Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 1 : What is a Looperator? / https://lnkd.in/dzw2nwH3
Combining the words 'loop' and 'operator', the term 'Looperator' refers to a revolutionary fusion technology. It uses the quantum mechanical properties of fermions and bosons to achieve permanent magnetic plasma confinement. The plasma container consists of four identical semicircular pipe bends surrounded by many evenly spaced ring- or spiral-shaped coils. The plasma volume enclosed by these coils is formed into a double helix by a multitude of magnetic field lines, each of which is designed as an endless loop. To fuse deuterium and tritium, the core temperature must be between 100 and 400 million degrees Celsius. The double helix contains a central magnetic field line (m1) around which a large number of eccentric magnetic field lines wind. Offsetting the magnetic field surfaces by a factor of four creates the double-helix structure of the plasma volume. This structure surrounds the central magnetic field line (m1) with stable, concentric, fluid-dynamic layers that have a decreasing temperature gradient from the inside to the outside. Before plasma ignites from its hot core, the heavy hydrogen isotopes — deuterium and tritium — exist as fermions. Deuterium consists of a proton, a neutron and an electron. Tritium consists of a proton, two neutrons and an electron. Both of these heavy isotopes belong to the category of fermions, which follow Fermi–Dirac statistics. However, this changes when the plasma ignites, as each isotope loses an electron. The resulting tritium cation (³H), known as a 'triton', has a nuclear spin of 1/2 due to its odd number of nucleons (one proton and two neutrons). Therefore, it remains a fermion. In contrast, the deuterium ion, or deuteron, has a nuclear spin of 1, as the spins of its proton and neutron (1/2 each) add up to a total spin of 1. As the magnetic field is stronger on the concave inner side than the convex outer side of the plasma volume, particles (+, -) gyrating around the magnetic field lines generate undesirable shear forces transverse to the plasma's flow direction. In a tokamak, these forces destroy the layer structure of the plasma within a short time. To reverse the spin deviation of fermions, particles must change their spin twice within one half of the double helix or one ring oscillation period. They must also change their spin four times within two periods to return to the same spin state at the start of an orbital revolution. However, in order for the spin deviation of fermions and bosons to be completely cancelled out within one ring oscillation period in one of the two mirror-image halves of the double helix, a helical magnetic field gradient is essential. This enables the plasma to be magnetically confined in the 'looperator' indefinitely. The beauty of the double helix is that the deuteron must complete two full revolutions to return to the same spin state at the beginning of an orbital cycle. A quantum mechanical mechanism within the double-helix-shaped plasma volume triggers a chain reaction in which the nuclei of the deuterium and tritium atoms fuse to form helium. This process releases a million fold more energy than any combustion process. To maintain the chain reaction and enable uninterrupted power production, a continuous fuel supply and efficient slag removal are required. This technology is set to usher in an era of abundant energy by enabling magnetic plasma to be confined on an unlimited scale. Nuclear fusion provides an additional energy source that is independent of the stochastic availability of solar and wind power. It will provide humanity with a plentiful energy supply, allowing us to flourish in an environment conducive to life and free from threats of migration and conflict caused by climate change.
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 2 : True Origin of the Double Helix / https://lnkd.in/ekbZFzCQ
Leonardo da Vinci designed a double helix staircase at the Château de Chambord in France even before the concept of the double helix became widely known through Watson and Crick's discovery of the structure of DNA. Construction of the staircase was completed in 1519. The proposed double helix for the 'Looperator' consists of a central magnetic field line m₁ and four semicircular arcs B with a radius r_B. The mirror-symmetric structure of the central magnetic field line m₁, depicted in yellow, encircles a central point M₁ and is located on the surface of a uniform transformation sphere with a radius R₁. The four semicircles B, depicted in blue, connect at four points J₁–J₄ in a common torque plane β′ and can be interpreted as two periods of ring-shaped, curved oscillation forming an endless double helix. The fusion reactor introduced in Chapter 1 has a tubular plasma volume with a radius r_P. A multitude of eccentric magnetic field lines, shown in IMPC 9, wind around the central magnetic field line m₁. In accordance with the first law of thermodynamics and driven by the inertia of the mass-carrying particles, these field lines oscillate regularly from inside to outside and back again within the tubular plasma volume. The magnetic field lines lie on the surface of a uniform virtual transformation sphere with a radius of r₁. These field lines consist of four curved elliptical arcs (B′₁–B′₄), each of which is connected to the others in the torque plane β′. Each arc has the same length as the semicircular arc B, and the maximum possible radius of the tubular plasma volume, r_P, is 1/2 x r_B.
