Chapter 1: 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 plasma vessel at the top. Outside the vessel, a superheater further heats the steam until it becomes dry, superheated steam that contains 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 that faces the plasma volume and an outer shell that is 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 supply or return lines. Due to their connection by ribs, the inner and outer shells act as thermally activatable masses. Water is transported from the inner shell (23) to the outer shell (24) of the plasma vessel (20) through the duct space between the left and right halves' longitudinal ribs (25). Twisted steel ribs with a helical pitch transport water from the inner shell (23) to the outer shell (24) via an S-shaped route. Since the ribs (25) are a monolithic composite with the inner and outer shells of this heat transfer system (6), heat is transferred from the entire plasma vessel (20) to the heat transfer fluid. As shown in the video, the ribs twist once per period. An alternative method would involve a fourfold twist using the central magnetic field line (m1, depicted in yellow) as a trajectory between four connection points (J1–J4) and four vertices (V1–V4). This fourfold change corresponds to the fermions' fourfold spin change (s, s') from up to down within the plasma volume (2). The gradient of the double helical magnetic field lines reverses particle deflection completely within one period of annular oscillation (T, T'). 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 using an intricate zigzag pattern of magnetic field lines. In the "Looperator," however, the particles' intrinsic angular momentum 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!"
#resmpc1#resuft #Looperator #resmpc1 out of hashtags resmpc1 to resmpc14 #resfusion14 #heattransfer #plasmaphysics #teamres #heureka
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 2: The Origin of the Double Helix, https://lnkd.in/eiCbPWuT
Leonardo da Vinci designed the double-helix staircase at the Château de Chambord in France long before Watson and Crick popularized the concept through their discovery of DNA's structure. Construction of the staircase was completed in 1519. However, the double helix of the "Looperator" is not formed by four semicircular arcs with radius r_B. Rather, it arises in the magnetic field generated by the Helmholtz coils (Q1–Qn), which are shown in Chapter 1. The central magnetic field line (m1) of the tubular plasma volume (2), shown in red, consists of four semicircular arcs (B), each offset by 90° relative to the next. All of the arcs have the same radius (rB), and they are interconnected within a common torque plane (β′). The four arcs lie on the surface of a transformation sphere with a radius of r₁ and can be understood as two periods (T and T') of an annular oscillation. The fusion reactor (1) described in Chapter 1 has a tubular plasma volume (2) with a radius (r1) for the central magnetic field line (m1). A multitude of eccentric magnetic field lines (m2) coil around the central trajectory of the plasma volume (2) represented by the magnetic field line (m1), as shown in Chapter 9. In accordance with the first law of thermodynamics and driven by the inertia of the mass-carrying particles (+, -), the magnetic field lines (m2-mn) oscillate regularly from the inside to the outside and back within the tubular plasma volume (2) along the endless loops of a double helix (3). In doing so, the magnetic field lines (m1, m2-mn) lie on the surface of a virtual transformation sphere with radius (r1). The field lines (m2) consist of four curved elliptical arcs (B′) that are connected to one another in the torque plane (β′). Each arc (B′) has the same length as a semicircular arc (B). The maximum possible radius of the tubular plasma volume is given by (r2 = 1/2 ×rB).
#resmpc2 #resuft #Looperator #ResFusion2 #ResGeometry #Solution4Fusion #PlasmaPhysics #eureka
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Chapter 3: The Uniform Transformation Sphere, https://lnkd.in/ejKFBvqu
The spherical magnetic field of the proposed fusion reactor contains a central magnetic field line (m1, depicted in yellow), which lies on the surface of a uniform transformation sphere. This is referred to as the central trajectory of the plasma volume. The tubular plasma volume has a layered structure arranged concentrically around four identical semicircles formed by the central magnetic field line (m1). These semicircles are connected to each other within a common angular momentum plane (β'), as detailed in Chapter 4. The double helical shape of the magnetic field is exemplified by four eccentric magnetic field lines lying on the outer surface of the tubular plasma volume and depicted in different colors. As illustrated in Chapter 1, the Lorentz force induced by the Helmholtz coils creates a clockwise magnetohydrodynamic flux within the plasma. These four magnetic field lines are characterized by elliptical space curves connected within the angular momentum plane (β′) . 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 (m1). The curvature of the magnetic field lines (m1, m2-mn) results from equal forces in both halves of the plasma volume (2) and can be described mathematically using Jacobi functions. According to the first law of thermodynamics, the magnetic field lines oscillate regularly between the interior and exterior of the tubular plasma volume. This eliminates the need for additional poloidal coils. Thus, the self-induced twist of the magnetic field lines in both mirror-image halves of the plasma volume can be explained by the first law of thermodynamics. The collective interaction of electrons and ions with the magnetic field lines can be described mathematically using Poincaré's conjecture. This conjecture introduces a Dirac group for fermions, which is characterized by three geometric operations: Lorentz transformations, translations, and rotations. Chapter 4 describes a second quantum mechanical phenomenon that takes advantage of the inertia of fermions.
