FUSION REACTOR

The DEINOS Project has patented a "Fusion Energy Reactor" and a "Transmutation Device". If built, this fusion reactor could be generating power today.

The "Transmutation Egg" explores quantum phenomena effects which require advanced physics AI simulation models and multiple  single-shot fusion test burns. 

We follow one paradigm:

       To create an artificial star, simply emulate what God has perfected.

We are guided by one principle: 

             To provide [virtually] free unlimited clean energy for all mankind 

                                in order to improve the quality of life 

Our belief system:

             These are God's secret formulas.  No  one person owns them.

• Mass: ≈0.08M⊙=1.6×1029kg
• Radius: ≈0.1R⊙=7×107m
• Core Temp: T≈4×106K
• Core Density: ρ≈150g/cm3=1.5×105kg/m3
• Pressure: From hydrostatic equilibrium, P≈1016Pa

Parameter Value / Range Minimum 

------------------------------------------------------------

Plasma Radius   ~ 0.8 m (sustained burn, low output)

Nominal Radius  5–6 m (your current design)

Maximum Radius 10 m (before thermal dilution)

Minimum Particle Density 4×10^19m−3

Nominal Density 10^20–10^21m−3

Core Temperature Range 275–500 million K

Magnetic Beta Target  0.2 – 1 (tuned dynamically)

Confinement Time Goal > 1 second 

Maximizing Quantum Tunneling Probability in Fusion Plasma Systems

I. Summary of Conclusions

Our primary goal is to maximize quantum tunneling probability in the nebula region surrounding a fusion plasma core.
The key conclusion is that tunneling probability, which governs the fusion rate, is highly sensitive to parameters we can influence.
Key physics models like the Gamow factor, Fowler–Nordheim tunneling, Hill-Wheeler barrier models, and quantum delay/resonance effects all suggest ways to amplify tunneling probability under real experimental conditions.
We concluded that the most promising enhancements involve electric fields, resonance synchronization, pressure wave alignment, thermal gradients, and material selection in the surrounding medium.

II. Quantum Physics Parameters and Controllability

We classify all relevant parameters into three categories:

1. Easily Controlled & High Impact:
   • Electric Field Strength (E): directly controlled via electrodes – increases tunneling probability via Fowler–Nordheim mechanism.
   • Fuel Injection Timing (Δt): can be synchronized with field pulses – critical for coherence.
   • Waveform Frequency (f): RF/Microwave/Sonic – used to create resonance in barrier width and reduce effective tunneling barrier.
   • Pressure in Nebula Region (P): lithium deuteride medium provides high thermal inertia and uniform pressure.
   • Spin Alignment / Polarization: can be influenced with magnetic field orientation of injected ions.

2. Difficult to Control:
   • Plasma Potential (Φ): varies with temperature and charge density – must be inferred/measured in real-time.
   • Barrier Width (d): depends on local field strength, tunneling path, and fuel distribution.
   • Tunneling Delay Time (τ): indirectly observable via temperature and neutron/alpha spike timing.

3. Not Directly Controllable:
   • Nuclear Charge (Z): fixed for each element – although choice of fuel/transmutable elements is selectable.
   • Reduced Mass (μ): depends on fusion pair – selectable through fuel mix (e.g., D+T, D+D, p+B).

III. Key Quantum Tunneling Formulas

1. Gamow Factor:
   P ∼ exp(-2π Z₁Z₂ √(μ / 2E))
   – Controls tunneling in D+D or D+T reactions.

2. Fowler–Nordheim Tunneling:
   J ∼ E² exp(-B φ^(3/2) / E)
   – Field-enhanced tunneling in solid-state or pre-ionization regions.

3. Hill-Wheeler Transmission Coefficient:
   T(E) = 1 / (1 + exp[(2π(V₀ - E)/ℏω)])
   – Used for compound nucleus formation modeling and barrier shape adaptation.

4. Delay/Phase Resonance Tunneling:
   – Quantum dwell time and delay time influence barrier width dynamically through resonance effects.