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 3 : The Uniform Transformation Sphere / https://lnkd.in/ejKFBvqu
The spherical magnetic field of the proposed fusion reactor has a central guideline, depicted in yellow. This guideline represents the central magnetic field line (m1) of the 'Looperator'. The tubular plasma volume of the double helix has a layered structure arranged concentrically around four identical semicircles. These semicircles are connected to each other within a common angular momentum plane β', as detailed in the 'IMPC 4' article. Four exemplary eccentric magnetic field lines in different colours are shown on the outer surface of the plasma volume. As illustrated in Chapter 1, the Lorentz force induced by the Helmholtz coils creates a clockwise magnetodynamic flux within the plasma. These four magnetic field lines are characterised by elliptical space curves that are connected within the β′ angular momentum plane. Unwinding the magnetic field lines from the surface of the transformation sphere reveals that their length is precisely equal to that of the central magnetic field line. According to the first law of thermodynamics, this demonstrates the self-induced twist of the eccentric magnetic field lines. The Lorentz force is equal in both mirror-image halves of the double helix. These equal forces cause the magnetic field lines to oscillate regularly between the interior and exterior of the tubular plasma volume. This eliminates the need for poloidal coils. The collective interaction of electrons and ions with the magnetic field lines can be described mathematically using the Poincaré conjecture. This conjecture represents a Dirac group for fermions, characterised by three geometric operations: the Lorentz transformation, translation, and rotation. Chapter 4 explains a second quantum mechanical effect that exploits the inertia of fermions.
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 4: How to Twist the Magnetic Field / https://lnkd.in/dGEwtb-m
As the English philosopher and statesman Francis Bacon (1561–1626) once said, 'Natura non nisi parendo vincitur' – 'Nature can only be conquered by obeying it.' In keeping with this idea, the 'Looperator's' quadruple magnetic field offset prevents unwanted turbulence in the plasma. The chiasma of intersecting, endless loops — a feature also found in a Möbius strip — causes the magnetic field lines to twist without any further intervention. The video shows how the red arrows at the corners of the torque plane generate a torque that twists the magnetic field lines within the plasma volume due to the mass of charged particles. In a spherical, endless loop, four magnetic field lines on the outer surface of the tubular plasma volume are arranged at radial distances from one another, alternating regularly from inside to outside the plasma tube. In the torque plane (β'), the four magnetic field planes of the plasma volume are connected at connection points (J1–J4). Both mirror-image halves of the double helix are driven by the Lorentz force, with electrons (red) and ions (blue) moving along magnetic field lines in spiral paths at an orbital velocity of approximately 1,000 km/s. This does not include the speed of their gyral oscillation. As subatomic particles have mass, they are subject to centrifugal force. These forces are depicted by white arrows for negatively charged particles and black arrows for positively charged particles. The arrows are coplanar with their respective magnetic field plane. When the gyration speed resulting from a gyration frequency of 10⁻¹¹ is added to the orbital speed of 1,000 km/s, the particles move close to the speed of light. This gives them a strong enough gravitational impact to twist the magnetic field lines. The asymmetry of the magnetic field induces an electric field that exerts transverse forces on positively and negatively charged particles, causing them to move away from each other in opposite directions. As shown by the blue arrow for positively charged particles and the red arrows for negatively charged particles, this undesirable effect can be fully compensated for within the four magnetic field planes of the plasma volume. Each plane is offset by 90 degrees relative to the others. Chapter 5 provides a detailed explanation of how the electric field generated by the gyration of charged particles affects the stability of plasma confinement. In tokamak experiments, the layered structure of the plasma is quickly destroyed by increased shear flows. For this reason, tokamak experiments have a relatively short operating time. The 'Looperator' was developed to enable permanent magnetic plasma confinement. This is thanks to its exceptional ability to keep charged particles on course.