#resmpc3 #resuft #Looperator out of hashtags resmpc1 to resmpc14 #resfusion3 #resgeometry #solution4fusion #plasmaphysics #teamres #heureka
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Induction System for a Spherical Field Magnetic Fusion Reactor
Chapter 4: Twisting the Magnetic Field Lines, https://lnkd.in/dGEwtb-m
As the English philosopher and statesman Francis Bacon (1561–1626) said, "Natura non nisi parendo vincitur," which means "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 (X), consisting of intersecting, endless loops — a feature also found in a Möbius strip — causes the magnetic field lines (m1, m2-mn) to twist without further intervention. The video shows how red arrows at the corners of the torque plane generate a torque that twists magnetic field lines within the plasma volume due to charged particle mass. In a spherical, endless loop, four magnetic field lines (mn) on the outer surface of the tubular plasma volume (2) 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). In both mirror-image halves of the the four semicircular arcs (B, B') , electrons (red) and ions (blue) move along double helical magnetic field line trajectories (m₂) in spiral paths at an orbital velocity of approximately 1,000 km/s. This motion is driven by the Lorentz force. This does not include the speed of their gyral oscillation. Since 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, which is defined by the four semicircular arcs (B, B') of the tubular plasma volume (2). The particles move even faster when the gyration speed resulting from a gyration frequency of 10⁻¹¹ Hz is added to the orbital speed of 1,000 km/s. This does not take into account the speed of their gyral oscillation. Since 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, which is defined by the four semicircular arcs (B1–B4) of the tubular plasma volume (2). When the gyration speed resulting from a frequency of 10⁻¹¹ Hz is added to an orbital speed of 1,000 km/s, the particles move faster. 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 is compensated for as the particles orbit through the four magnetic field planes defined by the semicircular arcs (B, B'). 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 plasma confinement stability. In tokamak experiments, the layered structure of the plasma quickly breaks down due to increased shear flows. For this reason, tokamak experiments have a relatively short operating time. The "Looperator" was developed to enable permanent magnetic plasma confinement. It has an exceptional ability to keep charged particles on course.
#resmpc4 #resuft #Looperator #resmpc4 #resfusion4 #resfluiddynamic #plasmaphysics #teamres #heureka
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Induction system for a spherical field magnetic fusion reactor
Chapter 5: The Dynamic model of quantum gravity, https://lnkd.in/dChP_Gs4
The "Looperator" was developed to keep negatively (red) and positively (blue) charged particles on their respective trajectories. Due to an electric field induced by magnetic field asymmetry, these particles move in opposite directions along magnetic field lines. To explain particle track fidelity in quantum electrodynamic terms, one may first apply the three-finger rule. Building on this, 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. First, let us consider the simpler explanatory model. As shown in Chapter 1, the arrangement of the Helmholtz coils (Q1–Q32) determines the magnetic field. Starting from magnetic field line m1—the central trajectory of the tubular plasma volume's magnetohydrodynamic behavior—the video demonstrates how electrons and ions move in spirals at a speed of 1,000 km/s along this field line. They form closed loops along these spiral paths by following the magnetodynamic flow direction, which is determined by the magnetic field induced by the Helmholtz coils. The magnetic field is stronger on the concave inner surface of the four semicircular arcs (B, B') surrounding the plasma vessel than on the convex outer surface because the distance between the Helmholtz coils is smaller on the inner surface. This asymmetry distorts the Larmor angle, which defines the particle gyration radius. Consequently, positively and negatively charged particles orbit the magnetic field lines at different radii, facing inward and outward, respectively. Different charges on subatomic particles cause them to orbit magnetic field lines in opposite directions. This creates an electric field perpendicular to the magnetic field plane. These gyral, transverse forces then cause electrons and ions to move away from the magnetic field line in opposite directions. The red and blue arrows in the video represent these forces. During one orbital revolution, 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 characterized by their intrinsic half-integer spin. In order 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 deuteron, a type of boson. This change in spin direction 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 semicircular arcs (B, B') 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, 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.
