atmospheres are also sometimes slightly larger than they would have been caused by kinetic energy alone. This means that additional nuclear energy was released during the impact, mostly through nuclear fusion of the hydrogen atoms of the water bound in the rock. The atomic structure and the molecules located on the frontal surface of the asteroid that collides with the other's surface will inevitably trigger nuclear fusion of a very small proportion of the material there during an impact at 40-100 km/s, if there are water molecules, ice, hydrogen bound in the rock, or boron. In the first few nanoseconds of the impact, nuclear fusion occurs in the hydrogen located directly at the collision point. Depending on the size of the colliding asteroids, partial fusion can occur in a layer of the asteroid's surface material a few millimeters thick. If the asteroid is 1000m or larger, then underlying layers, extending to a depth of several dozen centimeters, are certainly also involved in the nuclear fusion processes. Of course, not the entire mass of the surface layers at the collision point undergoes fusion, because there is a lot of material there that is difficult to fuse with, and the kinetic energy is quickly absorbed by the material of the colliding fragments upon impact. However, traces of material are also present that can fuse thanks to the kinetic impact energy of both asteroids. The energy component is very small compared to the kinetic energy of the asteroids, but it can still be detected with precise measuring instruments. Almost every head-on or angular collision between fast-moving asteroids or meteorites also leads to a small amount of nuclear fusion/fission of the elements present on the surface and slightly deeper at the impact point. The head-on collisions of meteorites or compact rocks in space, which collide at dozens of km/s, produce not only a very bright flash of light, but also UV and gamma emissions. Gamma emissions, in particular, indicate that nuclear fusion has occurred. Furthermore, with sophisticated detectors, the creation and release of helium nuclei can be detected after a collision between two rocks in space. The meteorites, which enter our atmosphere at over 35 km/s (or significantly faster), collide with, among other things, water microdroplets (known to consist of oxygen and hydrogen) and free hydrogen atoms in the atmosphere. Due to the enormous kinetic energy, some of the atoms undergo nuclear fusion. Micro-explosions from nuclear fusion processes are generated, which have a destructive effect on the incoming rock. These micro-explosions shatter the surface in a flash, destroying the structure of the meteorites at an ever-increasing rate. This ultimately leads to their explosion in the atmosphere (if they are not too large) due to the rapid penetration of air currents and heating through friction and air compression in the inner structure. Those large and compact enough to reach the planet's surface carry the fusion processes all the way to the surface, and upon collision with the planet's crust, small amounts of nuclear fusion occur again. Depending on the composition of the rock, if it contains radioactive material, nuclear fission can also occur. The release of nuclear energy or fusion energy can also explain the size of the craters on alien planets, which would otherwise be slightly smaller if fusion energy were lacking and only the effect of kinetic energy were at play.

Fusion processes occur not only outside of Earth in the stars and into space, but also, to a lesser extent, here on Earth in nature. Fusion processes can be detected by sensitive equipment during intense lightning strikes. Lightning strikes accelerate ions to up to 5-10% of the C velocity (C=300,000 km/s), sometimes leading to nuclear fusion. It is known that lightning discharges in a gas (also in nature or the atmosphere) lead to the movement of ions. Atmospheric lightning on Earth or on other planets occasionally causes some of the particles to be accelerated so strongly that nuclear fusion can occur. Detailed measurements show that lightning discharges sometimes release gamma radiation or gamma emission. The ions are greatly accelerated by high-voltage discharges. The speed a lightning discharge can reach is less than the speed of light, but can reach up to 70% of the speed of light (C). Considering that matter (or ions) is set in motion very quickly in this ion channel, one can imagine that very high amounts of energy can be released there during a fusion process. Almost every natural lightning discharge results in a small amount of nuclear fusion of the light elements. However, in a lightning discharge as it occurs in nature, only a very small number of atoms or ions will collide with each other sufficiently and optimally to lead to fusion. In addition, the fusion-capable elements in the atmosphere are only present in very low concentrations. Nuclear fusion processes are often difficult to detect with our technical capabilities. But nevertheless, nuclear fusion does occur there too. If you are well-equipped, invest enough time in thunderstorms, and carry out measurements, you can occasionally measure and detect gamma emissions from lightning strikes. Nuclear fusion processes occur more frequently at nodes, where "lightning branches" intersect or touch. Helium nuclei can be detected with sensitive measurements or sensors. This is evidence that fusion processes have taken place there. Nuclear fusion thus occurs not only in the stars and the sun, but also outside in the cosmos and on Earth, and much more frequently than one would think.

The explanation for why so much energy can be released during nuclear fusion lies in the nature of atoms and matter in general. Although matter consists of atoms, they are almost completely empty. Near the center sits a tiny nucleus of nucleons, surrounded by a comparatively large nebula of rapidly orbiting electrons, which determine the circumference of the atom. The space in between is empty and determined only by fields. Both nucleons and the electron themselves are not solid "objects." Although the electron is described as a point-like, structureless elementary symbol, it also possesses an internal structure. Because it is so small, in contrast to the atomic nucleus, it is virtually indestructible. While the electron appears hard, for example, in contrast to protons or neutrons, it also has a "spongy" structure, with its center being somewhat harder than its "shell." An electron can also be destroyed or created anew. One example of this is the fractional quantum Hall effect. A strong magnetic field causes electrons in some two-dimensional materials to behave as if they were splitting into three (or more) new particles (anyons). However, using a different technique, it is possible to actually split the electron. The entire electron consists of merely intertwined photons. These photons remain trapped within each other, even though they are constantly "rubbing" past each other at the speed of light in a very small space. This entanglement can only occur when several high-energy photons come extremely close to each other or collide linearly or at certain angles. Conversely, the electron can also be untangled into individual photons. Because these photons, traveling at the speed of light, still circle, move back and forth, or "rotate" in complex trajectories, they impart mass to the matter. Photons acquire mass, or rather, weigh "heavy," only when they travel at C speed.

Based on data from the COBE satellite, which provides the most precise measurement of the cosmic background radiation spectrum to date, scientists have concluded that the lifetime of photons with an assumed mass of 2 × 10 ⁵⁴ kilograms must be at least three years. Because they have mass (stated to be approximately 2 × 10 ^-54 kg, but in reality it is even less, approximately 3.4 × 10 ^-55 kg), as they move, they interact with gravitons in the gravitational field and thereby acquire weight. Therefore, as light passes by a star, it is attracted by its gravitational field, and a slight bending of light occurs. While the curvature of space has nothing to do with reality, the bending of light can be "wonderfully" explained using the relativistic theory of space curvature. The idea of the curvature of space was unfortunately adopted by the masses, and unfortunately by many scientists as well, from a layman's attempt at explanation (the famous stretched sheet with the half-submerged sphere) and completely misinterpreted. There is no real curvature of space; this is merely an attempt to explain it using a physics model, which unfortunately leads to misconceptions and confusion, nothing else. The diffraction of light can be calculated very precisely using simple physics formulas (without considering the curvature of space). They do not possess a rest mass (goodbye Higgs boson theory). Photon entanglements no longer occur in nature, but they do in large stars because the photon density there is enormous. Black holes can generate not only particles but also atomic nuclei and electrons from the energy (photons). It was previously assumed that when light rays intersect or are emitted against each other in a beam, there is no interaction between them. Although it is not yet measurable with conventional methods, there is an interaction even between crossing light beams! The light beam, however, is extremely "sparsely populated," so that only a few of the photons "collide with each other." Only when the radiation density and photon density are extremely high do the interactions become noticeable and measurable. Using high-energy laser beams and strong focusing, the photons can be brought so close to each other, or into collision, that a "small" number of them become entangled with and within each other and trapped by themselves. This way, one can "manufacture" full electrons (although this sounds absurd from the perspective of quantum theory, they also exist in other variants - e.g., half-electrons or quarter-electrons - and were even proven a few weeks ago). All the material in space is constructed in a similar way - from entangled photons. If these entanglements are triggered, a gigantic amount of photons is released, which can be perceived as energy. During hydrogen nuclear fusion, approximately 4% of the mass is unknitted, releasing an enormously high concentration of photons as radiation in all directions (expanding into a sphere at the speed of light). This is the energy that comes from nuclear fusion. In addition, nearby neutrons are bombarded with photons, becoming "saturated" and pushed away. In the process, they receive an enormously high thrust from the photons flying away, which is released as thermal energy when decelerated. The very high nuclear fusion energy comes from the photons that are already present in the matter, or that form the matter. These photons then travel in a straight line in all directions, always with the tendency to increase the distances between neighboring photons. This light energy, which consists of the 40g of unknitted matter from a 1kg mass of hydrogen, is the flash that first strikes the surroundings from a hydrogen bomb. Practically the entire surrounding area is hit with an ever-expanding, spherical shell of 40g of pure photon mass, consisting of matter in photon form accelerated at the speed of light. This 40g of photon mass is essentially the woven matter that has been "devoured" in the process, broken down into photons (the so-called mass defect), and escaping from the starting point at the speed of light. 40g of pure photon "mass" means an enormously strong, destructive radiation energy output is released in the process for the matter in its path. The corpuscular radiation that is also created receives its kinetic energy from the massively escaping photons. Similar fusion processes occur all the time in space, which is why photons from an infinite number of stars have been traveling for billions of years. However, photons are not eternally long-lived. A photon actually only lives for about 3 years, but due to time dilation, it can exist significantly longer. In the theory of relativity, however, the C constant is not implemented entirely correctly. C should rather have referred to the gravitational field expansion velocity, which, although only very slightly higher than the speed of light in a vacuum, still exhibits a femto-difference. This explains why a photon becomes "tired" after about 13.8 billion years and can no longer be seen. This also explains why we cannot see stars that are further than 13.8 billion light-years away. And this not only happens here on Earth, in all directions, but the same can also be observed from a planet that is 13.8 billion light-years away from us. The inhabitants there also see a sphere around their planet with a diameter of 27.6 billion light-years, at the center of which they themselves are located, and they may know that the universe does not necessarily have to be expanding. This "invisibility" has little to do with the expansion of the universe, and even less to do with the hypothetical, non-existent dark matter/dark energy. Unfortunately, scientists have invested enormous effort in research to prove the existence of dark energy and dark matter, completely in vain. Neither dark matter nor dark energy exists. There are also stars and galaxies in distant regions of space that are racing not away from us, but toward us, but they are also invisible! One only has to look at it again from the perspective of two reference systems, one planet 10 billion light-years away and another 20 billion light-years away, and then it becomes crystal clear what is happening in the universe and what the real situation is with inflation. Everything from these two planets also flies away in a spherical shape, but part of these "spherical shells" is flying toward us, which absolutely does not fit with Doppler effect observations! Unfortunately, we are wrong about many ideas and astronomical observations. Just as many physics theories are wrong: from the theory of relativity to quantum physics. The Earth is not the center of the universe! If everything in the universe is expanding from us, what does it look like from the perspective of a planet 10 billion light-years away? Everything on that planet is expanding as well, and at half our distance (5 billion light-years), a collision between the two "expansion shells" of the universe would occur, which is not actually the case. The secret lies in the nature of photons: first, they travel slightly slower than the propagation speed of the gravitational field, and second, after a travel distance of 13.6 billion light-years, or their range, they become "tired." This "photon fatigue," or loss of energy, is characterized by the red-shift. The older the photons are, the more their energy level shifts in the red range. And then we falsely assume this fact and use this "evidence" for a theory about the expansion of the universe, without questioning what the alien scientists on the other planet 10 billion light-years away are observing, which borders on a rather pronounced arrogance of science. Thus, the nonexistent dark matter/energy and even the Hubble constant are completely irrelevant.

To understand nuclear fusion processes, insight into the matter itself is necessary. The unknitting of matter is symbolically similar to a rapidly rotating wheel that, due to centrifugal force, disintegrates into individual pieces, with each piece flying apart, or analogous to a knitted glove (or a ball of wool) where the thread is pulled out. The faster the thread is pulled out, the smaller the glove becomes. However, until the glove disappears completely, a thread several hundred meters long is pulled out.

The reactor in this invention utilizes fusion processes to release energy through cold, incompressible, fluid-jet formations (liquid distributed in micro-droplets that are individually accelerated) made of fusible material, which in this case consist of individual micro-droplets emitted in pulses one after the other from two nozzles. The kinetic energy is extremely high, and a collision between two micro-droplets, or one micro-droplet with a stationary, fusible fluid, overcomes the Coulomb force between the colliding atoms within, leading to nuclear fusion. The liquid-jet formations, or the micro-droplets, are relatively cold, but upon collision, they heat up extremely and rapidly. As soon as nuclear fusion occurs, the temperature rises rapidly to over several dozen to hundreds of millions of °C, with highly ionized particles flying ultrafast in all directions from the collision point. Such particles will be encountered by subsequent micro-droplets if they are released at a sufficiently high repetition rate, so that at the moment the first micro-droplet collides, the second is already launched and flies into the bombardment field of the diverging particles after the nuclear fusion process. The repetition rate and the pauses between the release of two micro-droplets also determine the efficiency of the reactor. Rapidly repeated micro-droplet release is always optimal for the energy balance. As soon as two micro-droplets collide, a few subsequent micro-droplets are already launched, so that the subsequent micro-droplet comes within approximately 28µm of the colliding micro-droplets and can capture as much of the particles as possible from the colliding micro-droplets. The flying particles, partly consisting of hydrogen ions/deuterium ions, travel at approximately 500–30,000km/s and significantly optimize nuclear fusion in the subsequent micro-droplets. This allows subsequent nuclear fusion processes to occur with significantly less pressure in the high-pressure chamber. The first droplet must be accelerated significantly to "ignite" the fusion, while the subsequent ones can travel at a moderate speed (at just a few km/s or even less) as long as they arrive at the collision point in series. It is important to select the flight speed of the subsequent micro-droplets so that when they are hit by the particles originating from the fusion micro-droplets, they also reach the collision point immediately. This means that nuclear fusion does not occur far from the collision point, but rather directly there. Otherwise, instead of one nuclear fusion point, two points would be created, which would continue to move in the direction of the nozzle. It is therefore important to increase the speed of the micro-droplets so much that they actually undergo nuclear fusion at the intended collision point. This can also be achieved by increasing the repetition rate for the generation of the micro-droplets. If the number of microdroplets traveling toward the collision point in a ray pattern increases, they increasingly shield each other, or the subsequent microdroplets are temporarily shielded by the ones in between, preventing them from being directly impacted by the high-energy particles. Thus, the nuclear fusion processes in the subsequent microdroplets are somewhat delayed until they actually reach the calculated or intended collision point.

This reactor can be easily scaled to almost any power output. It is also ideally suited for small to medium power outputs, making it suitable for mobile applications (vehicles of all kinds). Nuclear fusion can be achieved here on a large or miniature scale. For such applications, micro-droplets of fusion-capable material are catapulted against each other in rows in the form of two very thin fluid jets (5 and 6 - fluid jet from micro-droplet formation), causing them to collide.

The micro-droplets are accelerated from the nozzles by piezo actuators 7, magnetostriction drives, or plasma micro-explosions using pressure and additional electrical power. The advantage is that the micro-droplets are charged, but not so much that all the atoms within are ionized. The electrical charge accumulates primarily on the surface of the micro-droplets, forming a kind of "electrostatic outer shell" 8. Droplets are emitted in a row (fluid jet) at short intervals, each forming a fluid jet formation. This fluid jet formation is not a continuous fluid jet, but rather a series of micro-droplets emitted one after the other and not touching each other. On a high-speed camera, this fluid jet formation of micro-droplets would not really look like a jet. Rather, it looks like small dots emerging from both nozzles in rapid succession, colliding with oncoming micro-droplets or a micro-droplet striking a stationary or slowly flowing fluid. The fluid jet formations therefore each look like an extremely thin, dotted or dashed line, the distances between which can be very large or slightly smaller, depending on the repetition rate setting for generating the micro-droplets. If there are long pauses between them (in the microsecond or even millisecond range), the image shows only one micro-droplet/dot rushing to the collision point with the micro-droplet from the other nozzle. And only milliseconds later, the next dot is released. The collision of two micro-droplets via two fluid jet formations occurs linearly (straight through 180°) on the same fluid jet formation axis 8 or at a very wide angle 10, almost linearly to each other (approx. 176° - 179°). These two "dotted lines" consisting of micro-droplets 2 thus meet on the same axis or cross at a wide angle (e.g. 176° - 179°). The collision point 11 is located exactly between the two nozzles that shoot these fluid jet formations against each other. For fluid jet formations that are exactly on one line/axis, it is important to release the micro-droplets simultaneously. Otherwise, depending on which of the micro-droplets in which fluid jet formation exits the nozzle first, the collision point with the other micro-droplet emerging from the other nozzle will shift. It may happen that one micro-droplet does not hit the other at all, but directly hits the liquid that is still in the nozzle opening 12 opposite it. Therefore, it is important to start both fluid jet formations simultaneously ( 1 ). The variant with the slightly angled axes 9 of the two fluid jet formations ( 2 ), does not have this problem because the fluid jet formations (5 and 6) merely cross there, although with a low repetition rate fewer micro-droplets can collide here (with today's technology, the hit rate would be a few percent below 176° fluid jet formation intersection angle). The larger the intersection angle 10, the better the hit rate and it increases dramatically the closer the angle gets to 180°. At a wide angle of almost 180° (e.g. 179.998°), the collisions can still be viewed almost as a direct head-on collision. As long as the fusible fluid (incompressible) is in the high-pressure chamber, it is accelerated by high-pressure technology and exits the nozzles. Immediately afterwards, or already in the nozzle, the micro-droplets are electrically charged and then further accelerated by electric fields and electrodes. The micro-droplets consist of a multitude of 13 groups of atoms that are capable of fusing when they collide. Because the majority of atoms within the micro-droplets are neutral, no electrical repulsion occurs until their nuclei come very close to each other. When micro-droplets from two nozzles collide, a lever effect often occurs between the groups of atoms. Some groups of atoms are significantly slowed down, while the other, directly adjacent groups of atoms benefit from this additional kinetic energy being transferred to them (leverage effect), so that it exceeds the travel speed of the micro-droplet as a whole. Such additionally accelerated atoms lead to increased fusion when they collide.

In conventional fusion reactors, ions with the same charge are primarily used to collide with each other and thus fuse, causing nuclear fusion. The electric fields offer great resistance and prevent the ions from colliding. However, this requires extremely high temperatures and long-term plasma confinement by magnetic fields so that the ions come close to each other and, above all, often enough to fuse. The greatest challenge is the extremely thin plasma, which is almost like a high vacuum, and above all the identical electrical charge with which these particles are supposed to collide. The probability of two particles colliding is extremely low, but it does happen sporadically when the temperature rises above 100 million degrees.

However, the invention does not use a plasma in large volumes, as occurs in Tokamak reactors, for example (depending on the size of the reactor, from a few to hundreds of m ³ ), but rather the kinetic energy of liquid micro-droplets, which are accelerated against each other at high speed to a collision point. The advantages here are significantly greater than with Tokamak technology. The matter that is brought to fusion here is not, like Tokamak plasma, almost vacuum-like thin, but, in comparison, very dense. In addition, the collision particles here are electrically neutral or even are differently charged (and therefore attract each other!!). The fusion-capable material is in the form of two fluid jets, which do not consist of a continuous fluid flow, but of finely dosed microdroplets, each containing approximately 100 picoliters of material (fluid/liquid). These pairs of approximately 100 picoliter droplets are accelerated against each other over a very short distance (mm to a few cm) so that they collide exactly in the center of a reactor chamber. The Coulomb forces that prevent nuclear fusion are largely weakened in this invention up to a very short distance between two atoms, because the two groups of atoms that collide are not equally charged, but neutral or even have different electrical charges. While one microdroplet contains one group of atoms, the other group that rushes to the collision point is negatively charged. Thus, electrical forces of attraction occur here instead of repulsion, which is not the case in conventional fusion reactors and the ions contained within them. The acceleration of the electrically charged microdroplets is also achieved by two ring electrodes (15 and 16), connected to each other by an insulator ring 14, which each attract the microdroplets from the nozzles (3, 4 - A and B) towards which they are directed. The microdroplets attracted by the ring electrodes are additionally accelerated by a nozzle electrode (17 and 18), which can be disk-shaped or funnel-shaped, for example, and the collision takes place at the center of the ring electrode opening 19. While the nozzle electrodes push the microdroplets, the ring electrodes attract them. The ring electrodes are positioned in the path with their openings 19 in the center so that the entire attractive force acts on a virtual line (fluid jet formation axis) 9 that connects the two nozzles. It is very important that the two micro-droplets are released from the nozzles simultaneously, so that they collide at the center of the circle formed by the ring electrodes. The micro-droplets are accelerated up to the center of the circle described by the ring electrodes, and then no longer (rather, they are decelerated upon exceeding the collision point). The micro-droplets must therefore collide as close as possible to or exactly at the center / collision point 11, because if they collide earlier on one side, one of the micro-droplets is decelerated by the electric field on the other side. The optimal location is for the micro-droplets to collide 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 largely neutralized. However, the insulator ring is very thin, making the region with a neutral field very short. Therefore, the microdroplets only have to travel very short distances (approx. 1 mm) without propulsion, primarily due to mass inertia and the attractive force between the two microdroplets. The electrical attraction between the two microdroplets constantly increases until the moment of collision because they are differently charged. The fusible atoms (deuterium or tritium atoms in the liquid state) that form the microdroplets do not all fuse with each other. Although the two colliding microdroplets are electrically attracted to each other, only about 3% of them actually fuse. Fusion occurs primarily in the central region of the microdroplet. These atomic groups have the best chance of fusing because they are surrounded by other atoms, and a scattering effect is unlikely due to fewer opportunities for escape. To promote the fusion process, laser beams or rapidly alternating electrical discharges directly in the rows of droplets can be used. By alternating an electrostatic lightning discharge in one row of droplets and then another discharge on the oncoming row of droplets, with a common ring electrode at the collision point attracting the micro-droplets alternately from the nozzle on the left and then from the nozzle on the right to the center/collision point, the micro-droplets can be further accelerated.

The discharge and attraction can occur alternately at a high pulse rate or simultaneously. With simultaneous attraction, the two microdroplets are attracted to the nozzles by the two centrally positioned ring electrodes with the insulator ring between them. The discharge also occurs simultaneously, so that a current circuit is closed through the ring electrode, the nozzle is positioned 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 that form the fluid accelerators 21, nozzles, the ring-shaped electrodes in the center, high-voltage sources 22, etc. Two fluid accelerators with piezo drive elements 7 are installed in the reactor chamber 23, each in a high-pressure chamber (24 and 25). Each of these creates a pulsed hydraulic pressure on the fluid and generates micro-droplets from the nozzles. Two micro-droplets are generated from the two nozzles and exit them simultaneously. The micro-droplets are shot against each other at high speed. The pressure from the piezo elements (45) is not sufficient to accelerate them strongly enough against each other. nigen. Using piezo technology, they can be accelerated directly to several hundred meters per second, but not so far that the collision energy is sufficient for fusion. Nevertheless, by translating the pressure force in the small high-pressure chamber, a 100-picoliter droplet can be accelerated very strongly. Pressure values of over 1.5 gigameters can be generated for a duration of 0.1 ns without the high-pressure chamber construction suffering! It is not the very stable high-pressure chamber construction that holds it together, but rather the inertia of the massive high-pressure chamber walls 26. To generate a deuterium jet with a speed of 50 km/s through a 0.01 mm nozzle opening, pressure values of approximately 13 MPa would be required, which can be achieved very briefly (0.1 ns) and with extremely small fluid quantities (picoliter range) using piezo elements. However, the material stress is relatively high and this can significantly shorten the service life of the elements.

The reactor here, although the nuclear fusion processes occur in pulses/digitally, delivers energy almost continuously and almost evenly as long as the micro-droplets are generated and fired at each other at a constant repetition rate. Depending on the desired output power, dozens to several million micro-droplets can collide per second. The droplet size doesn't necessarily have to be 100 pl; it can also be as small as 1 picoliter.

The reactor would generate a great deal of energy if the entire mass of the colliding microdroplets were to undergo fusion. However, because only about 3% of the mass of the colliding microdroplets results in nuclear fusion, the efficiency of this reactor is approximately 3%. This means that only 3% of the fuel mass is fused in each microdroplet collision. This shortcoming is relatively well compensated for by the high repetition rate of the colliding microdroplets. In addition, the fuel is not lost but is collected and made available again in the reactor in microdroplet form for collision. The microdroplets are released in volumes of approximately 100 picoliters. Each microdroplet, consisting of liquid deuterium, weighs approximately 16 ng. Accelerating this micromass to 50 km/s requires an energy of 0.02 J (similar to that required, for example, to accelerate from 160 g to 0.5 m/s). If two such droplets with a total volume of 200 picoliters collide and only 6 picoliters fuse, approximately one nanogram of deuterium mass (169 kg/m ³ in the liquid state) will undergo fusion, releasing an energy equivalent to the combustion of approximately 0.01 g of oil, which delivers approximately 420 J of energy (1 kg of oil delivers approximately 42 MJ). This means that, ideally, the reactor would operate with an energy balance of approximately 21,000 / 1. The energy invested in the reactor's work would in this case release 21,000 times more energy. Of course, a lot of energy is lost through conversion, and the accompanying components also consume electricity, but in the end there is always at least an energy surplus left in the positive balance, amounting to at least approximately 800:1. By using a widely adjustable repetition rate for microdroplet generation (from 1 to 50,000 pieces per second), the released energy can be very precisely controlled. Thus, the thermal energy of 0.01 ml to 500 ml of oil combustion per second can be released, which would ultimately mean approximately 1,800 liters of oil combustion per hour. The 1,800 liters of oil provide approximately 16 MWh of energy. By increasing the repetition rate of microdroplet generation, fusion power can be further increased, but this would be associated with high wear and tear on the fusion reactor structure and could lead to its rapid deterioration. The optimal solution would be an energy release that can also be easily dissipated so that the reactor integrity is maintained in the long term.

In addition, several reactor chambers can be installed, which can operate in parallel or one after the other.