#resuft #Looperator #resmpc4 #resfusion4 #resfluiddynamic #plasmaphysics #teamres #heureka
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 5: Dynamic Model of Quantum Gravity / https://lnkd.in/dChP_Gs4
The 'Looperator' was developed to keep negatively (red) and positively (blue) charged particles, which move in opposite directions along magnetic field lines due to an electric field induced by magnetic field asymmetry, on their respective trajectories. This functional requirement can be explained using classical physics and knowledge at secondary school level. Furthermore, the ‘Looperator’ introduces a dynamic model of quantum gravity for the first time, significantly simplifying the explanation of the functional requirement for sustained plasma confinement. Let us first consider the simpler explanatory model. As shown in Chapter 1, the arrangement of the Helmholtz coils determines the magnetic field. Starting from the central trajectory — the guideline of the tubular plasma volume shown in yellow — the video demonstrates how electrons and ions move in spirals along the magnetic field lines at a speed of 1000 km/s. They form closed loops along these spiral paths by following the magnetodynamic flow direction, which is determined by the current induced by the Helmholtz coils. The magnetic field is stronger on the concave inner surface of the four semicircular arcs surrounding the plasma vessel than on the convex outer surface, since the distance between the Helmholtz coils is smaller on the inner surface. This asymmetry distorts the Larmor angle, which defines the gyration radius. Consequently, positively and negatively charged particles orbit the magnetic field lines with a smaller inward-facing radius and a larger outward-facing radius. The different charges of subatomic particles also cause them to orbit the magnetic field lines in opposite directions. This creates an electric field perpendicular to the magnetic field plane. These gyral, transverse forces cause electrons and ions to move away from the magnetic field line in opposite directions. These forces are represented by the red and blue arrows in the video. During the orbital revolution of electrons and ions, these forces cancel each other out. This innovative approach achieves exceptional track stability for both positively and negatively charged subatomic particles, eliminating the need for additional poloidal coils. The following section presents a dynamic quantum mechanical model that explains the track stability of fermions and bosons within a generally applicable orbital model. Electrons, positrons and tritium nuclei ('tritons') are characterised by their intrinsic half-integer spin. To return to the same spin state at the starting point within a single orbit defined by two periods of a standing wave, they require a fourfold change in spin direction. By contrast, a boson requires only a twofold change in spin direction to return to the same spin state within a single orbit. When the plasma is ignited, the deuterium atom loses an electron. This changes its spin quantum number from 1/2 to 1, transforming it into a boson known as a deuteron. This change in spin direction also satisfies Ampère's law, which states that an electric current generates a magnetic field around itself. The line integral of the magnetic field strength along a closed curve corresponds to the total current flowing through the four arcs of the 'Looperator'. According to Newton's fourth law, one of Maxwell's equations establishes a direct relationship between magnetic flux density and electric current. The video shows how four magnetic field planes, offset by 90 degrees, ensure tracking, even for a boson. Electrons and ions drift the most when passing through two arcs, and reverse completely when passing through two more. This results in the electrons and ions being perfectly tracked within the plasma, which is a prerequisite for time-limited magnetic plasma confinement. Chapter 6 provides a more detailed explanation of the ECE theory, which predicts a 20% increase in efficiency for the quantum mechanical explanatory model of the Looperator.
