DE102022002234A1 - Beam weapon - Google Patents

Abstract

The invention relates to a radiation weapon that is able to achieve a significantly higher energy output in the form of a destructive beam by fusing hydrogen isotopes with low energy input.
The weapon features a nuclear fusion reactor that is not used for power, but as a source of radiation energy generated in an unconventional way. Instead of plasma and associated magnetic field confinement measures, the reactor uses high-speed fluid jets whose kinetic energy is sufficient to enable the fusion of hydrogen isotopes with the support of strong electrostatic fields that ensure optimal orientation of the atoms in the collision point enable to achieve. The fusion reactor can be scaled as desired and can be used in all types of military vehicles (airplanes, tanks, ships, etc.) as well as a large system for city and facility defense. The weapon is able to generate a directed beam that is similarly destructive to the lightning radiation at the time of a nuclear weapon detonation.
The energy for the rays is generated from primary energy carriers that are abundant in nature.

Description

The invention relates to a radiation gun that can emit a focused, destructive directional beam with high intensity through nuclear fusion.

Intense IR, UV and other light rays that can be used to attack a target can produce laser beams. Powerful laser emitters that can attack targets at greater distances, e.g. several dozen km, are indeed feasible, but they consume enormous amounts of energy and are also bulky and large because they involve numerous accompanying elements. Powerful, active coolers are used to cool the laser emitter. The alignment devices are also included. Powerful laser devices are usually installed on warships because they have the carrying capacity, payload and infrastructure for laser operation. Strong power sources and other accompanying elements can be easily installed on a ship or are already present.

There are also other types of weapons that fall into the category of beam weapons. Microwave cannons are known that are capable of heating or even heating a person's skin when they are aimed at him. Such cannons were once used to drive away demonstrators.

Beam weapons can also work using ultrasound or sound waves. In certain versions even infra-sound waves are used.

Radiation weapons of any kind are not widely available. Despite advantages, they also come with many disadvantages. Most of the time they are bulky, large, fragile and use quite a lot of energy for what little they can do. Weapons supported by nuclear fusion do not yet exist. If nuclear fusion could be used as an energy source for this, they would be much more compact to build. Supported by nuclear fusion, one could very well create powerful and effective weapons. Although weapons are abhorred by many because they destroy lives, sometimes they are needed to defend democratic values and peaceful peoples against aggressive nations that do not value life and peace. Unfortunately, there will always be a few aggressive nations and peoples who will use war against others and that makes it necessary to be prepared for this.

Nuclear fusion, when mastered, provides almost unlimited amounts of energy that can also be used for weapon systems.

There is a lot, enormous amount of energy in every type of matter itself. No matter whether sand, rocks, wood, water, metal, air, earth, each of these materials contains an extremely high amount of energy. However, this does not (only) mean chemical energy. Actually, all matter is made of energy. Matter is a form of extremely concentrated energy. The energy in the form of photons, which is strongly concentrated, can form stable structures and keep them trapped there. If you destroy these structures, the energy is released in the form of photons. There are numerous ways to elicit energy from matter or to initiate these transformations. The most common and simplest methods are chemical in nature. In such processes, matter will simply enter into chemical reactions and form new chemical bonds or break them. The most common method of releasing energy is to burn matter. However, this only provides a very small proportion of the energy that would actually be available; on the other hand, the initial energy required to start this process is relatively low. In addition, this method only works with combustible substances, which form a fraction of the total matter on the earth's surface, for example.

Rather, energy can be gained or released through nuclear reactions. The nuclear energy production methods available to us are nuclear fission and nuclear fusion. There is a third option, annihilation, which is very difficult to implement because it requires antimatter, which can only be produced with extremely high energy expenditure. When a group of atoms made of antimatter and analogous matter collide, both groups of atoms are completely converted into energy and radiated away from the collision point in all directions at the speed of light.

Initiating nuclear fission is technically relatively easy these days. This method is also quite common in commercial nuclear reactors and is used for wide-scale power supply. Radioactive elements are enriched until they are suitable for an optimal nuclear reaction. The radioactive material is introduced into a reactor filled with heavy water in the form of elongated rods. Because uncontrolled nuclear fission would lead to an atomic explosion, cadmium grids or rods (or boric acid dissolved in the heavy water) are placed between the fissile radioactive material. The cadmium or graphite grids or rods determine the power of energy release or the speed at which nuclear fission occurs. Depending on how far they are inserted between the uranium (or plutonium) rods, the higher or lower the energy release. Every time a When an atom is split, it releases a neutron, which in turn destabilizes one of the atoms in the neighborhood by penetrating its nucleus. The cadmium rods are able to absorb free neutrons and therefore control the nuclear fission processes quite well. Nuclear reactors with graphite as a moderator are no longer used because they are not so easy to control. If the cooling in the reactor fails, a core meltdown can occur very quickly. In the event of a breakdown, the nuclear reaction increase can occur suddenly and should not be underestimated. It can increase thousands of times within a millisecond, which can lead to a violent explosion and thus contamination.

Fusion reactors should actually achieve better efficiency in terms of energy yield. Commonly known and existing fusion reactors are built in different versions. Toroidal reactors and tokamak machines are relatively well known.

However, such reactors have unfortunately been 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. While nuclear fusion works without any problems with a hydrogen bomb, the continuous, controlled yield of energy in nuclear fusion reactors is associated with many problems, the solution of which makes the process very expensive and therefore unattractive for industry. The fusion reactors require a lot of start-up energy, which must first be provided. In addition, today's reactors cannot run permanently or the processes there come to a standstill quite quickly and the energy yield is therefore relatively small. If you invest a few MW of energy in the start-up phase and then the process only runs for a few seconds or, in the best case, a few minutes, with only fractions of the invested energy being recovered, that is not a commercially interesting level of efficiency that is achieved. For such purposes, the reactor must be able to supply energy permanently and not only be in active operation for a few minutes or seconds every few resting hours or even days. Unfortunately, today's fusion reactors usually have a negative energy balance: more energy is put into them than is gained through the process. It is 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 combustion engine would not be sufficient to recharge it via the alternator.

Nuclear fusion is an energy-producing process that has been occurring in the sun and stars for billions of years. The fusion process takes place at extraordinarily high temperatures, at which the matter is in the fourth state of aggregation, the so-called plasma. A plasma consists of atomic nuclei (ions) and electrons that are no longer bound to each other.

Inside the sun, fusion reactions take place at around 15 million degrees. Under the conditions on Earth, the plasma is enclosed by strong magnetic fields at temperatures of over 100 million degrees and at extremely low density (approx. 250,000 times thinner than the Earth's atmosphere). What the magnetic fields try to achieve on Earth is not necessary on the stars. There the plasma is compressed very strongly by the unimaginably large star mass and the gravitational forces acting on this mass. The highly heated plasma that causes fusion is located primarily in a mantle, more or less close to the star's core, depending on the size of the star. The fusion does not take place in the core of the star, as previously assumed, but in a shell that is located between the core and the surface. If fusion only took place in the core, then all stars would be of similar size and there would be no very large or small stars. Each star has its nuclear fusion envelope at a different distance from the star center. The jacket is created where there is the balance between pressure and temperature that is necessary for hydrogen fusion. Further casings, arranged concentrically deeper, fuse other materials and elements. In the core of the star, the pressure is so high that the matter is very compressed, and the atomic structural integrity is no longer guaranteed. The neutrons that are supposed to keep fusion going are slowed down far too quickly and prematurely bound into heavy atomic structures. The situation is different in the star mantle layer, which is more or less distant from the core. The distance from the star's 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 shell does not always remain the same size. It changes size and shape as the star ages and can become unstable. It also plays a big role in supernova explosion. If the star becomes unstable, the first thing this mantle will do is rupture itself and the layers above it. Because the mantle also expands inward during the explosion, it compresses the star's matter toward the core. That's why after a supernova explosion, significantly smaller remains of the star remain back. Firstly, the material above the jacket is blasted away and secondly, the material underneath is largely strongly compressed by the increase in pressure.

As far as fusion is concerned, the situation on Earth is different. This does not occur naturally on earth. Here, engineers and scientists are trying to melt the light nuclei (preferably hydrogen isotopes) through strong heating and magnetic field confinement. A number of fusion reactions between light nuclei are conceivable. The first generation of future fusion power reactors will use the deuterium-tritium reaction, which offers a comparatively high fusion power density: the core of the heavy hydrogen deuterium (one proton, one neutron) fuses with the core of the superheavy hydrogen tritium (one proton, two neutrons ) to the helium-4 nucleus, the so-called particle (two protons, two neutrons) with the emission of a neutron. Approximately four times as much energy is released per nucleon as when a uranium nucleus splits. 80% of this energy is bound to the neutron, which, as a neutral particle, can leave the magnetic cage unhindered. By braking the neutrons in the structural material and in the jacket of the plasma chamber, the so-called blanket, heat is generated, which is converted into electricity via a conventional steam cycle. The particle transfers kinetic energy through interaction with plasma particles and thus contributes 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”.

The world's largest systems based on the tokamak principle today are the Joint Eruopean Torus (JET) in Culham / Great Britain and ITER (International Thermonuclear Experimental Reactor) in France, which has been under construction since 2007 and will be completed around May 2043. 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 now able to generate 17 MW of power for a short period of time, which corresponds to approximately 70% of the power used to heat the plasma. However, unfortunately it does not create a positive energy balance.

In parallel with the tokamak, which releases energy in long pulses, the “stellarator” line is being further developed, enabling continuous plasma operation. The Wendelstein 7X stellarator facility is currently being built in Greifswald under the direction of the Max Plank Institute for Plasma Physics.

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

A fusion reactor works with very small amounts of plasma, which consists of just 1g of hydrogen ions. The thermal energy of the hot 1g hydrogen plasma is enough to heat and melt 100kg of steel to 2000°C.

In order to be able to work with these high temperatures, the plasmas and their thermal radiation are captured in a vacuum using magnetic fields whose strength exceeds 100,000 times the earth's magnetic field. The extremely high temperature is necessary to compensate for the very low ion density (approx. 10 to the power of 14 ions/cm ³ ).

Most techniques involve high-energy neutrons. Since they cannot be forced onto a defined path by magnets, they hit the material surrounding the plasma and are responsible for its radiation. However, they are used to produce the most commonly needed tritium with lithium.

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

The method of generating magnetic confinement fusion is used in many fusion reactors and is carried out in closed vacuum chambers. The gas, consisting of hydrogen, deuterium or tritium or combinations of these substances, is heated in this chamber to 50 to 400 million degrees and is then present as plasma, i.e. the gas is completely ionized. Magnetic fields force the plasma onto a path that prevents the plasma from touching the wall. A touch would instantly cool the plasma and fusion would be interrupted. Thermonuclear burning ultimately occurs at high temperatures.