IV. Experimental Implementation in Fusion Reactor

• Implement vertical electric fields using top-mounted positive and bottom-mounted negative electrodes around the nebula.
• Shape the chamber to allow wave convergence near the plasma using carefully placed reflectors.
• Pre-ionize and spin-align injected fuel using spiraling nozzles under electric and magnetic fields.
• Use capacitive or pulsed EM field bursts in resonance with tunneling timing (10-100 fs scales).
• Embed RF/microwave emitters in the plasma support structure to seed resonance and barrier shaping.
• Select medium-Z elements in the barrier region (Re, Os, Pd) to support alpha capture and scattering.

Separate Testbeds Proposed:
• Quantum Delay Experiment: measure phase delay of alpha emissions versus ignition field spike.
• Electric Field Shell Test: test isolated field strength effects on tunneling rates using deuterated metal lattices.
• Harmonic Resonance Chamber: simulate pressure + RF + spin-alignment under chamber geometry in a subscale burn.

V. Conclusion

Maximizing quantum tunneling in our artificial star requires tuning a range of quantum and classical parameters.

From electric field geometry to resonance timing, every implementation step is anchored in foundational quantum physics.

By mapping theory directly to hardware and simulation, we will empirically test and optimize this new class of spherical, harmonically-resonant, field-driven fusion ignition systems.

• Effect: Allows charged nuclei to overcome the Coulomb barrier at lower than classical energies.
• Relevance: The core quantum mechanism that permits fusion to occur at achievable temperatures.
• Control Variables:
  • ↑ Energy (E) of incident particles
  • ↓ Z₁, Z₂ (effective for light elements; becomes harder for heavy elements)
  • ↑ Tunneling probability exponentially increases with higher relative kinetic energy and lower nuclear charge.

• Effect: Models fusion as barrier penetration through a compound nucleus formation channel.
• Relevance: Especially important for transmutation and heavier nuclei interactions in the plasma or shell.
• Control Variables:
  • ↑ Matching nuclear energy levels (resonances)
  • ↓ Width of the effective barrier through structural design or external fields

• Effect: Strong electric fields can enhance tunneling by distorting the potential barrier.
• Relevance: Applies to the nebula shell region where pre-ionization and electric field shaping can dramatically raise tunneling probability.
• Control Variables:
  • ↑ Electric field strength (E_field)
  • ↑ Surface charge / ionization state of fuel streams
  • ↑ Nozzle or electrode design precision

• Effect: Frequent measurement or interaction “freezes” quantum evolution.
• Relevance: Could help stabilize certain quantum states in plasma or delay decoherence in specific particle clusters or reactants.
• Control Variables:
  • ↑ Observation frequency or interaction rate
  • Used to “freeze” high-energy quantum states in confined plasma regions

• Effect: Coherent wave functions reinforce constructive interference and amplify collective particle behavior.
• Relevance: May lead to enhanced fusion rates via stimulated or synchronized reaction chains, particularly in structured plasma or field environments.
• Control Variables:
  • ↑ Field phase locking (RF, microwave, X-ray)
  • ↑ Spatial and temporal coherence of particle wave packets
  • ↑ Matching field geometries and timing for resonance

• Effect: Aligned nuclear spins can alter the fusion cross-section, in some cases enhancing it.
• Relevance: Polarized fuel streams could be injected using magnetic or spin-selective nozzles to increase reaction probability.
• Control Variables:
  • ↑ Spin polarization in D or T fuel
  • ↑ Control over magnetic injection geometry
  • 
    

• Effect: Particle wave functions form resonance modes that amplify reaction likelihood at certain frequencies or geometries.
• Relevance: Achievable using standing wave cavities (RF/microwave/X-ray) tuned to nuclear or subnuclear energy scales.
• Control Variables:
  • ↑ Resonant cavity Q-factor
  • ↑ Coupling of EM frequency to fuel shell geometry
  • ↑ Harmonic matching of injected fields
  • 
    