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 6: The Directional Stability of the Deuteron / https://lnkd.in/dHHX_Hvm
Fermions, named after Enrico Fermi, are a group of subatomic particles with odd, half-integer spin values. In contrast, bosons such as photons, gravitons and the nucleus of a deuteron have even spin values (zero, one or two). The 'Looperator's' plasma chamber contains a magnetic field composed of four semicircular magnetic field planes, each offset by 90 degrees relative to the others. The number of magnetic field lines within each magnetic field plane that are interconnected within a common angular momentum plane β depends on the diameter of the plasma tube. The video exaggerates the restoring effect of gyral drift on negatively charged electrons and positively charged deuterons moving in opposite directions. This is demonstrated using an example of an eccentric magnetic field line, whose trajectory is shown in yellow on the outer surface of the tubular plasma volume. In order to achieve time-unlimited plasma confinement with minimal effort, it is necessary to take into account two advantageous properties of the double helix. Firstly, the chiasma of the magnetic field lines causes them to regularly alternate between the inner and outer surfaces of the tubular plasma volume. This effect is comparable to a Möbius strip. Secondly, displacement of the four planes of the plasma vessel causes the magnetic field lines to lie on the surface of a sphere with a uniform radius around their respective centres. The field lines twist as they transition from the exterior to the interior and vice versa. These two properties affect the plasma volume, causing the magnetic field lines to twist. Electrons (-) and ions (+) have different charges and can move along the field lines at speeds of up to 1,000 km/s. By simultaneously orbiting the magnetic field line at a frequency of 10⁻¹¹ Hz, they generate an electric field that is perpendicular to the magnetic field plane. Since the magnetic field is stronger on the concave inner side of a semicircular arc of the plasma volume than on the convex outer side, the electrons and ions follow magnetic field lines with different gyration radii. These radii are tighter on the inner side and wider on the outer side. This creates an electric field that causes the particles to move away from their respective field lines in opposite directions, perpendicular to the four magnetic field planes. According to the three-finger rule, which explains how an electric field is induced perpendicular to the magnetic field plane, the red electron moves away from the yellow trajectory in the direction indicated by the red arrow, while the blue deuteron moves away from the yellow trajectory in the direction indicated by the blue arrow. Regarding an orbital path, the transverse forces acting on negatively charged particles (such as electrons) and positively charged particles (such as ions or deuterons) cancel each other out. This means that the particles follow the magnetic field lines as if guided along railroad tracks. A fluid dynamic equilibrium is established within the plasma volume by Helmholtz coils surrounding the plasma vessel at regular radial intervals. For the gyral drift of fermions and bosons to be cancelled out completely within a single period of the double helix, the gradient of the helical field lines is crucial. The video shows how the gyral drift of an electron and a deuteron cancels itself out completely within one orbital revolution, characterised by two periods of a standing wave. This ensures that the plasma in the looprator remains magnetically confined indefinitely.
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 7: Why the Magnetic Field Lines Twist / https://lnkd.in/dcSQEUuy
Chapter 1 introduces Helmholtz coils that are arranged at regular intervals and are perpendicular to the direction of the Lorentz force. The coils are also concentric with the central magnetic field line m1. These coils are located around the four semicircles of the plasma vessel. The arcs are offset by 90 degrees relative to one another and fit into a surrounding virtual cube. According to conventional magnetohydrodynamics (MHD), one would expect a concentric arrangement of magnetic field lines with different radii, as shown in the video on the left-hand side of the plasma volume. These field lines are considered stationary. Therefore, in both a tokamak and a stellarator, positively and negatively charged particles move away from the magnetic field lines. It is widely accepted that plasma weighing only a few grams in an experimental reactor cannot deflect a magnetic field with a strength of 2 to 15 tesla. However, the latest research results show that the regular change in the particles' spin, together with their velocity of 10¹¹ km/s, can deflect magnetic field lines. This phenomenon can be observed in coronal mass ejections from the Sun and in ball lightning. According to Einstein-Cartan-Evans (ECE) theory, the magnetic field lines on the right-hand side of the plasma volume shown in the video are twisted and lie on the surface of a uniform transformation sphere with the same radius. Based on torsion and curvature in the 'Looperator', particles (+, −) can bend magnetic field lines — a magnetohydrodynamic effect amplified by the fourfold change in the spin direction of fermions in an orbital circle. This satisfies Ampère's law, also known as the law of flux. The strength of the magnetic field along the double-helix magnetic field lines corresponds to the total current flowing, with a fourfold change in spin direction for fermions and a twofold change for bosons. This law is one of Maxwell's equations, establishing a direct link between magnetic flux and electric current. The mathematical framework required to demonstrate the assumption of self-induced torsion of magnetic field lines can be found in the book 'Principles of ECE Theory': A New Paradigm in Physics, published on 1 September 2016 by Myron W. Evans, Horst Eckardt, Douglas W. Lindstrom, and Stephen J. Crothers. Chapter 3, page 77, heading 'ECE THEORY AND BELTRAMI FIELDS': 'Every plane wave solution corresponds to two circularly polarised waves propagating in opposite directions and combining to form a standing wave. This standing wave does not possess the standard properties of linearly or circularly polarised waves with E ⊥ B, since the combined Pointing vectors of the circularly polarised waves cancel each other out, similar to the situations previously described in connection with Beltrami plasma vortex filaments." In essence, the combination of these two waves produces a standing wave with non-zero magnetic helicity. Marsh's book [1] also explores the relationship between helicity and energy densities in this context. It reveals the fascinating fact that any magnetostatic solution to the FFMF equations can be used to construct a solution to the Maxwell equations when E is perpendicular to B (see Chapter 8, 'Cosmology', for an illustration on page 233 showing that the velocity curve of a spiral galaxy resembles a Möbius strip). G. E. Marsh, Force-Free Magnetic Fields, World Scientific, Singapore, 1994. Waves with E ⊥ B are possible, as the combined Pointing vectors of circularly polarised waves cancel each other out in a manner similar to that of Beltrami plasma vortex filaments. [1] G. E. Marsh, Force-Free Magnetic Fields, World Scientific, Singapore, 1994.