• Durch die Schwierigkeiten beim Plasma-Einschluss und durch Verunreinigungen kommt es zu Energieverlusten. Durch Neutronenbeschuss wird das Reaktormaterial radioaktiv. Die extremen Bedingungen führen zu hohe Materialermüdung und damit zu hohen Kosten. Große gespeicherte Energiemengen in den Magnetfeldern und radioaktives Inventar stellen ein Gefahrenpotential dar. Der hohe Energiebedarf beim Betrieb durch die benötigte Heizung und Magnete (ca. 300 MW, was der Verbrauch einer mittleren Großstadt entspricht) rechtfertigt nicht mal Wiederholungen von solchen Versuche.

In general, the following problems arise with magnetic inclusion:

• Difficulties in plasma confinement and impurities lead to energy losses. The reactor material becomes radioactive through neutron bombardment. The extreme conditions lead to high material fatigue and therefore high costs. Large amounts of energy stored in the magnetic fields and radioactive inventory represent a potential danger. The high energy requirement for operation due to the required heating and magnets (approx. 300 MW, which corresponds to the consumption of a medium-sized city) does not even justify repeating such experiments.

• - Stelleratoren
  • Hier ist das Reaktorgefäß ähnlich wie beim Tokamak eine ringförmige Röhre, also ein Torus. Das Plasma fließt hier im Kreis, wobei es durch geeignete Magnetfelder in sich verwunden wird, um Abstrahlungsverluste zu minimieren. Diese zusätzlichen Magnetfelder verkomplizieren die Technik des Reaktors. Auch erreicht man derzeit nicht den gewünschten Einschlussgrad, was den Produkt aus Druck mal Zeit entspricht. Der Stellerator ist aber für die Konstruktion eines energieliefernden Reaktors dadurch sehr interessant, da er sich zum kontinuierlichen Betrieb eignet.
• - Tokamak
  • Tokamak ist eine Abkürzung für die Russische Bezeichnung von Toroidkammer im Magnetfeld. Beim Tokamak handelt es sich um einen Torus, in dem das Plasma im Kreis fliesst. Über äußere Spulen wird ähnlich wie bei einem Transformator ein Strom im Plasma induziert. Durch diesen Strom werden die Abstrahlungsverluste minimiert, so dass kein Magnetfeld für die Verwindung des Plasmas notwendig wird. Zusätzlich stellt der Strom im Plasma eine Heizmethode dar. Mit den Tokamaks ist man den Bedingungen für selbsterhaltendes thermonukleares Brennen bisher am nächsten gekommen, was vielleicht aber auch daran liegt, dass hier die intensivsten Forschungen getätigt werden. Als Hauptnachteil des Tokamak ist zu nennen, dass er sich nicht für einen kontinuierlichen Betrieb eignet, sondern regelmäßig wieder neu mit Plasma aufgeladen werden muss, was auch eine extreme Belastung der Anlage ausmacht.
• - Spiegelmaschinen
  • Das Reaktorgefäß bildet eine gerade Röhre. An den Enden wird das Plasma durch entsprechende Magnetfelder in seiner Flussrichtung reflektiert. Bei der Reflexion an dem Ende kommt es zu erhöhten Energieverlusten.
• - MIGMA-Konzept
  • Bei dem MIGMA-Verfahren werden aus einem Teilchenbeschleuniger Teilchen (z.B. Deuteronen und Trionen) wiederholt zur Kollision gebracht und verschmelzen. Es ist mit diesem Konzept auch eine Fusion zwischen Protonen und dem Bor-11 Isotops möglich. Es entstehen vier energiereiche Alphateilchen (4He2+). Das besondere an diesem Ansatz ist, dass kein radioaktives und toxisches Tritium benötigt wird und keine Neutronen entstehen, welche für die unerwünschte Radioaktivität verantwortlich sind. Hauptproblem bei dieser Technik sind laut KfK die Energieverluste der Teilchen durch die entstehende Synchrotronstrahlung. Leider wird diese von einigen Physikern für genial gehaltene Technik weltweit ignoriert. Es werden zur Weiterentwicklung trotz ansehnlicher Anfangserfolge in den 70 Jahren nicht genügend Fördermittel zur Verfügung gestellt. Grund hierfür könnte sein, dass bei dieser Reaktion keine energiereichen Neutronen entstehen, die zu dem sehr interessanten Nebenprodukt, dem spaltbaren Material, führen.
• - Induzierte Trägheitsfusion
  • Ein Gemisch aus Deuterium und Tritium wird von einer kleinen kugelförmigen Hülle umgeben. Diese 1mm großen Kügelchen (Pellets) werden im Vakuum mit einem Hochenergielaser oder einem Leicht- oder Schwerionenstrahl beschossen. Bei der so herbeigeführten Implosion wird das Wasserstoffgemisch auf ein fünfzigstel seines Volumens komprimiert. Die extreme Erhitzung lässt das fusionierende Plasma entstehen. Durch Simulationen ließ sich ermitteln, dass der thermonukleare Energieausstoß typischerweise das Hundertfache der Laserenergie beträgt. Hauptproblem ist die Konstruktion der benötigten kurzwelligen Hochenergielaser bzw. Beschleuniger. Des Weiteren entstehen auch hier hochenergetische Neutronen. Die Konstruktion eines energiegewinnenden Reaktors, der z.B. zehn Pellets pro Sekunde zünden würde, wäre denkbar.
• - Kalte Kernfusion
  • Die Reaktion wurde aus theoretischen Überlegungen schon in den vierziger Jahren von F. Frank und Andrej D. Sacharov vorhergesagt und 10 Jahre später durch einen Zufall von Luis W. Alvarez experimentell „nachgewiesen“. Bei der kalten Kernfusion oder auch Myon -katalysierten kalten Kernfusion kann man die hohen Temperaturen und riesigen Versuchsaufbauten umgehen. Die kalte Kernfusion läuft bei Temperaturen ab 13 bis über 1000 Kelvin in festen, flüssigen oder gasförmigen Medien ab. Die Reaktion kann in einer einfachen mit Tritium und Deuterium gefüllten Kammer durchgeführt werden. Hierzu lässt man negative Myonen in die Kammer eindringen. Die Myonen stellen durch besondere Stoßprozesse enge Bindungen zwischen den Wasserstoffmolekülen her. Die so myonisch gebundenen Kerne verschmelzen und es wird Energie in Form von Wärme frei. Die Myonen werden dabei wieder freigesetzt und können unter bestimmten Bedingungen weitere Fusionen katalysieren. Myonen kann man künstlich mit Hilfe von Teilchenbeschleunigern erzeugen. Damit ein Myon mehrere Kernfusionen katalysieren kann, sind hohe Energien für dessen Erzeugung notwendig. Soweit die Theorie. Eine Umsetzung in der Praxis ist jedoch bis heute noch nicht erfolgreich absolviert worden und es gibt zumindest keine wirtschaftlich funktionierenden Reaktoren.

When it comes to magnetic confinement, it is important to distinguish between three reactor types:

• - Stellerators
  • Here, the reactor vessel, similar to the tokamak, is a ring-shaped tube, i.e. a torus. The plasma flows in a circle, being twisted by suitable magnetic fields in order to minimize radiation losses. These additional magnetic fields complicate the reactor's technology. The desired degree of inclusion, which corresponds to the product of pressure times time, is currently not achieved. However, the actuator is very interesting for the construction of an energy-supplying reactor because it is suitable for continuous operation.
• - Tokamak
  • Tokamak is an abbreviation for the Russian name for toroid chamber in the magnetic field. The 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 necessary to twist the plasma. In addition, the electricity in the plasma represents a heating method. Tokamaks are the closest we have come to the conditions for self-sustaining thermonuclear burning, but this may also be because the most intensive research is being carried out here. The main disadvantage of the tokamak is that it is not suitable for continuous operation, but must be regularly recharged with plasma, which also places extreme strain on the system.
• - 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 end results in increased energy losses.
• - MIGMA concept
  • In the MIGMA process, particles (e.g. deuterons and trions) are repeatedly brought into collision from a particle accelerator and fuse. With this concept, a fusion between protons and the boron-11 isotope is also possible. Four high-energy alpha particles (4He2+) are created. The special thing about this approach is that no radioactive and toxic tritium is required and no neutrons are produced, which are responsible for unwanted radioactivity. According to KfK, the main problem with this technology is the energy losses of the particles due to the resulting synchrotron radiation. Unfortunately, this technology, which some physicists consider to be ingenious, is ignored worldwide. Despite considerable initial successes over the 70 years, not enough 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, the fissile material.
• - Induced inertial fusion
  • A mixture of deuterium and tritium is surrounded by a small spherical shell. These 1mm beads (pellets) are bombarded in a vacuum with a high-energy laser or a light or heavy ion beam. During the implosion caused in this way, the hydrogen mixture is compressed to one fiftieth of its volume. The extreme heating creates the fusion plasma. Simulations have shown that the thermonuclear energy output is typically a 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 created here. The construction of an energy-generating reactor that would, for example, ignite ten pellets per second would be conceivable.
• - Cold nuclear fusion
  • The reaction was predicted from theoretical considerations in the 1940s by F. Frank and Andrej D. Sakharov and 10 years later, by chance, it was “proven” experimentally by Luis W. Alvarez. With cold nuclear fusion or muon-catalyzed cold nuclear fusion, the high temperatures and huge experimental setups can be avoided. Cold nuclear fusion is underway at Tempe 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. To do this, negative muons are allowed to penetrate the chamber. The muons create tight bonds between the hydrogen molecules through special collision processes. The muonically bound nuclei fuse and energy is released in the form of heat. The muons are released again and can catalyze further fusions under certain conditions. Muons can be created artificially using particle accelerators. In order for a muon to catalyze multiple nuclear fusions, high energies are required for its generation. So much for the theory. However, implementation in practice has not yet been successfully completed and there are at least no economically functioning reactors.

The chemists Martin Fleischmann and Stanley Pons worked on cold fusion and announced at a press conference on March 23, 1989 that they had built and successfully tested a cold fusion reactor. Unfortunately, this technical miracle has not been confirmed. The two chemists were also unable to demonstrate any excess heat in the built reactor in front of witnesses. Cold fusion is currently interesting for basic research. Unfortunately, to date there is no reproducible experimental setup with a positive energy balance.

The major technical challenge that has to be overcome in nuclear fusion is the energy balance. Unfortunately, more energy is required to make the reaction occur than energy is released later.

In order to get fusion processes going, ideas were put forward decades ago to shoot ultra-fast projectiles at targets that were filled with deuterium and tritium. Such projectiles that impact a target at high speed have been used for several years. In recent years, experiments have been carried out with the collision of disks, which are accelerated to up to approx. 6 km/s by gas pressure tubes or cannons, which are placed on a cube-shaped target with an edge length of approx. 1 cm, which has two chambers each with deuterium and tritium , bounce. A collision compresses the gases into a hot plasma, causing the atoms to partially fuse. In the first experiments, around 50 neutrons were generated per shot. If one were to optimize the shape of the target and no longer use the targets in cube shape, but rather a pyramidal construction with 16 edges and a ratio of 1:1.24, in which one would use a 4-chamber construction with a 103° arrangement in pairs installed, neutron emissions can be significantly increased.