• Effect: Correlated states between particles can transmit information non-locally or reduce entropy.
• Relevance: Hypothetical use in synchronizing quantum fields or coordinating wave collapse to favor tunneling.
• Control Variables:
  • ↑ Initial entanglement preparation
  • Potential application in plasma structuring or diagnostic sensors
  • 
    

• Effect: Time a particle spends in the tunneling barrier can affect the phase and interference pattern.
• Relevance: Tuning field oscillations or nebula densities to hold particles longer in critical zones may aid energy transfer.
• Control Variables:
  • ↑ Barrier width control via electric/magnetic shaping
  • ↓ Effective barrier speed / velocity matching of wavefronts

• Effect: In dense bosonic systems or plasmas, collective quantum states can form, enhancing coherence and amplifying reactions.
• Relevance: Fusion plasma may exhibit collective modes that increase energy transfer efficiency.
• Control Variables:
  • ↑ Plasma density and temperature control
  • ↑ Alignment of field pulses and plasma oscillations

The Key advantage of the Deinos reactor design is low-cost of operation and simplicity. 

It includes the process of flowing heavy water-based fluid into, and supercritical heavy water steam out of a chamber which contains a self-sustaining fusion plasma. The Deinos process defines the dynamically created thermal barrier which allows us to place plasma support devices closer to the plasma core. 

 Key Aspects of Design 

The key aspects of this design include:

1. Self-Stabilizing Thermal Atmosphere – Heavy water-based liquid dynamically vaporizes into a thermal barrier containing the plasma. 

2. Real-Time Plasma Type (Composition) Control – Plasma composition transitions from D-T fusion to Helium-3, and to aneutronic boron-proton fusion.

3. Element Transmutation & Fuel Breeding – Neutron capture reactions enable transmutation of common elements into high-value materials (e.g., lead to gold) and creates its own fuel (e.g., Lithium to Tritium) depending on configuration. 

4. Rotational Stability – This generator can adjust [in real-time] rotational parameters of the plasma, the thermal atmosphere, the gaseous layer and the surrounding liquid medium. 

5. Fuel Injection - This system allows continuous fuel injection that provides stabilization of the plasma by injecting it with positively and negatively charged pellets and/or gas (puffer) along strategic locations. 

6. Existing Fusion Ignition and Energy Extraction – This system works with proven low-cost fusion ignition and sustaining methods. It also utilizes proven methods of extracting energy. This system does not require any new technology. 

7. Additional Controls: Magnetic and Electrical – This system relies on a thermodynamic encapsulation of a fusion plasma in heavy water-based liquid for containment and stability.  Additional electrical and magnetic fields can be applied for additional stability. Since the temperature is dramatically reduced within a short distance, a variety of electrical and magnetic fields can take advantage of the proximity and geometry for each configuration.

8. Low-cost Ignition - Ignition can be achieved through a low-cost 25 mega-amp Z-pinch mechanism, initiating fusion within a dense deuterium-tritium (D-T) sphere known as the ignition egg.

9. Self-Sustaining: “Bigger is Better” - This system requires a large initial plasma ignition (plasma ball radius = 2 to 4 m) to create an initial large ‘Hot Zone’ in the fusion plasma core. This allows the fusion plasma to be self-sustaining.  It is estimated that a hot zone between the size of a hardball to the size of a softball is required.  A plasma ball with a 3.5 m radius is estimated to give us a hot zone approximately the size of a bowling ball, so it should be relatively easy to sustain the fusion plasma ball. Once the plasma is under control the reactor can experiment with minimum sizes through tuning the fuel injection along with other parameters.

10. Fusion Ball Expansion - The initial large fusion plasma ball can be created by surrounding a smaller D-T fusion ignition with dense compressed fuel (ex: tritium, deuterium).  This will expand the fusion plasma within the heavy water fluid to an initial steam sphere [or ‘plasma ball’] with a radius of 3.5 to 4 meters.  It is estimated [by extrapolation] that a 25 MA z-pinch type ignition is sufficient to ignite such a large fusion plasma. 