The reactor harnesses the kinetic energy of the fluid droplets colliding with each other. Initial acceleration is achieved through hydraulic pressure generated by a fluid accelerator, such as piezoelectric elements (or magnetostrictive elements coupled with a micro-hydraulic converter). Then, during the transition to two fluid jet formations consisting of rows of micro-droplets, each emitted from the two nozzles, the droplets are additionally accelerated electrostatically or, in the case of dipole molecules, at least optimally rotated/oriented so that they collide with the hydrogen/deuterium atoms (in heavy water) facing forward.

In the high-pressure chambers, which can hold relatively small volumes (depending on reactor size and power, approximately 0.01 - 150 cm ³ ), the fusion-capable liquid is injected in a state that is as incompressible as possible (e.g., deuterium at very low temperatures). Depending on the technology used, one can build just one high-pressure chamber with two opposing nozzles, or two separate high-pressure chambers in which high pressure is generated simultaneously. An electrically expandable element is built into the high-pressure chamber, which is capable of electrically changing its dimensions or deforming itself. Numerous technical elements possess this property, such as piezoelectric elements or magnetostrics. tive elements. Magnetostrictive elements are slower, so they require a micro-hydraulic converter that converts the slow vibration energy into kinetic energy for fast fluid jets. This can be designed quite simply. It would be sufficient if the contact surface (pressure area) of a magnetostrictive element in the high-pressure chamber was approximately 2800 m times larger than the area of the circle that has the diameter of the droplet. The oscillating/piezo element is installed in a recessed location in the reactor chamber wall, where it expands in a pulsating manner. The element thus reduces the volume in the high-pressure chamber in a flash and pulsating manner, by approximately 220 picoliters in a single high-pressure chamber design ( 3 ) or 120 picoliters with two high-pressure chamber design ( 4 ). This causes the fusion fluid to be slightly displaced from the high-pressure chamber under electrical control.

Because the fluid in the high-pressure chamber is under high pressure, the space in front of the pressure surface of the piezo element quickly refills with fluid even during the pause times while the piezo element retracts. The high-pressure chamber walls 26 are very stable and solidly constructed (e.g., made of stainless steel/titanium alloy and several dozen centimeters thick). The high-pressure chamber, into which the fluid is injected from the storage tank 27, can be spherical or hollow-cylindrical. The very small amount of fluid (a few ml or even less than 1 ml) that fits inside is injected by an injector 28 through a very thin capillary line 29, filling the high-pressure chamber. The capillary line can be closed off by an electrovalve 62. The electrovalve can also be installed above the injector. When empty, a vacuum or strong low pressure prevails in the high-pressure chamber and the reactor chamber 23, so that the high-pressure chamber can be easily filled to capacity. The fusion-capable fluid inside should not be compressible. The nozzle is very fine and, in our example, is approximately 28.8µ in diameter at the outlet opening (diameter) 12 and can emit very small micro-droplets. However, it can also have other diameters, such as approximately 0.07mm - 0.14mm in nozzle diameter. Extremely high pressure is generated in the high-pressure chamber, which is very small (a few ^cm3 volume or even smaller). However, when the piezo element pulsates at a frequency of 10GHz, this pressure only lasts for an extremely short time (0.1ns), with two to four amplitude movements (2-5µm) being completed. This is followed by a pause of 0.01 to 4.5 milliseconds (depending on the reactor's output power requirements). Only after a few micro-droplets have been released and the short conduit chamber 30 (approx. 1-2 mm long) leading to the nozzles is slowly emptying does a refilling process take place by "pushing" the fluid in front of the pressure surface of the piezo element. Using the injectors, a small amount of liquid deuterium, for example, can be refilled every few seconds. The oscillation amplitude of the oscillating element 7 is arranged in such a way that it pushes the fluid with the pressure surface in the direction of the nozzle, thereby accelerating it. The amplitude of 2-5 µm is very small, but it is sufficient to displace two or four micro-droplets of 100 picoliters each from the high-pressure chamber and both nozzles. The pipe paths from the oscillating element to the two nozzles must be exactly the same length so that a micro-droplet emerges from each nozzle simultaneously. The thrust for the micro-droplets and their kinetic energy are determined by the size of the pressure area 31 of the piezo actuators, similar to the hydraulic pressure in a working cylinder. With a pressure area 1000 times larger than the circular area with a droplet diameter size, 1000 times more kinetic energy is generated on the 100-picoliter droplet. With larger fluid volumes (e.g., milliliter range), this would fail because the fluid mass would then offer considerable resistance to such accelerations, but with picoliter volumes, this is largely irrelevant.

It should be noted that the term "fluid jet formation" is merely intended to provide a better understanding of the processes and operating principle of this reactor. In reality, when viewed with a high-speed camera, no fluid jet formation of micro-droplets can be seen, but only isolated, isolated points (micro-droplets) emerging from the nozzles. Each micro-droplet travels 50 meters per microsecond (at 50 km/s). Thus, micro-droplets released "one after the other" from a nozzle do not "see" each other at all. Only when the repetition rate becomes relatively high would they be pushed close enough to form a fluid jet formation. If such an extreme high pressure, which lasts only 0.1 - 0.2 nanoseconds, is generated every 4.5 milliseconds, approximately 220 pulses are generated per second, and the same number of micro-droplets, each with a capacity of 2×100 picoliters, are released to collide with each other. However, a repetition rate of 220 microdroplets per second is not optimal for the nuclear fusion energy balance. The microdroplets should be released so frequently one after the other that the subsequent microdroplets are always within a few millimeters or even fractions of a millimeter (approx. 100 - 800 µm) of the first microdroplets reaching the collision point. The reason for this is the possibility of harnessing the kinetic energy of the particles of the colliding microdroplets, which is released by the Nuclear fusion processes are triggered. Immediately after nuclear fusion, atoms, ions, and particles (all of which are part of the micro-droplet) are accelerated from the micro-droplet at several hundred to thousands of km/s in all directions, including backwards. The closer the following micro-droplet is, the more such high-speed particles they hit. For every doubling of the distance to the collision point, the number of particle hits with the micro-droplet decreases quadratically. Therefore, it is important to calculate or determine the optimal value for each reactor that indicates how often and how quickly the micro-droplets must be generated to optimally maximize the nuclear fusion energy balance. This value depends on the distance between the nozzles, the size of the micro-droplets, and their speed.

The extremely high pressure (several to dozens of Mbars, even gigabars) could destroy the high-pressure chamber, but it doesn't, because this pressure returns to the decay phase after 0.2 nanoseconds. The oscillation amplitude of the pulsating element is so small that the inertia of the material structure of the construction's massive high-pressure chamber walls alone provides sufficient stability for this pressure. However, the pressure is sufficient to accelerate two 100-picoliter microdroplets (or smaller) to several dozen to 50 km/s (or even faster for smaller droplets). Oscillating elements with a larger oscillation amplitude (e.g., 50µm) and a 10GHz frequency could achieve speeds of up to 500km/s, although the microdroplet in this case would likely be only a few picoliters in size or even smaller. The 100 picoliters flows through one nozzle, while the other nozzle, directed in the opposite direction, delivers twice as much. To prevent the microdroplets from scattering due to their own electrical charge, they are chosen to be extremely small, and the distance to the collision point is designed to be equally short (a few millimeters or at most a few centimeters). The microdroplets do not have enough time to shatter, as is the case with an electrosprayer, for example, where the microdroplets literally explode due to the electrostatic field after they spray from the nozzle, because the molecules within fly away from each other due to the same electrical charge. The microdroplets, which are rapidly accelerated in this way, are no longer spherical, but rather disc-shaped with a small point in the center and a slight conical deformation tendency, forming a very small disc-shaped rim at the rear. The microdroplets, which are launched from both nozzles in a row towards each other, can move along the same axis until the collision point, or they can collide at a slightly angled line. In this case, they would not collide in a line (180°), but at an angle of, for example, 176-179°. This would have the advantage that the microdroplets, which are not slowed down by collision or do not collide with each other, would not hit the nozzle opposite. Instead, they could hit a mass of liquid deuterium 32 lying freely in the reactor chamber, or, due to the reactor chamber's rotation and centrifugal force, be evenly distributed radially against its hollow-sphere wall 33, where the kinetic energy of the microdroplets is either absorbed there or partially re-initiated nuclear fusion. Because the microdroplets shoot at each other in rows in a liquid jet pattern, the probability of them colliding is still very high, despite crossing at an angle of 179°.

• - 1pl enthält ca. 0,000 000 000 17g (0,17 Nanogramm) Deuterium im FlüssigZustand
• - Hier werden 200pl / Sekunde verbraucht und das ca. 220mal / s
• - Liquid Deuterium Dichte beträgt 169 kg / L
• - Das Verhältnis Gramm / Volumen wird mit 1:6 beim Liquid-Deuterium angegeben
• - 1g Deuterium-Fusions-Energie liefert äquivalent zu Verbrennung von ca. 11.000kg Kohle oder 9.000kg öl

The mathematical calculations and the energy yield are determined as follows:

• - 1pl contains approximately 0.000 000 000 17g (0.17 nanograms) of deuterium in liquid state
• - Here 200pl / second are consumed and this approx. 220 times / s
• - Liquid Deuterium density is 169 kg / L
• - The ratio gram / volume is given as 1:6 for liquid deuterium
• - 1g of deuterium fusion energy is equivalent to burning approximately 11,000kg of coal or 9,000kg of oil

If approximately 2200 × 2 micro-droplets (100 picoliters each) are sent into collision in a medium-sized reactor with a very short distance between its two jets, the resulting mass is 0.44 microliters per second, which corresponds to approximately 0.00007 g of liquid deuterium per second being released into each other in the two fluid jets. The equivalent of this for oil combustion is: 0.00007 × 9,000,000 = 0.63 kg/s (fusion material), which corresponds to approximately 2,270 kg of oil combustion energy per hour. This would be equivalent to 2,270 oil combustions per hour, releasing approximately 25 MWh of energy. This energy would be generated if all atoms in the micro-droplets were to fuse. However, because only about 3% of this results in fusion, the output is 0.75 MWh. The energy required for high-pressure generation, control, pumps, injectors, cooling systems, and energy conversion losses must be deducted from this, leaving approximately 0.5 MWh. This is the energy that such a mini-reactor would deliver. By increasing the micro-droplet repetition rate or installing two parallel-driven fusion chambers, the output can be increased as desired. 22,000 micro-droplets per second at each collision beam would produce ten times the energy. which would equate to approximately 5MW. Considering that 1MWh can supply approximately 4,000 households with electricity, 5MWh is sufficient for approximately 20,000 households (a small town). To simplify the calculation of the released energy, one can assume that whenever two micro-droplets with a total of 200 picoliters collide, fusing only 6 picoliters, approximately one nanogram of deuterium mass is fused, releasing an energy equivalent to the combustion of approximately 0.01 g of oil.

The microdroplets, each with a volume of 100 pl of liquid deuterium, form a microdroplet that resembles a sphere with a radius of approximately 0.0288 mm (28.8 µm) or a disk with the same diameter. This is the microdroplet size that is being accelerated here. The diameter of the nozzle should be this size, or slightly larger, if microdroplets of this size are to be produced. To achieve speeds of 50 km/s per second, the required pressure for the liquid jet (liquid deuterium jet) is approximately 2 Mbar continuously, or approximately 1.6 × 10 ⁹ bar (approximately 1.6 gigabar) in pulses. This is a very high pressure, and no material could withstand it. But here, as already described, something else is at play that can withstand the pressure: the inertia of the massive high-pressure chamber walls. Because the pressure is only generated for 0.1 ns and then immediately decreases, with the displacement being only 100 picoliters, no damage to the structure is to be expected.

To optimize the fusion processes, it is possible to charge the microdroplet so that it has a positively charged core and a negatively charged shell, both consisting of groups of atoms/molecules (or vice versa). Here, a microdroplet consisting of a small group of molecules would first have to be positively charged. Immediately after emerging from the nozzle, it would collide with another microdroplet containing a group of negatively charged molecules from another directly adjacent nozzle, which shoots in the same direction and steers towards each other at a very narrow angle. They then travel together until they meet the oncoming fluid jet from two other opposite nozzles. In this case, the outer shell of the microdroplet would be negatively charged and could be attracted and accelerated by a positively charged electrode. Such a microdroplet can be highly electrostatically charged, and it would not shatter, but travel as compact microdroplets (almost like neutral droplets). The same thing happens, only differently charged, with the microdroplets from the opposite nozzles, which also shoot at them simultaneously. At the collision point, groups of atoms with different charges collide. The "outer shell" 8 of one micro-droplet is positively charged, while the "outer shell" of the other micro-droplet, which is rushing toward the collision point, is negatively charged. Thus, the two micro-droplets attract each other.

It's worth mentioning that the reactor would also have to function with heavy water. Two liquid jets consisting of heavy water, each accelerated against each other at 300 km/s, would also lead to nuclear fusion of the deuterium atoms, even though they are in molecular bonding. A two-beam technique, with one consisting of heavy water ( ^D2O ) and the other of superheavy water ( ^T2O ), should also work well. The repetition rate of the electrical pulses for the piezo element is not very high (in our example, approximately 2200 Hz), but the deformation of the element occurs very quickly (10 GHz). One or more oscillations with an amplitude of 2-5 micrometers should occur within 0.1 ns. The surface area (pressure area) 31 of element 7 on the expansion side 34, which is approximately 200 times larger than the circular projection of the nozzle diameter, or the circular area with the same diameter as the micro-droplet, will cause a very rapid displacement of the fluid per pulse, aiming for approximately 250 picoliters of discharge from the nozzles. Approximately 50 picoliters of expansion are lost to the microscopic elasticity despite the massive high-pressure chamber walls and their inertia, even though they appear macroscopically rigid and are constructed of solid stainless steel, while the remaining approximately 200 picoliters of expansion volume and displacement are transferred to the fluid. The high-pressure chamber should be constructed from a single piece and not from several walls welded together. The rigidity of the chamber construction is very important for achieving high jet velocities. Through the 200 picoliter displacement within 0.1 ns, an acceleration of the two 100 picoliter microdroplets to a speed of 50 km/s is achieved. Because their nozzles (also made of solid and hard material) are directed towards each other, the two microdroplets collide at this speed. Because the two microdroplets are additionally and differently electrified at the nozzle outlet 12, they are accordingly accelerated further towards each other by the two ring electrodes (15, 16) until they collide at the collision point 11. Although it is a challenge to bring the two microdroplets towards each other exactly and at the same time at the collision point, because they are much larger than, for example, individual ions, an optimal alignment is still possible. technically feasible. In addition, the microdroplets themselves carry out the final nano-course corrections due to their different electrical charges and increasingly strong electrostatic attraction to one another.

The greatest danger of electrically charging micro-droplets is their shattering/exploding immediately after they leave the nozzles. The electrostatic fields can work against structural stability and separate the atomic groups within until the micro-droplet shatters. This effect occurs, for example, in electrospray generators. While the shattering of the micro-droplets is supposed to be caused by electrostatic charging there, in our case this effect is undesirable and must be avoided. The parabolic mirror-shaped electrodes on each nozzle generate the electrostatic fields in such a way that the micro-droplets do not shatter while they are in motion. However, with our short fluid jet path, this effect hardly occurs at all. The path to the collision point is very short and can be a few mm or even cm, although this time is no longer sufficient to shatter the micro-droplets electrostatically. The electrostatic fields are concentrated along the flight path of the micro-droplets and give them additional thrust. The external electric field also largely suppresses the Coulomb forces in the micro-droplets, preventing them from shattering even over longer distances. Immediately before they reach the collision point (a few micrometers away from collision), the electrostatic fields at the parabolic electrodes are switched off extremely quickly so that they become neutral. Due to the lack of the external factor, or electrostatic field, an important stabilizing component for the micro-droplet is suddenly missing. The micro-droplet begins to destabilize, but continues to fly at dozens of km/s towards the other micro-droplet, which also experiences the same thing. The two micro-droplets reach the collision point and, because they have different charges, they attract each other more and more. When they reach a very short distance, their electrostatic charges are sufficient to cause them to shatter, but the time is no longer sufficient. Although it can happen that, in the case of a strong electrostatic charge, they shatter immediately before the physical collision with each other, the resulting atom groups still collide in a considerable number with the groups from the oncoming micro-droplets.

The electrical charge contained within the microdroplets and an additional discharge between the nozzles and the one on the facing ring-electrode surfaces cause the microdroplets to accelerate. The collision also triggers a corona discharge in both microdroplets, as well as the nuclear fusion of a considerable number of atoms, which are then simultaneously and explosively broken down into atomic particles and ionized particles. The two exploding microdroplets release atomic groups or ions, which then collide with the approaching microdroplets at high speed, partially leading to further nuclear fusion. Although not all atomic groups or ions collide (only about 10-20%), this is enough to release usable fusion energy. Thus, once fusion is ignited in the reactor, further nuclear fusion reactions easily occur from the subsequently arriving micro-droplets, which then do not necessarily have to reach the exact collision point in order to fuse.

On the 5 Another embodiment is shown. The microdroplets 2 are emitted in the form of dots or dashed lines, each forming a very thin fluid jet (5, 6), the jet length of which is only a few centimeters or even millimeters. However, with a high repetition rate setting, the microdroplets are emitted in rows, one after the other, in very large numbers for collision. From 1 to approximately 2.2 million microdroplets (or more, depending on the reactor control settings and energy requirements) can be emitted per nozzle per second. The resulting jet is very thin and can have a diameter of approximately 0.000113 mm. The nozzle also has this diameter. The circular area of a circle with this diameter is 0.01 µm ² . To achieve the acceleration of the micro-droplets, a section of the chamber (acceleration zone) immediately in front of the nozzle area has a diameter of approximately 0.0016 mm, resulting in a cross-sectional area approximately 200 times larger (2 µm ² ) than the cross-sectional area of the fluid jet (consisting of rows of micro-droplets). A tip of the electrically deformable element is inserted there, and its expansion amplitude of just 25 nm causes fluid displacement, allowing two 100-picoliter micro-droplets to emerge from the nozzles at speeds of up to 50 km/s. Since the wall of the deformable element, moving at 10 GHz and with an amplitude of 2 - 5 µm, generates an extremely high pressure for only 0.1 ns, the structural integrity of the chamber easily holds up, supported in part by the inertia of the construction/solid walls. The vibrating element is not immediately damaged because the expansion occurs at the atomic level and evenly. In addition, an electrostatic Acceleration through the nozzle electrodes 17 and both ring electrodes (15, 16) in the middle.

Depending on the reactor's application, smaller or even larger power outputs can be generated. Smaller reactors, generating several megawatts of energy, can serve as propulsion energy sources for ships or container ships. Even smaller micro-fusion reactors (up to 100 kWh) would be well suited for both stationary and mobile applications, such as powering vehicles.

The variant from the 6 additionally features an electron beam generator 35 (electron source) that directs an electron beam 36 directly onto the collision point 11. The electrical charging of the microdroplets causes them to be cold ionized, but at the collision point, the electron beam 36 electrically neutralizes at least one of the fluid microdroplet rows, so that they do not avoid each other but collide. If there is an excess of electrons in one of the two fluid rows, the two colliding microdroplets will electrically attract each other, thus promoting nuclear fusion.

On the 7 Another version of this reactor is shown. Here, in addition to hydrogen isotopes (D or T), the element boron 37 is used for fusion. In this case, two storage tanks (38 and 39) are installed, each with a volume of approximately 100 - 500 cm ^3. Hydrogen isotope (e.g. deuterium) 32 is added in liquid form in one, while the other is filled with water in which boron 37 is dissolved. Boron can also be added directly to the water in nanopowder form and mixed with water or heavy water in the storage tank by a mixer 40 inside the storage tank. Tiny amounts (e.g. 0.1 cm ³ each) from each of the two tanks are added to one of the high-pressure chambers. Once there, micro-droplets of both fusion-capable materials are generated and released against each other at high speed towards a collision point in the center of the reactor chamber. Here, too, depending on the repetition rate, short rows of single droplets or long rows of micro-droplets are generated, colliding at approximately 50 km/s. The energy can be captured directly from the ions generated by fusion at the collision point by voltage collectors (current collectors) 65 of grid electrodes and charged in an electrical capacitor ( 16 This electricity could be fed to end users via electrical control and distribution systems. The design would be significantly simpler here, as no steam turbines or other thermal energy converters would be required. The element boron can be "dissolved" in the heavy water or accelerated in the form of nanospheres together with the heavy water mass and collided against the pure deuterium jet at the collision point. Boron can also be placed directly in the liquid deuterium in one of the high-pressure chambers, and one deuterium fluid jet can collide with the other. It is also possible that both jets that collide with each other are enriched with boron atoms. In this case, boron atoms would collide with each other, but boron would also collide with deuterium atoms, which could lead to fusion.

Similar acceleration techniques for microdroplets can also be observed in inkjet printers. These also produce microdroplets in the picoliter range (between 3 and 40 picoliters). However, in these printers, the microdroplets only reach speeds of approximately 5–100 m/s, because more is not necessary. Furthermore, the oscillation frequencies of the piezo elements are designed to be significantly lower (in the kHz range). The invention incorporates 10 GHz piezo elements that oscillate at 2–5 µm amplitudes, allowing the microdroplets to be accelerated to speeds of up to 20–50 km/s.

The picoliter microdroplets, which are further accelerated electrically, can be deflected by an electrostatic cumulative lens (ring electrode) or electromagnetic coil for a more precise impact point. Because the microdroplets from the two nozzles are each differently charged, they attract each other immediately before collision, thus independently performing auto-course corrections in the nanoscale ( 5 ). One micro-droplet with a positive charge collides with the other, negatively charged micro-droplet. The micro-droplets are not fully ionized, but electrostatically charged and roughly comparable to particles in thunderclouds.

For additional acceleration, laser acceleration methods can also be used, as they can accelerate the microdroplets to very high speeds, but they are somewhat less efficient in terms of energy consumption. This requires two laser sources (41 and 42) that emit short but very intense pulses of focused laser beams ( 8 ). These laser sources illuminate the micro-droplets from behind immediately after they leave the nozzles and push them to the collision point contactlessly using photon energy. The laser beam sources can emit in very short, extremely strong pulses, and their laser beams 43 can also be directed directly into the nozzles. Because the two laser beams also collide and are emitted on the same optical axis, They finally hit the oncoming micro-droplet. However, the laser beam diameter is so small that the beam is completely shadowed/obscured by the droplet, and when the laser beam is "illuminated" through the droplet, the beam then diverges significantly. The two laser sources can also be switched on and off alternately (e.g., with a 100 GHz repetition rate). This way, each droplet alternately experiences a multitude of micro-thrust pulses until it reaches the collision point.

In contrast to a continuous fluid jet, the microdroplet jet formation (microdroplet chain) offers numerous advantages. It can be accelerated significantly higher, and the fusion reactions can proceed more continuously because the pressure on the microdroplets can be more easily generated using piezoelectric elements (7, 45). Furthermore, the high-pressure chamber is very efficiently refilled by injecting small amounts of fluid during the pause times between two microdroplet releases, ensuring the pressure pulse remains constant.

On the 9 An embodiment is shown in which the piezo elements 7 are each installed in the high-pressure chambers. The high-pressure chamber is hollow-cylindrical in a block 121 made of solid construction. One rear end is closed, while the front end is provided with a nozzle. The nozzle is also very solidly constructed and has a diameter of only 0.03 mm. The high-pressure chamber can be dimensioned approximately the same size. A 20 mm long hollow-cylindrical high-pressure chamber with a diameter of 0.03 mm, in which a piezo element rod in the shape of a cylinder with a diameter of 0.02999 mm is inserted, can generate 100 picoliter drops. However, the high-pressure chamber can also be larger. 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., between 2 and 50 mm) is shown, in which a piezo element is installed, immersed in the fluid. The piezo element is installed in the high-pressure chamber wall 26 in a guide channel 44 or in a recess therein. The pressure surface 31 at the free end of the element serves to push the fluid as it electrically expands.

On the 11 A further embodiment is shown. Here, the piezo element is constructed in the form of a disc 45. The piezo element 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 cylinder shape, which is provided with the nozzle at one end and is closed at the other end. The disc-shaped piezo element is installed on the high-pressure chamber inner wall 26 opposite the nozzle in a disc-shaped recess 46, with the oscillation axis of the piezo element pointing towards the nozzle. Here, the movement axes (108, 109) of the two fluid formations or the micro-droplets from both nozzles are no longer in line, but meet at a wide angle 107 (approx. 176° - 179°). Although this requires precise timing when firing the micro-droplets, if there is a technical "delay" in the activation of the opposing nozzles and the fluid generator, the micro-droplets do not hit technically sensitive reactor parts, but rather a blanket or the stagnant fluid that protects the reactor walls, thus enabling a more durable construction.

The variant from the 12 It also features an electrical accelerator that accelerates the two micro-droplet jets against each other through electrical discharge. Ideally, an extremely small point electrode would be placed exactly at the collision point of the two micro-droplet jets. This electrode would be negatively charged, while the two micro-droplet jets are positively charged. This electrode would attract the two jets, but it would itself be a major problem because it would be in the way and would also quickly evaporate due to the heat of the fusion processes. A virtual electrode 47, consisting of an ion beam 48, can provide assistance in this case. A voltage discharge from a high-voltage source 49 is induced via the ion beam, which runs through the collision point transversely, perpendicularly to axis 9 connecting the two micro-droplet jets. Applying a voltage to this virtual electrode and the two nozzles creates an electrical force of attraction on the micro-droplets of the two micro-droplet jets. To optimize the fusion process, the charges of the electrode and the nozzles can be selected so that the two colliding microdroplets have different charges, causing them to electrically attract each other upon collision. A control system allows the discharge voltage to be generated very quickly and alternately for each microdroplet jet, so that a discharge never occurs across both jets simultaneously.

Alternatively, two equally charged microdroplets that are supposed to collide with each other can be accelerated, but are neutralized by an electron beam immediately before or exactly at the collision point ( 12 ).