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

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

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

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

DE 102007022302B4 describes a method for accelerating solids with the aim of causing a fusion reaction. Here, several beam emitters are used, each of which emits an energy beam on a solid body made of fusion material, which is then explosively vaporized and its parts are thereby accelerated.

DE 102017000653A1 describes a fusion reactor that, in contrast to conventional reactors, is open and designed as a flow reactor. There are no hints or solutions in the description as to how a merger should take place or what contributes to it.

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

The invention specified in claims 1 to 41 is based on the problem of creating a radiation weapon that is capable of causing nuclear fusion of fusion-capable, light atoms with a relatively low input energy level and thereby generating radiation that can be concentrated and directed destructively at a target at a great distance.

This problem is solved by the nuclear fusion reactor with the features of the patent Proverbs 1 to 41 solved. Advantageous developments of the device are specified in the subclaims.

• - vergleichsweise niedrige Anlauf-Energie Bedarf,
• - relativ kompakt gebaut und auch für mobile Fahrzeuge einsetzbar,
• - sehr große Mengen an das Brennmaterial in der Natur vorhanden.

Advantages of the invention are:

• - comparatively low start-up energy requirement,
• - relatively compact and can also be used for mobile vehicles,
• - very large quantities of fuel exist in nature.

• 1 eine Ausführungsmöglichkeit mit einem Massenkörper (ein Zylinder oder Kugel, je nach Konstruktion), der durch Elektromagnetspulen beschleunigt wird und auf dem Piston aufschlagen soll,
• 2 das Reflektor-System mit einem massiven Parabel-Reflektor aus Metall oder Keramik, der verspiegelt ist,
• 3 eine weitere Ausführung, bei der einige Elektromagneten eingebaut werden, die ein Piston in die Hochdruckkammer drücken,
• 4 eine Ausführung mit einer Schwungscheibe, die beim Bremsen ein starkes Elektromagnetfeld generiert,
• 5 die Ausrichtung der Atome im Fluidstrahlen-Aufprallpunkt durch ein elektrisches Feld zwischen zwei Elektroden,
• 6 eine weitere Methode eine Masse durch elektromagnetische Linear-Beschleuniger, gegen das Piston zu beschleunigen,
• 7 eine sehr kompakte Waffen-Ausführung, wobei ein Fusions-Reaktor mit zwei gegenläufig auf derselben Achse elektrisch schnell drehenden Schwungscheiben ausgestattet ist,
• 8 eine weitere kompakte Variante mit gegenläufig rotierenden Schwungscheiben und durch Zentrifugalkraft ausfahrbaren Klemmen,
• 9 weitere Methoden, um blitzartig Druck auf eine Hochdruckkammer aufzubauen durch eine Knallgas-Explosion,
• 10 zwei getrennte Hochdruckkammer, in denen getrennt Deuterium und Tritium sich befinden,
• 11 eine Ausführung mit elektrostatischen Feldern in der Nähe des Kollisionspunktes, welche die Wahrscheinlichkeit für eine Kern-Fusion etwas erhöht,
• 12 das Auffangen der Rest der Flüssigkeit, die in den Flüssigkeitsstrahlen drin war und nicht zu Fusion geführt hat, sowie das Befüllen der Hochdruckkammern mit Fluid (schwerem Wasser),
• 13 eine Einsatzmöglichkeit dieses Waffen-Systems,
• 14 eine weitere Ausführung mit einer Brennkammer, die gleichzeitig auch eine Hochdruckkammer ist und ohne Piston auskommt.

Embodiments of the invention are based on 1 until 14 explained. Show it:

• 1 a design option with a mass body (a cylinder or ball, depending on the design), which is accelerated by electromagnetic coils and is supposed to hit the piston,
• 2 the reflector system with a massive parabolic reflector made of metal or ceramic that is mirrored,
• 3 another version in which some electromagnets are installed that push a piston into the high-pressure chamber,
• 4 a version with a flywheel that generates a strong electromagnetic field when braking,
• 5 the alignment of the atoms in the fluid jet impact point by an electric field between two electrodes,
• 6 another method of accelerating a mass against the piston using electromagnetic linear accelerators,
• 7 a very compact weapon version, in which a fusion reactor is equipped with two flywheels rotating in opposite directions on the same axis,
• 8th another compact variant with counter-rotating flywheels and clamps that can be extended by centrifugal force,
• 9 other methods for building up pressure in a high-pressure chamber in a flash using an oxyhydrogen explosion,
• 10 two separate high-pressure chambers in which deuterium and tritium are located separately,
• 11 a version with electrostatic fields near the collision point, which slightly increases the probability of nuclear fusion,
• 12 collecting the rest of the liquid that was in the liquid jets and did not lead to fusion, as well as filling the high-pressure chambers with fluid (heavy water),
• 13 a possible application of this weapon system,
• 14 Another version with a combustion chamber that is also a high-pressure chamber and does not require a piston.

The invention is a radiation weapon 1 that is capable of generating energy from controlled nuclear fusion for the generation of highly effective radiation, which is delivered precisely to a target 3 in the form of focused beams 2.

This radiation weapon can be installed stationary and used for effective defense of cities or facilities. Thanks to its high accuracy and instantaneous energy pulses, it can take down almost any target 3 from the air. The high-energy pulsed radiation, which is emitted in the form of a lightning bolt and bundled, can hit any flying object in the air, no matter how fast it is. The weapon simply has to be aimed precisely at the flying object and visually follow it briefly. The firing takes place in real time and at a distance of 10km there is only 0.00003s between impulse generation and hit. Even a flying object that flies at MACH-20 (6.7km/s) can only travel 20cm and only avoid being hit by 20cm, which makes absolutely no difference with a beam with a light diameter of approx. 18m at the point of impact (approx. 1% shift in the point of impact on the flying object), so that it is not even necessary to carry out an aim correction on the weapon. The flying object is immediately hit fully when the weapon is fired and is damaged or destroyed by the lightning beam energy.

The weapon can also be built compactly, so that it can be installed in all types of mobile vehicles, such as aircraft 4, helicopters, ships, tanks, etc., thereby ensuring dynamic adjustment of the defense line.

The weapon uses nuclear fusion energy to generate a beam that occurs in the first microseconds, similar to that of a nuclear weapon detonation. Nuclear fusion is not used here to generate electricity, but rather the radiation energy that is released by nuclear fusion is emitted directly from the weapon in the target direction using a reflector 5 through collimation in a highly focused beam. A principle is presented here for the merger processes beat, which works somewhat differently than conventional fusion reactors.

Obtaining energy from matter through nuclear physics processes such as nuclear fission or nuclear fusion is nothing new. These processes have been taking place in space since the beginning of time. Every star is, so to speak, a nuclear reactor in which light elements fuse to form heavy ones, releasing enormous amounts of energy. Humanity has had the knowledge of how to create these processes artificially for over 75 years. Two important processes have been known since this time: nuclear fission and nuclear fusion. During nuclear fission, more energy is released than is possible through chemical processes. Nuclear fusion is a step higher in terms of energy release. At the very top of energy yield and release comes the process of matter annihilation. While in nuclear fusion around 3-5% of the matter is converted into energy (which is still a lot), in annihilation almost 100% of the matter is converted into energy and therefore the energy yield is highest here. Atoms of matter and antimatter meet each other and trigger the reaction.

In an atomic explosion, the energy is released in the form of radiation (approx. 50%), pressure waves and heat. During nuclear fusion, the radiation is very intense and is emitted in the form of a flash of light, gamma radiation and light. This radiation emission is used in this invention to generate a very intense beam, which occurs similarly to a nuclear fusion bomb, but in a focused form and with a comparatively very low total energy input.

Here, a nuclear fusion of a small amount of atoms is generated in a nuclear fusion reactor 6, which releases intense radiation. The fusion reactor here uses the kinetic energy of the high-speed fluid jets 7 that collide with each other to initiate fusion processes. The fluid jets consist of fusionable atoms or molecules that have such atoms. At collision point 8, a small number of atoms will fuse with each other, releasing enormous energy in the form of rays. This released energy comes from a fusion point, is focused by a reflector and emitted precisely.

To generate the fluid jets, some techniques can be used that do not consume a lot of energy and can still accelerate the fluid from a high-pressure chamber very efficiently.

A relatively simple technique is to use electromagnets 9 to accelerate a mass in the form of a ferromagnetic cylinder 10, which collides with its kinetic energy on a piston 11 and this is used to generate high pressure. When a mass of almost non-deformable material hits a piston, it immediately releases an enormous amount of energy, which is transferred to a fluid 12 into a high-pressure chamber 13 and thereby generates a very high pressure. A very rapid transfer of kinetic energy within fractions of a millisecond is crucial for the fluid acceleration required to cause at least a small number of the atoms to fuse. The high-pressure chamber in which the piston is installed, as well as the piston itself, are made of very hard material and can withstand quite high pressure values for short periods of time. Hardened steel probably wouldn't be enough, but titanium alloys or new carbon nanostructures or carbine would be well suited for this. The piston should be built as light and at the same time stable as possible. New materials or composites meet these requirements. In recent years, numerous new materials have been introduced that are harder than diamond. For example, graphene and carbine are included. Every year new materials are successfully tested and manufactured that are far harder than diamond. Exactly such materials are well needed here.