#resmpc5 #resuft #Looperator out of hashtags resmpc1 to resmpc14 #resfusion5 #resfluiddynamic5 #Looperator #solution4fusion #plasmaphysics #resorbital #teamres #heureka
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Induction system for a spherical field magnetic fusion reactor
Chapter 6: How Beltrami vortices cancel out the gyral drift of particles, https://lnkd.in/ej2XYDc9
Named after Enrico Fermi, fermions 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 is defined by four semicircular arches (B ,B') and contains a magnetic field composed of four magnetic field planes. Each plane is offset by 90° 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 plasma tube's diameter. The video exaggerates the restoring effect of gyral drift on negatively charged electrons and positively charged deuterons spiraling the magnetic field line (m1) in opposite directions. The trajectory of these particles is shown in yellow. To achieve time-unlimited plasma confinement with minimal effort, two advantageous properties of the double helical magnetic field must be considered. First, the chiasma (X) of the magnetic field's figure-of-eight configuration alternates the gradient of each magnetic field line (m1, m2-mn) regularly between the inner and outer surfaces of its respective layer (L₁–Ln) within the tubular plasma volume. Second, a holographic effect is associated with the movement of the magnetic field lines lying on the surfaces of transformation spheres with a uniform radius at their respective midpoints (M1–Mn). The field lines twist as they transition from the exterior to the interior and vice versa. Electrons and ions have different charges and can move along the field lines at speeds of up to 1,000 km/s. Orbiting the magnetic field at a frequency of 10⁻¹¹ Hz creates an electric field that is perpendicular to the magnetic field plane. Since the magnetic field is stronger on the concave inner side than on the convex outer side of a semicircular arc of the plasma volume, 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. The resulting electric field 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 a magnetic field, the red electron moves away from the yellow trajectory in the direction indicated by the red arrow. Meanwhile, 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 they were guided by railroad tracks. Helmholtz coils (Q1–Q32) are arranged at regular, radial intervals around the plasma vessel to establish fluid dynamic equilibrium within the plasma volume. For the gyral drift of fermions and bosons to cancel 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 drifts of an electron and a deuteron—described as Beltrami vortices—cancel each other out within two periods of a standing wave. Because one orbital revolution satisfies the quantum rule that a particle returns to its starting point in the same spin state after a full 720-degree angular rotation, the plasma in the Looperator can remain magnetically confined indefinitely.
#resmpc6 #resuft #Looperator out of hashtags resmpc1 to resmpc14 #resfusion6 #Looperator #resfluiddynamik #solution4fusion #plasmaphysics #teamres #heureka
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Induction system for a spherical field magnetic fusion reactor
Chapter 7: Introducing the ECE-Theory, https://lnkd.in/dcSQEUuy
Chapter 1 discusses Helmholtz coils (Q1-Q32) 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 semicircular arches (B, B') defining the plasma vessel (20). The arcs (B, B') 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. There is a fourfold change in spin direction for fermions and a twofold change for bosons. This law is one of Maxwell's equations and establishes 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 September 1, 2016, by Myron W. Evans, Horst Eckardt, Douglas W. Lindstrom, and Stephen J. Crothers. See 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.