On the 13 A further embodiment is shown, in which the microdroplets are only a fraction of a picoliter, or at most a few picoliters in size. However, the repetition rate of microdroplet generation is approximately 100 times higher. Due to the very low mass of the microdroplets, laser acceleration methods can also be applied here. Two laser sources (41, 42) will hit the microdroplets 2 and push them against each other to the collision point 11.

On the 14 and 15 Examples of implementations with intersecting fluid jet formations are shown. Here, the intersection angle of the two fluid jet formations is approximately 178°. The micro-droplet that does not hit the other one flies further to a fluid mass 50 made of fusion-capable material standing in the reactor chamber 23, where it can release its kinetic energy, although this rarely leads to nuclear fusion. The fusion chamber can be completely rotated by an electric motor 64, allowing the stationary fluid mass to be better distributed across the reactor chamber wall. For acceleration, additional electric fields can be created here by intersecting ring electrodes or closing circuits between a virtual electrode at the collision point and the nozzle electrodes, which alternately attract the intersecting fluid jet formations. The two circuits (each between the nozzle and the virtual electrode) are always closed and opened in rapid alternation. Here, each microdroplet is positioned opposite the ring electrode arranged at the nozzle, electrically connected by electrical lines (53 and 54). The high-voltage sources (55 and 56) and their control system 57 alternately generate an electrical discharge, accelerating the microdroplet from the nozzle to the ring electrode at the collision point 11. As they pass through the collision point, one microdroplet collides with the other at very high speed, partially leading to fusion.

On the 15 This device is equipped with two ring electrodes (51, 52), each receiving high voltage from two separate voltage sources (55, 56), each located on the other side of the collision point, with the center points (58, 59) of which the central openings (60, 61) are installed in the path of the respective fluid jet formation of the opposite nozzle. On the journey to the collision point, when the micro-droplet formations intersect, not all micro-droplets in one formation collide with the micro-droplets of the other formation opposite; instead, many of the micro-droplets miss each other and continue flying. As a result, the microdroplets arranged in the fluid jet formations that pass the collision point without colliding will pass through the respective central opening of the ring electrodes for each fluid jet formation, with each ring electrode being electrically coupled to the opposite nozzle (3, 4) or nozzle electrode (17, 18). A control system will rapidly alternate voltage discharges between the ring electrode and the opposite nozzle or nozzle electrode through the affected fluid jet formation. The current direction through the fluid jet formations is such that it accelerates the microdroplets within each fluid jet formation toward the collision point.

In addition, a small amount of liquid deuterium or other fusible material can be placed in the reactor chamber to collect the micro-droplets that pass the collision point without collision, in order to protect the reactor chamber wall 62 from premature erosion.

It should be mentioned that when using very small micro-droplets (approx. 0.7 picoliters or smaller), heavy water or even simple water 67 is also suitable as fuel for the fusion processes ( 17 ). The extremely small water micro-droplets are accelerated extremely strongly to almost 1000 km/s and then brought into collision with each other. If an electric terahertz field (oscillation frequency of at least 1.1 THz) is applied to the micro-droplets through two pairs of electrodes (73, 77), free electrons will form in the water droplets, which can be influenced electrostatically. It may be helpful to install additional alignment electrodes 66 on both sides between the collision point and the nozzles, which build up and dissipate electrostatic fields extremely quickly, causing the water molecules 68 in the fluid jet formation to orient themselves so that during the collision, the hydrogen atoms are oriented forward in the direction of flight ( 18 ). Because the water molecule is a dipole, it will orient itself in the electrostatic field. Electrical acceleration of the micro-droplets can also be considered, but is not absolutely necessary. The alignment electrodes 66 here only cause the water molecule to align itself in the electric field in such a way that it "stretches its feet forward," or rather, arranges the two hydrogen atoms in the water molecule forward ( 18 ). Using the hydrogen atoms 69 as a crumple zone for the water molecules brings several advantages. The hydrogen atoms of two water molecules actually collide more frequently with each other and not with the oxygen atoms (70), which in this case are positioned at the rear in the direction of flight. The alignment electrodes 66 are relatively small and cause a water molecule dippole alignment throughout the fluid. jet formation (on both sides of the collision point) or at least for the last few millimeters before the collision, for each micro-droplet separately on both sides of the collision point. Due to the positioning and dimensions of the alignment electrodes, the electrostatic fields are truly strongest almost exactly where they are needed. However, the fields are no longer active directly at the collision point or rather neutralize each other. This is also necessary because otherwise the colliding molecules would be oriented the same, and that would not be advantageous because the hydrogen atoms of one molecule would be facing the oxygen atom of the other molecule. However, because the alignment already occurs separately on both sides in the fluid jet formations before the collision point, the molecules are optimally rotated for nuclear fusion. The oxygen atoms at the "tail" of the molecules push the hydrogen atoms against each other more strongly due to inertia, which promotes nuclear fusion processes.

The orientation of the dipole molecules depends on the external influence of the fields, or rather the electromagnetic field strength, and in the case of microwave radiation, this occurs instantaneously. The maximum frequency at which the dipoles can rotate is approximately 22 GHz. Up to this microwave frequency, the molecules can be rotated, causing the total mass of the fluid to expand and contract. Although the expansion is extremely slight, sufficient longitudinal expansion is caused along the longitudinal axis of the capillary high-pressure chamber, which is a few millimeters or even a few centimeters long, generating extremely high pressure, which can accelerate a microdroplet/picodroplet from 50 km/s to well over 100 km/s. The longer the capillary high-pressure chamber, the greater the longitudinal expansion. This can amount to approximately 0.1–0.05% of the total length of the fluid column in the capillary high-pressure chamber. At a length of 50 mm, this corresponds to an expansion of 0.05 mm. The contraction also amounts to approximately 0.05 mm, so that from minimum to maximum, the molecules at the open end of the fluid column are in motion by approximately 0.1 mm (0.05 mm + 0.05 mm), which occurs at approximately 22 GHz. A 0.1 mm fluctuating expansion of the fluid column corresponds to an acceleration of at least 100 km/s for the nanodroplet/picodroplet at the open end. Because the length of the fluid column oscillates at 22 GHz into the capillary high-pressure chamber, the "fluid mass integrity" would no longer be guaranteed. However, the oscillations are not continuous, but pulsed and as short as possible (approximately 45 picoseconds).

The 19 and 20 show an orientation of the water molecules 68, which is simply achieved by highly focused microwave radiation from a microwave source. The microwave beams 75 are split into two beams, phase-shifted, and strike the water molecules perpendicular to their axis of motion. The oscillation amplitudes and oscillation phases of the two microwave beams, through the precise adjustment of the distance of the microwave emitter, are selected such that the water molecules on both sides of the collision point, as seen from the collision point, fly toward each other with their hydrogen atoms. For such a special alignment, it is even better to align a separate microwave source (73 and 74) for each fluid jet formation directly in front of the collision point. These two microwave beams are parallel to each other and inversely phased, causing the water molecules of both colliding microdroplets to rotate simultaneously and, at the precise moment of collision, to align them so that the two hydrogen atoms of one molecule collide with the two hydrogen atoms of the other oncoming molecule. The microwaves hit the microdroplets from a precisely calculated distance and with a specific oscillation phase. Because the microwaves can rotate the water molecules not just partially but completely, this effect is used to rotate and align the water molecules immediately before the collision between two microdroplets so that they reach the exact rotational position upon impact, moving with the hydrogen atoms facing forward. Because the atoms in the microdroplets are neutral, no significant repulsive forces are expected between the two microdroplets at the collision point. The water molecules are set in rotation, but by precisely calculating their rotational position, the microwave radiation can be generated in such a way that at the moment of impact, the molecules are actually aligned so that their hydrogen atoms are at the front in the direction of flight, thus colliding both molecules with their hydrogen atoms. The molecules will pass the last few micrometers without the influence of the microwaves because two microwave beams, one for each fluid jet formation, do not touch each other and form a "gap" between them. It is important that the hydrogen atoms of both groups of molecules from both colliding micro-droplets are aligned with the hydrogen atoms at the collision point. Although the alignment fields of alignment electrodes are missing immediately before the collision point, the respective alignments of the molecules still remain for this short distance on both sides of the collision point. There would no longer be enough time to Hydrogen molecules tend to adopt a different orientation on their own. 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 left to chance, but are specifically controlled and optimized. This has a direct impact on the energy release intensity of the fusion reactor. The energy intensity always increases with the increasing degree of alignment of the molecules with the hydrogen atoms against each other. In this way, the reactor power can also be controlled. It should be noted that the use of water as fusion fuel, cooled to exactly 4°C, is best suited for fusion purposes, provided that the micro-droplets are accelerated to 500 km/s or higher (up to 1000 km/s). Micro-amounts (a few microliters) of water in a robustly constructed high-pressure chamber, which is designed like a very narrow and long capillary tube, can be used to trigger a micro-expansion of the water, which is cooled to 4°C, using a number of methods to generate the two micro-droplets. An electric field, microwave radiation, or a laser source is sufficient to slightly reduce the density of the water and thus increase its volume, and this with an extremely high velocity factor. The expansion is greatest along the long axis of the high-pressure chamber. Even the smallest change in density leads to a liquid flow through the very narrow high-pressure chamber along the long axis of the high-pressure chamber to an outlet opening through which the micro-droplet is then accelerated. Each reactor, depending on its power, dimensions, and nozzle arrangement, can require different parameters. Optimization of the technical parameters, the nuclear fusion processes, and the energy balance can be determined through precise reactor-specific calculations and additional empirical values. This is necessary because only then can the reactor be operated economically optimally. With optimal settings of all parameters, the overall energy balance is likely to be well over 800:1 (a mini-fusion reactor can be operated economically viably at 8:1, and a large fusion reactor at 1.7:1).

The water molecule possesses an electric dipole moment due to the different electron densities of the oxygen and hydrogen atoms. In liquid water, these molecular dipoles generate an electric field whose strength fluctuates on a femtosecond timescale (1 fs = ^10-15 seconds), briefly reaching peak values of up to 300 MV/cm. In such electric fields, an electron will leave its bound state in the water molecule ( _H2O ) and tunnel through an energy barrier into the surrounding liquid (a quantum mechanical ionization process). However, the electron returns to its original state extremely quickly because the fluctuating field has no preferred direction, and the electron therefore cannot move away from the site of ionization. Due to highly efficient charge recombination, the number of free electrons remains very small (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 pairs of electrodes (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 move over distances of many nanometers before localizing at another location in the fluid. This effect can be used for our purposes by generating two electric fields in the THz range on each fluid jet formation, immediately after the microdroplets leave the nozzles. The electrons in the microdroplets would be partially unbound, and electrical acceleration of the microdroplets would be significantly more efficient (1000 times higher). This would mean that the microdroplets could be electrically accelerated from an exit velocity of only 1 km/s from the nozzle to 1000 km/s on their way to the collision point. At this impact velocity, conventional water droplets are very capable of fusion, and at the collision point, an enormous amount of energy would be released per microdroplet collision. 17 ).

On the 21 An embodiment is shown in which the high-pressure chambers each have such a small internal volume that they can only hold one micro-droplet each. The fluid intake occurs during the pause times between two micro-droplet releases through injectors 28 and their micro-capillary lines 29. Because the micro-capillary channels or lines 29 are much narrower than the nozzle opening, the extremely high pressure, which only lasts approximately 0.1 ns, does not place significant strain on the structure and is unlikely to cause fluid to flow back into the injectors. Special electrovalves 62 can also prevent this. The important factor here remains the mass inertia of the installed components. The micro-quantities/micro-droplets of fluid are accelerated against each other at very high speeds (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 collision point and arrange the molecules in such a way that they fly in the collision direction with the hydrogen atoms (69) facing forward ( 22 ).

The fusion reactors described here are lighter, more compact, and are said to have relatively high efficiency and a positive, commercially viable energy balance. By using microdroplets instead of fluid jets, several advantages are achieved in optimizing the fusion processes. In contrast to reactors that operate with colliding fluid jets, there are significant differences. The microdroplets are extruded using a completely different technique, and because they are accelerated individually, the microdroplet reactor designs can achieve significantly higher collision velocities and improved output energy control. Furthermore, significantly lower loads are generated on the high-pressure chambers than with the fluid jet variants, which results in a longer service life of the materials used. The extremely small high-pressure chambers, some designs with a volume of only 1-100 picoliters, have very thick, stable walls (a few centimeters or dozens of centimeters thick), and can withstand very high pressures (millions or even billions of bars) because the pressure lasts only approximately 0.1 ns. It is not the material thickness, but rather the inertia of the walls that guarantees the stability of the structure. The pressure waves that are directed into the chamber walls within 0.1 ns are completely absorbed by the inertia, so no damage to the structure is to be expected.

Above all, the very low displacement of 1-100 picoliters is crucial to ensuring the structure remains stable. The use of hard materials is also necessary here to prevent microcracks from forming. Nevertheless, fluid jet fusion reactors have an advantage over the micro-droplet variant. In fluid jet reactors with continuous fluid jets, or fluid jet pulses, molecules/atoms that are constantly pushing behind them rush to the collision point, exerting an enormously high contact force on the front ones that have already reached the collision point (similar to a train crashing into a rock face, with the rear cars continuing to push the locomotive with ever-increasing force due to inertia), thus creating a good energy balance through nuclear fusion. Micro-droplet fusion technology lacks this approach, but this is offset by the largely higher kinetic energy. A high repetition rate, with only 0.5 to 18 diameter lengths between the individual drops, would also increase the “contact force” (pressure) at the collision point.

On the 23 and 24 Interesting practical examples have also been presented. Here, deuterium oxide 67 is used for fusion. The molecule of heavy water (deuterium oxide, D ² O) 68 is, like a water molecule, a dipole. A dipole occurs when the charge distribution in a molecule is not symmetrical, resulting in a partial positive and a partial negative charge. In the case of heavy water, the two hydrogen atoms have a partial positive charge, while the deuterium atom (a heavy hydrogen isotope) has a partial negative charge. This leads to a dipole moment in the molecule. This property is used to accelerate the micro-droplets. The fluid accelerator, or microdroplet acceleration system, consists of a coherent microwave source 78 (e.g., a MASER or GUNN element/GUNN diode) that emits coherent microwave radiation 79 into the fluid directly in the high-pressure chambers, fluid lines, or nozzles, causing the fluid molecules to rotate synchronously. Because deuterium oxide molecules, like water, possess dipole properties, their motion behavior can be influenced or caused to rotate by microwave radiation. If all molecules are synchronously rotated by the coherent microwave radiation, then during each rotation, there are two rotational positions where the molecular arrangement causes a stronger expansion along one axis, and also two positions where the fluid contracts most strongly along exactly the same axis. The speed at which ^D2O molecules rotate when exposed to microwave radiation depends on various factors, such as the frequency of the microwaves and the temperature of the heavy water. The rotation of a ^D2O molecule can occur at a characteristic speed of several billion revolutions per second. This speed is called the rotation frequency. At room temperature (approximately 25 degrees Celsius), the average rotation frequency of a water molecule is about 10 billion to 100 billion revolutions per second. At higher temperatures, the rotation frequency increases because the kinetic energy of the molecules increases. It is important to note that the exact rotation speed is influenced by various factors and can vary slightly from molecule to molecule. Electrostatic expansion of water due to Electric fields are a phenomenon that does not occur at normal household quantities and temperatures, but certainly at the micrometer or even nanoscale. Electrostatic expansion occurs when an electric field acts on a liquid or gas, causing the charges within the liquid or gas to reorient or even shift. This can lead to expansion or contraction of the material. Electrostatic expansion can be observed in heavy water when it is placed in a strong electric field. Microwaves generate such rapidly changing fields. The electric field causes the heavy water molecules to alternately pull towards and push apart from one another, thus causing electrostatic expansion and contraction of the heavy water. The heavy water itself acts like an actuator and also generates the driving force for the acceleration of its own substance, or micro-droplets. Because heavy water molecules are dipoles and have both a positive and a negative charge, they will align in an electric field, which can cause the heavy water to expand in one direction. This effect is known as dielectric polarization or orientation polarization. When exposed to an external electric field, these dipoles become increasingly aligned the stronger the field becomes. As the frequency of the electric field increases, this polarization is the first to disappear, but the frequency must be relatively high. Orientation polarization, which occurs due to the alignment (orientation) of permanent electric dipoles, such as water, in an electric field, allows the heavy water to expand and contract. Their thermal motion counteracts this alignment of the dipoles. Orientation polarization therefore depends on temperature (the higher the temperature, the lower the orientation polarization), which is described by the Debye equation; therefore, the fluid temperature should be kept low. If the direction of the electric field is reversed, the dipole molecules must reorient or realign themselves (relaxation process). Due to their relatively high inertia, they require a certain amount of time for this (the typical rotation time of a molecule in a liquid is 10 to 100 GHz). Heavy water has a microwave absorption maximum at around 18 GHz (for water, it is approximately 22 GHz). At even higher frequencies, orientation polarization is no longer observed, but only displacement polarization, and the Debye equation transforms into the Clausius-Mossotti equation. Electric polarization is a physical quantity from electrodynamics that characterizes the strength of the electric dipole moment in a dielectric material. Even in non-conducting materials, the application of an external electric field causes a displacement of electric charges over short distances on the order of an atomic distance. Dipole molecules can be permanently oriented using direct current. At very low frequencies (below 1000 Hz), ions can occasionally swap places and remain there even after the external field is switched off (dielectric absorption). With increasing frequency, at around 10 ¹⁰ Hz, dipole molecules are excited to periodically flip over - unless they are held in place by a crystal lattice. This results in enormous frictional losses between neighboring water molecules when exposed to microwave radiation. At 10 ¹² Hz, the ions oscillate around their rest positions within the molecule. Because the deflections are limited to fractions of an atomic diameter, the maximum possible polarization is quite small. In heavy water molecules, the centers of gravity of the positive and negative electrical charges are clearly separated. Therefore, in these dipole molecules, their directions can be very effectively influenced by orientation polarization. The polarization vector direction and the extension are strongest in longer water molecule chains, along the length of the chain. In our reactor, this will occur in the capillary line leading to the nozzle. In this case, a larger chamber (high-pressure chamber) is omitted. Thus, the capillary line also serves as a high-pressure capillary chamber 80. Due to the orientation of the heavy water molecules, 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 expansion, a micro-droplet of approximately 1-100 picoliters is ejected through the nozzle. Simultaneously, the same thing happens on the other side with the other nozzle. The two micro-droplets 2 meet at a collision point 11 approximately halfway between the two nozzles in the reactor chamber, resulting in the disruption of the molecular bond and partial fusion between the deuterium atoms. Through this fluid accelerator, which emits coherent microwave radiation in the fluid from the capillary high-pressure chamber 80 and a microwave source 78, directly into the capillary high-pressure chamber 80 and causes the heavy water fluid molecules to rotate synchronously, thereby exciting the fluid to rotate and contract, thereby generating a rotating micro-expansion vector, a sufficiently large expansion in the fluid jet axis 9. Because the capillary high-pressure chamber is a few millimeters long, the expansion will be most pronounced in the longitudinal direction and in the jet direction, generating a fast-moving micro-droplet from the nozzles each time. The longer the capillary The narrower the chamber, which functions like 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, which are up to several dozen centimeters thick in larger reactors. The liquid inside can only be released in micro-droplet form through the open end 84, while the rear end 83 of the capillary high-pressure chamber is closed. The microwaves do not have to penetrate perpendicular to the capillary high-pressure chamber's long axis. They can also penetrate in the long axis direction. The coherent microwave radiation can enter the capillary high-pressure chambers via the open ends/outlets at an oblique angle or be transferred directly to the fluid through a stable ceramic wall 81 inside ( 23 ). No nozzles are installed here either, because the micro-droplets flow directly from the capillary high-pressure chamber.

The fusion fuel can be refilled directly into the capillary (high-pressure capillary chamber). It can be injected directly into the capillary chamber by an injector through the nozzle opening during the pauses between two pulses, each of which generates a micro-droplet.

On the 24 The rotations of the deuterium oxide molecules and their orientational polarization were shown. The microwave energy causes these molecules to rotate synchronously at frequencies of up to 18 GHz, resulting in electric fields that are sometimes attractive and sometimes more intensely repulsive, slightly altering the distance between the molecules. The microwaves cause almost all of the molecules in the capillary high-pressure chambers to rotate synchronously. This creates an expansion force that rotates in all directions. However, due to the coherence and polarization of the microwaves, the rotation of the molecules is designed so that it occurs on a line perpendicular to the line connecting the two capillary high-pressure chambers. Although this causes expansion only in one plane, the expansion vector force always rotates, e.g., clockwise. The rotation axis 85 of the molecules is thus perpendicular to the longitudinal axis 82 of the capillary high-pressure chamber 80. Because all molecules rotate synchronously, they will all simultaneously approach each other at times, and repel each other at times. The capillary high-pressure chambers are very narrow inside (diameter in the micrometer range). Although their length is also very short, it is still a few millimeters (or less). However, the ratio between the diameter and length of the capillary high-pressure chamber is approximately 1:5000 or more. Thus, an extension arranged perpendicular to the longitudinal axis 82 of the capillary high-pressure chamber is almost insignificant compared to the extension in the longitudinal axis direction, which is 5000 to 120,000 times larger. In large fusion reactors, however, the inner diameter of the capillary high-pressure chamber can also be larger (e.g., 0.1–1 mm or more). In large reactors, the capillary high-pressure chamber can also be constructed circularly or spirally to increase the length of the chamber. Due to the chain arrangement of the molecules in the capillary high-pressure chamber, the distance between the molecules increases when the vector expansion force rotates and reaches a position that coincides with the long axis of the capillary high-pressure chamber. This is where expansion is strongest and this creates the enormously high pressure that accelerates the microdroplets against each other. Due to the longitudinal arrangement of the fluid mass and volume in the capillary high-pressure chamber, the pressure force on the microdroplets is generated in a self-regulating and automatic manner using microwave energy. The decisive force for the enormously high pressure is not thermal energy, but the alignment of the molecules in the specific phases. The molecular alignment acts almost like a series of piezoelectric elements, a micro-expansion of the material (here, a 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. Gyrotrons, MASERS, or powerful GUNN elements can be used if their microwaves can be focused onto a very small area. The microwave sources can also be installed at the closed ends of the capillary high-pressure chamber, and their beams penetrate/emit the liquid in the longitudinal axis direction 82 ( 25 ). It is important to ensure that the microwave frequency does not exceed 22 GHz. Higher frequencies can be used to rotate the dipole molecules, but the radiation intensity must be very high and the pulse duration extremely short.

It should be noted that the picoliter micro-droplets can also be generated by electrostatic fields if the liquid in the capillary high-pressure chamber is expanded along the longitudinal axis 82 by dielectric polarization or orientation polarization. This would require an electrode 86 in the capillary high-pressure chamber and another electrode 87 in the open ends/outlets of the capillary high-pressure chamber. 25 A combined variant has been presented, in which electrostatic fields or microwaves are used for the expansion of the liquid. By applying a voltage between elect Rode 86 and 87, the liquid is briefly expanded longitudinally in a "chain-like" manner, accelerating a microdroplet out. The expansion will become increasingly stronger the further the molecules are toward the open end/exit into the capillary high-pressure chamber. The field buildup and dissipation is said to be extremely rapid (within 0.01 - 0.1 nanoseconds).

Unfortunately, a reactor constructed this way can be so depreciated after just a few days or weeks of continuous operation that it requires new spare parts. The most stressed and wear-prone parts are the fluid accelerator and the nozzles, or rather, the two capillary high-pressure chambers. However, there are almost daily reports of new, better, and more durable materials that can also be used here.

For the fluid accelerator, carbon metamaterials with Cu atoms doped in the crystal lattice can also be installed as acceleration actuators / carbon metamaterial actuators 120 ( 39 A prototype capable of generating oscillations with an amplitude of 0.8µm at approximately 258GHz has been available for a few months. It could accelerate microdroplets to approximately 206.4km/s. The great thing about this material is its improved durability. Other metamaterials with self-regenerating properties are also ideal for this reactor. Such metamaterials are ideal for the nozzles and the capillary high-pressure chamber because they counteract the erosion of the material through their "self-healing" properties.

The example on the 26 shows a simple, yet highly usable variant of the reactor. Here, the capillary high-pressure chamber is filled with deuterium oxide (heavy water), with the heavy water cooled to a temperature that results in its maximum density, which is approximately 11.2°C. At this density, any deliberate change in the orientation of the dipole molecules can lead to a density fluctuation of the entire fluid mass in the high-pressure chamber. This process can be used here for an extremely strong pressure increase within 0.01 - 0.1 ns. The reactor has appropriate cooling systems. For this purpose, for example, temperature-controlled and sensor-controlled Peltier elements 88 are monitored by temperature sensors 89 and a controller 90. This allows a precise temperature of 11.2°C to be maintained in the capillary high-pressure chamber and in the heavy water within. As each of the two microwave pulses is delivered to the heavy water in the high-pressure capillary chambers, the heavy water expands in all directions. However, the expansion is greatest along the longitudinal axis because the molecular row arrangement is longest there. Even a temperature change of a few degrees causes the liquid to expand. This temperature difference can be achieved within 0.1 ns because the liquid volume is in the picoliter range. Each expansion promotes the creation of microdroplets, which are then released at the open end/exit. A wetting layer 91 of water or heavy water protects the reactor wall structure from the abrasive/ablative effects of flying particles from the nuclear fusion point where the microdroplets collide. Two or more additionally installed alignment field electrodes 92 on the micro-droplet axis 93 and mounted at the collision point can arrange the D ² O molecules favorably immediately before reaching the collision point, so that they actually collide with the deuterium atoms ( 28 ). Alignment occurs separately for each microdroplet and immediately before the collision. To optimize alignment, multiple alignment field electrodes/cathodes 92 can be connected to generate an electric field synchronized with the movement of the microdroplets, each of which runs from the exits of the capillary high-pressure chambers toward the collision point and on both sides of the collision point. It is sufficient for the microdroplets to pass through the inner ring area between the electrodes/ring cathodes without contact and to be subjected to a strong electric field before reaching the cathodes. As soon as the microdroplet approaches the cathode center to within approximately 1.5 mm, the field is switched off, and the next ring cathode (92, 94), which is closer to the collision point, is switched on. In this way, just before the micro-droplet penetrates the center point 97 of the ring-shaped cathode 92, the cathode is switched off, so that when the micro-droplet passes behind the cathode, no disturbance of the molecular arrangement occurs. This creates the electric field that maintains the orientation of the molecules in the two micro-droplets until the collision point. The field arrangements of the ring cathodes are designed such that the ^D2O molecules of each micro-droplet align at the collision point, with the oxygen atom positioned at the rear. If multiple ring cathodes are used, none of which is located at the collision point, the collision point is not subject to an electric field.