On the 1 one possible embodiment is shown. A mass body 14 (a cylinder or ball, depending on the design), which is supposed to hit the piston, is electrically accelerated by electromagnetic coils 9 up to approx. 51 m/s. The mass body weighing only 3kg is braked from 51 m/s to zero within 0.0002s and the piston is pushed down 5mm. The piston is partially inserted into the high pressure chamber. The high-pressure chamber is cylindrical in shape, approx. 50mm high and has a diameter of 5mm. It is filled with a liquid, but only to a height of 5mm, so there is only about 98mm ³ liquid there. The liquid consists of a fusion-capable isotope mixture in liquid form. This can be, for example, pure heavy water or a mixture of heavy and superheavy water (deuterium oxide and tritium oxide - D ² O + T ² O). The piston lies directly on the fluid 12 and it also has a cylindrical shape. It is at least 50mm long and at least the last top 5-10mm are outside the high pressure chamber. This external part 15 of the piston is hit by the electromagnetically accelerated mass 14 colliding with it and is pushed downwards in a flash. To ensure a stable construction, the part of the piston that protrudes at least more than 5mm beyond the chamber is equipped with a larger, stable disk 16 on which the mass body will impact. However, the piston can be built without this disc, so that it is completely recessed until the mass hits the high-pressure chamber. At this point, the high-pressure chamber construction can have a damper disk 17, which acts like a shock absorber and absorbs the excess kinetic energy of the colliding mass. For a mass that is spherical, the disk will be built like a bowl 18 at the top and have the same curvature as the ball so that it lies evenly on the disk at the time of impact. This shell construction is pushed down by the mass and at the end of its travel it touches the surface of the chamber construction and thus the piston movement is abruptly braked (the piston movement only lasts approx. 0.0002s). To protect the material, a spring force element or the shock absorber disk (damper disk) will be installed at the point under the shell, which absorbs the remaining kinetic energy and thus protects the construction. The pressure that is generated in the liquid is enormously high and two fluid jets are created on the liquid in the cylindrical pressure chamber with a diameter of 30mm and a piston movement height of 6mm, which consist of the fluid with the hydrogen isotopes , which reach the outside within 0.0002s through the liquid lines 19 from the high-pressure chamber and finally from two nozzles 20, each with a 1.2mm opening (approx. 1.13mm ² ). The two liquid jets (fluid jets) 7 are pressed out at the same time via the nozzles and collide against each other outside the high-pressure chamber at the focal point of a reflector 5. The fluid jets are each only approx. 43.6cm long. The jet speed is approx. 8558m/s, which is very high. In the immediate vicinity, after the liquid jets leave the nozzles, they will collide with each other. The nozzles are built facing each other at a distance of 30 - 80mm, so that the liquid jets inevitably collide with each other. It goes without saying that the fluid jets do not flow out in a sharply defined manner, but at such a short distance they inevitably collide. The liquid lines (fluid lines/channels) inside the block/high-pressure chamber construction must be built as short as possible and of absolutely the same length. There should be no angled spots there because all of this increases the flow resistance of the liquid. The nozzles are also completely the same. However, no matter how closely you make the fluid lines and nozzles the same, the fluid jets will not be absolutely the same length. Always one of the fluid jets will be slightly longer or shorter than the other jet (at least fractions of a percent). This is determined by the internal molecular/atomic forces, current arrangement of the molecules/atoms and viscosity. This means that always, or at least often, one of the liquid jets will be a few millimeters shorter. In our example, the liquid jets should ideally have a length of 430mm each, but one of them will certainly be slightly longer (eg a few mm longer) than the other, eg jet A-429mm and B-431mm. This means that the last two mm of the beam B will shoot into space. Where this beam hits, it can cause material damage. In order to avoid damage as a result, the nozzles do not have to be directed towards one another on the same fluid jet axis 21 and exactly at 180°, but rather the jets can hit each other at an angle, for example 172°. At this angle, the part of the jet that shoots into the void can no longer hit the nozzle opposite. In the fluid jet collision point 8, almost all molecules of the two jets collide with each other and the chemical bonds are partially destroyed. The leverage causes some of the colliding atoms to become much faster than the jet of fluid itself, resulting in fusion. A small number of colliding atoms fuse with each other and release enormous amounts of energy, which is bundled by the reflector and released in the target direction.

At the impact point/collision point 8 of the two liquid jets 7, a partial nuclear fusion takes place, which is accompanied by an extremely bright flash and heat radiation/neutron radiation. Gamma radiation, UV light, visible light and IR radiation are also emitted. The energy released is released in all directions, but the reflector system bundles it in one direction in the form of a beam 2. The reflector system includes a massive parabolic reflector 5, which is made of metal or ceramic with a thick metal jacket that can be made mirrored. The fluid jet collision point is located at the focal point 22 of the reflector. A small mirror reflector 23 can also be installed in front of the fluid jet collision point, which first reflects the radiation onto the large reflector and then bundles it from the large reflector in the target direction ( 2 ). This structure would be similar to reflecting telescopes, which each have two curved mirrors. The cumulative beam 2 is a mixture of several types of beams. It consists of gamma rays, UV rays, light rays and IR rays and is emitted in flashes with the intensity of a hydrogen bomb explosion. Focused by the reflector, the beam can hit and destroy very distant targets. The radiation intensity at a large distance per unit area is even higher than the flash of a nuclear fusion Bomb explosion because it is highly concentrated. As a hydrogen bomb explodes, it emits a very strong radiation a few microseconds after nuclear fusion, which appears like a very powerful lightning bolt. This flash, which lasts extremely briefly, is so intense that a hydrogen bomb with a power of 1 MT can burn objects in all directions even 15 km from the explosion center. The invention also produces a miniature lightning bolt, but instead of allowing it to spread in all directions, it only creates a highly focused beam. Depending on the performance of the reactor (impact speed of the fluid jets and the amount of fluid in it), this jet can set fire to or destroy targets several hundred kilometers away. The beam is much more intense than that of a powerful laser device in the MW range. The beam here in particular contains a destructive mix of beam types that can cause devastating damage when striking a target. The radiation values per unit area are almost similar to those of a nuclear weapon explosion, although the irradiated area is comparatively extremely small. With high-quality reflector systems, the radiation can be focused well, so that at a distance of 30 km on a circle of light 24 with a diameter of 250 m and an area of approx. 50,000 m ² it can emit a similar level of radiation energy, which is almost as high as like a 10MT hydrogen bomb detonation (even at a distance of 30km).

The radiation generated by this weapon is similar to that of a thermonuclear weapon explosion, but here the radiation is not spread out in a spherical manner, but rather in a concentrated manner. In addition, the total radiation intensity is nowhere near as high as the total radiation from a nuclear bomb. Similar radiation values per unit area are only achieved by bundling the rays. The advantage of this weapon is that nuclear fusion takes significantly longer than is the case with a thermonuclear bomb. While gamma radiation, X-rays, UV, light, IR and other destructive EM radiation are only emitted there for a few microseconds, here a few milliseconds are available for the generation of the radiation.

The fluid jets can be emitted repeatedly at any time intervals. Depending on the design of the weapon, the process can take a while or can be repeated quite quickly, but the wear and tear on the components is extremely high. The piston in particular wears out quickly, so it would need to be replaced after a few operations. That's why the piston is not installed enclosed, but simply inserted into the high-pressure chamber so that it can be easily removed and replaced with a new one. In addition, the outer part of the piston, which is not inserted into the chamber, is shaped slightly wider, so it can withstand quite a bit of force. A guide ring or hollow cylinder outside the high-pressure chamber ensures that the linear movement is precisely maintained during this extremely fast stroke movement of the piston. The piston looks like a pin or bolt and has to be made of very hard material, otherwise it will be bent over, deformed or completely destroyed on the first try. The impact causes the liquid jet to become very fast right from the start and nuclear fusion can be partially initiated. It is enough for just a few billion atoms to fuse with each other per liquid jet to provide enough energy to produce the jet with a very high energy output. The reflector is another sensitive part. It will also wear out relatively quickly or become brittle or corrode due to the very intense radiation. The weapon tube 25 (barrel) is quite short but wide and would have to be installed to suit the weapon's performance. For low-power beam weapons, the tube can have an inner diameter of 20 - 40cm and a length of 100 - 200cm. The diameter of the tube should be the same as the diameter of the reflector. The tube is smooth or matt mirrored on the inside. It can also be a telescopic tube that can be electrically powered, lengthened or shortened. The reflector is connected directly to the tube. At the very beginning, the pipe should have numerous holes or openings 26 or a grid structure 27, because this allows the steam and excess fluid that has not fused to escape. Wherever the pipe is pointed, a target can be attacked. The range is very long, but there are no ballistic effects. “Shooting” this weapon from behind a hill is not feasible. It can only hit targets that can be seen. With each pulse shot the weapon gets quite hot and therefore needs to be cooled. Air cooling is simpler, but water cooling can be even more effective. When the weapon is “fired”, a recoil force is created, which should not be underestimated. This force comes less from the radiation (which also creates a recoil here, but it is so small that it can be neglected), but rather from the hot steam and residual liquid that flows from the fusion point 8 partially through the pipe is accelerated at the front. However, the recoil has no influence on the accuracy of the weapon because before the recoil occurs, the radiation impulse has already reached the target. The steam 28 arises just as much later (from approx. 0.07s after firing) and cannot influence the “visibility” of the weapon because here too the radiation impulse has already left the weapon. There is no impact on the reflector only the EM radiation, but also a very hot plasma that comes from the collision point of the fluid jets, but which is cooled down very quickly. If soldiers are to be nearby to operate the weapon, only deuterium as a hydrogen isotope, in liquid form or in the form of heavy water should be used. Tritium is poisonous or radioactive, so only an automatic defense system with such radiation weapons could be used without people nearby.

Electronic target search systems 29, automatic target trackers, radar systems and optical detection components are to be coupled with the weapon, all of which would help to intercept and destroy very fast-flying missiles, such as ballistic or hypersonic missiles 30.

The construction of the high pressure chamber can consist of two solid parts, which look like large, solid block disks, which are connected together by a multitude of thick screws. This design has advantages because the high-pressure chamber can be restored more easily after wear or deformation. To do this, you would have to screw the two blocks apart and process the exposed high-pressure chamber (e.g. re-milling or drilling).

3 shows a further embodiment in which some electromagnetic coils 9 or electromagnets are installed, which press a piston 11 into the high-pressure chamber 13. The electromagnetic coil is briefly fed with a very strong current, for example from one or more large capacitors 31, thereby generating a strong magnetic field. The magnetic field is generated in impulses, only lasts approx. 0.0003s and is extremely strong. This impulse attracts the piston, which is partly made of a permanent magnet or iron 32 or has such a material on its piston rod, and moves it at lightning speed, exerting an enormously high pressure on the fluid in the high pressure chamber. Here, strong and high-capacity capacitors are charged and then all the energy is passed into an electromagnetic coil, which generates an extremely strong magnetic field and sets the piston in motion in a flash, which then generates the fluid jets 7 via the high-pressure chamber 13 and the nozzles 20. Several electromagnetic coils or electromagnets can also be installed, which press the piston into the high-pressure chamber. The electromagnet coil only has a few turns, but has a fairly strong wire. It is even better if superconductors are used for this. In this way, extremely strong electromagnetic fields can be generated, which can also be built up at lightning speed. It is very important that the liquid jets become very fast right from the start and that the impact of the liquid takes place at maximum speed. Unfortunately, the acceleration of a piston using electromagnets can only be achieved using very high currents. It is much easier to strongly accelerate a bolt 14 using the electromagnet, which strikes against the piston, which then presses the liquid into the high-pressure chamber and is displaced through the nozzles. The piston path is very short (a few millimeters), and a fast-moving bolt can drive it through impact at maximum speed. The piston can be built from titanium alloy and is intended to be as light as possible. The kinetic energy of the bolt (1-3kg, approx. 50m/s) should be absorbed as completely or largely by the liquid, which accelerates it strongly by displacing it from the high-pressure chamber. This variant can also be built very compactly and has very good efficiency and performance. The piston is pushed down with extremely high pressure by electromagnetic force and the heavy water is pressed through the nozzles into the high-pressure chamber. The heavy water mass flows simultaneously in both liquid lines and is pressed outwards in the form of fluid jets 7. To generate the high current, as is usual in some particle accelerators, the energy from a rapidly rotating flywheel (this is electromagnetically braked abruptly and the electrical energy is released or generated in the coils) or capacitors can be used. The reactor and the weapon would therefore be quite compact and could easily be used for mobile purposes. Instead of heavy/superheavy water, acetone or another liquid that has hydrogen isotopes instead of ^H2 can also be used. Because the radiation weapon is also intended to be operated by humans, it would be important that only deuterium is used as the hydrogen isotope and not tritium. For proper function, there must be no air bubbles in the liquid. Theoretically, you can also place small hollow spheres or small micro-balloons with pure deuterium or a gas mixture of deuterium and tritium there, which can then be pressed extremely quickly using high pressure. When the liquid is forced through the piston, the bubbles or small elastic balloons with D ² + T ² shrink into the pressure chamber, flow out through the nozzles and fusion occurs at the collision point.