#resmpc7#resuft #Looperator out of hashtags resmpc1 to resmpc14 #resfusion7 #resfluiddynamik #solution4fusion #plasmaphysics #teamres #heureka
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Chapter 8: The effect of four magnetic field planes (I-IV), https://lnkd.in/dBWsSxey
The video on the left uses the "three-finger rule" from electrical engineering to show how fermions and bosons move along double-helix magnetic field lines within a 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, charged particles follow magnetic field lines in closed loops, thereby inducing electric fields. This is also the case in the plasma of a fusion reactor. The electric field force moves electrons (-) and ions (+) perpendicular to the direction of the magnetodynamic flow generated by the Lorentz force (represented by the middle finger). This forces them to orbit the magnetic field lines along spiral trajectories at a frequency of 10⁻¹¹ Hz. On these spiral trajectories, the charged particles complete an orbit spanning two periods at a speed of 1,000 km/s within two periods of a standing wave. The asymmetry of the magnetic field causes electrons and ions to move away from their respective field lines in opposite directions within one period of the standing wave. To compensate for this deflection, the electrons must travel through an additional period of the standing wave. During this time, they move toward each other. Since the four magnetic field planes are offset by 90° relative to each other, the gradient of the double-helix magnetic field changes direction four times. Therefore, two periods of a standing wave are required before the gyral deflection of fermions and bosons is fully reset. 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 perpendicular to the field direction to reverse completely within two periods of the standing wave. For fermions with a spin quantum number of 1/2 and bosons with a spin quantum number of 1, these particles essentially follow magnetic field lines as if they were railway tracks. In a tokamak, additional poloidal coils are needed to counteract the particles' transverse drift by twisting the magnetic field. Stellarators achieve the same result through an extremely complex zigzag pattern of coils. However, the magnetic field geometry in the LoPrator is designed so that particle guidance can be achieved exclusively 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 behavior in the plasma. To twist the magnetic field lines using only Helmholtz coils and eliminate the transverse drift caused by magnetic field asymmetry, the particles' spin must change from "up" to "down" twice within one period. This fourfold change in spin direction within two periods of the standing wave also cancels out the gyral drift. The fourth Maxwell equation describes how currents flowing in an electric field influence the magnetic field. However, Maxwell’s equations do not immediately reveal that varying currents can generate light and radiation.
#resuft #Looperator #resmpc8 #resfusion8 #solution4fusion #plasmaphysics #teamres #heureka
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Chapter 9: The Geometric Structure of Time, https://lnkd.in/dCBxqf39 ,discovered within the plasma structure of the "Looperator." As discussed in Chapter 1, the Helmholtz coils are arranged in a concentric pattern around the central magnetic field line within the plasma vessel. The coils 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 of which lies on a virtual uniform transformation sphere. The field lines in the two mirror-inverted halves of the double helix 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. In order 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 necessary to cancel the spin deviation of fermions and bosons completely within one oscillation period of the double helix. This allows the plasma to be magnetically confined in the "Looperator" indefinitely. Because the Lorentz force is equal in both halves of the plasma volume, the magnetic field lines automatically twist. This eliminates the need for additional coils to manipulate the magnetic field. As Chapter 9 shows, 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. A Lorentz transformation causes jitter in the uniform transformation sphere. The frequency of this jitter depends on temperature and pressure, increasing from the cooler exterior to the hotter center of the tubular plasma volume. Temperatures can range from 100 to 400 million degrees Celsius. The holographic effect caused by the double helix 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 DT fusion field that offers significant advantages over existing technology. The "Looperator" features precise magnetic field topologies arranged in concentric layers, which are more accurate than those of the Wendelstein 7-X stellarator experiment. The video shows twelve magnetic field lines of the spherical magnetic field that can be made visible inside the plasma chamber's vacuum. This is achieved by injecting an electron beam that aligns with the magnetic field lines. This process maps the lines and enables the creation of an accurate 3D model of the expected magnetohydrodynamic processes.
#resmpc9 #resuft #Looperator out of hashtags resmpc1 to resmpc14 #resfusion9 #solution4fusion #plasmaphysics #teamres #heureka
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Chapter 10: 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 (m2-mn) wind. Offsetting the magnetic field surfaces by a factor of four creates the double-helix structure of the plasma volume (2). 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 (2), particles (+, -) gyrating around the magnetic field lines undergo undesirable Bx(gradB) drift perpendicular to the plasma's flow direction. In a tokamak, these forces destroy the layer structure of the plasma within a short time. To reverse deviation of fermions, imposed by gyration particles must change their spin (s, s') twice within one half of the double helix or one ring oscillation period (T, T'). They must also change their spin (s, s') four times within two periods (T, T') to return to the same spin state at the start of an orbital revolution (U1-Un). However, in order for the spin (s, s') 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 (3) 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 (2) 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.