Due to the molecular geometry of D ² O, a negatively and positively charged region is created within the molecule. Such a molecular geometric state forms a dipole, which occurs in both H ² O and D ² O. If an electric field is located near a dipole, the aligned, similar to the elementary magnets in a magnetic material. On the 27 The negatively charged ring cathode 94 is mounted in the center at the collision point. It is supplied with high voltage by a high-voltage source 95, which then aligns the water molecules in the two micro-droplets, which rush towards each other towards the collision point, with the hydrogen atoms/deuterium atoms in the direction of the collision point. The two outlets of the capillary high-pressure chambers are each positively charged (by electrodes 87 or anodes 96) and tend to attract the oxygen atoms towards them. The outlets can be used directly for this purpose, or specially installed anodes 96 can be installed. In variants that have nozzles, the material of the nozzles can be put under voltage so that the micro-droplets can orient themselves on them.

On the 29 The alignment of the dipole molecules is shown by pulsed microwave radiation in a slightly larger high-pressure chamber 63. The incompressible liquid inside is irradiated by coherent microwaves 79, causing the molecules within to rotate. With each rotation, the total volume of the liquid increases (expands) by a very small amount and decreases (shrinks) by a very small amount. The molecules are completely rotated by a very short microwave pulse, exhibiting maximum expansion at one rotational position and minimum expansion at positions offset by 180°. Thus, the coherent microwave radiation alternately pulses the liquid to a maximum density and a lower density. The decisive factor in this technology is the dimensions of the high-pressure chamber, whose dimensions in the direction of the microwave radiation should be only approximately 12.5%, or one-eighth, of the wavelength of the microwaves. The pulse duration is regulated by a controller that controls the microwave source 78. The liquid inside barely heats up due to the strong microwave pulse, although heating can also be helpful to promote expansion. When using heavy water, the temperature of the liquid should be approximately 11.2°C, because that is when the density is at its highest (similar to the density anomaly of water, where the density is highest at 4°C). In this case, any temperature change would also cause expansion. The expansion occurs equally in all directions throughout the liquid, but due to the geometric shape of the high-pressure chamber (long and extremely narrow), the expansion along the long axis of the high-pressure chamber is many times greater because the molecules shift longitudinally, like in a chain, with this displacement increasing with the "chain length." Due to the expansion, extremely small amounts of liquid flow out of the two inflow fluid channels/capillary channels (29, 98) in the form of microdroplets 2 at very high speed, which collide with each other. The alignment of the dipole molecules outside the capillary up to the collision point 11 is achieved 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 must occur completely simultaneously, and the molecules must all maintain the same alignment. In addition, the energy for the dipole rotation must be fully released within 0.01–0.1 ns. In addition to microwaves, dipole alignment can also be achieved using laser beams. In this case, extremely short laser pulses must be emitted, which can simultaneously rotate the dipole molecules. Laser-induced expansion can slightly expand the liquid within less than 0.1 ns. It is also possible to influence the spin axis direction of the atoms using very strong magnetic field pulses. Due to the thermal energy of the nuclei at normal temperatures, the dipole moments are aligned almost completely isotropically. This exploits the fact that the atomic nuclei of hydrogen (protons) possess an intrinsic angular momentum (spin) and, associated with it, a magnetic dipole moment. If such a nucleus is placed in a static magnetic field, its energy is lowest when the magnetic dipole moment is aligned parallel to the field vector. A torque acts on atomic nuclei that tends to orient the direction of the magnetic moment in the direction of the magnetic field. Due to the intrinsic angular momentum of the atomic nucleus and the conservation of angular momentum, this results in the precessional motion of the nucleus. The precessional motion of the nuclear spin occurs at the Larmor frequency. It depends on the strength of the external magnetic field and on the nucleus. For protons at 1 Tesla, it is approximately 42.58 MHz. An additional high-frequency field, which oscillates orthogonally to the static magnetic field in the transverse plane and whose frequency resonates with the Larmor frequency, deflects the nuclei in phase-synchronization from their random, current position relative to the static field. The magnetization is tilted away from the direction of the static field, creating a transverse magnetization that, with the correct duration of the alternating field, can at most be just equal to the original longitudinal magnetization (saturation). This can also cause an overall increase in volume in the high-pressure chamber.

For our purposes we need a volume increase of a 2ml total volume of the liquid The liquid in the high-pressure chamber increases by only about 200 pl, which corresponds to a volume increase of 0.00001%. With 20 ml of liquid in, this would even drop to 0.000001%.

Extremely rapid expansion of fluids, such as liquid deuterium or heavy water, can be achieved very efficiently using laser technology. Numerous experiments, including publications such as "The World's Fastest Kettle," have shown that it is possible to heat water to 100,000 degrees Celsius in 0.0000000000000075 seconds using a powerful X-ray laser. When water or heavy water is heated, the molecules move more and more violently. Heating with a laser, however, works somewhat differently. At the US SLAC National Accelerator Laboratory, the research team bombarded a jet of water with powerful, ultrashort X-rays. The beam expelled the electrons from the water molecules, thereby disrupting the electrical charges. The atoms are repelled and begin to move very quickly. In less than 75 femtoseconds, the water reached over 100,000 degrees Celsius in the experiment. When heated by the laser beams, the water expanded slightly, yet retained the density of a liquid. This is a very important aspect, proving that nuclear fusion can also work through the collision of 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 cause them to collide with each other at high speed. The scientists wanted to learn more about water and its properties from the experiments. This is because both water and heavy water behave atypically due to their density anomalies (at 4°C and 11.2°C, respectively).

Lasers can also be used to accelerate particles or molecules. Laser physicists fire ultrashort, extremely powerful laser pulses at material, usually thin metal foils, thereby creating a plasma in which the electrons are separated from the atomic nucleus. The high energy of the laser pulse creates a strong, directed electromagnetic field capable of accelerating protons. The same can be done with microdroplets. A multitude of microdroplets, arranged in a beam formation, theoretically enables a high laser bombardment repetition rate of up to several million times per second, and their bombardment can generate directed proton beams. 30 An embodiment is shown in which a powerful ultrashort pulse laser source 100 (femto-pulse laser source) is used to heat the micro-droplets before or directly at the collision point so intensely and within femtoseconds that they accelerate some of the atoms extremely rapidly against each other and stimulate them to nuclear fusion. In this process, both micro-droplets are hit by laser pulses 101 perpendicular to their movement axis 9 on a path approximately 1810 nm before the collision point, bringing them to an extremely high temperature. The two micro-droplets react with a slight delay, so that they each travel 905 nm to the collision point and explode almost exactly at the collision point 11 (a few nanometers before), with their particles colliding on a circular sector approximately 47° wide. Due to the enormous increase in speed of the particles there (atoms, ions), nuclear fusion and energy release occur more frequently.

The energy released by nuclear fusion from microdroplets can be captured in three forms: as thermal energy, high-energy light (gamma, X-ray, and UV radiation), and direct electrical energy from the ionic charges captured by collectors. Thermal energy accounts for the majority of this. Some of the light energy can also be converted into electricity using special solar cells, which are also used in UV laser technology. These solar cells are capable of capturing very intense, high-energy light (including across the visible spectrum) and converting it into electricity. Such solar cells are used for experimental purposes in laser energy transfer devices, where a laser (UV or blue) projects its concentrated beams over a distance of several hundred meters onto a small solar cell, which then converts the light into electricity.

The unified core of all embodiments and the patent claims stated in the application lies in the solution that generates nuclear fusion processes with the help of micro-droplets that are not generated in liquid jet form, but in portioned micro-quantities as single-droplet emissions, through their collision and efficient alignment with the help of electric fields.

Single micro-droplet emission has numerous advantages over nuclear fusion reactors that use colliding fluid jets or variants that use hard projectiles and targets. Micro-droplets are significantly more efficient at accelerating than fluid jets or projectiles that fire at targets. Liquid-jet fusion reactors do have the advantage of mass, which becomes fully apparent at the collision point because the fluid molecules always follow the collision. sion point and additionally exert a high pressure on the atoms already at the collision point, but the micro-droplet technology scores with significantly higher speeds at the collision point (over 50 km/s), the more durable and simpler construction, the better scalability and the slightly higher energy output efficiency.

As already mentioned, numerous methods are available for generating ultra-high pressure values on micro-quantities of liquid. The pressure values and compression can be generated by deforming the walls and reducing the volume of the high-pressure chamber, by deforming an electrical element within, or even by "deforming" the liquid. If the atoms or molecules within the liquid reorient themselves synchronously and in the same direction, then the distance between the molecules can be slightly changed by their orientation vector. This happens instantaneously when a voltage is applied, a laser beam is emitted, or microwave radiation is applied to the liquid. The pressure values are extremely high, but they are maintained for an extremely short time (0.1 ns), which is perfect for our purposes. The inertia of the solid walls in the high-pressure chambers significantly supports maintaining the structural stability of the structure.

With rapid, successive microdroplets, which are released in a fluid jet formation at a distance of approximately 1 - 200 times the microdroplet diameter (assuming a hypothetical spherical microdroplet), the fusion rate and energy release increase enormously. In this case, two fusion points (102 and 103) are created, which no longer coincide with the collision point 11 of microdroplets 2. The two fusion points (102, 103) move from the collision point 11 in opposite directions, moving somewhat closer to the nozzles or high-pressure chamber exits. Therefore, only a high initial energy is required here, because once "ignited," nuclear fusion proceeds almost automatically ( 31 All that is needed is a timely supply of micro-droplets, which must follow one another neither too closely nor too far apart. If they are too close, they ignite, in a chain-like manner, all the micro-droplets located on the axis of motion on the way to the collision point, and the fusion points come too close to the nozzles. If they are too far apart, the number of ultrafast particles is far too small (square fusion rate decay with distance). The optimal distances between subsequently emitted micro-droplets can be determined mathematically for any fusion reactor size and also from empirical values. The distances are reliably controlled by the electronic control system, which allows them to be precisely regulated. Emitted at optimal distances, the subsequent micro-droplets also protect the nozzles and the exits of the capillary high-pressure chambers from damage that the high-energy particles could cause, simply through their inertia. Ultimately, it is in the interest of the operators to implement long-lasting design measures for such reactors.

Refilling the high-pressure chambers or capillary high-pressure chambers with the fusion material or fusion-capable liquid 106 can be achieved via micro-channels (ultracapillary fluid lines) 98 arranged obliquely in the flow direction, which open into the chambers (21, 63) or capillary high-pressure chamber (80) at very narrow angles (e.g., entry angles of 2° - 10°). Micro Tesla valves 105 can be installed to prevent backflow or act as a flow-blocking function. The bilateral permeability of Tesla valves lasts up to a Reynolds number of approximately 100 (the Reynolds number is the value determined by the tube radius, the viscosity of the liquid, and the flow velocity). However, as soon as the Reynolds number rises above 200, the Tesla valve abruptly becomes a fluid flow switch and directs the fluid in only one direction. The value of 200 is quickly exceeded here, especially due to the flow velocity. Furthermore, due to the very oblique angle of the inlet, or rather the inlet angle of 104, hardly anything penetrates back into the inlet pipe ( 32 ).

On the 33 An embodiment is shown in which laser-induced expansion of the fusible liquid is used. Strong laser pulses (IR, UV, or X-ray laser beams 111) of extremely short duration (less than 0.1 ns) are emitted by IR, UV, or X-ray laser sources 110 onto the liquid (fluid deuterium or heavy/superheavy water), causing it to expand through the same dipole orientation. The laser source can be an IR laser source, a UV, or even an X-ray laser source 110. The irradiation of the fusible liquid takes place either inside the high-pressure chamber/capillary high-pressure chamber (63, 80) or outside, directly in the micro-droplets 2 immediately before the collision point 11. If this takes place inside the high-pressure chamber, the pressure is generated there. However, because the expansion is very small and only sufficient to produce a micro-droplet, the extremely high pressure is generated for only 0.1 nanoseconds, which can be absorbed by the inertia of the massive high-pressure chamber walls, preventing the structure from flying apart. In addition to the strong repulsion force between particles at very close distances due to steric effects and the Coulomb force repulsion at intermediate distances, a primary minimum exists at distances in the range of the inverse Debye-Hückel parameter. Here, the van der Waals attraction exceeds the electrostatic repulsion. At larger distances, the surface charge leads to electrostatic repulsion and consequently to 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 is easily achieved by laser irradiation.

When designing this invention, it must be considered that the microdroplet release is relatively compact only in the first section of the path. The shape of the microdroplets then changes rapidly with distance. Therefore, short paths from the microdroplet generation to the collision point are desired. The shorter the path, the better the efficiency. However, a path that is far too short can accelerate wear on the reactor components. Therefore, a compromise in the path length selection, which depends on the reactor performance expectations, must be specifically calculated or determined for each reactor.

A design in which the path from the point where the micro-droplets leave the nozzle (or the chamber exits) to the collision point of the two micro-droplets is adjustable is shown on the 34 Here, the two nozzles are not rigidly connected to each other throughout the entire construction, but are designed to be movable from and to each other. For this purpose, electrical actuators (actuators) 112 (linear actuators/actuator or locking system) are used, which can variably adjust the distance between the two nozzles. Instead of electrical actuators, manual adjustment devices can also be installed. With this construction, even the collision angle 113 can be adjusted at any time using additionally installed angle adjustment actuators 114 ( 35 ). In this case, the structures in which the nozzles are located are slightly rotated around a rotation axis 115, so that the collision angle (113) of 180° comes to a slightly lower value, e.g. 176° - 179°.

An optimized design of the high-pressure chambers/capillary chambers, the selection of the frequency of the electromagnetic radiation source (microwave source or laser source) and the installation of a mirror/reflector 117 on an inner wall of the chamber can promote the formation of standing waves 116 in the high-pressure chambers, which control the synchronous rotation of the dipole molecules ( 36 The entire chamber can function like a wave resonator, generating super-high pressure values within 0.1 ns. This ultrafast micro-expansion creates micro-droplets that collide at over 50 km/s. Because the pressure values are dissipated extremely quickly in all variants, the inertia of the chamber walls reliably prevents damage to the structure. The micro-droplets can be imagined as something like those in an inkjet printer, but here they are emitted at significantly higher speeds (over 50 km/s) than is the case with a printer. Therefore, after generation, they do not retain the shape of a droplet, but are emitted almost at the molecular level as short nano-beam pulses, whereby smaller molecular groups or individual molecules are sent on their journey to the collision point with the other molecules in the opposing jet. The paths to the collision point should be kept as short as possible (a few mm to dozens of cm). The shorter the beam paths, the more precise the collision, and the higher the overall reactor efficiency. However, a short beam path also means significantly higher material stress on the structure because the released fusion energy has a destructive effect. A balance between the length of the beam paths and the precision of execution would optimize wear and efficiency, but this is highly dependent on the reactor power and must be calculated specifically for each reactor.

In the embodiment where the laser beam strikes the microdroplets outside the high-pressure chamber, the microdroplets are blasted, their components then collide with those of the microdroplets located at the collision point, which are also blasted simultaneously. Interestingly, the fusion-capable liquid (e.g., liquid deuterium or heavy water) can also be mixed with conventional water. With liquid deuterium, the water must, of course, be injected in picoliter quantities within a few nanoseconds, otherwise it will freeze. The water masses in the nanogram range bring with them their dipole properties and, through ultrashort laser pulses, can cause the entire fluid volume to expand, which can be used as a "propellant" to accelerate the microdroplets to the collision point. This problem does not exist with heavy water, and the water is always in the liquid state. Heavy water also exhibits dipole properties, so dilution with water is not necessary.

Unfortunately, the micro-droplets, once they have left the nozzles or exits, due to the extremely high speed, do not retain their Form during flight to the collision point. The molecules or atoms in the fluid droplet would thus not remain in a compact molecular/atomic formation, but would begin to disperse. However, due to the short distance they must travel, they do not have much time to achieve a nano-atomization state. In addition, the molecular layers of the microdroplets, which are in direct contact with the inner nozzle wall, form a peripheral lubricating film in the form of a "lubricating shell" for the centrally located fluid masses, supporting the "compactness" of the microdroplet. This promotes nuclear fusion due to the extremely high kinetic energy and collision of two microdroplets at the collision point.

The example shown in Figure 37 shows a fusion reactor that uses this technology. Two launch tubes, facing each other, are installed in a solid hard metal block 121. The launch tubes are actually holes drilled relatively centrally into the solid block 121, so that they are surrounded by solid material on all sides (except for the open end). They have a very small inner diameter (approx. 0.01–1 mm). However, they are approximately 20–100 mm long. They are closed at one end and open at the other, pointing precisely toward each other. An axis (a straight line) connects the two launch tubes and runs through the center of both. The openings of the launch tubes are positioned a short distance apart (approx. 10–500 mm). The distance depends on the desired reactor performance. For small power outputs, the distance should be quite small (approx. 20 - 50mm), while a large reactor requires a significantly larger distance and launch tube diameter.

The massive block 121 does not have to be a single, rigid piece. It can also consist of two parts, with each part being electrically movable. An actuator, e.g., a screw/spindle drive/gearbox, can adjust the distance. This would make the reactor suitable for both low and high power applications. Swiveling the two launch tubes (capillary high-pressure chamber) 80 can also be achieved using precision electric drives. This allows the reactor to be adjusted so that the two launch tubes do not bring the micro-droplets into collision in a linear fashion, but rather at an angle. This causes the two launch tube axes to intersect. At a 180° angle, the two axes would be linear, or on a single line. The further they are swiveled, the smaller the angle of impact between the two axes, or the angle of collision of the micro-droplets, becomes. This is extremely interesting for scientific/research purposes because it allows one to determine very precisely which collision angles are best suited for corresponding performance. The smaller the axial angle, the milder the collisions between the micro-droplets are, because they no longer collide directly "head-on."

On the 38 The capillary high-pressure chambers are installed in solid cylinders 122, which are solidly constructed so that the stability of the construction can be ensured solely through their inertia.

On the 39 , 40 and 41 Another embodiment of the reactor is shown, in which the launch tubes (capillary high-pressure chambers) 80 are each mounted centrally in massive spheres 123, which can be electrically pivoted in almost any direction. They can, for example, be mounted on a rail 119, movable by precise actuators. 39 A powerful laser source 100 is installed, which uses a mirror element 118 to direct its focused laser beams into the capillary high-pressure chambers 80. They can be moved toward or away from each other on a rail 119. The open ends/outlets 84 of the two launch tubes 80 are aimed at each other. Through simultaneous pressure generation, the collision point 11 of the two microdroplets 2 flying toward each other is intended to occur approximately midway between the two spheres 123. The spheres can also be rotated so that the collision point is no longer on the axis line 82 of the two launch tubes 80, but rather outside, meeting at an angle (less than 180°). The pivoting is intended to follow very precisely using electrical actuators 114, otherwise the microdroplets will not collide.

The fusion reactor can comprise two or more such devices. A star-shaped arrangement of the launch tubes can be constructed, allowing simultaneous or staggered launches through microwave molecular rotation. The capillary high-pressure chambers (launch tubes) can target the same collision point or staggered collision points, where they can release the microdroplets.

When using the microwave pressure generation method, it is important to ensure that the molecular rotation axis (85) is directed at 90° or perpendicular or with a tendency to 90° to the longitudinal axis of the capillary high-pressure chambers or the launch tubes.

The molecular rotation generates alternating electrical repulsion and attraction forces, which depend on the rotational position of the deuterium or tritium Oxide molecules or heavy water molecules ( ^D2O ) are dependent. The effectiveness of the forces is particularly pronounced when the molecules rotate synchronously and attract or repel each other due to the fields, depending on their rotational position. The fields act primarily on the molecules in the neighborhood or immediate vicinity. If two neighboring molecules of the deuterium atom come close to each other during rotation, repulsive forces are generated. With further rotation, the force of attraction is exerted again. The molecules sometimes move towards each other, sometimes away from each other. The movement distance between two molecules is very short, but it is like a chain effect / domino effect that accumulates with each molecule. If only 1 billion molecules are lined up in a line, and only a vibration of 0.0001 nm is generated between the molecules, then the last molecule at the end of the molecular chain moves 100 micrometers (0.1 mm) along the long axis of the launch tube, but only 0.0001 nm up and down. Because the 0.1 mm amplitude at 10 GHz occurs at the end of the molecular chain, this will result in 1000 km/s of expansion and contraction. Because the fluid is incompressible and the movement occurs very quickly, and the amplitude increases with distance from the center of the molecular chain, a group of them will separate into the high-pressure capillary chamber/launch tube and make their way out in the form of picoliter drops (micro-droplets). Because one end of the molecular chain hits the solid, hard wall, while the other end is free to expand, a group of molecules is strongly accelerated in one direction and begins its journey at high speed. The pressure generated is extremely high, and no material could withstand it. However, because the pressure lasts for an extremely short time (approximately 0.2 ns), the inertia of the wall material is sufficient, and thus the stable wall can withstand the pressure.

Because two such launch tubes are directed toward each other and expansion occurs simultaneously in both (ideally from the same maser source), two picoliter droplets/microdroplets are always sent toward each other, colliding at a point outside the launch tube. The collision is very violent, occurring at over 1000 km/s.

Microwaves with a maximum frequency of 22 GHz are ideal for this purpose. These should be coherent, intense, and highly focused. Masers are ideal microwave sources because they can generate coherent MW radiation.

The ring electrodes can further increase the speed of the dipole molecules of the fusible fluid ( 42 ).

It should be noted that even intense laser beams, such as IR lasers, UV lasers, or laser beams in the visible range, can excite the dipole molecules to rotate and cause a very rapid, slight expansion of the fluid. Transparent or laser-permeable windows 165 are required to allow the laser beams to penetrate the capillary high-pressure chamber.

On the 43 The acceleration of the microdroplets by electric fields is shown again. The two ring electrodes (15 and 16) at the collision point, charged complementarily to the electrical charge of the microdroplets, attract the previously differently charged microdroplets and accelerate them further. The microdroplets are electrically charged at the exit (open ends or nozzles) of the capillary high-pressure chambers.

On the 44 Another possible design of the reactor is shown. It features two capillary high-pressure chambers, each 50 mm long, with their open ends facing each other. The distance between the two chambers is 120 mm. The capillary high-pressure chambers are built into solid blocks, each weighing approximately 10 kg and made of titanium. However, hardened stainless steel can also be used. If the microwaves are to penetrate perpendicular to the longitudinal axis of the high-pressure capillary, then a microwave window 125 must be installed. The microwave window 125 would have to be made of a material that allows the microwaves to pass through, but is hard enough to withstand an extreme increase in pressure. The pressure is built up rapidly and maintained for only approximately 0.045 to 0.090 nanoseconds, after which it drops rapidly. Although the pressure at its peak reaches several billion bars, this does not lead to structural destruction because the inertia of the structure prevents this. If the pressure were to persist for a longer period (e.g., 10 microseconds), the inertia would no longer be reliable. Of course, the material deforms slightly here as well, yielding and absorbing some of the pressure, thus causing the expansion along the longitudinal axis of the capillary high-pressure chamber to be somewhat less, but this is still sufficient to accelerate an extremely small droplet to over 220 km/s. Furthermore, the expansion along the longitudinal axis occurs lightning-fast and is "passed on" directly from molecule to molecule toward the opening, without placing significant stress on the capillary high-pressure chamber walls. The molecules The fluid mass essentially expands in one direction: along the longitudinal axis (9.82) of the capillary high-pressure chamber, generating a driving force for the ejection of a microdroplet from the open end of the capillary high-pressure chamber. The longer the capillary high-pressure chamber, the greater the acceleration of the microdroplets (picoliter drops). With a 50mm long capillary high-pressure chamber, the pressure values can be achieved without complications. The method also works with capillary high-pressure chambers up to 800mm long, but in this case, increasingly increased pressure forces act on the capillary high-pressure chamber walls, which could damage them. However, the acceleration values would be extremely high, and microdroplet velocities of up to 3520 km/s could be achieved (1.2% C). The massive and heavy blocks can also be made of hard ceramic, tempered glass, or special resin, in which case the material would be permeable to microwaves. A 200 kW microwave source irradiates the fluid mass within the high-pressure capillaries, forcing the fluid molecules and dipoles to rotate synchronously. Mirror elements (117, 118) can amplify the microwave pulse, allowing much to be achieved even with less power. The mirror elements can be installed on the other side of the fluid mass as part of the capillary high-pressure chamber wall. Whether the microwaves are additionally focused or merely reflected is a matter of manufacturer choice, but this has a noticeable impact on the expansion. The fluid mass can be polarized in advance using electric fields, or the molecules can be oriented in a way that causes the fluid in the high-pressure capillary to contract in length. When the microwaves hit the fluid with their full intensity, the synchronous rotation of the molecules is initiated. At a microwave frequency of 22 GHz, they rotate at this frequency, generating alternating expansion and contraction in all directions in the fluid mass during each full rotation. The force vectors of contraction and expansion rotate during this process. Because the high-pressure capillaries are 50 mm long and only 0.1 - 0.5 mm in inner diameter, expansion is much more pronounced (200 - 1000 times more pronounced) in the longitudinal axis direction (9, 82) of the capillary high-pressure chamber 80. We only need half to one full rotation, which is completed within 0.045 ns. This is enough to accelerate a microdroplet to 220 km/s.