For a compact weapon design, the electrical capacitors are not quite optimal, but are still useful. Here, strong and high-capacity capacitors are charged and then all the energy is discharged into an electromagnetic coil with a few, very thick turns (or superconductors). The piston is partially in the coil and when it becomes active, the coil fully retracts the piston. This puts the liquid in the high pressure chamber under strong pressure. The only problem here is the strength of the current and the acceleration of the piston. The piston must become fast immediately and it should not initially displace the liquid with low pressure.

A version with a flywheel 33, which generates a strong electromagnetic field when braking, is on the 4 been presented.

The massive flywheel is set in rapid rotation by an electric motor 34. The electromagnets 35 below are only switched and absorb the induced energy when the piston is to be pressed. As soon as the maximum rotational speed of the flywheel has been reached, the electromagnets under the disk 33 are switched on and the current induced by the disk is conducted into the electromagnetic coil of the piston using superconductor technology. This induced electrical energy is used for piston movement and fluid jet generation. The piston is then moved down with full force and high pressure is applied to the liquid (heavy water). The piston acceleration is not as good as the version with the striking bolt, but here the wear is significantly less. An electronic control 36 regulates the processes.

It is enough for deuterium atoms to collide with one another with very high kinetic energy to initiate fusion processes. Of course, not all colliding atoms will fuse using the fluid jet method. Only a very small proportion of collisions will lead to fusion, but because the number of atoms that collide with one another is extremely high, the small proportion of fusion processes is sufficient to generate intense radiation energy.

For increased fusion possibility or neutron release, two pistons and two high-pressure chambers can be installed, each with heavy water - deuterium oxide (D ² O) 37 and superheavy water - tritium oxide (T ² O) 38 are filled.

We will explain here what happens at the meeting point of the fluid jets. The fluid jets will collide against each other at extremely high speeds (approx. 7 - 9km/s). The lines for the liquid are not external or thin lines, but are milled/drilled into a solid hard metal block 39 (or alloy, e.g. titanium alloy) so that they can withstand enormous pressure. The nozzles are not necessarily screwed-in parts, but are designed so that they are part of the solid metal block 39. Because the two liquid lines for fluid transport are of the same length and drain the liquid from the same high-pressure chamber, the two fluid jets are actually generated simultaneously and collide with each other. In order to release separate deuterium and tritium liquid jets and let them collide against each other, you can install two high-pressure chambers and two pistons, which are pressed downwards at lightning speed by the same system and completely at the same time. In this case, each chamber would have a liquid line connected to it, which directs the liquid jets outwards in the direction of collision. The liquid lines are constructed in such a way that they are arranged somewhat cone-like from the wall of the pressure chamber with the tip facing outwards. The liquid enters the liquid lines as soon as the pressure is built up. No closing valves are necessary because the liquid stays there simply through a negative pressure in the high-pressure chamber as long as the piston is at the top. The fluid lines are smooth and also drilled into the solid block (or cast using casting technology). It is important that the solid block is compact and, if possible, built in one piece. It may be possible to construct the block from two solid parts, which then look like large, solid disks that are connected together by a multitude of thick screws. Any other construction method would potentially cause the structure to explode due to the extreme pressure. The piston that compresses the liquid into the pressure chamber has a relatively small area and a very short path. Depending on the version, it only moves approx. 5 - 8mm and when pressed completely displaces the few ml of liquid from the high-pressure chamber. The piston is made of a solid, hard material. The pressure that exists in the high-pressure chamber when the piston is pressed is briefly several hundred thousand bars. A brief, strong increase in temperature is registered in the fluid jet collision point. This causes a reliable breakdown of the molecular structure and also causes atomic fusion in a small proportion of the atoms at the collision point. An additional neutron beam can be delivered to the collision point of the liquid jets (fluid jets) to promote fusion. At the point of impact, only a small proportion of the atoms will melt together, but this is enough to produce an energy gain several times higher than that used to create pressure or lift the mass to a certain height. The atoms will collide against each other at the fluid jet impact point, largely being thrown apart and radially away from the fluid jet axis 21 in all directions. An electric field built up there between two electrodes 40, which are coupled to a high-voltage generator 41, forces the molecules to maintain an optimal orientation at the collision point. Instead of the electric field, you can also use a strong, focused microwave beam 42 from a microwave source (e.g. magnetron or even better - Gunn diodes) 43 ( 5 ). MASER are ideal for this. These are designed similarly to lasers and emit coherent microwave radiation, but are bulky and relatively large. Gunn diodes are very small and compact, but only deliver low power. The coherence of the microwaves is important because then the oscillation phases of the atoms in the liquid jets 7 always remain the same. Only a phase calculation and the wavelength or distance for generating a hot spot in the beam meeting point would have to be calibrated. This allows the electron shells of the atoms to be deformed and the atoms to hit each other in such a way that the probability of a core meltdown is higher. The electron shell normally prevents a core meltdown, but here it is deformed to such an extent by the impact and electro-magnetic field interaction that its field forces actually promote a core meltdown.

Another method is to electromagnetically accelerate a mass against the piston using a linearly arranged series electromagnet, which then hits the piston. This ensures that the energy of the mass is immediately transferred to the piston in order to avoid a slower increase in pressure into the high-pressure chamber ( 6 ). The linear movement and acceleration of the mass can be realized with the help of inductance sensors 44 or optical light barriers and a controller.

On the 7 A very compact weapon version is shown, with a fusion reactor for this radiation weapon being relatively small. Here, two flywheels 33 rotating in opposite directions on the same axis are installed, each of which is equipped with electrically driven mechanisms or actuators 45, each of which has a bolt, wedge, lever or clamp 46, installed in the flywheel, when a maximum speed is reached the flywheels move out at lightning speed parallel to their rotation axis direction 47 and then hit the pistons 11 when they reach a rotational position and press them into the respective high-pressure chambers 13.

Another compact variant with the two counter-rotating flywheels can be arranged with two clamps (levers, wedges or cylinders) that can be extended by centrifugal force on both sides or mutually / diametrically for balance and because of two pistons and high-pressure chambers as well as their fluid lines, which are during Rotation is released electrically after reaching the maximum speed and then hits the pistons (one piston for each fluid jet) and generates the fluid jets. The clamps can be extended by actuators or by a trigger mechanism in combination with the centrifugal force of the rapidly rotating flywheels ( 8th ). In the centrifugal force variant, two diametrically arranged bolts 46 are each inserted radially into the disc in a wooden cylinder 48. They are released at lightning speed by an electrically controllable release mechanism 49 when a maximum rotational speed is reached and they move radially out in the perimeter of the flywheel at lightning speed using centrifugal force alone. As soon as the bolts move out, they each form an obstacle that hits the pistons as soon as they come close to them with the rotation of the disk. The fast-rotating flywheels are ideal for compact designs. These are accelerated by electric motors, brought to high speed and then braked immediately in order to invest the rotational energy of the mass into hydraulic pressure. Braking is carried out by radial displacement of the two clamps (levers, bolts, wedges), or by levers that can be moved parallel to the axis of rotation, which are coupled directly to the pistons and thus transmit the pressure of the flywheel directly to the pistons, which causes the braking and the absorbs energy there. Practically all of the rotational energy of the flywheels is immediately transferred to the piston and thus to the fluid in the high-pressure chambers. That's why the fluid jet comes out with such energy and high speed. When extending radially, in order to avoid imbalance, levers/clamps arranged radially and diametrically should always extend at the same time. In order to avoid strong vibrations in the reactor chamber caused by the abrupt braking of the flywheel, the two counter-rotating flywheels rotate at the same speed on the same axis and are both braked at the same time.

There are numerous other methods for building up pressure in a high-pressure chamber in a flash. To generate the pressure on the piston, an oxyhydrogen explosion or another explosive process can also be used optimally. A wider combustion chamber 50 is installed here, with the piston being a double piston ( 9 ). It practically consists of two pistons that are linearly connected to each other or are built in one piece. The upper piston (or depending on the arrangement, also on the side), or the combustion chamber piston 51 has a wide working surface at the top (approx. 500cm ² ), which is located in the combustion chamber, while the lower piston (the high-pressure chamber piston) 52 has a very small working surface (approx. 19mm ² and a diameter of 5mm), which flows into the high-pressure chamber. An explosive or, even better, oxyhydrogen 53 is passed into the combustion chamber and is ignited by an electronic control 54, high-voltage source 55 and electrodes 56. The oxyhydrogen ignition pushes the combustion chamber piston downwards by approx. 5mm and because it is connected to the high-pressure chamber piston and forms a unit, it simultaneously creates pressure on the liquid. Due to the different piston surfaces, the pressure in the high-pressure chamber arrives at a very high ratio (approx. 2500:1). Although the expansion speed due to the explosion is very high, there may be slight delays when accelerating the piston. Every mass has an inertia and it takes a few fractions of a millisecond to overcome it. That's why two jets of liquid, each 75cm long, are only released at maximum speed after about a few dozen cm. This means that the nuclear fusion would not take place immediately with the first atoms colliding with one another, but with the subsequent ones, which start from approx. 5 - 10cm of the first area of the liquid jets, and would therefore take place somewhat delayed. The energy from the collision point spreads like a ball in every direction, but is focused in one direction by the reflector 5 and emitted in the form of a concentrated beam 2.

In the invention, the fluid jet length means the length of the liquid jet coming out of the nozzle, which would move unhindered into the air (or in a vacuum). Here the jet of liquid is only a few cm long because it collides with the other jet of liquid directed in the opposite direction. The nozzles are not far apart (just a few cm or less). But both fluid jets continue to flow with replenishment until the full fluid jet length is completely used up. It is very important in the invention that the pressure on the liquid is very high from the beginning, from the first microseconds, and does not increase slowly. That's why with this method, a mass 14 can first be accelerated by the oxyhydrogen ignition, which then hits the piston with full force. In this case, the liquid jets would emerge from the high-pressure chamber relatively quickly and at maximum speed and would collide. For this reason, a very small amount of the liquid used to generate the jets is accelerated so that it can fully utilize the kinetic energy.