#resmpc10 #resuft #Looperator #resmpc10 out of hashtags resmpc1 to resmpc14 #resfusion10 #fermions #bosons #plasmaphysics #teamres #heureka
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Chapter 11: Time Depends on Frequency, 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 (T, T') of a standing wave. The frequency (f2- fn) of double helical oscillations over two periods (T, T') 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 (Ln), which are displayed in different colours, as well as in the central red magnetic field line (m1). 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 the life span of a mayfly. Two periods (T, T') 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.
#resmpc11#resuft #Looperator out of hashtags resmpc1 to resmpc14 #resfusion11 #solution4fusion #plasmaphysics #teamres #heureka
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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 lines (m2–mn), around which the blue ion will rotate. Since the central magnetic field line consists of four flat semicircles (B, B') with a radius of (r1), its length can easily be calculated. Since all magnetic field lines lie on the surface of a virtual transformation sphere with a radius of (r1), the magnetodynamic flow dynamics of the "Looperator" undergo a Lorentz transformation that combines three geometric operations: a Lorentz transformation, a translation, and a rotation. As illustrated in Chapter 2, the four magnetic field planes (I–IV) of the double-helical plasma volume (20) are offset by 90° from one another and are connected at four points (J1–J4) 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 (r1) 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 (20), two equidistant magnetic field lines are shown as examples. These field lines (mn) are at their maximum and minimum distances from the center (Mn) of the fusion reactor, which is located at the vertices (V1–V4) of their double helical orbit. At the four connection points (J1–J4) in the angular momentum plane ( β′) , 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 (U1). Conversely, twisting of the magnetic field lines is caused by the chiasm (X) of endless loops that can be likened to a Möbius strip. Here, two equidistant lines regularly alternate between an outer side maximally distant from the center and an inner side minimally distant from it. 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 (m1, m2-mn), the particles must change spin (s, s') twice within one double-helix period (T, T'). The helical line gradient of the double helix (3) is sufficient to reverse the gyration drift of fermions and bosons within one annular oscillation period (T, T'). Chapter 9 will provide a more detailed examination of the boson circuit, explaining its function and role.
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Chapter 13: Introduction to a Novel Magnetic Heat Transfer System, https://lnkd.in/ei6yMA9a
The inner core of the tubular plasma volume (20) 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 (23 and 24) of the plasma container? The double-shell steel plasma vessel acts as a heat transfer device, absorbing heat from the plasma. It is equipped with eight magnetic coils, each of which has a multitude of magnetic poles (P1-Pn) that lie opposite each other on the inner shell. These coils' magnetic poles (P1-Pn) can be operated by either alternating current (AC) or direct current (DC). Sophisticated magnetic operation enables temporary contact between the electrically conductive tubular plasma volume (20) and the inner shell (23) of the plasma vessel (20). This facilitates heat transfer 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 opposite magnetic coil poles (P₁–Pn). This influences the trajectory of the magnetic field lines. In a coordinated motion, the tubular plasma volume briefly touches the inner shell (23) of the plasma vessel (20), allowing heat to transfer by conduction.
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Chapter 14: Structure and scalability, https://lnkd.in/e8aApViG
The plasma vessel consists of identical tubular modules that have either circular or oval cross-sections. The vessel modules (C1- Cn) are arranged concentrically around the central magnetic field line (m1), which is the central trajectory of the magnetically confined tubular plasma volume (2). The modules (C1- Cn) are bounded by inner and outer radii around the central magnetic field line (m1), as shown in Fig.1 - Fig.3. 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 (Q1–Q32) keeps the plasma volume (2) away from the blanket to prevent it from coming into contact with the inner shell (23) of the double-walled plasma vessel (20) carrying the blanket. The Helmholtz coils (Q1–Q32) are assigned to individual vessel modules. As shown with Fig.6 and Fig.7 the radial and longitudinal spacing (d, d', d'') between the coils is defined by the sector angles around (M1), the center of the fusion reactor. The central magnetic field line (m1) of the fusion reactor is surrounded by many concentric layers, each containing decentralized magnetic field lines (m2-mn) with analogous connection points (J1-J4) and vertices . 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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