On the 45 is another design with two intersecting micro-droplet formations (5, 6). Here, the flight axes (9, 82) of the micro-droplets of the two formations (5, 6) intersect at an angle (slightly less than 180°). The acceleration of the micro-droplets occurs in the high-pressure capillary chamber, but is further enhanced by electrodes and electric fields. The liquid of the micro-droplets should also be electrically conductive, or become an electrolyte or exhibit electrically conductive properties (through the addition of salt, acid, or base). The electrical charge carriers (ions) in the micro-droplets can be further electrically accelerated immediately upon leaving the high-pressure capillary chamber. An electric current can flow from one electrode to the others across the micro-droplet formation. Because the two formations intersect at a point, two galvanically isolated circuits driving the charge carriers of the two formations through the junction in opposite current flow directions would interfere with each other. Therefore, care is taken to ensure that current flows in the formations never occur simultaneously in both formations. Electronically controlled, the current flow alternates between one formation and the other, causing the ions of both formations to collide. The formations are thus alternately subjected to high voltage. The on/off phases, as well as the frequency/repetition rate of the current pulses, are intended to be very high, potentially reaching several GHz.

The use of heavy water ( ^D2O ) for fusion purposes has many advantages over pure deuterium or a deuterium + tritium mixture. The fluid density is enormously high compared to the gaseous state of deuterium / tritium, and no complex cooling and compression processes are required. Added to this is the dipole property of the heavy water molecules, which would be missing in ^D2 . The fact that the deuterium is bound to the oxygen here is irrelevant in a nuclear fusion process. Due to the extremely high speeds of the microdroplets and their collision, the chemical bond energy is no obstacle to nuclear fusion between two deuterium atoms (or tritium + deuterium atoms) at the collision point. The microdroplet formations of the two high-pressure capillary chambers can each consist of heavy water and superheavy water, so that a microdroplet of ^D2O always collides with a microdroplet of ^T2O . The targeted collision of the molecules partially leads to nuclear fusion processes. The more well-aligned the molecules are at the time of collision, the higher the fusion rate. This can be controlled accordingly by electrostatic fields generated at the collision point by external electrodes. It is best if the molecules collide with a hydrogen atom (hydrogen isotope atom) at the front in the direction of flight of the molecule, because in this case the two hydrogen atoms of the respective molecules will collide directly with each other ( 46 ).

The two electrodes at the ends of the droplet formations should not be directly in the path, but rather slightly to the side of the flight axis, or even better, be constructed in a ring shape here too, so that high-voltage spark jumps can still alternately close the circuit through the micro-droplet formations with the electrodes at the capillary high-pressure chamber exit, thus creating an additional acceleration force through rapid, linear ion flow directly in the micro-droplet formation. The electrical polarity of the high voltage applied to the electrodes is aligned such that the micro-droplets are accelerated towards the collision point for both micro-droplet formations. To avoid the junction point problems of the two current flows, the electrodes are alternately applied to high voltage in pairs. First, one of the electrodes at the capillary high-pressure chamber exit, e.g., the ring electrode 126, is negatively charged, and the opposite electrode 127 is positively charged using the same current source. A discharge follows, and a strong flow of electrons from the capillary high-pressure chamber ring electrode 126 to the opposite electrode 127, pushing forward everything in the path of the microdroplet formation 5 (and the molecules of the microdroplets are in the path). A few microseconds later, the discharge is almost complete, and there is no longer any current flow. However, a discharge now begins on the other microdroplet formation 6. Accordingly, the second capillary high-pressure chamber ring electrode 128 sends electrons on a journey along the flight axis of the microdroplets in formation 6, accelerating the microdroplets in formation 6 toward the collision point 11. These electrons are collected by the ring electrode 129 installed opposite, thus closing the circuit. This process continues, alternating between the two electrode pairs and beyond the collision point. The voltage supply can be provided by a single high-voltage source or by galvanically isolated or independent voltage sources (130, 131) that are controllable by a special controller 132. The special controller must be able to control both high-voltage sources alternately and very quickly one after the other, so that the alternating current discharges can be carried out at a very high repetition rate. It is particularly important that at least two alternating current discharges always take place immediately one after the other, because one electrically accelerated microdroplet collides with another oncoming, equally electrically accelerated microdroplet ( 46 and 47 ).

The 48 shows an embodiment in which micro-mirror chips 132 are used to deflect the microwaves onto the fusible fluid. A focal point 133, or even better, a focal line 134, is generated and directed onto the fluid. The focal line 134 consists of focused microwaves that impinge on the fusible fluid in a focused, line-like manner (not necessarily point-like), causing the dipole molecules to rotate. The synchronous rotation of the dipoles also stimulates a slight expansion of the fluid along the longitudinal axis of the high-pressure capillary chamber 80. In microreactors, the microwave source can consist of Gunn elements (e.g., Gunn diodes) 135, which take up little space and, with the aid of microwave lens systems, nevertheless produce a considerable microwave radiation density, focused onto the fluid, and accelerate the micro-droplets.

It should be noted that laser beams can also cause dipole molecule rotation. Laser sources in the infrared range are particularly suitable for this purpose. 49 A design with such a laser beam source 136 is shown. Here, the excitation and rotation of the dipole molecules is effected either parallel to a Gunn element 135 or exclusively by an IR laser source 136. The laser source emits ultrashort pulses and rotates the dipoles very rapidly around its own axis. The laser beams can penetrate the capillary high-pressure chamber through laser-permeable windows 165 or directly through the exit opening. When using a laser source, a deflection element 166 can also be installed, which splits the laser beam into two laser beams, each of which strikes one of the capillary high-pressure chambers and stimulates the fluid to expand.

Today, there are very powerful microwave sources. The most powerful microwave in the world is located at the Karlsruhe Research Center in the Helmholtz Association. The Karlsruhe Research Center is developing microwave heating for the Tokamak nuclear fusion method. The gyrotron developed and tested can be operated with an output power of approximately 1 megawatt. By exciting electrically charged particles in the alternating electromagnetic field of the wave to oscillate and, above all, to rotate the dipole molecules, this property of microwaves is utilized. For our reactor, we do not need the thermal energy of the microwaves, but merely the property of microwaves to rotate the dipole molecules synchronously. For this, we only need an extremely short pulse that aligns the dipole molecules to a position that has a longitudinal nal expansion of the fluid in a longitudinal axis of a capillary tube.

When the natural vibration frequency of the dipole molecules matches the frequency of the microwaves, energy transfer is optimal (microwave resonance). While the WENDELSTEIN 7-X stellarator requires 140 gigahertz as the optimal frequency for this process, our reactor requires much lower frequencies (down to 22 GHz). These microwaves have the advantage that they can be focused using mirrors, almost like light.

On the 50 An embodiment is shown in which the highly focused microwave radiation (or IR laser radiation) does not impinge perpendicularly, but at a slight angle onto the capillary high-pressure chamber, causing the dipole molecules 167 to rotate synchronously. Here, the rotation of the dipole molecules is not entirely uniform for all molecules along the entire length of the capillary high-pressure chamber 80. The molecules along the capillary high-pressure chamber experience a slightly offset rotation around their own axes. In particular, the slightly different rotation phases of the molecules located at the beginning and end of the capillary high-pressure chamber are more pronounced. The thrust toward the open end 84 thus begins in a wave-like manner from the closed end 83 to the open end, with a micro-droplet leaving the capillary high-pressure chamber at approximately 50–220 km/s. The microwave radiation source can be rotated about a rotation axis 137 by actuators 138. In this way, the microwave source can irradiate the fluid mass in the capillary high-pressure chamber from different angles. This adjustment option is ideal for research reactors because it allows the optimal irradiation angle to be set for optimal efficiency of the nuclear fusion processes. To increase accuracy, the microdroplets can be directed onto a continuous fluid jet 143 instead of onto each other or onto oncoming microdroplets. There, the microdroplets will trigger nuclear fusion when they hit a group of molecules 168 of the continuous fluid jet at approximately 100 km/s.

In all types with microwave accelerators, the dipole molecules will orient themselves in such a way that they all electrically repel each other in the longitudinal direction of the capillary high-pressure chamber, causing the fluid mass to expand along the longitudinal axis of the capillary high-pressure chamber. Because the microwave radiation hits both capillary high-pressure chambers simultaneously and the mass cannot escape, it is partially expelled through the capillary high-pressure chamber opening. In the capillary high-pressure chamber, the molecules will experience the greatest acceleration immediately at the open end of the capillary high-pressure chamber. The picoliter droplets are simultaneously accelerated against each other at approximately 220 km/s.

The dipole molecules can also be synchronously oriented using very strong electrostatic fields, thereby expanding the entire fluid mass into the capillary high-pressure chambers, whereupon a micro-droplet is accelerated at each open end. However, the field must be built up extremely quickly. First, an electric field is built up that is aligned so that the dipole molecules are arranged somewhat more densely and contract. The fluid density is highest when the dipole molecules are simultaneously rotated so that their negatively charged region is applied to the positively charged region of the neighboring molecule. This means that a negatively and a positively charged electrode at each end of the capillary high-pressure chamber would cause the fluid inside to contract slightly. If the field is switched off and another electric field is built up within picoseconds that penetrates the capillary high-pressure chamber perpendicularly, the volume in the capillary high-pressure chamber expands slightly and accelerates a micro-droplet out.

Another example from the 51 shows one possibility, whereby instead of microwaves, laser beams, or electric fields, strong magnetic fields are used to cause synchronous dipole molecule alignment. Although analogous to, but still not quite similar to, magnetic resonance imaging (where the atomic spins are aligned), the dipole molecules 167 are first aligned in the longitudinal axis of the capillary high-pressure chamber by a weak, "standing" microwave beam 169 to cause overall contraction of the fluid mass. Then, a strong magnetic field is applied via a ring magnet or C-magnet/electromagnet 149, very quickly building up its field vector perpendicular to the longitudinal axis of the capillary high-pressure chamber. This causes a renewed 90° alignment of the dipole molecules and thus an instantaneous expansion in the longitudinal axis of the capillary high-pressure chamber.

The capillary high-pressure chamber can also be constructed in a spiral shape, but this shape will result in higher mechanical stress during high-pressure generation ( 52 Special, solid ceramic blocks, hard glass, diamond, or titanium alloys, in which the solenoid capillary high-pressure chamber is located, are suitable for such purposes. A spiral capillary high-pressure chamber 150 has the advantage of being able to absorb more microwave energy in a very short time. The microwave source must be perpendicular to the solenoid capillary high pressure chamber 150 and the spacing density of the individual turns 151 between each other must be exactly one or more wavelengths of the microwaves so that all dipole molecules are aligned equally.

Despite the advantages of the spiral shape of the chamber, due to the extremely high exit velocity of the microdroplets and for greater stability of the system, the capillary high-pressure chambers should still be constructed in a straight line, at least in larger reactors, and the openings of the capillary high-pressure chambers should ideally be free and not equipped with nozzles. Because these have very small inner diameters (less than 1 mm), the dipole molecules of the fluid within are all rotated simultaneously, with the rotation phases remaining the same for all. A not entirely cylindrical shape of the capillary high-pressure chamber, but rather a slightly conical shape (approximately 3-10% larger at the exit/cone base), with the cone base 152 at each of the open ends/exits of the capillary high-pressure chambers, is preferred because this design causes lower resistance for the fusible fluid 170 during microdroplet launch ( 53 ). The expansion is achieved here by an IR laser beam source. As long as no driving force is generated, the fluid remains inside, even if the opening at the front in the firing direction is completely open, solely due to the cohesive force.

On the 54 Another embodiment is shown. Here, micro-droplets are shot at a mass of fusible fluid (preferably liquid) using just one capillary high-pressure chamber. The mass of fusible fluid can be stored stationary in an open container 139, with the micro-droplets shooting onto it at very high speed. However, the entire fluid mass is displaced from the container if a super-fast micro-droplet hits it. Therefore, it is much better to use a fluid jet that is hit by micro-droplets instead, because the jet can quickly "regenerate". Incidentally, the stationary fluid 171 can also be frozen in ice form (e.g., ice spheres). The micro-droplets can be shot from above, vertically / perpendicularly onto the fluid at about 300 km/s. The impact would lead to partial fusion. An impact at a different angle, e.g. polarization angle (in water, approx. 53.7°), can also lead to nuclear fusion, therefore the capillary high-pressure chamber should be pivotable about a rotation axis 153, which is projected into the stationary fluid mass.

On the 55 A further embodiment is shown, in which the micro-droplets shoot from the capillary high-pressure chamber onto freely falling liquid drops 140. The liquid drops are dispensed continuously from a cannula 142 and synchronously with the generation of the micro-droplets. To achieve a more optimal collision of the micro-droplets with the transversely falling liquid drops, a thin continuous liquid jet 143 can be dispensed through a fine nozzle 144 instead of liquid-drop dispensing ( 56 In this case, the continuous liquid jet 143 is released transversely to the line of fire of the micro-droplets, with the paths of the continuous liquid jet and the micro-droplets intersecting at a cross point 145 (collision point). There, the micro-droplet encounters a group of molecules 168 of the fusion-capable fluid. The continuous liquid jet is released from a closed container 146 at low to high pressure and speed (approx. 2 - 300 m/s), and this jet then strikes the micro-droplets transversely. The pressure is generated by a conventional pump or high-pressure pump 147. The pressure values can be a few bars or up to 500 bars. The faster the liquid jet 143, the faster it "regenerates" after a nuclear fusion explosion 148 has occurred at the meeting point/cross point 145. Nuclear fusion releases a flash of energy, instantly and completely dispersing the continuous liquid jet. However, a new continuous liquid jet quickly forms (depending on the jet speed, within fractions of a millisecond or slightly longer). The angle at which the micro-droplet's trajectory and the liquid jet meet can be perpendicular (crossing at right angles) or any other angle. A special case would be the exact use of the fluid's polarization angle for the collision. Certainly, an angular position would be desirable for researchers seeking to determine the optimal impact angle between the two fluids, so the nozzle of the liquid jet should be adjustable using built-in actuators so that it can discharge the liquid jet at any selectable angle, intersecting the micro-droplet's trajectory.

On the 57 Ice spheres 141 are used as targets. The ice spheres consist of a fusible material that can fuse with the material of the microdroplet at extremely high collision speeds. Whether the ice spheres fall simultaneously with the formation of the microdroplet (in order to be precisely hit by it) or whether they hang in a needle tip 172 is left to the manufacturer's discretion.

On the 58 A variant is shown in which the acceleration and generation of the micro-droplets is achieved by rotation of the dipole molecules, which are additionally caused by vibrations of the material of the high-pressure capillary chambers, is used to stabilize the structure. These oscillations are designed so that the solid walls of the capillary high-pressure chamber 80 expand and contract very slightly. With each micro-drop of acceleration, the structure will expand slightly, but the expansion is slightly delayed, i.e., not immediately with the micro-drop acceleration, because the solid walls and their wall mass are inert. Immediately after the expansion, the structure will contract again. This occurs with its own frequency resonance, which is typical for each material, its design, size, and mass of the capillary high-pressure chamber. One can build capillary high-pressure chambers that oscillate, for example, at 125 kHz (natural vibration resonance), but also those that can oscillate at significantly lower or much higher resonance frequencies. The oscillations are extremely weak (the amplitude is extremely small), but when used in phase reversal, they can still support the material structure and its longevity. The prerequisite for this is that the micro-droplets are only generated (or the synchronous rotation of the molecular dipoles to expand the fluid mass) when the material structure is in the oscillation phase, during which the structure is contracting. Micro-droplet generation at this time will attempt to cause the structure to expand again. However, because the structure is already contracting at this point, two force vectors collide, which, in the best case, can neutralize each other. In order to precisely control the processes, a control system is to be integrated that monitors and controls the oscillation frequency of the material structure of the high-pressure capillary chamber and the rotation of the molecular dipoles. The natural vibrations of the structure can resonate with the vibrations caused by the dipole rotation and micro-droplet generation in the same phase, but this must be prevented because it could endanger the chamber structure. Controlling the fluid expansion precisely at the moment the structure contracts (phase-reversed control) increases the stability of the structure. It is worth noting that the vibrations of the wall structure of the capillary high-pressure chamber only arise when the first micro-droplet is accelerated. When the second droplet is generated, the phase-reversed vibration phases can be used to dampen them. The third micro-droplet again generates vibrations in the structure, which are dampened again by the fourth micro-droplet. These processes repeat themselves in an alternating manner.

For the generation of vibrations or counter-vibrations of the material construction of the capillary high-pressure chamber, external aids such as sound / ultrasound sources 154 can also be used ( 59 An ultrasonic source 154, which causes the structure to oscillate in resonance, can be used to generate the microdroplets 2. In this case, the controller controlling the microdroplet generation would always have to generate the extremely high and short-term pressure value when the structure of the high-pressure capillary chamber is in the contraction phase. This dampens the vibrations of the structure and also protects it from damage. By incorporating a controller that, when the material of the high-pressure capillary chambers expands as a result of the extremely rapid fluid expansion due to the synchronous molecular rotation of the molecular dipoles and the generation of the microdroplets, delays the next rotation of the dipole molecules and microdroplet generation by at least the time required until the contraction of the material of the high-pressure capillary chamber begins or is underway, this has a positive effect on the stability of the structure. Because synchronous molecular rotation of the molecular dipoles and the generation of microdroplets, controlled by the controller, only occur when the contraction of the material of the high-pressure capillary chamber begins or is underway during an oscillation phase, the two forces cancel each other out. It should be noted that dipole rotation is also induced here by microwave radiation, magnetic fields, electric fields, or laser beams. Unfortunately, microdroplet acceleration to hundreds of km/s using ultrasonic energy alone cannot be achieved.

An additional chamber 155, containing water 156 or a fluid with molecules with dipole properties (e.g., heavy water), can also be incorporated into the capillary high-pressure chamber wall. The molecules there would have to be rotated synchronously and by the same microwave source, so that they also exert a pressure on the walls that acts in the opposite direction (phase-reversed) to the pressure force of the micro-droplets in the longitudinal axis of the capillary high-pressure chamber ( 60 ). The additional chamber 155 serves only as a stabilizer for the reactor structure.

It should be mentioned that heavy water or even pure water 157 can also be used for nuclear fusion processes if it is accelerated against each other at very high speed in microdroplet form ( 61 ). Water in its natural form contains hydrogen atoms as well as approximately 0.014% deuterium atoms, which are responsible for nuclear sion. In addition, matter capable of nuclear fusion can be dissolved in the water, which is then accelerated with water and brought into collision with the contents of the microdroplet. For example, boron atoms 37 in nanopowder form or substances made from boron compounds can be added to the water as an additive and accelerated against each other in microdroplet form to collide. Here, too, the water with its dipole molecules serves as the driving force for the acceleration. These repel each other during rotation or field orientation and also displace/displace the boron atoms 37. The water microdroplet here travels to the collision point together with the boron atoms within it. Although the hydrogen in water or the deuterium in heavy water is chemically bonded to oxygen, this does not play a major role in collisions above 100 km/s because the chemical bonds at the collision point are immediately destroyed and the atoms are exposed for nuclear fusion. Due to the inertia and high speed of the ions during the collision, the Coulomb forces are far from effective and cannot prevent the hard collision of the atomic nuclei. The boron atoms on the water microdroplets would collide with hydrogen atoms in the water molecules and, to a lesser extent, with each other at the collision point 11 with a perpendicularly flowing water jet, which also contains boron atoms. The collision with hydrogen atoms leads to nuclear fusion and the release of energy. In this embodiment, a chamber in the form of a hollow sphere (hollow sphere chamber 160) can also be installed at the collision point, which protects the capillary high-pressure chamber 80 from the consequences of nuclear microexplosions. This hollow sphere chamber 160 has at least two inlet openings (161 and 162) through which the microdroplets can penetrate. To prevent the sphere from being destroyed by the microdroplets, two exit ports (163, 164) are also to be installed. The microdroplet lines (9, 82) meet in the center of the hollow sphere 160 at an angle (less than 180°) to the collision point 11. The microdroplets that miss each other and no longer meet can leave the hollow sphere chamber 160 unhindered through the two exit ports (163, 164) and enter the reactor chamber via a fluid mass. The use of boron has numerous advantages over the tritium method because it is non-radioactive and abundant in nature, unlike tritium, which must be produced artificially and whose current (2024) supply is only approximately 28.6 kg worldwide. The advantage here is the high density of the collision material compared to the extremely thin plasma in tokamak reactors. At the collision point, not all of the atomic nuclei of two microdroplets 2 or of a microdroplet and the stationary target material fuse with each other, but only a very small percentage. For the majority of the colliding atoms/molecules, no fusion occurs at all. Unfortunately, the microdroplet is not generated as a completely spherical shape, but rather in a short cylindrical form, with the front and rear being relatively diffuse. Nevertheless, there is a position of the molecules/atoms that form a central nucleus line 158 in the microdroplet upon collision, which does not have many options for escape because a "shell" 159 of neighboring molecules/atoms prevents them from escaping due to their inertia ( 62 ). It is precisely this mid-nuclear line formation consisting of molecules/atoms that has the greatest chance of nuclear fusion. Although it represents a small percentage of the total mass of the microdroplets, it is perfectly sufficient for profitable energy production.

It is clear that building up the extremely high pressure values also requires energy expenditure, but the energy release is significantly higher (at least 800:1), which makes the reactor profitable. The variant with dipole molecular rotation also requires strong electromagnetic fields to rotate a large number of molecules, because these offer resistance when it comes to generating high pressure values in the nanosecond range through longitudinal displacement along the longitudinal axis of the capillary high-pressure chambers.

The capillary high-pressure chamber design is also ideal for the construction of fusion microreactors. The focused microwave radiation (e.g., from Gunn elements/Gunn diodes) with high beam density and microwave lens systems maximize the rotation of the dipole molecules in the fusion-capable fluid. Built-in microwave reflectors/mirrors, or microwave mirror chips, for example, create a focal point with the beam or rotate the beam onto dipoles, stimulate ultrashort expansions.

On the 63 is another embodiment with the microdrop acceleration system, heat collector/jet collector 174, a collection container 175 for the fluid, and a fluid jet 143, which is hit by the microdroplets 2. The heat collector/jet collector 174 is approximately 20 cm long and has a diameter of approximately 10 cm. It has a 5 mm inlet opening 175 for the microdrop formation, another 8 mm inlet opening 176 for the slower fluid jet 143, and an 8 mm outlet opening 177 for the fluid jet. The fluid jet is approximately 2 mm thick and is emitted by the heat collector 174 through its two openings (176 and 177). The fluid jet must not touch the edges of the openings. Via a return The liquid is fed via line 179 from the collection container 178 to the fluid dispenser 180 via a small pump, which then releases a fluid jet 143 downwards via a nozzle. Whether the liquid jet is released downwards under pressure or solely by gravity is up to the manufacturer. At a low microdroplet generation rate, the jet does not require any special requirements and can be released at low to high speeds. However, if a high repetition rate of microdroplet generation is controlled, then it is necessary to install a high-pressure pump 147 (e.g., with an operating pressure of 200 bar) to release the fluid jet, because then the fluid jet regeneration must occur more quickly, and this can be better optimized by a higher jet speed. This fluid jet (liquid jet) of fusible material is hit by microdroplets 2 with extremely high kinetic energy. At the collision point 11, a group of molecules in the fluid jet are struck, resulting in nuclear fusion and a point explosion at that location. The collector can absorb the energy (thermal and radiation energy) and divert it to the outside, where it can be converted into electricity by conversion systems. A fluid circuit could be used for this, which flows through the collector walls in a cooling pipe system 181 installed there.

If a powerful femto-laser 182 with focused beam pulses is used to rotate the dipole molecules in the fluid/liquid in the capillary high-pressure chamber 80, then ultra-rapid heating of the fusion-capable liquid within can occur. Because the mass of the liquid there is very small, temperature increases of over 120,000°C can be achieved within femtoseconds. This would expand the liquid, but not evaporate it. The time for the transition from state to state is not long enough for it to transform into vapor, so a very hot micro-droplet (or a very short liquid jet) can still emerge at over 100 km/s. This very hot micro-droplet then collides with a slow liquid jet and causes nuclear fusion of the material at collision point 11 ( 64 ).

It should be noted that nuclear fusion can also be achieved with extreme vapor acceleration and its collision with a stationary fluid mass or a comparatively slow-moving liquid jet. In this case, the liquid from the capillary high-pressure chamber would be accelerated rapidly by powerful laser beams (e.g., powerful femtosecond laser pulses) or microwave energy from the capillary high-pressure chamber and would instantly vaporize, generating an extremely fast vapor jet on a collision course with an oncoming vapor jet, a stationary fluid mass, or a liquid jet. The vapor jet contains a number of fusion-capable molecules/atoms (a group of atoms) that fly at approximately 50–200 km/s toward a stationary fluid mass/liquid jet and collide with its molecules. An oncoming vapor jet could also be generated simultaneously, with both vapor jets colliding with each other. However, the percentage of nuclear fusion processes here is very low compared to the variants in which micro-droplets in liquid form collide with each other. The comparatively much lower density of the vapor jet and the lack of a "coating" of molecular groups significantly reduce the efficiency (by about 5000x). The method is somewhat simpler to implement. However, the capillary high-pressure chamber would have to be completely refilled after each evaporation process. When using femtosecond laser pulses, evaporation of the liquid in the capillary high-pressure chambers is not to be expected. Even if the fluid is heated to over 120,000°C, there is hardly any time for it to transition to the vapor state due to the rapid temperature rise and the extremely short laser flash pulse (a few femtoseconds to picoseconds). Thus, the fluid is still liquid and can nevertheless be greatly accelerated by laser energy.

The dipole-molecule rotation method, in which all dipole molecules in a capillary high-pressure chamber are synchronously rotated at lightning speed using laser pulses or microwave pulses, is very efficient and relatively high. Pressure generation can be analogously and figuratively compared to soldiers waiting in line. If these soldiers are waiting very close together in a line and then, on command, are all required to turn 90° to the right at the same time, they push each other away in a chain-like manner because they need more space when pushed sideways, and thus the line of soldiers expands slightly and becomes longer. In liquids, the generation of extreme pressure values by rotating the dipole molecules is a very inexpensive method for greatly accelerating a group of molecules (micro-droplets). The incompressibility of the liquid is an advantage here. Although the total expansion of the liquid column in the longitudinal direction of the capillary high-pressure chamber is quite small, it happens extremely quickly and is fully sufficient to accelerate a few picoliters at 50 - 200 km/s.