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 8: The Four Magnetic Field Planes / https://lnkd.in/dBWsSxey
As demonstrated in the video on the left, the 'three-finger rule' clearly explains how fermions and bosons move along the double helix-shaped magnetic field lines within the plasma volume. While the thumb points in the direction of electron (-) and ion (+) flow along the curved magnetic field lines, the index finger, held perpendicular to the thumb, points in the direction of the magnetic field. According to Ampère's fundamental law of electrodynamics, a current flowing in a closed circuit induces a magnetic field with closed magnetic field lines. This is also the case in the plasma of a fusion reactor. Perpendicular to this magnetic field, the Lorentz force (represented by the middle finger) acts to move electrons (-) and ions (+) away from the magnetic field lines in opposite directions. They circle the magnetic field lines in spiral paths at a frequency of 10⁻¹¹ Hz. They complete one orbital revolution at a speed of 1,000 km/s within two periods of a standing wave. The asymmetry of the magnetic field causes the electrons and ions to move away from each other along the gradients of the double-helix magnetic field lines within two arc-shaped segments of the plasma volume. Conversely, they require a further two arc-shaped segments to move towards each other again. As the four magnetic field planes are offset by 90° relative to each other, the gradient of a double-helix magnetic field changes direction four times. This means that two periods of a standing wave are required for the gyral deflection of fermions and bosons to reverse completely. The inertia of massive particles subjected to an abrupt change in the direction of the Lorentz force within the torque planes spanned by the four magnetic field planes causes the deflection due to shear forces acting perpendicular to the field direction to reverse completely within two periods of the standing wave. This applies to fermions with a spin quantum number of 1/2 and to bosons with a spin quantum number of 1, meaning that the particles essentially follow the magnetic field lines as though they were railway tracks. In a tokamak, additional poloidal coils are required to counteract the particles' transverse drift by twisting the magnetic field. In stellarators, the same result is achieved using an extremely complex zigzag pattern of coils. However, the magnetic field geometry in the Looperator is designed so that particle guidance can be achieved solely through Helmholtz coils, rendering additional coils unnecessary. This approach aligns with Buckminster Fuller’s philosophy: ‘Don’t fight forces, use them instead!’ The video on the left illustrates the quantum mechanical approach to achieving perfect plasma stability. The gyration drift of an ion within a ring oscillation consisting of two periods cancels itself out within a single oscillation period. Consequently, the ion exhibits stable behaviour in the plasma. In order to twist the magnetic field lines using only Helmholtz coils and eliminate the transverse drift caused by particles spiralling around the field lines, the spin of the particles must change from 'up' to 'down' twice within a single rotation period. This causes the plasma to twist the magnetic field lines torsionally. Maxwell's fourth equation describes how currents flowing in an electric field influence the magnetic field. However, these equations do not immediately reveal that variable currents can generate light and radiation. In order for the flux law in a vacuum to be satisfied in the 'Looperator' plasma, the magnetic field lines described in Chapter 5 must cause the ions and electrons to travel on identical paths through the two mirror-image halves of the plasma volume.