The liquid jets with deuterium (or tritium) atoms in them (in the molecular state or “dissolved” atoms of the hydrogen isotopes) bring a small number of these atoms to nuclear fusion. The energy of the liquid jets alone would not be quite enough to achieve effective nuclear fusion operate, but here it must be taken into account that the circumstances and chances of fusion of the atoms are much greater than in other types of fusion reactors. Here almost all the atoms of a fluid jet collide with the atoms of the fluid jet opposite! The atom -Collision number is extremely high, and the atoms force each other to hold their position due to their inertia, which inevitably leads to partial fusion. Every time an atomic fusion takes place, parts of the atom groups from the explosion center are collided at even higher speeds further permanently flowing atoms of the two jets are accelerated, which again increases the chances of fusion. The liquid jets are disturbed for a few nanoseconds after each atomic fusion in the collision point, but this has a positive effect and dramatically increases the number of new fusion processes. It looks as if the two heavy water jets would burn up at the collision point and the molecules and atoms there would make a large number of jumps towards the collision point. Deuterium atoms will collide with each other, or with mixed water jets of deuterium and tritium atoms, and their fusion will occur. When using only a high-pressure chamber with mixed liquid (D ² O + T ² O), the neutron emission is slightly higher because there is a high percentage of collisions between dissimilar atoms. If an even higher neutron emission is desired, it is suggested to use two separate high-pressure chambers in which deuterium and tritium are located separately, but which are simultaneously brought under high pressure. In this case, one can safely assume that tritium and deuterium always collide with each other. Unlike ion collisions in an extremely thin plasma, here the atoms have hardly any escape options ( 10 ). Above all, the inertia of the liquid contributes a lot to the fact that the atoms from the molecular structure, which are on the central line 57 of the beam axis 21, necessarily collide with one another. In the molecular or atomic state, the atoms are not ionized and therefore the Coulomb forces are significantly weaker than in highly heated plasma. Here, too, the atoms and molecules are heated during the collision, but then there is hardly any time to avoid each other. The outer beam layer 58, which represents the last approximately 0.03mm (depending on the beam cross-section and beam speed), seen from the center of the beam cross-section (0.2mm), acts like a jacket that covers the center molecules / atoms 59 located in the fluid jet are prevented from being thrown away, at least for a very short time. This very short time is enough to cause some of the atoms to undergo nuclear fusion. Once ignited, a chain reaction can be set in motion, which, because supplies of atoms always come to the collision point with the fluid jets, continues until the jet is used up. Unfortunately, the entire energy generation process only takes a very short time. A liquid jet with a length of 1.5m will be completely consumed within 0.0003s at a speed of 5km/s. After 0.3ms the fusion stops, but it can be repeated within a short time. Automated refilling of the high-pressure chamber and acceleration of the flywheels can enable multiple jet firings per minute. As soon as the flywheels reach the maximum rotational speed, the weapon is considered ready to fire and can emit another radiation pulse. The flywheels can have small dimensions, for example a diameter of 12cm and a rotation speed of 9,500 rpm are enough to press a piston into the high-pressure chamber at 56m/s. The clamps are installed in the periphery of the flywheel and therefore have almost the same speed as the running speed of the flywheel in the perimeter.

In order to promote fusion, the probability of nuclear fusion is slightly increased with the help of electrostatic fields near the collision point. The electrostatic fields from electrodes 40 cause the molecules in the fluid immediately before the collision to align optimally and impact on the “side” that allows the two deuterium atoms to meet, thereby blasting the oxygen atom away from the chemical bond . The molecules in the liquid jets immediately after they emerge from the nozzles will be oriented by a strong electric field pulse. The molecules of D ² O and T ² O, like water, are electric dipoles and can be oriented by strong electric fields so that their collision is optimal ( 11 ). For such purposes, the molecules can also be irradiated with microwaves (e.g. from a MASER or strong Gunn diodes 43) or laser beams immediately before or directly at the collision point. The heavy and superheavy water (D ² O and T ² O), for example, can orient itself on it through the rotation of the water molecules through the electric field. However, the water molecules can rotate at a maximum of 20GHz because they have inertia. With heavy and super-heavy water, the rotation time is even longer due to the increased density and inertia and therefore the maximum frequency is below 20GHz (approx. 17GHz). Above 17GHz the molecules are no longer addressed by orientation polarization but only by displacement polarization. Electromagnetic radiation at around 17GHz could cause rotational polarization or at over 20GHz a displacement polarization, but the collision point would have to be determined extremely precisely. That's why the electrostatic fields are ideal here. Electrically variable fields with low frequency, in which the phases are precisely coordinated at the collision point, can also be used. The electrostatic fields orient the deuterium oxide and tritium oxide molecules and thereby align the bond angles of the deuterium / tritium atoms in the D ² O and T ² O molecules so that the largest possible number of molecules are in contact with each other collide, on the collision side where the hydrogen isotope atom is anchored. This means that mainly the deuterium and tritium atoms collide with each other, whereby the oxygen atoms are blasted out of the chemical bond. The molecular bond is destroyed and the deuterium atoms immediately undergo fusion. This increases the efficiency of nuclear fusion somewhat. In this case, nothing should be left to chance, but rather the dipolarity properties of the molecules should be used and they should collide with each other in an optimally aligned manner.

Whether the two hydrogen isotopes are mixed in the form of heavy water and superheavy water, or consist of pure deuterium and tritium in the liquid form, is an interpretation of the technical effort for fusion operation. Of course, it is optimal to use pure deuterium and tritium in liquid form and in separate high-pressure chambers, but the two isotopes must be cooled very strongly until they become liquid. The pressure also has to be quite high. All of this can weaken the structural integrity of the high pressure chamber. By using D ² O and T ² O, the problems described can be solved. In water form, these are liquid at room temperature, incompressible and can therefore be used without much effort. The fluid jets of deuterium oxide that collide with one another can also collide at less than 180°, for example at 175°. This has the advantage because if one of the liquid jets is slightly longer, it will not hit the nozzle opposite during the collision-free period.

The advantage of the invention is the extremely high number of atoms that collide with one another. While in conventional methods with plasma inclusions through magnetic fields, the ion density is very low (approx. 1g of plasma material distributed over a few m ³ ), a very high number of collisions will take place here. Of course, not nearly all atoms colliding with each other will fuse kidneys, but it is enough if only every millionth collision of atoms leads to nuclear fusion. The beam that is generated and, above all, focused by the reflector can be very suitable for attacking targets at long distances.

The collision energy of the fluid jets is very high, so that at the point of impact the liquid is heated extremely quickly and to a high degree, whereby the molecules and some atoms are also broken down into components and fly apart at an even higher speed. Many of the atoms and molecules will fly almost radially away from the fluid jet axis. A shield at this point would be completely milled away and destroyed within a very short time, which is not the point of the matter. A line area 60 made of a very hard material can be installed in the area of the reflector. You could also install a layer of ice there to protect the surface, but it would have to be replaced after each beam shot.

Although there are not very many atoms that will fuse per heavy water jet pulse, the energy released in the process still reaches a considerable level because, compared to other nuclear fusion methods, a lot of atoms collide with each other. The collision proportions are extremely high compared to a plasma confinement fusion reactor because the density of the liquid is much higher than plasma. Where the rays meet, a very intense flash light is generated, which partly contains gamma and X-rays, followed by UV, IR and light emission. Neutrons are only released when tritium is used. With deuterium these are almost non-existent. Helium, oxygen and ozone are then produced as end products.

With this weapon in its nuclear reactor with the liquid jets, they meet each other at extremely high speed, with their kinetic energy being very high. Although this initial energy is several times smaller than the energy invested in the particle accelerator, the number of atoms involved in collisions is several trillion times higher. This not only equalizes the chances of successful mergers, but significantly exceeds them. The pressure and kinetic energy of the atoms are highest, particularly in the center of the beam's meeting point. Above all, the options for evasion of the atoms that collide with each other are relatively small, or they can only avoid each other with a delay. Of the huge number of atoms that collide with each other here, a few million atoms will be so far that their favorable field orientations and outer shell deformation will lead to a core meltdown with the atoms of the opposing jet and produce helium. Of course, as a secondary effect (which benefits us), enormous energy is released, which takes shape in the form of gamma radiation, X-rays, fast neutrons and therefore heat. This energy is released in the form of a focused beam through the reflector in a targeted direction. The beam is electromagnetic and has a very wide light spectrum, ranging from gamma rays to infrared. The intensity of the flash light is comparable to that of a hydrogen bomb, with the difference that it is focused here and therefore remains intense over a longer period of time.

The nuclear fusion processes described here in the invention may also take place in nature in a different embodiment. When large meteorites, especially asteroids, fall on a planet with no or very thin atmosphere, an additional amount of energy is released through nuclear fusion, at least on the impact surface of the meteorite/asteroid. This can result in the scratch created by a meteorite being slightly larger than could be created using kinetic energy alone. Observation of asteroid collision shows that at the time of collision, ultra-short flashes are generated, which may be an indication that nuclear fusion of a small group of atoms may be occurring at the collision point. Of course, the lightning is generated primarily because of the rapid increase in temperature upon impact, but nuclear fusion also makes a small contribution. There, if the rocks collide with each other too quickly (at 30 - 120km/s), the kinetic energy will help some groups of atoms on the impact surface fuse with each other, thereby slightly increasing the energy released. This also increases the ultra-short flashes. It may only be a very small amount of material that fuses (depending on the asteroid size, between micrograms and milligrams), but still. Nuclear fission can also take place in the same way. The meteorites that hit Earth are usually small and are slowed down so much by the atmosphere that almost no nuclear fusion processes occur upon impact. From a diameter of 30m, with hard space bodies (e.g. those with a high iron content) that are compact and do not burn up in the atmosphere, something like this can happen upon impact or when entering the atmosphere due to a collision with air molecules. Occasionally, the hydrogen atoms in the atmosphere can fuse on the front surface of the rock when they enter the rock when they collide at extremely high speeds.

With this invention, the described reactors in the weapon can of course not successfully fuse all the material intended for fusion. However, it is completely sufficient if only 0.03-0.5% of them are involved in this process. This generates a considerable amount of energy, which would then have to be dissipated in the form of a focused beam through the reflector in order not to damage the reactor. The rest of the liquid that was in the liquid jets and did not lead to fusion can anyway be collected back into a reactor chamber at the bottom and the high-pressure chamber can be filled again. A liquid line 61 with a very small opening 62, which enables the high-pressure chambers to be filled with fluid (heavy water), can open into the wall in the upper area of the high-pressure chamber. This opening is closed by the piston itself immediately after the piston is inserted. Electric valves should not be used because they cannot withstand the extremely high pressure ( 12 ).

The weapon here can be equipped with other devices that can promote fusion. These include, for example, microwave generators, ultrasonic wave generators, X-ray emitters, electron accelerators, etc., which can have a beneficial effect on the liquid collision point and release their energy. It should be mentioned that the liquid jet collision point is located at the focal point of the reflector. In this way, the radiant energy coming from this point is aligned and released in a focused beam.

A strong pulse laser and a neutron source can also promote fusion at the collision point of the liquid jets. Both can be installed in the reactor. The pulse laser should of course be activated automatically and synchronously controlled by sensors. It would have to be switched on and release its energy exactly at the time of impact. However, this will significantly increase the input energy, which makes it necessary to carry powerful power sources.