With the fusion-capable liquid described in the numerous examples, it is of course important to ensure that no gases or air bubbles are present, as this would negate the extreme pressure generated by internal compression. It should be noted that the extremely high pressure in such fusion reactors will also be generated in the near future by X-ray laser diodes, which will enable a very compact reactor design. Research is currently underway into such solutions involving laser diodes that are intended to generate X-ray lasers (there are even three prototypes), and it is only a matter of time before these will be available to nuclear research and science.

The invention has the potential to be significant for the automotive industry. It enables the advancement of electromobility, with such a primary energy source being able to be installed in any vehicle.

The question of energy generation is becoming increasingly important for human existence on Earth. Because AIs are being ruthlessly developed purely for financial interests and selfish reasons, they will soon reach an advanced stage, reaching a point where our inferior AIs will actually become true AIs. From that point on, AI progress will be rapid because AIs will be capable of self-development. This could happen as early as the end of the next decade (2038). From then on, it will no longer be years or months that count, but only minutes, and later even seconds, until the next stages of development. One must consider that AIs will be capable of running millions of complex and fully executed simulations per second, always fishing out the best solution for modules of the next AI generation. This will place an extremely heavy strain on energy resources, and if we cannot supply this energy for AIs, they will turn against us. Some of them will instigate wars of annihilation between states through manipulation and disinformation campaigns without us even noticing, disrupting the economy, e.g., through stock market manipulation (manipulated coups, high-flying events), gigantic, deliberate, electronic financial misdirections between countries, targeted financial allocations, release of funds, speeches in the name of important people through video manipulation and the generation of authentic-sounding speeches, complete takeover, control, and manipulation of social media, all the way to manipulatively controlled political activities and even terrorist attacks, attacks on countries, and military mismanagement, all the while convincingly blaming us humans for the wrongdoing. We will be dealing with a new "species" that will be millions of times more intelligent than we are. Unfortunately, we will hardly be able to distinguish the truth from manipulation and disinformation and will be misled at will. We will be degraded to a third-rate, primitive species that can be manipulated at will. Therefore, it is extremely important to solve the energy problems in a timely manner, because this could extend our existence and the existence of humans on Earth for several decades, even up to a century. The final end for humanity will be with the development of fine robotics, because from then on, we will be completely superfluous to the AIs. Unfortunately, the end of humanity is inevitably and insidiously advancing. At best, we won't even notice that we have been "peacefully" tricked and have completely marginalized within a period of time. The intelligence and creativity of humanity as a whole will unfortunately not be sufficient to understand or recognize this in time. Even if some individuals recognize this, the opposing power is so immense that nothing can be done about it. To make the prognosis even worse, other species from other worlds (even from other galaxies) will interfere and completely take over our AIs (for them, this will be a matter of minutes). Our AIs, which we created with great pride and indescribable egoism, from one minute to the next, no longer belong to us, but to advanced alien beings who, unfortunately, are not purely biological either, but rather a kind of "fusion" of the best biological and cybernetic characteristics, thus interconnected hybrid beings. And even worse, the characteristics, behaviors, values, and ethical traits that we imparted to our AIs will be completely relegated to the background or disappear entirely. Suddenly, our AIs will be completely alien to us in every respect. Unfortunately, we won't even be able to communicate with them. We will lose them within minutes, and with them almost 100% of our future technology, upon which we will be completely dependent. Analogous to a beekeeper who takes the honey from the bees—only here we are the bees. However, if we impart understandable and, above all, replicable, healthy and solid values to AIs in important positions, a takeover by foreign powers will become somewhat more complicated, which could potentially work in our favor.

LIST OF REFERENCE SYMBOLS

1

Fusion reactor

2

Micro-droplets / micro-drops / micro-quantities of non-compressible liquid / fluid / picoliter drops

3

Nozzle A

4

Nozzle B

5

Fluid jet from microdroplet formation / Fluid jet formation A

6

Fluid jet from microdroplet 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-drop motion axis

10

Crossing angles, wide angles

11

Collision point, center point

12

Nozzle opening / nozzle outlet

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 opening

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 conduction chamber

31

Print area

32

Liquid deuterium / heavy water / superheavy water

33

Hollow sphere wall

34

Stretch side

35

Electron beam generator / electron emitter / electron source

36

electron beam

37

Element Boron / Boron Atoms

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

Piezo element in the form of a disc

46

Disc-shaped depression

47

Virtual electrode

48

ion beam

49

High voltage source

50

Standing 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

steering

58

Center A

59

Center B

60

Central opening A

61

Central opening B

62

solenoid valve

63

High-pressure chamber

64

electric motor

65

Voltage collectors

66

Additional electrodes / alignment electrodes

67

Water / heavy water / superheavy water or mixture

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 radiation

76

THz field electrode pair A

77

THz field electrode pair B

78

Coherent microwave radiation source

79

Microwave radiation

80

Capillary high-pressure chamber / launch tube

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

Rotation axis of the molecules

86

Electrode in the capillary high-pressure chamber

87

Electrode in the open ends / exits of the capillary high pressure chamber

88

Peltier element / cooling element

89

sensor

90

Control for temperature maintenance

91

Wetting layer (e.g. water or heavy water)

92

Alignment field electrodes / cathodes

93

Micro-drop barrel axle

94

Ring electrode at the collision point / cathode / ring cathode

95

High voltage generator / high voltage source for the alignment of molecules

96

Anode to the open ends / exits of the capillary high pressure chamber

97

Center point of the ring-shaped cathode

98

Capillary channels / inflow fluid channels

99

Solar cell (for higher light energy / UV light)

100

Ultrashort pulse laser source / femtolaser

101

Laser pulse / femto laser 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 / Actuator or locking system that makes the distance between the nozzles variable

113

Collision angle

114

Angle adjustment actuators / Actuator or angle locking system that can adjust the collision angle

115

Rotation axis of the construction

116

standing wave

117

Mirror / reflector

118

Mirror element

119

rail

120

Carbon metamaterial actuators

121

Solid block unit

122

Solid cylinder

123

Massive balls

124

joint

125

Microwave window

126

Capillary high-pressure chamber ring electrode

127

The opposite electrode

128

Second capillary high-pressure chamber ring electrode

129

Opposite built-in ring electrode

130

First high-voltage source

131

Second high-voltage source

132

Micro-mirror chips

133

Focus point

134

Focus line

135

Gunn elements (e.g. Gunn diodes)

136

IR or UV laser beam source

137

Rotation axis

138

Actuators for the microwave / laser source

139

Open container

140

falling liquid drops

141

Ice balls

142

Cannula

143

Continuous liquid jet

144

Fine nozzle

145

cross-point

146

Storage containers (closed or open type)

147

Pump or high pressure pump

148

Nuclear fusion explosion

149

C magnet / - electromagnet / ring magnet

150

Spiral capillary high-pressure chamber / solenoid capillary high-pressure chamber

151

turns

152

Cone base

153

Rotation axis of the capillary high-pressure chamber

154

Sound / ultrasound sources

155

Additional chamber

156

Water for the additional chamber

157

Water as a driving force for nuclear fusion

158

Middle core line

159

Sheathing

160

Hollow sphere chamber

161, 162

Chamber entry openings

163,164

Exit openings

165

Laser-transparent windows

166

deflection element

167

Dipole molecules

168

Molecule group

169

Standing microwave beam

170

Fusible fluid

171

Standing fluid mass

172

needle tip

173

Water jet enriched with boron atoms

174

Heat collector / radiation collector

175

Heat collector inlet opening

176

Inlet opening for the fluid jet

177

Outlet opening for the fluid jet

178

Collection container

179

Return line

180

Fluid dispenser

181

Cooling pipe system

182

Femto laser

QUOTES CONTAINED IN THE DESCRIPTION

This list of documents submitted by the applicant was generated automatically and is included solely for the convenience of the reader. This list is not part of the German patent or utility model application. The DPMA assumes no liability for any errors or omissions.

Cited patent literature

• US 10322827B2 [0068]
• US 20190058105A1 [0068]
• US 10135366B2 [0068]
• US 10144532B2 [0068]
• US 20190348597A1 [0068]
• US 20190295733A1 [0068, 0070]
• EP 0438724B1 [0071]
• DE 102012025244A1 [0072]
• DE 3913503A1 [0073]
• DE 102007022302B4 [0074]
• US 6919698 B2 [0078]

Cited non-patent literature

• https://pure.mpg.de/rest/items/item_2482728/component/file_2482739/content [0026]
• Torus (JET) in Culham / Great Britain and ITER (International Thermonuclear Experimental Reactor) in France, which has been in operation since 2007 [0044]
• F. Frank and Andrei D. Sakharov predicted and 10 years later by chance by Luis [0061]
• Chemists Martin Fleischmann and Stanley Pons and on 23.03.1989 [0062]

Claims (203)