11. Gas Gap – The water is separated by the initial ignition via centrifugal force or other force, creating a gap between the initial ignition egg and the surrounding heavy water-based fluid. The shockwave of fusion ignition is absorbed by the “Gas Gap” between the ignition and the surrounding water from all sides.

Self-Stabilizing Thermal Atmosphere 

Heavy water-based liquid dynamically vaporizes into a thermal barrier containing the plasma. Steam is continually exhausted from the system to maintain the atmospheric layer thickness while generating electricity. 

This thermal barrier contains the plasma core far from the chamber walls which prevents degradation to the chamber walls. The main chamber is filled with heavy water which is continuously evaporated into steam which generates energy via a standard steam engine. Much of the plasma support structures, devices and chambers can be safely placed in the heavy water or in the steam layer. The plasma core can be over 150 million degrees kelvin, yet the temperature is moderate only a small distance away.  

This distance is based on the rate of fuel added to the plasma core and is a unique method of describing a “plasma ball” of any specific composition or type.  A “plasma ball” is defined by the radius from the center of the plasma core to the steam layer and is unique to every plasma type.

Real-Time Plasma Type (Composition) Control 

Plasma composition transitions from D-T fusion to Helium-3, and to aneutronic boron-proton fusion, reducing neutron emissions and enhancing energy efficiency. The key to fusion energy is to move to aneutronic as soon as possible.  Dinostar proposes a specially doped heavy water mix that can withstand the high 600 million degrees Kelvin in complete safety.  

The DinoFusion process transitions to a fully aneutronic fusion plasma in less than 3 seconds, transitioning quickly to near zero-cost boron-hydrogen fuel which is cheap and abundant. The only way to contain all that heat is by suspending the fusion plasma and growing it quickly in heavy water. 

It starts with a low-cost z-pinch small ignition which ignites a larger D-T and He-3 fusion plasma, which is heated during initial fusion, which causes a chain reaction with the boron to produce a 600-to-900-million-degree Kelvin fusion plasma.  This is why we need a large tank or chamber of heavy water at 100 atm.

Rotational Stability 

This generator can adjust [in real-time] rotational parameters of the plasma, the thermal atmosphere, the gaseous layer and the surrounding liquid medium. 

a. Plasma rotation provides gyroscopic stabilization, reducing turbulence and improving confinement efficiency. It also reinforces the magnetohydrodynamic spinning motion of the surrounding heavy water.

b. Thermal barrier atmosphere rotation reinforces containment.  As the water evaporates and is exhausted via the steam vents, a consistent atmospheric movement begins to take shape much like the jet stream on Earth.  However it will be more of a vortex like a tornado with an exit point at the north pole and south pole of the chamber.

c. Rotation of the gaseous layer between the initial ignition egg and the surrounding medium. This helps absorb the initial shockwave from ignition and provides a transition zone between the liquid and the steam layers.

d. Rotation of the surrounding medium [such as heavy water] allows for graceful introduction to the plasma core through centrifugal forces. This is fine-tuned in real-time to create the thermal barrier atmosphere. These rotational forces in the liquid medium reinforce magnetohydrodynamic effects of the rotating charged plasma. 

Fuel Injection 

This system allows continuous fuel injection that provides stabilization of the plasma by injecting it along strategic locations. A continuous flow of pellets or gas (puffers) is injected into the plasma from all directions. There are fuel injectors above at the north pole, below [at the south pole] and along the equator. There are 12 nozzles around the equator, 12 nozzles between the equator and the north pole, 12 nozzles between the equator and the south pole. The positions of the positively and negatively charged pellets further affect the plasma movement. Gimbels can be implemented if further refinement is needed.

Existing Fusion Ignition and Energy Extraction 

This system works with proven low-cost fusion ignition and sustaining methods. It utilizes proven methods of extracting energy. This system does not require any new technology. In addition to supplying electricity, this generator produces high-value solids, liquids, gases and plasmas. This system requires a large initial plasma size which can be created by surrounding a small fusion ignition with dense compressed fuel (ex: deuterium, tritium).  This will create a larger plasma core which allows more time and more area to begin injecting fuel.  Existing gas puffer methods of injecting hot fuel gases into the core at supersonic level speeds can be used.  Cryogenic fuel pellets can also be injected for a more delayed effect.