#resuft #Looperator #resmpc8 #resfusion8 #solution4fusion #plasmaphysics #teamres #heureka
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 9 : Making the Plasma Structure Visible / https://lnkd.in/dwfGymRs
As discussed in Chapter 1, the Helmholtz coils are arranged in a concentric pattern around the central magnetic field line within the plasma vessel. They comprise four equal semicircular arcs. These coils cause multiple magnetic field lines to wind helically around the central field line m₁ within the plasma volume. The video shows twelve exemplary magnetic field lines on the outer surface of the plasma volume, each lying on a virtual uniform transformation sphere. In the two mirror-inverted halves of the double helix, the field lines regularly change direction, moving from the inside to the outside of their respective field layer and back again. This means they are exactly the same length. To twist the magnetic field lines using only regularly spaced Helmholtz coils and reverse the spin deviation of fermions, the spin of the particles must change four times within one orbital revolution, representing two periods of a standing wave. However, a magnetic field gradient is essential to fully cancel the spin deviation of fermions and bosons within one oscillation period of the double helix. This enables the plasma to be magnetically confined in the 'Looperator' indefinitely. Since the Lorentz force is equal in both halves of the plasma volume, the magnetic field lines automatically twist, eliminating the need for additional coils to manipulate the magnetic field. As shown in Chapter 9, the central magnetic field line determines the trajectory of the plasma volume. The radius of the tubular plasma volume corresponds to the amplitude of the circular standing wave, which has two periods. As temperature and pressure increase due to the central magnetic field, the oscillation frequency rises from the cooler exterior to the hotter interior. Temperatures in this region can reach between 100 and 400 million degrees Celsius. According to the Lorentz transformation, the amplitude of this spherical oscillation corresponds to the radius of a virtual sphere centred on the 'locator'. The double helix effect is similar to that of a Möbius strip. At the connection point, two evenly spaced lines alternate between the inside and outside. This invention is an induction system for a spherical magnetic D-T fusion field, offering significant advantages over existing technology. The 'Looperator' features precise magnetic field topologies arranged in concentric layers that are more accurate than those of the Wendelstein 7-X stellarator experiment. The video shows twelve magnetic field lines of the spherical magnetic field, which can be made visible inside the vacuum of the plasma chamber. As in the Wendelstein 7-X experiment, this is achieved by injecting an electron beam along the magnetic field lines. The beam follows these lines and maps them, enabling an accurate 3D model of the expected magnetohydrodynamic processes to be created..
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 10 : Chapter 10 : Structure and Scalability / https://lnkd.in/e8aApViG
The plasma container consists of identical circular or oval modules. These modules are arranged concentrically around the central magnetic field line (M1) and the centre of the plasma volume. The modules are bounded by inner and outer radii around M1. The modules can be bolted or welded together to form four arc-shaped units. As described in Chapter 1, the magnetic field generated by the Helmholtz coils suspends the plasma volume at a distance from the blanket to ensure that it does not come into contact with the inner shell of the double-walled plasma vessel formed by the blanket. The Helmholtz coils are assigned to individual container modules. The radial and longitudinal distances between the coils are defined by the sector angles around M1, the centre point of the fusion reactor. The central magnetic field line (M1) of the fusion reactor is surrounded by a large number of concentric layers, each containing decentralised magnetic field lines with analogous connection and vertex points. Once the plasma has been ignited, the heavy hydrogen isotopes, deuterium and tritium, each lose one electron. Triton, the cation of tritium, remains a fermion with an odd number of nucleons. In the video, it is depicted as a blue sphere moving along a magnetic field line on the exterior of the plasma volume. As described in Chapter 5, its gyration radius occupies the space indicated by the dark and light stripes on the outer surface of the plasma. However, during this process, the deuteron (the cation of deuterium) becomes a boson with an even number of nucleons. The direction of fluid dynamics and the orientation of the angular momentum axes and planes of fermions and bosons are determined by the Lorentz force. At least one zero line, located between the connection points of the central magnetic field line m1, divides a ring oscillation into two mirror-image halves. This differentiation occurs within the individual layers of the plasma volume. Each layer has specific frequencies, and the frequency band of these oscillations ranges from 50 Hz at the outer edge of the plasma volume to several kilohertz around the hot centre, defined by the m1 trajectory. Fermions and bosons follow magnetic field lines so precisely that a plasma vessel with a diameter of between 0.3 and 0.4 metres can be used to ignite plasma. This enables the construction of compact fusion reactors, including their power supply and energy conversion systems. Such reactors can therefore be installed on Earth, in space and on vehicles, particularly watercraft.