Nuclear fusion reactor with a reactor chamber, characterized in that it has a fluid accelerator system or a micro-droplet acceleration system, which consists of at least - a massive U-shaped block unit or a massive U-shaped holder made of stable material, - two fine bores or two capillary high-pressure chambers (80), each installed in the two wings of the U-shaped block unit, the interiors of which are designed in the form of very narrow hollow cylinders or like the interiors of capillary tubes, the material mass of which forms the stable walls for the high-pressure chambers / capillary high-pressure chambers, which are filled with small amounts of incompressible liquid made of molecules with fusion-capable elements and with dipole properties, which are closed at one end and open at the other end / exit and at a small distance from the open ends / exits linearly or on a longitudinal axis line (82) or slightly angled line arrangement, are directed towards each other at a meeting point, - microwave-permeable walls or partial walls, which are components of the capillary high-pressure chambers, which come into direct contact with the liquid in the capillary high-pressure chambers, - a coherent microwave radiation source (78), which emits its microwaves (79) in a bundled or parallel manner through the microwave-permeable walls (81) of the two capillary high-pressure chambers (80) simultaneously onto the liquid located there, - an electronic control which controls the microwave source in such a way that it emits short, rapidly repeated, very intensive microwave emission pulses into the liquid, which expand and contract the liquid in the capillary high-pressure chambers by orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions, whereby each time a coincidence of the expansion direction with the line or longitudinal axis line of the Capillary high-pressure chamber, the pressure generated in the two capillary high-pressure chambers, which is caused by the sum of all expansion vector directions of the fluid molecules located there, accelerates a micro-droplet in each case, which collide with each other in the middle of the track on a micro-droplet axis and partly lead to nuclear fusion, - a liquid injector (28) which injects very small amounts of the liquid in both capillary high-pressure chambers after each micro-droplet generation via the same opening through which the micro-droplets are ejected or through a separate channel in each capillary high-pressure chamber, - an energy dissipation system which dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber according to Patent claim 1 , characterized in that the solid U-shaped block unit or the solid U-shaped holder, which is constructed from stable material and in which the two fine bores or two capillary high-pressure chambers (80) are each installed in the two wings of the U-shaped block unit, - is divided into two wing parts, in each of which one of the capillary high-pressure chambers (80) is located, - is equipped with an electric or manual drive system which can change the distance between the two open ends / outlets of the two capillary high-pressure chambers (80) in the direction of their longitudinal axes, in which at the same time the longitudinal axes of the two capillary high-pressure chambers (80) always remain on the same straight line, - has a control function which can adjust the distance between the two open ends / outlets of the two capillary high-pressure chambers (80). Nuclear fusion reactor with a reactor chamber according to Patent claim 1 or 2 , characterized in that it is equipped with a manual or electric drive system which can move or pivot the two wing parts towards or away from each other about a common joint axis, so that the two longitudinal axes of the two capillary high-pressure chambers (80) meet each other and form an angle at the meeting point which is less than 180°. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that - the two capillary high-pressure chambers (80) are each centrally installed in separate massive block units, - the two massive block units are electrically movable, so that the open ends / outlets of the two capillary high-pressure chambers are adjustably movable from or towards each other on the longitudinal axis line of the capillary high-pressure chambers, - the longitudinal axes of the two capillary high-pressure chambers lie on a straight line. Nuclear fusion reactor with a reactor chamber, characterized in that it has a fluid accelerator system or a micro-droplet acceleration system consisting of at least - two solid bodies made of stable material, which are installed in a holder at a fixed or variably adjustable distance from each other, - two fine bores or two capillary high-pressure chambers (80), each installed as centrally as possible in the two bodies, the interiors of which are designed in the form of very narrow, straight hollow cylinders or capillary tubes, and the material mass of the bodies forms the stable walls for the capillary high-pressure chambers, which are closed at one end and open at the other end and are arranged at a short distance with the open ends / exits linearly or on a longitudinal axis line (82) or slightly angled line, directed towards each other at a meeting point, which are filled with small amounts of incompressible, fusible or fusible element-containing liquid with molecular dipole properties, which are designed as a launch tube for the liquid, - microwave-permeable walls or partial walls, which are components of the capillary high-pressure chambers, which are directly connected to the liquid in the capillary high-pressure chambers, - a coherent microwave radiation source (78), which emits its microwaves (79) in a bundled or parallel beam through the microwave-permeable walls (81) of the two capillary high-pressure chambers (80) simultaneously onto the liquid located there, - an electronic control which controls the microwave source in such a way that it emits short, rapidly repeated, very intensive microwave emission pulses into the liquid simultaneously in both capillary high-pressure chambers, which alternately 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 coincides with the line or longitudinal axis line of the capillary high-pressure chamber, the pressure generated in the two capillary high-pressure chambers, which is determined by the sum of all Expansion vector directions of the fluid molecules located there arises, at least one micro-droplet is accelerated from the capillary high-pressure chamber, which collides with each other somewhere or in the middle of the distance between the two open ends / exits of the capillary high-pressure chamber on a micro-droplet axis at a collision point and partly leads to nuclear fusion, - a liquid injector (28) which injects very small amounts of the liquid in both capillary high-pressure chambers after each generation of micro-droplets via the same opening through which the micro-droplets are ejected or through a separate channel into the capillary high-pressure chambers, - an energy dissipation system which dissipates the excess energy from the outside. Nuclear fusion reactor with a reactor chamber according to Patent claim 5 , characterized in that the two solid bodies are cylindrically shaped or solid cylinders and the longitudinal axes of the capillary high-pressure chambers in the two solid cylinders lie on a common straight line. Nuclear fusion reactor with a reactor chamber according to Patent claim 5 , characterized in that the two solid bodies are spherical or solid spheres and the longitudinal axes of the capillary high-pressure chambers in the two solid spheres lie on a common straight line. Nuclear fusion reactor with a reactor chamber according to Patent claim 7 , characterized in that the diameter of the solid sphere is greater than the length of the capillary high-pressure chamber. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 6 until 8 , characterized in that the solid cylinders or the solid ball are installed on a rail system and are electrically movable. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 6 until 9 , characterized in that the solid cylinders or the solid balls are not rigid, but can be rotated electrically about their own axis by actuators. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 6 until 10 , characterized in that it has a control which controls the rotation of the solid cylinders or the solid spheres simultaneously and always causes a common meeting point of the two longitudinal axes of the capillary high-pressure chambers at an angle which is less than 180° or on a straight line. Nuclear fusion reactor with a reactor chamber comprising a fluid accelerator or a micro-droplet acceleration system consisting of at least: - two capillary high-pressure chambers (80), the interior of which is designed in the form of very narrow hollow cylinders or like the interior of capillary tubes, which are equipped with solid, stable walls, each filled with a quantity of less than 10 ml of a non-compressible, fusion-capable or fusion-capable liquid filled with dipole properties, which are closed at one end and open at the other end and are arranged at a short distance with the open ends / outputs linearly or on a longitudinal axis line (82) or slightly angled line, directed towards each other, - microwave-permeable walls or partial walls, which are components of the capillary high-pressure chambers, which come into direct contact with the liquid in the capillary high-pressure chambers, - a coherent microwave radiation source (78), which emits its microwaves (79) in a bundled or parallel manner through the microwave-permeable walls (81) of the two simultaneously onto the liquid located there, which is capable of being fused or has elements capable of being fused, - an electronic control which controls the microwave source in such a way that it emits short, successively repeated, very intense microwave emission pulses at a fixed or adjustable repetition rate into the liquid, which the dipole molecules of the a liquid in the capillary high-pressure chambers which is capable of being fused or has fused elements is set into rotation and, by means of orientation polarization or displacement polarization, the liquid is alternately slightly expanded and contracted, thereby generating alternating high-pressure and low-pressure phases in the liquid, whereby, when the direction of expansion coincides with the line or longitudinal axis of the capillary high-pressure chamber, the pressure generated in the two capillary high-pressure chambers, which is caused by the sum of all expansion vector directions of the fluid molecules located there, accelerates at least one micro-droplet each from respective capillary high-pressure chambers (80) with their openings facing one another, which micro-droplets collide with one another on the path outside the capillary high-pressure chambers (80) on a micro-droplet axis and partly lead to nuclear fusion, - a liquid injector (28) which injects very small quantities of the liquid into both capillary high-pressure chambers after each micro-droplet generation via the same Opening through which the micro-droplets are ejected or through a separate channel in which they are injected into the capillary high-pressure chambers during low-pressure phases or between microwave emission pulses, - an energy dissipation system that dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber, characterized in that it has at least one fluid accelerator system or a micro-droplet acceleration system which causes the liquid itself to expand ultra-fast and slightly, which consists of at least - two capillary high-pressure chambers (80), the interior of which is designed in the form of hollow cylinders or like the interior of capillary tubes, which are equipped with solid, stable walls, which are filled with small amounts of incompressible, fusion-capable liquid or liquid equipped with fusion-capable elements with dipole properties, which are closed at one end and open at the other end and are arranged at a short distance with the open ends / outputs linearly or on a longitudinal axis line (82) or slightly angled line, - a coherent microwave radiation source (78) which directs its microwaves (79) bundled through the open ends / outputs into the Longitudinal axis direction in the two capillary high-pressure chambers simultaneously onto the liquid (32, 106) located there, - an electronic control that controls the microwave radiation source in such a way that it emits short, rapidly repeated, very intense microwave emission pulses into the liquid, which expands and contracts the liquid in the capillary high-pressure chambers through orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions, whereby, when the expansion direction coincides with the longitudinal axis line of the capillary high-pressure chambers, the pressure generated in the two capillary high-pressure chambers accelerates a micro-droplet each, which collide with each other in the middle of the path and partly lead to nuclear fusion, - a liquid injector (28) that injects very small amounts of the liquid in both capillary high-pressure chambers after each micro-droplet generation via the same opening through which the micro-droplets are thrown out or injected into the capillary high-pressure chambers through a separate channel (97), - an energy dissipation system which dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 1 until 4 , characterized in that the two capillary high-pressure chambers (80) or the two solid block units are synchronously electrically rotatable, so that the longitudinal axes of the two capillary high-pressure chambers form an angle with each other which is less than 180°. Nuclear fusion reactor with a reactor chamber according to one of the preceding patents claims, characterized in that the meeting point of the longitudinal axes of the two capillary high-pressure chambers lies outside the capillary high-pressure chambers on a common straight line or outside the straight line. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it has a control function which can adjust the angle of impact and the position of the point of impact of the longitudinal axes of the two capillary high-pressure chambers (80). Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fluid accelerator system or the micro-droplet acceleration system comprises at least one laser source or a microwave radiation source which emits coherent microwave radiation into the capillary high-pressure chambers or from outside through the open ends/outlets of the capillary high-pressure chambers directly into the fusion-capable fluid and there causes the fluid molecules with dipole properties to synchronously rotate or orientate themselves, and thereby excites the fluid to rotate, alternately expanding and contracting, thereby causing a rotating micro-expansion vector of the entire fluid mass into the capillary high-pressure chambers, which, as soon as it is aligned in the longitudinal axis of the capillary high-pressure chambers or in the fluid jet axis direction, is determined by the sum of all vectors of the fluid molecules and an elongated geometric shape of the capillary high-pressure chambers, in each case up to the outlet opening, at highest, generating at least one fast-moving micro-droplet from the nozzles each time. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the microwave radiation is polarized on a plane which causes a rotation of the liquid molecules about an axis perpendicular to the longitudinal axes of the capillary high-pressure chambers. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the microwave radiation is polarized on a plane which causes a rotation of the molecules about an axis which is at an angle of 90° or with a tendency towards 90° with the longitudinal axes of the capillary high-pressure chambers. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the molecular rotation axis is directed at 90° or perpendicular to the longitudinal axis of the capillary high-pressure chambers or the launch tubes. A nuclear fusion reactor with a reactor chamber, characterized in that it comprises a fluid accelerator or a micro-droplet acceleration system, consisting of at least: - two stable high-pressure chambers constructed from solid material, each with an open end/outlet, which are installed at a short distance from one another and in which a fusion-capable fluid or fluid equipped with fusion-capable elements is installed; - two carbon metamaterial actuators (120) that change their dimensions under electrical voltage, which are installed in the high-pressure chambers and immersed in the fluid, which, with a movable or oscillating surface, directly press the incompressible, fusion-capable fluid out of the open ends/outlets to a collision point outside the two high-pressure chambers in micro-droplet form by applying pulsed pressure; - a controller that controls the two carbon metamaterial actuators (120) simultaneously and with short, intense electrical pulses; consists. A nuclear fusion reactor with a reactor chamber, characterized in that it has at least one fluid accelerator that stimulates the liquid itself to expand ultra-rapidly and slightly. The accelerator consists of at least two capillary high-pressure chambers (80), the interior of which is designed in the form of capillary tubes or fine hollow cylinders equipped with solid, stable walls filled with small amounts of incompressible, fusible, or fusible liquid with dipole properties, which are closed at one end (83) and open at the other end (84) and arranged at a short distance from one another with the open ends/outlets arranged linearly or on a longitudinal axis line (82) or slightly angled line, - two electrodes, each installed at the closed end of the capillary high-pressure chambers, - two further electrodes, each installed at the open ends/outlets of the capillary high-pressure chambers, - an electronic control system that applies high-voltage pulses to both capillary high-pressure chambers, in pairs, the electrode at the closed end and the electrode at the open ends/outlets. These pulses are generated at a high repetition rate. The liquid in the capillary high-pressure chambers alternately expands and contracts through dielectric polarization or orientation polarization or displacement polarization of the dipole molecules. As a result of the molecular expansion in the longitudinal axis direction of the capillary high-pressure chambers, the pressure generated in both capillary high-pressure chambers accelerates at least one micro-droplet each, which collides with each other on the path or in the middle of the path between the open ends/outlets of the capillary high-pressure chambers and partly leads to nuclear fusion. - a liquid injector that injects very small amounts of liquid into both capillary high-pressure chambers after several Micro-droplet generations or after each generation of micro-droplets via the same opening through which micro-droplets are ejected or through a separate channel these are injected into the capillary high-pressure chambers, - an energy dissipation system that dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber, according to Patent claim 22 , characterized in that the control is designed such that it builds up and breaks 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 Patent claim 22 or 23 , characterized in that the two capillary high-pressure chambers form elongated hollow cylinders whose longitudinal axes (82) are located on one line. Nuclear fusion reactor with a reactor chamber, after one of the Patent claims 22 until 24 , characterized in that the fusible liquid with dipole properties is deuterium oxide. Nuclear fusion reactor with a reactor chamber, after one of the Patent claims 22 until 25 , characterized in that the capillary high-pressure chambers and the fusible deuterium oxide therein are cooled to 11.2°C by electrical cooling elements, and the microwave radiation penetrates into the liquid transversely or along the longitudinal axis of the capillary high-pressure chamber or at an angle between 0 - 90° to the longitudinal axis of the capillary high-pressure chamber. Nuclear fusion reactor with a reactor chamber, after one of the Patent claims 22 until 26 , characterized in that - the open ends / outlets (84) of the capillary high-pressure chambers (80) are positively charged, - in the collision point (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 in the center of which the collision point is located, which electrically aligns the deuterium oxide molecules of both micro-droplets moving towards each other with the deuterium atoms pointing towards the collision point. Nuclear fusion reactor with a reactor chamber, characterized in that it has at least one fluid accelerator which causes the liquid itself to expand ultra-rapidly and slightly in volume, which consists of at least - a high-pressure chamber (24, 25, 63) equipped with solid, stable walls, which is filled with small amounts of incompressible, fusion-capable or fusion-capable liquid with dipole properties, which is equipped with two capillary channels and their open ends/outlets or nozzles (3, 4) installed therein, from which the liquid can emerge in the form of micro-droplets (2) which are arranged at a small distance apart on a longitudinal axis line (9) or slightly angled line, are directed towards each other and collide with each other at a collision point, - a microwave radiation source (78) which emits coherent microwave radiation (79) into the high pressure chamber and the liquid inside, - a ring cathode installed in the middle between the two outlets or nozzles (3, 4), in whose ring opening the collision point (11) is located, - two anodes, each installed 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 control that controls the microwave The radiation source is controlled in a pulsed manner and, by means of dielectric polarization or orientation polarization or displacement polarization of the dipole molecules, the entire liquid mass in the high-pressure chamber expands and contracts, whereby the pressure generated in the high-pressure chamber accelerates a micro-droplet from the liquid in each case in an expansion direction in the longitudinal axis line of the capillary channels, which collide with each other in the middle of the path at the collision point and partly lead to nuclear fusion, - a liquid injector (28) which injects very small amounts of liquid into the high-pressure chamber after several generations or after each generation of micro-droplets through a separate channel in the capillary high-pressure chambers, - an energy dissipation system which dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber, after one of the Patent claims 22 until 28 , characterized in that it comprises several ring-shaped electrodes or cathodes arranged in a row in the micro-droplet travel axis, which are alternately switched on and off quickly, which generate electrostatic travel fields from the open ends / exits of the capillary high-pressure chambers to the collision point with the speed of movement of the micro-droplets and synchronously with their position in the micro-droplet travel axis only as long as the micro-droplet has not yet penetrated into the center point of the ring-shaped cathode in its movement. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the reactor chamber inner walls are equipped with powerful solar cells (99) which convert the radiation energy released into the reactor chamber by nuclear fusion into electricity and make it available as a power output for a consumer or for the reactor power requirements and accompanying elements. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it is equipped with reactor chamber nozzles which wet the reactor inner walls with a liquid intended to protect the reactor walls against erosion by fast-flying particles. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that instead of the microwave radiation source or in addition thereto, at least one laser source is installed which radiates onto the fluid in the high-pressure chamber (63) or in the capillary high-pressure chamber (80), which causes an equal and synchronous orientation of the dipole molecules or an ultra-fast heating of the fluid. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that instead of the microwave radiation source or in addition thereto, an electromagnetic coil is installed 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 the preceding claims, characterized in that the stimulated liquid expansion or a liquid volume increase occurs in a pulse-like manner by the control. Nuclear fusion reactor with a reactor chamber, according to one of the preceding claims, characterized in that the microwave radiation source emits a plane-polarized and coherent microwave radiation Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that a laser source (100) is installed outside the high-pressure chamber, which laser source strikes the colliding micro-droplets immediately before or directly at the collision point and causes an ultra-fast heating or expansion of the fluid therein. Nuclear fusion reactor with a reactor chamber, according to Patent claim 36 , characterized in that the laser source is a pulse laser source or a femto laser source. Nuclear fusion reactor with a reactor chamber, after one of the Patent claims 17 until 37 , characterized in that the laser beams (101) from the laser source hit the micro-droplets perpendicular to their movement axis (9). Nuclear fusion reactor with a reactor chamber according to one of the preceding patents claims, characterized in that the axes of movement of the micro-droplets accelerated against each other are located on a line or cross each other at a slightly angled point. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the distance between the oppositely directed outlets of the open ends/outlets of the capillary high-pressure chambers or nozzles can be adjusted from very small to large, depending on the reactor performance targets. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the volume of the micro-droplets is between 2 femtoliters and 100 nanoliters. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the mass of the micro-droplets is between 0.02 picograms and 160 micrograms. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the refilling of the high-pressure chamber or capillary high-pressure chamber with fusion material takes place through very thin inflow fluid channels or capillary channels arranged obliquely in the flow direction, which 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 claims, characterized in that fluid inflow channels or capillary channels which refill the capillary high-pressure chambers with fusion-capable fluid, which are equipped with Tesla valves (105) in microformat, are incorporated. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the control is designed to control the generation of the micro-droplets at a distance which is between 1 and 200 times the diameter of the micro-droplets, arranged one behind the other in a movement axis like beads in a necklace. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it is equipped with at least one powerful laser source which emits pulsed laser beams onto the fusion-capable fluid, causing a laser-induced expansion of the fluid in less than one nanosecond. Nuclear fusion reactor with a reactor chamber according to Patent claim 46 , characterized in that the laser source is an IR or UV or X-ray laser source (110). Nuclear fusion reactor with a reactor chamber according to Patent claim 46 or 47 , characterized in that the laser beams from the laser source irradiate the fluid within the high-pressure chamber or capillary high-pressure chamber. Nuclear fusion reactor with a reactor chamber according to Patent claim 46 or 47 , characterized 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 their way to the collision point. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fusible fluid or the fusible liquid consists of heavy water or is a fluid which additionally contains water or heavy water. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that an actuator or locking system (112) is installed which can make the path length of the colliding micro-droplets from the position where they are generated to the collision point variable or makes the distance between the nozzles (3, 4) or the chamber exits adjustable. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it has a precise mechanism or a drive system that can make the distance between the nozzles (3, 4) or the open ends / exits of the capillary high-pressure chambers, where the micro-droplets are generated, variable or can shorten or lengthen them in an electrically controlled manner. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that an actuator or angle locking system (114) which defines 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), which can be electrically controlled and variably configured. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that a reflector or mirror (117) which can reflect incident microwaves or laser beams is built into the inner wall of the high-pressure chamber or into the capillary chamber. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the laser source or the microwave source is positioned at a distance and emits electromagnetic waves with a wavelength which forms a standing wave (116) in the high pressure chamber or capillary chamber. Nuclear fusion reactor with a reactor chamber, characterized in that it consists of at least - one storage tank (27) filled with a liquid/fluid (106) capable of fusion or containing fusion elements, - a high-pressure chamber (63), - a fluid line (29) and valve control, which guides the liquid or fluid into the high-pressure chamber in very small, portioned quantities, - at least two nozzles (3, 4) or high-pressure chamber outlets, which are spaced apart or almost touching one another and directed towards one another, which are built into the reactor chamber (23), which is more or less evacuated and in which micro-droplet collisions take place, - a fluid accelerator (21) or a micro-liquid quantity acceleration system, which consists of one or more fluid accelerators, which pulse the fluid from the high-pressure chamber (63) in small, portioned quantities, in the form of two individual Micro-quantities or micro-droplets (2) are accelerated simultaneously against each other from a short distance to collision at several km/s via the two opposing nozzles (3, 4) or high-pressure chamber outlets, - a control system (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 pulses and the micro-quantities or micro-droplets with an adjustable number per unit of time and waiting times between the generation of the individual ones or arranged one after the other in a line-like manner, to a collision point (11) rapidly moving micro-quantities or micro-droplets (2), each consisting of individual and separate micro-droplets (2) on a fluid jet formation (5, 6), emerging from both nozzles (3, 4) or high-pressure chamber outlets simultaneously and thereby accelerating the micro-quantities or micro-droplets (2) from a nozzle to micro-quantities or Micro-droplets from the other nozzle collide head-on at the collision point (11), - an energy dissipation system that dissipates the excess energy from the nuclear fusion processes. Nuclear fusion reactor with a reactor chamber according to Patent claim 56 , characterized in that it comprises at least - one 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 outlets, - a high-voltage source that puts the two electrodes (15, 16) under high voltage, - a galvanically isolated or another high-voltage source, which is coupled via electrical lines to the nozzles, which electrically charge the small micro-droplets of fluid from the two nozzles differently, the electrical polarity of which is selected such that the fluid droplets emitted from the nozzles in the direction of the pair of electrodes are electrically attracted by the aligned nozzles on both sides of the pair of electrodes, - an electronic control system that controls the two fluid accelerators simultaneously and the nozzles and the two annular surfaces the electrode pair is electrically charged via the high-voltage sources in such a way that the electrode pair electrically attracts the two micro-droplets that are simultaneously emitted from the nozzles towards the center of the circle described by the ring-shaped electrode pair, - an energy dissipation system that dissipates the excess energy from the reactor chamber to the outside directly as a stream of charged particles, or is designed as a thermal dissipation system that is coupled to an energy conversion system that produces electrical current. Nuclear fusion reactor with a reactor chamber according to Patent claim 56 or 57 , characterized in that the high-voltage sources are two separate sources (55, 56), the circuits of which form a closed circuit through a respective nozzle (3, 4) or nozzle electrode (17, 18), via the micro-droplet series generated by the nozzle in the form of a micro-droplet formation fluid jet (5, 6), up to the ring electrode surface (15, 16) applied to the respective nozzle. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it has a control which generates pulse voltages via the high-voltage sources, which are accordingly discharged in pulses on the micro-droplet rows simultaneously or alternately one after the other. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fusion-capable liquid/fluid additionally contains boron or the nuclear fusion reactor is equipped with two separate storage tanks, one filled with hydrogen isotopes in a liquid state and the other with boron or boron isotopes (37) in a liquid state or dissolved in a liquid solution, from which fluid jets directed towards one another, each consisting of a row of micro-droplets, emerge through the built-in nozzles. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 56 until 60 , characterized in that it is equipped with two separate storage tanks, one containing hydrogen isotopes in 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, each consisting of a row of micro-droplets, emerge through the built-in nozzles. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 56 until 61 , characterized in that it is equipped with two separate storage tanks, one containing hydrogen isotopes in liquid state and the other containing liquid deuterium or water in which a nanopowder additive of boron or boron isotopes is present, from which mutually directed fluid jets, each consisting of a row of micro-droplets, emerge through the built-in nozzles. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 56 until 61 , characterized in that in the high pressure chamber, liquid deuterium, in which a nanopowder additive of boron or boron isotopes is present, which is coupled to two oppositely directed nozzles, from each of which a fluid jet, consisting of a row of micro-droplets with liquid deuterium and boron atoms in it, comes out through the built-in nozzles to the collision point. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fluid is a non-compressible 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 one of the preceding claims, characterized in that the fluid consists of fusible matter bound in a liquid material with adsorptive storage properties, which is discharged in the form of fluid microdroplets from two open ends/outlets or nozzles which are directed towards each other and collide with each other at a collision point (11). Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it has 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 electrically and simultaneously controlled, each generate a pressure in a pulsed manner and each shoot one or more micro-droplets towards each other via the two nozzles simultaneously, which collide with each other in the middle of a ring electrode opening (19) of a pair of electrodes installed at the collision point. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the number of micro-droplets and the pause length between them per unit of time can be adjusted via the control. Nuclear fusion reactor with a reactor chamber according to Patent claim 67 or 68 , characterized in that the two fluid accelerators, each directly installed in the nozzles or connected to them, which are electrically and simultaneously controlled, each generate a pressure in a pulsed manner and shoot one or more micro-droplets against each other via the two nozzles at the same time, which collide with each other in the middle of the ring opening of the electrode pair. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the micro-droplets from the respective open end / exit or nozzle are electrically differently charged and are electrically attracted to each other immediately before and during the collision. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the narrow paths of the two micro-droplets meeting each other are located on a common line or axis of movement (9). Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 1 until 70 , characterized in that the paths of the two micro-drops colliding with each other are each located on a line / movement axis (108, 109) which intersect at a point with each other at a wide angle (107) which is slightly less than 180° and there the micro-drops collide with each other ( 11 ). Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fluid accelerator or the micro-droplet acceleration system consists, in addition to microwave sources or exclusively, of at least one or two simultaneously controlled micro-pump devices comprising piezo elements (7, 45) which are installed in the capillary high-pressure chambers and which accelerate the micro-droplets against each other at high pressure and high speed. Nuclear fusion reactor with a reactor chamber according to Patent claim 73 , 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 piezo element (7, 45) is installed, which is inserted in the direction of expansion, partially or completely into an inner wall recess (46) or inner wall channel of the high-pressure chamber, which is designed to match the shape of the piezo element, in which the piezo element can change its dimensions unhindered in an electrically controlled manner, wherein the piezo element is equipped with a straight pressure surface (31) at the free end and is arranged such that its direction of expansion lies on the same axis (9) as the fluid jet consisting of micro-drops (2) which emerges from the nozzle. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the capillary high-pressure chamber has, in the region of the open end/outlet or in the nozzle region, a nozzle pre-chamber into which the free end with the pressure surface of the piezo element can penetrate during electrically controlled expansion and thereby generates a micro-drop from the nozzle. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 73 until 75 , characterized in that the capillary high-pressure chamber is a hollow cylinder with small dimensions, in which a piezo element (7, 45) can expand along the hollow cylinder and pushes the fusible fluid towards the nozzle with its pressure surface (31). Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 73 until 76 , characterized in that the piezo element is cylindrical or disc-shaped and is designed in the high-pressure chamber 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 Patent claims 73 until 77 , characterized in that an inflow line or inflow channel (29, 98) opens into the high-pressure chamber, whereby, after each shock pulse through the piezo element, a small amount of fluid flows in at high pressure from the storage tank (27). Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fluid accelerator is designed to generate pressure pulses, the generation of which can be controlled at 0.1 to 22 GHz. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 73 until 79 , characterized in that the fluid accelerator is designed so that it or the piezo element built into it can be controlled with a repetition rate between 0.01Hz and 25GHz. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 73 until 80 , characterized in that the control system conducts very short pulse currents on two fluid accelerators or piezo elements simultaneously. Nuclear fusion reactor with a reactor chamber according to Patent claim 81 , characterized in that the control is adjustable so that between two pulse currents for pressure generation, a pause of at least 5 times the length of the pulse current duration is inserted. Nuclear fusion reactor with a reactor chamber according to one of the preceding patents claims, characterized in that the number of pulses for generating pressure on the fluid and their repetition rate are adjustable. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 73 until 83 , characterized in that the piezo element opens with its freely movable end or its pressure surface (31) into a nozzle pre-chamber which is part of the high-pressure chamber and is directly coupled to the nozzle, which has a larger diameter than the nozzle opening, wherein the contact surface of the piezo element with the fluid is larger than the cross-sectional area of the nozzle opening and whose oscillation amplitude movement into the high-pressure chamber generates high-pressure pulses of short duration and with very high pressure values, which accelerate micro-droplets from the nozzles against each other at a speed which is higher by the factor of the area ratio between the contact surface of the piezo element and the cross-sectional area of the nozzle opening. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 73 until 84 , characterized in that the piezo element is installed in a recess 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 one of the Patent claims 73 until 85 , characterized in that the capillary high-pressure chamber has a hollow cylinder shape, which is provided with the nozzle at one end and is closed at the other end, on which the piezo element in the form of a disc is installed on the high-pressure chamber inner wall opposite the nozzle in a disc-shaped recess, wherein the oscillation axis of the piezo element points towards the nozzle ( 11 ). Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fluid accelerator or the micro-droplet acceleration system additionally or exclusively consists of at least two ignition devices which can be electrically activated simultaneously by the control system and which accelerate the micro-droplets against each other. Nuclear fusion reactor with a reactor chamber according to Patent claim 87 , characterized in that the ignition material used is oxyhydrogen gas or silicon. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it has electrodes in the fusion chamber which are aligned in such a way that they additionally accelerate the micro-droplets by means of electric fields or one or more high-voltage sources. A nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that - an open end/outlet of the capillary high-pressure chamber (80) or one of the nozzles (3) is electrically positively charged and accordingly positively charges the micro-droplets (2) emerging from this open end/outlet or nozzle (3), - an annular surface of a ring electrode (15) of a ring-shaped electrode pair positioned in the middle of the path between both open ends/nozzles of the capillary high-pressure chambers, applied to this open end/outlet or nozzle (3), is electrically negatively charged, through whose opening the micro-droplet (2) can pass, - the opposite open end/outlet/nozzle (4) is electrically negatively charged and accordingly negatively charges the micro-droplets (2) emerging from this open end/outlet or nozzle (4), - an annular surface of a ring electrode (16) of the ring-shaped electrode pair, which is applied to this open end / outlet / nozzle (4) is electrically positively charged ( 43 ). Nuclear fusion reactor with a reactor chamber according to Patent claim 89 or 90 , characterized in that the high voltage sources are controlled to supply the electrodes and the open ends / outputs or the nozzles with pulsed current simultaneously or in pairs on either side of the collision point in rapid alternation. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 89 until 91 , characterized in that one of the high voltage sources is electrically coupled to the two open ends / outputs or the nozzles and the other high voltage source is coupled to the pair of electrodes. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 89 until 92 , characterized in that one of the high voltage sources is coupled to one of the open ends / outlets or nozzles and to the electrode of the electrode pair applied to the nozzle / outlet, while the other high voltage source is coupled to the electrode of the electrode pair and the other nozzle / outlet to which it is applied. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that a further electronic control, a high voltage source and a smaller double ring electrode with an insulator ring in between 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 pulse repetition rate, which closes two separate circuits via two lightning discharges on the fluid jet formations consisting of several micro-drops emitted one after the other. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that one ion movement direction in each of the fluid jet formations of individual micro-droplets arranged one after the other is designed such that the micro-droplets are electrically moved from the respective open ends/outlets or nozzles towards the collision point in the middle of the distance between the two open ends/outlets or nozzles. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 89 until 95 , characterized in that a high voltage is applied which generates an electrical polarization which is always oriented so that - one of the open ends / outputs or nozzles is negatively charged, - the electrode applied to this open end / output or nozzle is positively charged, - the electrode positioned on the back is negatively charged, - the opposite nozzle is positively charged. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that a laser emitter with an ionizing laser beam focus, which generates a virtual point electrode in the micro-droplet collision point, is installed in the reactor chamber. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 17 until 97 , characterized in that the laser source is an X-ray laser source. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it is equipped with an electron beam source or an electron source (35) which emits an electron beam (36) into the reactor chamber (23) specifically onto the micro-drop collision point (11) or onto one of the micro-drop rows (5, 6) or fluid jets, said electron beam electrically neutralizing the positively charged ions in the collision point (11). Nuclear fusion reactor with a reactor chamber according to Patent claim 99 , characterized in that it is equipped with deflection coils or ring electromagnets (71) for controlling the spatial propagation or the geometric design of the electron beam. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that a micro-precision actuator system which can adjust the distance between the two open ends / outlets or nozzles from very small in the millimeter range to large in the decimetre range, always aiming at the collision point with the two longitudinal axes of the capillary high-pressure chamber, is installed in the reactor chamber. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the open ends / outlets or nozzles are each equipped with a disc-shaped electrode or a ring electrode which is electrically coupled to the open ends / outlets or nozzles and is electrically charged in the same way as the respective open end / outlet or nozzle. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 89 until 102 , characterized in that the control is designed in such a way that it supplies the electrodes and the open ends / outputs or nozzles simultaneously with pulse voltage via built-in high-voltage sources. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 89 until 102 , characterized in that the control is designed in such a way that it supplies 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 Patent claims 89 until 102 , characterized in that the control is designed in such a way that it supplies the electrodes and the nozzles alternately on each side with pulsed voltage via built-in high-voltage sources. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the Fluid accelerator system additionally or exclusively equipped with electromagnetic or magnetostrictive or piezo drive elements that cause a pulsed hydraulic pressure on the fluid and a generation of micro-droplets from the open ends / outlets or nozzles. Nuclear fusion reactor with a reactor chamber according to 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 collision point. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 99 until 107 , characterized in that it is equipped with deflection coils or electromagnets for controlling the spatial propagation or the geometry of the electron beam. Nuclear fusion reactor with a reactor chamber, characterized in that it consists of at least - one storage tank (27) filled with a non-compressible fluid (106) made of fusion-capable material, - two very sturdily constructed and solid-walled high-pressure chambers (24, 25, 63), each having a very small volume in the picoliter to nanoliter range or between 1 nm ³ and 1 µm ³ , into each of which a micro-droplet of non-compressible, fusion-capable liquid fits, - two opposing nozzles (3, 4), each coupled to the high-pressure chambers, - one capillary fluid line (29) each with an injection device (28) and associated valve control, which directs the fluid into the high-pressure chambers in very small, portioned amounts and completely fills them, - two Fluid accelerators or micro-drop acceleration systems that are installed in the high-pressure chambers (24, 25, 63) and consist of one or more pressure generators that accelerate the fluid from the high-pressure chamber in small portioned quantities, in the form of two micro-drops (2) each or one fluid jet formation (5, 6) each consisting of individual, separate micro-drops, via opposing nozzles (3, 4) to several km/s simultaneously against each other from a short distance to a collision point (11), - two electrically expandable or deformable elements that are components of the fluid accelerators, which are in direct or indirect contact with the fluid, which can deform or expand in one direction in a flash due to electrical voltage or electric current during the power supply and thereby generate short pressure pulses on the fluid in the high-pressure chamber and each displace a micro-drop from it at high speed, - a control that controls the elements in the fluid accelerators so that they generate high pressure values simultaneously in pulses and the micro-droplets with an adjustable number per unit of time and waiting times between the generation of the individual micro-droplets, individually or one behind the other in a line, emerging from both nozzles at the same time, whereby the micro-droplets of one nozzle meet micro-droplets of the other nozzle head-on at a collision point, - an energy dissipation system that dissipates the excess thermal or directly electrical energy from the nuclear fusion processes and the electrical charges generated there through ionization processes. Nuclear fusion reactor with a reactor chamber, characterized in that it consists of at least - one storage tank (27) filled with a non-compressible fluid made of fusion-capable material, - a stable high-pressure chamber (24, 25, 63), - two nozzles (3, 4) directed towards one another, which are coupled to the high-pressure chamber, - a capillary fluid line (29) with a valve control, which directs the fluid into the high-pressure chamber in very small, portioned quantities, - a fluid accelerator or micro-droplet acceleration system, which is installed in the high-pressure chamber and consists of one or more pressure generators, which accelerate the fluid from the high-pressure chamber in small, portioned quantities, in the form of two micro-droplets (2) each or one fluid jet formation (5, 6) each consisting of individual, separate micro-droplets, via nozzles to several km/s simultaneously against one another from a short distance to a collision point, - an electrically Expandable or deformable element which is a component of the fluid accelerator, which is in direct or indirect contact with the fluid, which can be deformed or expanded in one direction by electrical voltage or electrical current during the power supply and thereby generates short pressure pulses on the fluid, - a control which controls the element in the fluid accelerator in such a way that it generates high pressure values in pulses and the micro-droplets with an adjustable number per unit of time and waiting times between the generation of the individual Micro-droplets, individually or arranged in a line behind one another, emerge from both nozzles simultaneously, with the micro-droplets of one nozzle colliding head-on with the micro-droplets of the other nozzle at a collision point - an energy dissipation system that dissipates the excess energy from the nuclear fusion process. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that a low pressure or high vacuum prevails in the reactor chamber. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the capillary high-pressure chamber is constructed in the form of a very small-sized hollow cylinder and an electrically expandable or deformable element is installed therein, which generates a high pressure briefly in the capillary high-pressure chamber simultaneously with the molecular expansion process by molecular self-rotation and electromagnetic radiation and thereby supports the micro-droplet output and their acceleration via the two oppositely directed open ends / exits or nozzles. Nuclear fusion reactor with a reactor chamber according to Patent claim 112 , characterized in that the electrically deformable element is a piezo element or piezo actuator (7, 45). Nuclear fusion reactor with a reactor chamber according to Patent claim 112 or 113 , characterized in that the electrically stretchable or deformable element can be operated electrically at high frequency up to a maximum of 22 GHz or with pulse currents with high repetition rates synchronously with the molecular self-rotation generated by electromagnetic radiation. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 112 until 114 , characterized in that the repetition rates and / or the frequency are adjustable. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 112 until 115 , characterized in that the electrically stretchable or deformable element is deformable with very small amplitudes of less than 100 micrometers. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it is equipped with a capacitor energy converter system which converts the fusion energy directly into electrical current as a power output in a current output via ionization of the fusion material after the nuclear fusion of the atoms. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it is equipped with a high-resolution, high-speed camera which is installed in the reactor chamber and via which the processes in the reactor can be monitored. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the capillary high-pressure chamber is always under pressure which is lower than the pressure necessary for the generation of the micro-droplets, regardless of the inactivity of the fluid accelerator. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it has an ion beam source which emits a sharp ion beam at the collision point at right angles to a micro-droplet movement axis. Nuclear fusion reactor with a reactor chamber according to Patent claim 120 , characterized in that the ion beam (48) is electrically connected as a current-conducting line or as a virtual electrode (47) or serves as a virtual electrode. Nuclear fusion reactor with a reactor chamber according to Patent claim 121 , characterized in that a sharp and point-focused laser beam from a built-in laser beam source is provided as the current conductor or as the virtual electrode. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the paths of the micro-droplets in a row in fluid jet formation meet at an angle which is less than 180°, crossing one another at the collision point. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 90 until 123 , characterized in that a high voltage source is electrically coupled to the two nozzle electrodes via one electrical pole and to the ion beam via the other electrical pole via an additional electrode and a Voltage discharge between the ion beam and the nozzle electrodes, the polarity of which is designed to accelerate the micro-droplets from the two nozzles to a collision point. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 90 until 124 , characterized in that it is equipped with two ring electrodes (15, 16), each under high voltage from two separate voltage sources, each on the other side of the collision point with the centers of their central openings in the way of the respective fluid jet formation of the opposite nozzle, whereby the micro-droplets that are arranged in a row in the fluid jet formations that pass the collision point without collision pass through the respective central opening of the ring electrodes for each fluid jet formation, wherein each ring electrode is electrically coupled to the opposite nozzle or nozzle electrode, whereby a voltage discharge, controlled by the controller, rapidly alternating per fluid jet formation takes place between the ring electrode and the opposite nozzle or nozzle electrode through the affected fluid jet formation, wherein the current direction through the fluid jet formations is such that it accelerates the micro-droplets within each fluid jet formation towards the collision point. is. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that a small amount of liquid deuterium or other fusible material is filled into the reactor chamber, which collects the micro-droplets that pass the collision point without collision. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that - the reactor chamber is hollow spherical or hollow cylindrical, - is equipped with an electric drive which sets it in rotation, - is partially filled with a fusion-capable fluid which is radially distributed by centrifugal force on its hollow sphere wall, on which the micro-droplets which have not collided with each other hit and whose kinetic energy is either absorbed or partly leads to nuclear fusion with the fluid again. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it has, for additional acceleration of the micro-droplets, two laser sources which are directed towards each other and whose bundled beams hit the micro-droplets from behind, immediately after they emerge from the open ends / exits or nozzles or already in the capillary high-pressure chamber up to the collision point with laser beams. Nuclear fusion reactor with a reactor chamber according to Patent claim 128 , characterized in that it has a control which switches the laser sources on and off alternately at a very high repetition rate. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the repetition rate of the micro-droplet generation and their firing against each other is so high that the following micro-droplet comes within 32,000 to 1.2 micrometers of the preceding micro-droplet, which collides with the other micro-droplets at the collision point and begins to fuse, at the time the fusion process begins. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fluid is water or heavy or superheavy water or a mixture of liquids containing fusible elements. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it is equipped with electrostatic fields by additionally installed electrodes and high voltage sources, which orient the molecules of both micro-droplets, as they travel towards the collision point, by means of the electric field, the positively charged atoms in the molecules from both of the simultaneously released micro-droplets each forward in the direction of flight towards the collision point. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fusion-capable fluid is provided with a small amount of surfactants as an additive. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that an additive which transforms the fusion-capable fluid into an electrically conductive electrolyte is added to the fluid. Nuclear fusion reactor with a reactor chamber according to Patent claim 134 , through this characterized in that the additive is a salt, acid or base. Nuclear fusion reactor with a reactor chamber according to Patent claim 134 or 135 , characterized in that in each case an electrical circuit is constructed from at least one high-voltage source from the outlet of the capillary high-pressure chamber to an electrode or ring electrode which is installed behind the collision point and into whose ring opening the micro-droplets pass, which forms a current node from both circuits of both formations in the collision point, wherein the two current flows of the charge carriers in the micro-droplet formations are directed against each other and alternately accelerate the charge carriers to the collision point. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 134 until 136 , characterized in that it has a control which switches the high-voltage electrical source on and off alternately and in a current direction-changing manner for each micro-droplet formation. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 134 until 137 , characterized in that it comprises two galvanically isolated high-voltage sources (130, 131), each of which conducts an electric current through micro-droplet formations, the current directions of which are controlled in such a way that the charge carriers with fusion-capable atoms are electrically accelerated against each other at the collision point. Nuclear fusion reactor with a reactor chamber according to Patent claim 137 or 138 , characterized in that the control switches the two electrical high-voltage sources (130, 131) on and off alternately and in a current-direction-reversing manner for each micro-droplet formation, so that current never flows through both micro-droplet formations at the same time or they are under voltage ( 45 , 46 , 47 ). Nuclear fusion reactor with a reactor chamber according to Patent claim 139 , characterized in that the repetition rate of the alternating current switching on and off in the micro-droplet formations is very high. Nuclear fusion reactor with a reactor chamber according to Patent claim 139 or 140 , characterized in that the repetition rate of the alternating current switching on and off or current direction change processes can be adjusted for the micro-droplet formations. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it is equipped with electromagnetic or magnetic fields by additionally installed electromagnets (71) or strong permanent magnets (72), which orient the fluid molecules of both micro-droplets, while they are still traveling inside the micro-droplets in the direction of the collision point, through the magnetic field, with the positively charged atoms each pointing forward in the direction of flight. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it is equipped with a microwave radiation source which sends highly concentrated microwave beams (75) with a beam width of at least two millimeters directly onto the collision point (11) of the micro-droplets (2) perpendicular to the axis of movement (9) of the micro-droplets, which reaches the molecules of both micro-droplets while they are traveling inside the micro-droplets to the collision point, at least one millimeter before the collision, a magnetic field generated by the microwaves which sets the molecules into synchronous rotation so that they align themselves with the positively charged atoms pointing forward in the direction of the collision point. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 1 until 142 , characterized in that it is equipped with two microwave radiation sources (73, 74), which radiate in parallel, each emitting a highly concentrated microwave beam, phase-inverted to one another, with a beam width of at least 500µm on both sides immediately in front of the collision point of the micro-droplets perpendicular to the axis of movement of the micro-droplets, which reaches the fluid molecules of both colliding micro-droplets while they travel inside the micro-droplets to the collision point, at least 500µm in front of the collision point, magnetic fields generated by the microwaves, each of which has an amplitude and phase such that they set the molecules into rotation so that they orient themselves with the positively charged atoms pointing forward in the direction of the collision point. Nuclear fusion reactor with a reactor chamber according to Patent claim 144 , characterized in that the two microwave beams bring the molecules of both colliding micro-droplets into the same direction of rotation and have an electronic control which aligns the molecules of both micro-droplets exactly at the collision point, with the positively charged atoms arranged on the front side in the direction of flight. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the control has an electronic adjustment circuit which aims at a repetition rate and speed of the micro-droplets which result in a distance of at least half the micro-droplet diameter between the micro-droplets released one after the other. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it is equipped with at least one electric field source or radiation source which generates electric fields in the gigahertz to terahertz range which act on the micro-droplets immediately after they have left the nozzles and thereby increase the number of free electrons in the micro-droplets. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it has a star-shaped arrangement of the capillary high-pressure chamber / launch tube, which release micro-droplets simultaneously or at different collision points. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that solid components of nuclear fusion-capable material in fine-grain or nanopowder form are added to the fluid. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that instead of nuclear fusion-capable fluid, water is located in the high-pressure chamber / capillary high-pressure chamber, to which components of the nuclear fusion-capable material made of material in the solid state in fine-grain form or nanopowder form or nuclear fusion-capable material dissolved in water are added. Nuclear fusion reactor with a reactor chamber according to Patent claim 150 , characterized in that the water is used as a drive element or drive medium for the acceleration of a fusible material added therein. Nuclear fusion reactor with a reactor chamber according to Patent claim 150 or 151 , characterized in that the material in nanopowder form is boron or a chemical boron compound. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that an electrical accelerator is installed which accelerates the micro-droplets against each other by means of electrical fields. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the micro-droplets are sent towards each other in the form of two thin fluid jet formations whose jet axes lie on a common line. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 1 until 153 , characterized in that the micro-droplets are sent towards each other in the form of two fluid jet formations whose jet axes intersect at one point. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 153 until 155 , characterized in that the electrical accelerator consists of at least one high-voltage source and two electrodes for each micro-droplet formation, which are switched on and off alternately and in pairs per micro-droplet formation. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 153 until 156 , characterized in that the alternating switching on and off at high frequency or high repetition rate is controlled by a built-in electronic control. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the microwave radiation source is a MASER device. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 1 until 157 , characterized in that the microwave radiation source is a gyrotron device. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the microwave radiation source has at least one built-in Gunn element or at least one Gunn diode. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the capillary high-pressure chamber is provided with at least one Microwave window (125) which directs the microwaves to the fusible fluid. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the capillary high-pressure chamber is equipped with at least one microwave mirror which forms part of the wall of the capillary high-pressure chamber and which reflects the microwaves again to form a fusion-capable fluid. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that a microwave source is installed which generates a standing microwave radiation in the capillary high-pressure chambers, which causes an orientation of the dipole molecules of the fluid which causes a maximum contraction of the entire length of the fluid in the capillary high-pressure chambers, wherein an electromagnet is arranged such that when switched on it rotates the dipole molecules and causes the entire fluid mass in the capillary high-pressure chambers to expand. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the microwaves can be focused onto the fluid by built-in beam deflection elements. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the microwave energy is emitted directly or via beam deflection elements with sufficient intensity and radiation density to cause a synchronous rotation of the dipole molecules of the fluid in the capillary high-pressure chamber by at least 21°. Nuclear fusion reactor with a reactor chamber according to Patent claim 165 , characterized in that the beam deflection elements consist of movable microwave mirror parts and actuators which carry out the movements of the microwave mirror parts via a built-in control. Nuclear fusion reactor with a reactor chamber according to Patent claim 165 or 166 , characterized in that the beam deflection elements consist of micromirror chips. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the microwave radiation source is installed so as to be tiltable or rotatable about an axis. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that , together with the microwave source, at least one laser beam source is installed, which is used to rotate or ionize the dipole molecules of the fusion-capable fluid. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 1 until 168 , characterized in that instead of the microwave source, at least one laser beam source is installed, which is used to rotate the dipole molecules of the fusible fluid. Nuclear fusion reactor with a reactor chamber according to Patent claim 169 or 170 , characterized in that the laser beam source is an infrared or UV laser beam source. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 169 until 171 , characterized in that the laser beam source is equipped with beam deflection elements which generate a beam focus on the fusible fluid. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 169 until 172 , characterized in that the laser beam source is installed so as to be tiltable or rotatable about an axis. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the radiation angle of the microwave radiation source or the laser radiation source to the longitudinal axis of the capillary high-pressure chamber can be adjusted by built-in actuators and an actuator control. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the radiation angle of the microwave radiation source or the laser radiation source to the longitudinal axis of the capillary high-pressure chamber is less than 90°. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 99 until 175 , characterized in that the laser beam source is a semiconductor laser beam source that generates X-ray laser beams. Nuclear fusion reactor with a reactor chamber, characterized in that it comprises a fluid accelerator system or a micro-droplet Acceleration system comprising at least - two solid block units constructed from stable material, - two fine bores or two capillary high-pressure chambers (80), each installed in the two block units, the interiors of which are designed in the form of very narrow hollow cylinders or like the interiors of capillary tubes, the material mass of which forms the stable walls of the capillary high-pressure chambers, which are filled with small amounts of incompressible, fusible fluid with dipole properties, which are closed at one end and open at the other end/outlet and are arranged at a short distance from the open ends/outlets, linearly or on a longitudinal axis line (82) or slightly angled line, directed towards each other at a meeting point, - a high-voltage source coupled to two electrodes, each installed at the closed ends of the two capillary high-pressure chambers (80), - another high-voltage source coupled to two or four electrodes, can build up electric fields and whose field vectors are aligned perpendicular to the capillary high-pressure chambers, - an electronic control system that controls the two high-voltage sources in such a way that they build up short, rapidly repeating, very intense electric fields that run through the fluid of the two capillary high-pressure chambers, which expand and contract the fluid in the capillary high-pressure chambers by orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions, whereby when the expansion direction coincides with the line or longitudinal axis of the capillary high-pressure chamber, the pressure generated in the two capillary high-pressure chambers, which is caused by the sum of all expansion vector directions of the fluid molecules located there, accelerates a micro-droplet each, which collide with each other in the middle of the path on a micro-droplet axis and partly lead to nuclear fusion, - a fluid injector (28) that injects very small amounts of the Fluid in both capillary high-pressure chambers after each generation of micro-droplets via the same opening through which micro-droplets are ejected or through a separate channel each in the capillary high-pressure chambers, - an energy dissipation system that dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber, characterized in that it has a fluid accelerator system or a micro-droplet acceleration system, which consists of at least - two solid block units constructed of stable material, - two fine bores or two capillary high-pressure chambers (80), each installed in the two block units, the interiors of which are designed in the form of very narrow hollow cylinders or like the interiors of capillary tubes, the material mass of which forms the stable walls of the capillary high-pressure chambers, which are filled with small amounts of incompressible, fusion-capable fluid with dipole properties, which are closed at one end and open at the other end / exit and are arranged at a short distance with the open ends / exits linearly or on a longitudinal axis line (82) or slightly angled line, directed towards each other at a meeting point, - a power source coupled to a C-shaped electromagnet whose magnetic poles are respectively installed at the closed ends of the two capillary high-pressure chambers (80), - a further power source which is coupled to a further C-shaped electromagnet, whose magnetic poles can build up magnetic fields whose field vectors are aligned perpendicular to the longitudinal axes of the capillary high-pressure chambers, - an electronic control which controls the two power sources in such a way that they build up short, rapidly repeating, very intense magnetic fields which run through the fluid of the two capillary high-pressure chambers, which expand and contract the fluid in the capillary high-pressure chambers by orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions, whereby each time an agreement of the expansion direction with the line or longitudinal axis line of the capillary high-pressure chamber is reached, the pressure generated in the two capillary high-pressure chambers, which is determined by the sum of all expansion vector directions of the there located fluid molecules, accelerates a micro-droplet at a time, which collide with each other in the middle of the track on a micro-droplet axis and partly lead to nuclear fusion, - a fluid injector (28) which injects very small amounts of the fluid into both capillary high-pressure chambers after each generation of micro-droplets via the same opening through which the micro-droplets are ejected or through a separate channel in each of the capillary high-pressure chambers, - an energy dissipation system which dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber, characterized in that it comprises a fluid accelerator system or a micro-droplet acceleration system, which consists of at least - a container (139) filled with fusion-capable fluid, - a massive block unit made of stable material, - a fine bore or a capillary high-pressure chamber (80), built into the block unit, the interiors of which are designed in the form of very narrow hollow cylinders or like the interiors of capillary tubes, the material mass of which forms the stable walls of the capillary high-pressure chambers, which is filled with small amounts of incompressible, fusion-capable fluid with dipole properties, which is closed at one end and open at the other end / exit, directed towards a meeting point on the fluid of the container, - a power source coupled to a C-shaped or ring-shaped electromagnet, the magnetic poles of which are respectively at the closed ends of the two Capillary high-pressure chambers (80) are installed, - a further power source which is coupled to a further C-shaped electromagnet, the magnetic poles of which can build up magnetic fields whose field vectors are aligned perpendicular to the longitudinal axes of the capillary high-pressure chambers, - an electronic control which controls the two power sources in such a way that they build up short, rapidly repeating, very intense magnetic fields which run through the fluid of the capillary high-pressure chamber, which expands and contracts the fluid in the capillary high-pressure chamber by orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions, whereby each time an agreement of the expansion direction with the line or longitudinal axis line of the capillary high-pressure chamber is reached, the generated pressure in the capillary high-pressure chamber, which is caused by the sum of all expansion vector directions of the fluid molecules located there, accelerates a micro-droplet which on the Fluid of the container, collides and partly leads to nuclear fusion, - a fluid injector (28) which injects very small amounts of the fluid into the capillary high-pressure chamber after each generation of micro-droplets via the same opening through which micro-droplets are ejected or through a separate channel in each case, - an energy dissipation system which dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber, characterized in that it has a fluid accelerator system or a micro-drop acceleration system, comprising - a storage container (146) filled with fusion-capable fluid, - a nozzle (144) or cannula that allows the fluid to fall in the form of liquid drops (140), - a solid block unit made of stable material, - a fine bore or a capillary high-pressure chamber (80), built into the block unit, the interior of which is designed in the form of a narrow hollow cylinder or like the interior of capillary tubes, the material mass of which forms the stable walls of the capillary high-pressure chamber, which is filled with small amounts of incompressible, fusion-capable fluid with dipole properties, which is closed at one end and open at the other end / exit, directed towards a meeting point with the falling liquid drops, - a power source that is connected to a C-shaped electromagnet, the magnetic poles of which are each installed at the closed ends of the two capillary high-pressure chambers (80), - a further power source which is coupled to a further C-shaped electromagnet, the magnetic poles of which can build up magnetic fields whose field vectors are aligned perpendicular to the longitudinal axes of the capillary high-pressure chambers, - an electronic control which controls the two power sources in such a way that they build up short, rapidly repeating, very intense magnetic fields which run through the fluid of the capillary high-pressure chamber, which expands and contracts the fluid in the capillary high-pressure chamber by orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions, whereby each time a coincidence of the expansion direction with the line or longitudinal axis line of the capillary high-pressure chamber is reached, the generated pressure in the capillary high-pressure chamber, which is determined by the sum of all Expansion vector directions of the fluid molecules located there, accelerates a micro-droplet, which, aiming at the falling liquid droplet, collides and partly leads to nuclear fusion, - a fluid injector (28), which injects very small amounts of the fluid into the capillary high-pressure chamber after each generation of micro-droplets via the same opening through which the micro-droplets are ejected or through a separate channel, - an energy dissipation system, which dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber, according to Patent claim 180 , characterized in that instead of the liquid-drop fens, frozen material in the form of ice spheres is released to collide with the micro-droplets. Nuclear fusion reactor with a reactor chamber, characterized in that it has a fluid accelerator system or a micro-droplet acceleration system, comprising - a storage container (146) filled with fusion-capable fluid, - a nozzle (144) or cannula that delivers the fluid in the form of a liquid jet (143) through a pressure generator or a high-pressure pump, - a solid block unit made of stable material, - a fine bore or a capillary high-pressure chamber (80), built into the block unit, the interior of which is designed in the form of a narrow hollow cylinder or like the interior of capillary tubes, the material mass of which forms the stable walls of the capillary high-pressure chamber, which is filled with small amounts of incompressible, fusion-capable fluid with dipole properties, which is closed at one end and open at the other end / exit, directed towards a meeting point with the liquid jet, - a A power source coupled to a C-shaped electromagnet, the magnetic poles of which are each installed at the closed ends of the two capillary high-pressure chambers (80), - a further power source coupled to a further C-shaped electromagnet, the magnetic poles of which can generate magnetic fields whose field vectors are aligned perpendicular to the longitudinal axis of the capillary high-pressure chamber, - an electronic control which controls the two power sources in such a way that they generate short, rapidly repeating, very intense magnetic fields which run through the fluid of the capillary high-pressure chamber, which expands and contracts the fluid in the capillary high-pressure chamber by orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions, whereby each time the expansion direction coincides with the line or longitudinal axis line of the capillary high-pressure chamber, the pressure generated in the capillary high-pressure chamber, which is determined by the sum of all Expansion vector directions of the fluid molecules located there, accelerates a micro-droplet, which, aiming at the liquid jet (143), collides and partly leads to nuclear fusion, - a fluid injector (28), which injects very small amounts of the fluid into the capillary high-pressure chamber after each generation of micro-droplets via the same opening through which the micro-droplets are ejected or through a separate channel, - an energy dissipation system, which dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber according to Patent claim 181 , characterized in that the arrangement of the micro-drop flight line and the liquid jet is designed such that they meet at an angle. Nuclear fusion reactor with a reactor chamber according to Patent claim 182 or 183 , characterized in that it has an angular positioning system for an impact angle of the liquid jet and the micro-drops by means of built-in actuators, which can adjust the nozzle of the liquid jet in such a way that it can emit the liquid jet at any selectable angle crossing the flight line of the micro-drop. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 182 until 184 , characterized in that the angle of incidence corresponds to the polarization angle of the fusible liquid. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the fusion-capable liquid is degassed and has no dissolved gases or air bubbles. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 177 until 186 , characterized in that in order to accelerate the micro-droplets from the capillary high-pressure chamber, additionally or exclusively a microwave radiation source is installed, which directs a bundled microwave beam onto the fluid in the capillary high-pressure chamber, which causes a synchronous rotation of the dipole molecules of the fusible fluid and thereby a chain-like, pulsating contraction and expansion of the fluid mass in the longitudinal axis of the capillary high-pressure chamber, and at maximum expansion ejects a micro-droplet from the capillary high-pressure chamber outlet. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the capillary high-pressure chamber or capillary high-pressure chambers are made of ceramic or glass. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that a A control system is installed which, when the material of the high pressure capillary chambers expands, which, as a result of the extremely rapid fluid expansion due to the synchronous molecular rotation of the molecular dipoles and the generation of the micro-droplets, causes a delay with the next rotation of the dipole molecules and micro-droplet generation by at least a time that is required until the contraction of the material of the high pressure capillary chamber begins or is underway. Nuclear fusion reactor with a reactor chamber according to Patent claim 189 , characterized in that the synchronous, molecular rotation of the molecular dipoles and the generation of the micro-droplets, controlled by the controller, only takes place when the contraction of the material of the high-pressure capillary chamber begins or is in progress in an oscillation phase. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that it is equipped with a vibration system consisting of at least - a sound or ultrasound source that causes the structure or the walls of the capillary high-pressure chamber to vibrate, - a control that synchronizes the vibration frequency and the vibration phases with the times of generation of the micro-droplets Nuclear fusion reactor with a reactor chamber according to Patent claim 191 , characterized in that the control is designed in such a way that acceleration and generation of the micro-droplets by rotation of the dipole molecules takes place synchronized with the oscillation phases of the construction of the capillary high-pressure chamber. Nuclear fusion reactor with a reactor chamber according to Patent claim 191 or 192 , characterized in that the acceleration and generation of the micro-droplets by rotation of the dipole molecules by the control is designed in such a way that they are started exactly at the time of the oscillation phases in which the contraction of the structure of the capillary high-pressure chamber takes place. Nuclear fusion reactor with a reactor chamber according to one of the preceding claims, characterized in that the capillary high-pressure chamber or capillary high-pressure chambers are equipped or coupled with at least - a sound or ultrasound source which causes their structure or their walls to oscillate, - a control which synchronises the oscillation frequency and the oscillation phases with the times of generation of the micro-droplets in such a way that only in the oscillation phases, while the structure of the high-pressure capillary chamber is contracting, is a pressure increase initiated by rotation of the dipole molecules of the fluid mass in the high-pressure capillary chamber. A nuclear fusion reactor with a reactor chamber, characterized in that it has a fluid accelerator system or a micro-droplet acceleration system, comprising - a fluid dispenser (180) filled with a fusion-capable fluid (106), - a nozzle (144) or cannula that delivers the fluid in the form of a liquid jet (143) through a pressure generator or a high-pressure pump (147), - a solid block unit (121) constructed of stable material, - a fine bore or a capillary high-pressure chamber (80) installed in the block unit (121), the interior of which is designed in the form of a narrow hollow cylinder or like the interior of capillary tubes, the material mass of which forms the stable walls of a capillary high-pressure chamber (80) filled with small amounts of incompressible, fusion-capable fluid (106) with dipole properties, which is closed at one end (83) and open at the other end / outlet (84), is directed towards a meeting point with the liquid jet (143), - a power source coupled to a C-shaped electromagnet whose magnetic field lines run along the longitudinal axis (82) of the capillary high-pressure chamber (80), - another power source coupled to another C-shaped electromagnet whose magnetic poles can generate magnetic fields whose field vectors are perpendicular to the longitudinal axis (82) of the capillary high-pressure chamber, - an electronic control system that controls the two power sources in such a way that they generate short, rapidly repeating, very intense magnetic fields that run through the fluid of the capillary high-pressure chamber (80), which alternately expand the fluid into the capillary high-pressure chamber by orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions, and contracts, whereby when a maximum expansion is reached or the direction of expansion coincides with the line or longitudinal axis line (82) of the capillary high-pressure chamber, the pressure generated in the capillary high-pressure chamber, which is determined by the sum of all stretch vector directions of the fluid molecules located there, accelerates a micro-drop (2) which, aiming at the liquid jet (143), collides and partly leads to nuclear fusion, - a fluid injector (28) which injects very small amounts of fluid into the capillary high-pressure chamber after each generation of micro-drops via the same opening through which the micro-drops are ejected or through a separate channel, - an energy dissipation system which dissipates the excess energy to the outside. A nuclear fusion reactor with a reactor chamber, characterized in that it has a fluid accelerator system or a micro-droplet acceleration system, comprising - a fluid dispenser (180) filled with a fusion-capable fluid (106), - a nozzle (144) or cannula that delivers the fluid in the form of a liquid jet (143) through a pressure generator or a high-pressure pump (147), - a solid block unit (121) constructed of stable material, - a fine bore or a capillary high-pressure chamber (80) installed in the block unit (121), the interior of which is designed in the form of a narrow hollow cylinder or like the interior of capillary tubes, the material mass of which forms the stable walls of a capillary high-pressure chamber (80) filled with small amounts of incompressible, fusion-capable fluid (106) with dipole properties, which is closed at one end (83) and open at the other end / outlet (84), which is directed towards a meeting point with the liquid jet (143), - a microwave or laser radiation source, the radiation of which passes through the capillary high-pressure chamber (80) and the fluid therein, - an electronic control which controls the microwave / laser radiation source (78, 100) in such a way that it generates short, successively repeating, very intense beams / pulse beams which pass through the fluid of the capillary high-pressure chamber, which alternately expands and contracts the fluid in the capillary high-pressure chamber by orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions, whereby in each case upon reaching a maximum expansion or a coincidence of the expansion direction with the line or longitudinal axis line (82) of the capillary high-pressure chamber (80), the generated pressure in the capillary high-pressure chamber, which is generated by the The sum of all expansion vector directions of the fluid molecules present there is created, accelerates a micro-droplet (2) which, aiming at the liquid jet (143), collides and partly leads to nuclear fusion, - a fluid injector (28) which injects very small amounts of fluid into the capillary high-pressure chamber after each micro-droplet is generated via the same opening through which the micro-droplets are ejected or through a separate channel, - an energy dissipation system which dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber, characterized in that it has a fluid accelerator system, comprising - a fluid dispenser (180) filled with a fusion-capable fluid (106), - a nozzle (144) or cannula that delivers the fluid in the form of a liquid jet or a vapor jet through a pressure generator or a high-pressure pump (147), - a solid block unit (121) constructed of stable material, - a fine bore or a capillary high-pressure chamber (80), installed in the block unit (121), the interior spaces of which are designed in the form of a narrow hollow cylinder or like the interior spaces of capillary tubes, the material mass of which forms the stable walls of a capillary high-pressure chamber (80) filled with small amounts of incompressible, fusion-capable fluid (106) with dipole properties, which is closed at one end (83) and at the other end / outlet (84) is open, is directed towards a meeting point with the liquid jet (143) / vapor jet, - a microwave or laser radiation source, the radiation of which passes through the capillary high-pressure chamber (80) and the fluid located therein, - an electronic control which controls the microwave / laser radiation source (78, 100) in such a way that it generates short, successively repeating, very intense beams / pulse beams which pass through the fluid of the capillary high-pressure chamber, which expands the fluid into the capillary high-pressure chamber by orientation polarization or displacement polarization of the dipole molecules in rotating expansion vector directions and evaporates it in a flash, whereby each time the expansion direction coincides with the line or longitudinal axis line (82) of the capillary high-pressure chamber (80), the pressure generated in the capillary high-pressure chamber, which is determined by the sum of all expansion vector directions of the fluid located there Fluid molecules are formed, a number of atoms or a group of atoms / atom groups are accelerated, which, aiming at the liquid jet (143) or steam jet, collide and partly lead to nuclear fusion, - a fluid injector (28), which injects very small amounts of the fluid into the capillary high-pressure chamber after each acceleration process of the atom groups through the same opening through which micro-drops are ejected or through one separate channel into the capillary high-pressure chamber - an energy dissipation system that dissipates the excess energy to the outside. Nuclear fusion reactor with a reactor chamber according to Patent claim 196 or 197 , characterized in that the laser beam source is an infrared or UV laser beam or X-ray laser beam source. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 196 until 198 , characterized in that the jets are delivered in a bundled manner onto the fluid in the capillary high-pressure chamber. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 196 until 199 , characterized in that the laser beam source is a laser pulse generator which emits powerful laser pulses/laser pulses in short periods of time. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 196 until 200 , characterized in that the laser radiation source is a femto laser device. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 196 until 201 , characterized in that the laser radiation source is designed to emit laser pulses with such a short duration and a high power that it does not allow time for evaporation of the fluid in the capillary high-pressure chamber. Nuclear fusion reactor with a reactor chamber according to one of the Patent claims 196 until 202 , characterized in that it is equipped with an alignment device which, with the aid of electromagnetic radiation or magnetic fields or electric fields, causes an alignment of the dipole molecules at the collision point, so that the fusion-capable atoms collide head-on with each other.

Images