A version with two counter-rotating flywheels 33, which are installed on the same axis of rotation 47, can be built very compactly. The two disks are accelerated together, but also braked/stopped at the same time in order to direct their kinetic rotational energy to the liquid in the high-pressure chambers in the form of high pressure generation. Braking is carried out by clamps that can be extended electrically in a flash, which move out of the flywheels and then collide with the pistons of the high-pressure chambers after half the rotation. All the flywheel torque is used to push the pistons into the high pressure chamber. The terminals 46 are moved out electrically, by actuators 45 and precisely controlled by a controller. Four high-pressure chambers 13 and four pistons 11 are installed here. Four liquid jets 7 are also generated, which collide with each other in pairs. The collision points 8 are deliberately placed very close to one another, so that the spreading liquid circular surfaces also collide with one another and are all at the focal point or very close to the focal point of the reflector. Because there are no external forces when accelerating or immediately braking the flywheels, this method is ideal for compact weapons that can also be used in vehicles. Because the flywheels are rotated in opposite directions, they do not generate any significant vibrations on the axle and its axle bearing holder or weapon system, either during acceleration and increasing speed or during abrupt braking. The flywheels can have relatively compact dimensions. The method with parallel flywheels that rotate quickly in opposite directions is very efficient and allows for a compact design of the weapon. If these each weigh 2kg, have a diameter of 12cm and rotate at 9,000 rpm, then they come to 150 rpm, which, with a perimeter of 37cm, gives a speed of the points on the perimeter of 56m/s. Braking this flywheel within 24mm (the distance based on a point in the perimeter) only takes approx. 0.0006s. During this time, the four pistons are each pushed into the high-pressure chambers and the liquid is displaced there. The liquid jets are released in pairs and almost diametrically (slightly offset) from each other, with the collision points on a line located near the axis of rotation. If the flywheels are arranged horizontally with a vertical axis of rotation, then the pistons and the high-pressure chambers are installed statically between the two flywheels. The nozzles are installed further close to each other and the liquid jets meet in two collision points that are very close to each other. It should be noted that the liquid jets that collide in pairs each transport the appropriate hydrogen isotopes. If the jet A comes from the high-pressure chamber A1, then there should be deuterium atoms in the high-pressure chamber A1, which come out with the liquid jet A, while in the jet B and high-pressure chamber B1, there should be tritium atoms. The same applies to jet C and high-pressure chamber C1, as well as D and D1. The liquid If possible, rays of light should run parallel in pairs and the two collision points should be very close to each other. At the collision point, two fluid circles 63 are created, which consist of the residual liquid, which also collide with one another at an area/sector of the circle, which slightly increases the fusion efficiency again. The liquid jets colliding against each other should not necessarily be on a line, but rather they can be at an angle that is slightly smaller than 180° (e.g. 160 - 178°) on the collision journey to each other. Maximum impact and collision force is achieved under 180°. The smaller the angle, the lower the collision speed against each other and thus the chances of nuclear fusion decrease. The weapon with this nuclear reactor variant can be built quite compactly. It can be built permanently on a tank, plane, ship or even portable.

What is important with this weapon is that the pressure on the liquid in the high-pressure chambers is built up very quickly. Therefore, solid walls (block parts) made of hard material (e.g. titanium alloys) will form the pressure chamber so that expansion is kept as small as possible. The smaller the expansion of the pressure chamber, the better the fusion process works. It is very important that the liquid jets at the point of impact reach their maximum speed after just a few cm. This means, for example, if a liquid jet with a total length of e.g. 76cm is generated, after the first few cm, the rest of the jet rushes to the point of impact at maximum speed. Of course it is impossible for the first cm of the beam to come at maximum speed, but the rest of the beam should reach this speed if possible. That's why the variants with the impact mass on the piston have advantages over the electromagnetic or oxyhydrogen ignition variants. The pressure on the piston is highest in the first fraction of a millisecond. The fluid absorbs some of the kinetic energy and the piston movement slows down. But because the first cm are accelerated to the maximum, nuclear fusion occurs, which then also accelerates the slightly slower atoms in the beam enormously and initiates further fusion processes. Thus, a chain reaction is set in motion that burns the collision point of the fluid jets of heavy and superheavy water, creating a jet that is sustained for a few milliseconds.

On the 13 One possible application of this weapon system is shown. The weapon is well suited to hitting fast-moving targets. This can be used to reliably destroy hypersonic missiles, aircraft, ballistic missiles, etc.

Another version has a combustion chamber, which is also a high-pressure chamber and does not require a piston ( 14 ). Here the oxyhydrogen gas 53 will collect on the upper area of the combustion chamber 50, while D ² O is located at the bottom. As soon as the oxyhydrogen 53 is ignited, the heavy water masses are displaced and two fluid jets of D ² O are generated, which collide with each other and lead to nuclear fusion. The more oxyhydrogen gas is pumped into the combustion chambers, the higher the pressure will be in the event of an explosion. Here you absolutely need the device for electrostatic alignment of the molecules because the fluid jet speed is not particularly high.

Fluid jets released at 7-9km/s have enough kinetic energy to destroy the molecular bond and cause the hydrogen isotopes to collide. Because the fluid jets are quite “thick” by atomic standards, even with a cross-section of 0.2mm, they generate a very strong mass inertia, which leads to nuclear fusion of the colliding atoms located in the central area of the jet. The "outer jacket" in the fluid jet, which makes up the outer "layer" in the perimeter of the circle of the jet cross-section, which contains a few percent of the fluid jet mass, has a crucial role in preventing the atomic "deserters" following the collision “wanting” to avoid “wanting” through Coulombs forces. The inertia of the outer fluid jet layers acts like a hard coat that briefly holds the atoms in the jet together. After the collision and partial fusion processes, the beam is exploded at the collision point and the remaining molecules, atoms and also the fused elements leave this point at high speed, which also leads to further collisions. Although the fluid jet is not extremely fast, some fusion of the atoms still occurs. This happens because not all atoms collide with each other at the time of collision at the speed that is caused by the fluid flow. A small number of atoms reach significantly higher speeds and accelerations through interactive collisions and field repulsion processes, which can lead to fusion. The meeting angles between the colliding atoms also play an important role. But as soon as fusion occurs, the fluid jet “burns” and creates very intense flashes of light that reach the gamma radiation range.

It should be mentioned that in all variants that only use one high-pressure chamber Chamber only one of the hydrogen isotopes is required to get the fusion going. D ² O is completely sufficient. A liquid mixture of D ² O and T ² O is not required. Deuterium atoms can certainly fuse with each other. A fusion between deuterium and tritium is somewhat easier to achieve, but neutrons are also released, which have a destructive effect on the reflector.

To saturate the ions from hydrogen isotopes resulting from collision, electron beam emitters / cathode ray tubes can be installed, which are directed at the fluid jet collision point. Immediately before the fluid jet collision occurs, a cathode emitter emits a well-focused electron beam onto the collision point of the fluid jets. These electrons are captured by the ions and thereby transformed into neutral atoms, which somewhat weakens the barrier created by the Coulumb forces so that a collision between atoms and their fusion can be initiated. The molecules can be oriented immediately before the collision using electrodes and a high-voltage generator. The electrostatic fields should be set up in such a way that the field lines are perpendicular to the direction of the fluid jet. This would also promote fusion because the oxygen atoms would be oriented so that they would not collide with the hydrogen isotopes (that would lead to nothing).

Depending on the design of the reflector technology, the weapon is suitable for destroying enemy targets at both long and short ranges. However, it is also suitable for destroying such targets in the air (airplanes, rockets, hypersonic missiles) or in space. This means, for example, that ballistic missiles, satellites, kinetic weapons in orbit that can drop tungsten projectiles, etc. can be effectively combated. You could even use this weapon to hit targets far away, such as in geostationary orbit or even on the moon. However, for this to happen, the reflector would have to be quite large and the focal point would have to be aligned exactly at the fluid jet collision point.

The weapon not only emits very strong radiation energy, but it can also generate a pressure wave of up to several thousand meters through plasma flow from the weapon barrel. That's why the components of the weapon should be made of stable material because then wear and tear progresses more slowly.

REFERENCE SYMBOL LIST:

1

Beam weapon

2

Rays

3

Goal

4

Airplanes

5

reflector

6

Nuclear fusion reactor

7

High speed fluid jets

8th

Collision point, fusion point

9

Electromagnet

10

Ferromagnetic cylinder

11

Piston

12

Fluid

13

High pressure chamber

14

Mass body, bolt, cylinder or ball

15

Outside part of the piston

16

Stable disc for the piston

17

Damper disk

18

Bowl on the piston

19

Fluid lines

20

nozzles

21

Fluid-jet axis

22

Focus of the reflector

23

Small mirror reflector

24

Circle of light

25

Weapon barrel, telescopic barrel/barrel

26

Holes or openings

27

Grid structure

28

steam

29

Target search system

30

Ballistic or hypersonic missile

31

Capacitors

32

Permanent magnet or iron area of the piston

33

flywheel

34

Electric motor

35

Electromagnets

36

Electronic control

37

Heavy water - deuterium oxide (D ² O)

38

Superheavy Water - Tritium Oxide (T ² O)

39

Solid hard metal block

40

Electrodes

41

High voltage generator

42

Microwave beam

43

Magnetron, Gunn diodes

44

Inductance sensors

45

Mechanisms or actuators

46

Bolt, wedge, lever, clamp

47

Rotation axis direction / axis of rotation

48

Wooden cylinder for the bolts

49

Trigger mechanism

50

Wide combustion chamber

51

Upper Piston / Combustion Chamber Piston

52

Lower Piston / High Pressure Chamber Piston

53

Oxyhydrogen

54

Electronic control

55

High voltage source

56

Electrodes in the combustion chamber

57

Central line of the fluid jet axis

58

The outer radiation layer

59

Molecules/atoms

60

Line area on the reflector

61

liquid pipe

62

a very small opening

63

Fluid circles

64

Return spring

65

Reset magnet

66

Cathode emitters / electron beam emitters

67

Electron beam

68

Guide tube for the mass body

QUOTES INCLUDED IN THE DESCRIPTION

This list of documents listed by the applicant was generated automatically and is included solely for the better information of the reader. The 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 20190295733 A1 [0028]
• EP 0438724 B1 [0029]
• DE 102012025244 A1 [0030]
• DE 3913503 A1 [0031]
• DE 102007022302 B4 [0032]
• DE 102017000653 A1 [0033]

Claims (42)