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 11 : Time is Looped / https://lnkd.in/ebFGJCNG
The 'Looperator' tubular plasma volume has a double helical shape comprising two mirror-symmetrically arranged S-shaped curves, each representing one period of spherical vibration. The frequency of double helical oscillations over two periods of the 'Looperator' is a temperature-dependent measure of time. The progression of this time depends on the temperature and density of the elementary particles within the layered, tubular plasma structure. In other words: Time only exists in the frequency of oscillations, which depend on temperature and the density of matter. Within the layers of the 'Looperator's' double-helical plasma tube, a macroscopic orbital model can be observed in which a uniform transformation sphere defines equal-radius, equal-length orbits for fermions and bosons. As illustrated in Chapter 5, fermions follow magnetic field lines in endless spiral loops. This regularity is evident in the decentralised magnetic field lines of the outer plasma layer, which are displayed in different colours, as well as in the central red magnetic field line. The gyration radius of electrons and ions is represented by the thickness of the coloured lines in the outermost layer of magnetically confined plasma in a double-helix plasma container. Chapters 1 to 6 demonstrate how these spherical oscillations can be used to confine plasmas magnetically on a permanent basis. In cosmological terms, the ring-shaped vibration of elementary particles constitutes a scalar field forming the background of the universe. The number of zero crossings in an even number of periods of these vibrations can be used to measure time. This number is affected by the different temperatures in the universe. Time passes more slowly in empty space than in areas where matter has condensed into a spongy structure. However, time passes infinitely quickly inside a black hole. This temperature-dependent measure of time can also be observed in living organisms: for example, an ice shark can live for several hundred years, whereas a mouse's lifespan is only a few years — not to mention that of a mayfly. Two periods of spherical ring vibration are also essential for creating a new orbital model for chemical elements. The regular change in electron spin within an orbital — whether s, p, d or f — is vital for the electromagnetic neutrality of atoms. Exceptions include incompletely filled orbitals, which are element-specific. Without this neutrality, electrons would interact chaotically, preventing the formation of chemical compounds. The aim is to integrate the new orbital model with the residence probability determined by Schrödinger's equations within a spherical model.
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 12 : Lorentz Transformation / https://lnkd.in/ebzkEmeb
Precise length measurements show that the yellow path representing the central magnetic field line m1 is exactly the same length as the eccentric magnetic field line around which the blue ion will rotate. Since the central magnetic field line consists of four flat semicircles with radius r_B, its length can easily be calculated. As all magnetic field lines lie on the surface of a virtual transformation sphere with the same radius, the magnetodynamic flow dynamics of the 'Looperator' undergo a Lorentz transformation, which combines three geometric operations: a Lorentz transformation, a translation and a rotation. As illustrated in Chapter 2, the four magnetic field planes of the double-helical plasma volume are offset by 90° from one another and are connected at four points within a shared angular momentum plane (β'). The flat semicircles of the yellow trajectory lie on the surface of a central transformation sphere defined by the x, y and z axes. For a given radius of the transformation sphere, the length of the central magnetic field line is 4π, which is equivalent to twice the circumference of a circle with the same radius. In the outermost layer of the plasma volume, two magnetic field lines equidistant from each other are shown. These field lines are at their maximum and minimum distances from the centre M1 of the fusion reactor, located at the vertices of their double helical orbit. At the four connection points in the β′ angular momentum plane, the precession of the fermions and bosons dissolved in the plasma causes them to change from an up spin to a down spin four times in order to return to their starting point with the same spin state within an orbit. Conversely, the twisting of the magnetic field lines is caused by the chiastrum of the endless loops, which can be likened to a Möbius strip. Here, two equidistant lines regularly alternate between an outer side that is maximally distant from the centre and an inner side that is minimally distant from it. In order to twist the magnetic field lines using Helmholtz coils alone and largely eliminate the counter-rotating gyration deflection of fermions caused by the electric field induced by gyrating particles around magnetic field lines, the particles must change spin twice within one double helix period. The helical line gradient of the double helix is sufficient to reverse the gyration drift of fermions and bosons within a ring oscillation period, which is defined as half a double helix period. Chapter 9 will provide a more detailed examination of the boson circuit, explaining its function and role.