Radiation weapon, characterized in that it consists of at least - a high-pressure chamber which is filled with a fluid containing hydrogen isotopes, - a fluid high-pressure generator which can generate a very high pressure in the high-pressure chamber and which removes the fluid from the High-pressure chamber can displace in a flash, - two high-pressure fluid jet nozzles, which are coupled to the high-pressure chamber, which emit high-speed fluid jets which are directed towards each other at a distance from one another and which shoot against one another with very high energy and speed, which are partially at the collision point cause an atomic nuclear fusion of the hydrogen isotopes, with the fluid jet collision point taking place at a small distance from the nozzles and the angle of the flow directions of the two fluid jets being 180° or less, - a parabolic mirror or reflector, at the focal point of which the collision point of the two fluid jets directed towards each other, which reflects the electromagnetic radiation energy released by the fluid jet collision and the resulting nuclear fusion, bundled in one direction, - a tube that is connected to the parabolic mirror or parabolic reflector and through that is, the focused beam is emitted from the weapon, - one or more actuators that aim the weapon at a target, - a control system that controls the high-speed fluid jet generation. Beam weapon after Patent claim 1 , characterized in that the fluid in the high-pressure chamber consists of pure deuterium oxide or forms a mixture of deuterium oxide and tritium oxide. Beam weapon after Patent claim 1 or 2 , characterized in that the fluid in the high-pressure chamber consists of deuterium or tritium in liquid form. Radiation weapon according to one of the preceding claims, characterized in that the liquid high-pressure generator has a special high-pressure pump system consisting of at least: - a combustion chamber with very stable walls in which an explosive gas or gas mixture is injected by an injector, - a high-pressure chamber, which has massive walls made of very hard material, in which the liquid for fusion-reaction purposes is located, which is built directly under the combustion chamber, - a linear and firmly connected double piston, the first piston of which is a has a larger working surface and is attached to the combustion chamber and the second piston with a smaller working surface is inserted into the high-pressure chamber, the piston bodies being made of very stable material and moving in a common longitudinal axis, - consisting of an electrical ignition system consisting of a high-voltage generator and electrodes installed in the combustion chamber for the ignition of the gas or gas mixture located there, - two fluid lines that are coupled to the mutually directed nozzles, which direct the liquid from the high-pressure chamber to the nozzles when high pressure is reached , - a return system or a return spring or one or more permanent magnets that bring the piston into the starting position through magnetic field interaction as soon as the high pressure in the high-pressure chamber decreases. Beam weapon after Patent claim 4 , characterized in that the gas is an oxyhydrogen. Beam weapon after Patent claim 4 or 5 , characterized in that - the piston or a piston rod coupled to the, has an iron part or ferromagnet part - an electromagnetic coil is installed, which, via an electrical control, exactly at the ignition time of the combustion gas into the combustion chamber, also pushes the piston downwards Electromagnetic force pushes without contact, and thus causes force amplification, - the electrical control controls both the ignition in the combustion chamber and the electromagnetic coil at the same time. Beam weapon after one of the Patent claims 1 until 3 , characterized in that the fluid high-pressure generator consists of an electromagnetic coil and a piston that is pushed electromagnetically into the high-pressure chamber. Beam weapon after one of the Patent claims 1 until 3 , characterized in that the high-pressure generator is a special high-pressure pump system consisting of at least: - a high-pressure chamber with very stable walls, in which there is a long cylinder in the form of a piston made of stable material, which is vertically movable into the high-pressure chamber , - a mass body that can be moved quickly electromagnetically or pyrotechnically by expanding an explosion medium, which is thereby accelerated and hits the piston and thus exerts a pressure force on it, - a guide mechanism that guides the moving mass body until it impacts on the piston, - a liquid that is in the high-pressure chamber and contains hydrogen isotopes, - two fluid lines that are in the high-pressure chamber which lead the liquid during the pressing process through the piston outside the high-pressure chamber, which are nozzle-shaped at the outer end or are equipped with nozzles, each of which emits a jet of liquid that is directed at one point to meet one another. Beam weapon after Patent claim 7 , characterized in that the mass body is a solid cylinder or a sphere. Beam weapon after Patent claim 7 or 8th , characterized in that the piston is in the upper area outside the piston guide. Beam weapon after one of the Patent claims 7 until 9 , characterized in that the upper area of the piston has a disc made of a very hard material. Beam weapon after one of the Patent claims 3 until 10 , characterized in that instead of one high-pressure chamber, two such chambers are installed, each with a piston in it, each of which is filled with heavy and super-heavy water, the two liquids being displaced simultaneously from the two high-pressure chambers and being released against each other in the form of two liquid jets and at the collision point, the atoms of deuterium and tritium cause nuclear fusion. Radiation weapon according to one of the preceding claims, characterized in that the piston and its components and/or the high-pressure chamber consist of titanium alloys. Beam weapon after one of the Patent claims 1 until 3 , characterized in that the high-pressure generator is a special high-pressure pump system, consisting of at least one electrically driven flywheel, which is coupled to a power transmission system that abruptly brakes the flywheel and releases its kinetic energy to a piston that produces a pressure into a high pressure chamber on the fluid containing fusible elements, thereby creating two jets of fluid at the same time that collide with each other. Beam weapon after Patent claim 13 , characterized in that the power transmission system consists of electrically controllable actuators. Beam weapon after Patent claim 13 or 14 , characterized in that the piston is non-positively coupled to a diametrically arranged lever mounted on the same axis as the rotating disk. Beam weapon after Patent claim 15 , characterized in that an electromagnetically driven brake system is installed in the axis of the lever, which, when activated, connects the diametrically arranged lever and the rotating disk to one another in a force-fitting manner. Beam weapon after one of the Patent claims 13 until 16 , characterized in that the reaction time of the actuator, which creates a frictional connection between the rotating disk and the lever, is less than 1ms. Radiation weapon according to one of the preceding claims, characterized in that the fluid consists of liquid deuterium or tritium. Beam weapon according to one of the preceding claims, characterized in that the fluid jets do not meet in a straight line, but at an angle slightly smaller than 180°. Radiation weapon according to one of the preceding claims, characterized in that it has at least one microwave emitter which emits its microwave energy into the fluid jet collision point. Beam weapon after Patent claim 20 , characterized in that the microwave emitter generates microwave frequency at a frequency that is in vibrational resonance with the molecules in the fluid jets. Beam weapon after Patent claim 20 or 21 , characterized in that the microwave radiators are arranged in such a way that their microwaves penetrate into the longitudinal axes of the respective liquid jets in the form of two bundled directional beams and, like the liquid jets, meet at the same point. Beam weapon according to one of the preceding claims, characterized in that it is installed with two coherent microwave emitters offset from a common axis and both of which are capable of liquid jet collision irradiate a point at an angle that is smaller than 180°. Beam weapon after one of the Patent claims 20 until 23 , characterized in that the frequency and/or the intensity of the microwaves is adjustable. Beam weapon after one of the Patent claims 20 until 24 , characterized in that the distance of the microwave radiators up to the liquid jet collision point can be adjusted so that the phases of the microwaves in the collision point arrange the molecules of heavy or superheavy water in such a way that their hydrogen isotopes are directed at each other, for Arrive collision point. Beam weapon according to one of the preceding claims, characterized in that it is equipped with at least one high-voltage generator which emits an electrical discharge in the fluid jet collision point through electrodes. Beam weapon according to one of the preceding patent claims, characterized in that the two fluid jets impacting one another are under high voltage and are electrified differently. Radiation weapon according to one of the preceding claims, characterized in that the fluid in the high-pressure chamber is provided with an additive or an acid or another liquid which increases the electrical conductivity of the liquid. Jet weapon according to one of the preceding claims, characterized in that the liquid of the fluid jets forms an electrolyte. Beam weapon according to one of the preceding claims, characterized in that the reactor is equipped with at least one laser emitter, which is focused with its laser beam in the fluid jet collision point and emits a laser beam with high intensity. Radiation weapon according to one of the preceding claims, characterized in that the reactor is equipped with at least one X-ray emitter which is focused in the fluid jet collision point and emits an X-ray with high intensity. Radiation weapon according to one of the preceding claims, characterized in that the fluid is water or heavy water with hydrogen isotopes dissolved therein. Radiation weapon according to one of the preceding claims, characterized in that the fluid in the high-pressure chamber is an acetone or other fluid whose hydrogen atoms have been replaced by hydrogen isotopes or deuterium. Radiation weapon according to one of the preceding claims, characterized in that the fusion reactor has or is coupled to a high-voltage generator which electrically charges the fluid jets. Radiation weapon according to one of the preceding claims, characterized in that the fluid jets come into contact with high-voltage electrodes and are thereby electrically charged. Beam weapon after Patent claim 35 , characterized in that the fluid jets have different electrical charges. Radiation weapon according to one of the preceding patent claims, characterized in that in the upper region of the high-pressure chamber, at least one liquid line, which leads the liquid with hydrogen isotopes into the high-pressure chamber, is installed. Radiation weapon consisting of at least: - four statically installed high-pressure chambers, each of which is filled in pairs with a liquid that contains hydrogen isotopes that are suitable for nuclear fusion in the event of a rapid collision, which are arranged in pairs diametrically in a circle, - a liquid high-pressure generator that can generate a very high pressure in the high-pressure chambers, consisting of at least - two counter-rotating flywheels, which are installed on the same axis of rotation, the radius of which is similar to or larger than that of the circle that determines the arrangement of the high-pressure chambers - clamps or wedges or bolts arranged in pairs diametrically on the flywheels, which are installed in the periphery of the flywheels, which are electrically controlled by built-in electric actuators in the flywheels in a direction parallel to the axis of rotation of the flywheels, which are quickly released from the wide surfaces of the flywheels can be moved out, - an electronic control that precisely determines the time for moving out the striking parts, wedges or bolts and emits the execution signal, - a rotational position detection system for detecting the current position of the striking parts, wedges or bolts during the rotation of the flywheels, - two drive systems for the respective flywheels or a drive that rotates the two flywheels synchronously and in opposite directions at the same speed, - each two pairs of pistons, which are partially inserted into the statically installed, stable high-pressure chambers, the direction of movement of which is perpendicular to the axis of rotation of the flywheel and parallel to the flywheel, which are arranged radially in pairs to the flywheels, which, when the striking parts, wedges or bolts are out move out the flywheels, when a rotational position is reached, they are pushed into the high-pressure chamber at the rotational speed of the flywheels due to the torque of the flywheels and the pressure on the liquids in the high-pressure chambers increases in a flash, displacing the liquids from the high-pressure chambers with full force and can produce liquid jets with very high energy and speed, - four high-pressure fluid jet nozzles, which are coupled to the high-pressure chambers, which emit sharp, high-speed fluid jets that are directed at a short distance from each other, in pairs, and which shoot against each other , where the fluid jets contain hydrogen isotopes which, when sufficiently velocized and colliding with one another, lead to core meltdown, the fluid jet collision point occurs at a small distance from the nozzles and the angle of both fluid jets is 180° or less, - a fusion reactor chamber or a housing in which the reactor elements, the flywheels, the high-pressure chamber and the mutually directed nozzles are attached and in which the fusion reaction takes place, - an energy dissipation system that takes the energy generated by the fusion to the outside for use or storage - a control system that controls nuclear fusion processes. Beam weapon after Patent claim 38 , characterized in that the clamps or wedges or bolts installed diametrically in pairs on the flywheels are not installed in the periphery of the wide disk surface, but in the perimeter surface of the flywheels, which are electrically controlled by built-in electric actuators in the flywheels Radial direction of the flywheels can be moved out of the narrow surfaces of the flywheels at lightning speed. Beam weapon after Patent claim 38 or 39 , characterized in that the clamps or wedges or bolts installed in pairs and diametrically on the flywheel are coupled to an electrical trigger, which can be activated at the appropriate time by an electronic control, which can be moved out radially from the flywheel by the centrifugal force. Radiation weapon according to one of the preceding claims, characterized in that it is equipped with a cathode emitter or an electron beam generator which emits an electron beam at the collision point of the fluid jets.

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