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Induction System for a Spherical Field Magnetic Fusion Reactor
The inner core of the tubular plasma has a temperature ranging from 100 to 400 million degrees Celsius. How can this heat be transferred to the water circulating between the inner and outer shells of the plasma container? The double-shell steel plasma container acts as a heat transfer device, absorbing heat from the plasma. It is equipped with eight magnetic coils, each of which has two magnetic poles lying opposite each other on the inner shell. These coils can be operated using both alternating and direct currents. A sophisticated circuit enables temporary contact to be established between the electrically conductive plasma volume and the inner shell of the plasma vessel. This facilitates the transfer of heat to the 'blanket' via thermal conduction. The 'blanket' is a layer on the inner shell of the plasma vessel that faces the plasma. Charged particles respond collectively to the attraction or repulsion exerted by the opposite poles of the magnetic coils. This influences the trajectory of the magnetic field lines. In a coordinated circuit of magnetic coils, the tubular plasma volume can be briefly brought into contact with the inner shell of the plasma vessel, enabling heat to be transferred by thermal conduction.
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 14 : Double Helical Heat Transfer / https://lnkd.in/e2raeTWn
The heat transfer helix is designed to heat water. Helical ribs located between the inner and outer shells of the plasma vessel facilitate this process. The fusion reaction provides the thermal energy that ensures wet steam leaves the coil at the top. Outside the coil, a superheater further heats the steam until it becomes dry, superheated steam containing no liquid droplets. This steam can then be used to drive turbines or be fed directly into a district heating network to heat buildings. Superheated steam has a temperature significantly above the saturation temperature of water, typically ranging from 300 to 600 °C. Due to its high temperature, superheated steam does not condense immediately upon cooling, making it ideal for driving steam turbines. The double-shell plasma vessel transfers heat from the outer layer of plasma, which is several thousand degrees hot, to a heat transfer fluid (ideally water). The plasma vessel consists of four identical arcs, each with an inner shell facing the plasma volume and an outer shell arranged at a radial distance from the inner shell. Water circulates in the duct space between the shells, which is approximately 15–20 cm thick. The fusion reactor has an inlet at the bottom and an outlet at the top for the heat transfer fluid. These can be used as the supply or return line. Due to their connection by ribs, the inner and outer shells act as thermally activatable masses. Water is transported from the inner shell to the outer shell of the fusion reactor through the duct space between the ribs of the left and right halves. This is achieved by twisted steel ribs with a helical pitch that transport water from the inner to the outer shell via an S-shaped route. Since the ribs form a monolithic composite with the inner and outer shells, heat is transferred from the entire plasma vessel to the heat transfer fluid. As shown in the video, the ribs twist once per period. An alternative method would involve achieving a fourfold twist using the central trajectory of the fusion reactor (depicted in yellow) between its four connection points and four vertices. This fourfold change would correspond to the fermions' fourfold change of spin from up to down within the plasma volume. The gradient of the double helical magnetic field lines reverses particle deflection completely within one period of annular oscillation. This ensures the tracking accuracy of the particles by eliminating unwanted shear forces within two periods of annular oscillation. In a tokamak, poloidal coils twist the magnetic field to compensate for the particles' transverse drift. Some stellarators eliminate transverse drift by employing an extremely intricate zigzag pattern of magnetic field lines. In the 'Looperator', however, it is the particles' intrinsic angular momentum that twists the magnetic field lines. This approach aligns with the philosophy of American architect and engineer Buckminster Fuller, who said, "Don't fight forces; use them instead!" .
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