Additional Controls: Magnetic / Electrical / Heaters

This system relies on a thermodynamic encapsulation of plasma in heavy water for containment.  

Additional electrical and magnetic fields can be applied for additional stability. Since the temperature is dramatically reduced within a short distance, a variety of electrical and magnetic fields can take advantage of the proximity and geometry for each configuration. Each application of this system allows for the inclusion of additional controls depending on the specific geometry. A magnetic mirror will be setup close to the plasma core to channel the steam out the north and south poles. Poloidal and toroidal coils may be optional in the final design but they will be implemented in the initial reactor design for maximum tuneability and control of the plasma. They must be waterproof coated. 

This invention creates and maintains an artificial star using a self-sustaining fusion cycle that controls plasma size, type, and containment properties.  Optional magnetic coils provide extra stability and can move dynamically to adjust to the plasma size.

Fuel Ignition 

Ignition can be achieved through a low-cost 25 mega-amp Z-pinch mechanism, initiating fusion within a dense deuterium-tritium (D-T) sphere known as the ignition egg. This egg is pressurized to approximately 3000 atm and is surrounded by a low-pressure gas gap formed by spinning the chamber, pinning water to the walls with a parabola at the bottom and water injected from above. This gas gap thermally isolates the ignition egg and absorbs the shockwave from ignition, allowing the plasma to expand into a stable configuration. Once ignited, the plasma naturally forms into a spherical ball that stabilizes within the steam and heavy water layers.

Self-Sustaining

The design of this reactor is based on the ability to sustain a fusion plasma by simply adding fuel to the hot zone of the fusion plasma core. To sustain this plasma, we’ll need to maximize exposure time within the hot zone [an area which is over 50 million degrees Kelvin]. “Bigger is Better” - This system requires a large initial aneutronic fusion plasma ignition (a plasma ball radius of 2 to 4 m) which has an initial ‘Hot Zone’ between the size of a hardball to the size of a softball. This allows the fusion plasma to be self-sustaining.  Once controlled the reactor can experiment with minimum sizes by tuning the fuel injection and other parameters.  

Fusion Ball Expansion

The initial large fusion ball can be created by surrounding a small fusion ignition with dense compressed fuel (ex: tritium, deuterium).  This will expand the fusion plasma within the heavy water fluid. 

There are multiple secondary reactions with Helium-3 and boron to reach temperatures of over 450 million degrees Kelvin to fuse boron with hydrogen.  

This large hot fusion plasma integrates with the heavy water-based liquid to create an initial steam sphere [or ‘plasma ball’] with a radius of 3.5 to 4 meters.  It is estimated [by extrapolation] that a 25 MA z-pinch type ignition is sufficient to ignite the initial D-T spark which has secondary fusion ignitions (He-3, boron) leading to a large fusion plasma.

The initial z-pinch ignition is surrounded by dense compressed deuterium and tritium which is in a state which is on the edge between a liquid and gaseous state. There are layered secondary fusion ignitions or more accurately, one large fusion expansion within one second or two.  This secondary expansion consumes the spherical eggshell [that contains the compressed fuel] before the shockwave reaches it. The shockwave is absorbed by the “Gas Gap” between the ignition and the surrounding water [from all sides in 3 dimensions].

Existing gas puffer methods of injecting hot fuel gases into the core at supersonic level speeds can be used.  Cryogenic fuel pellets can also be injected for a more delayed effect.  Excess boron can be injected once after 1.5 seconds which is why the chamber must be oversized.  

 Fusion Plasma Containment 

 Temperature Emulating Gravity 

The paradigm is to simulate or emulate the environment of a natural star. Since it is impossible to simulate gravity, we can emulate the effects with a steam shell.

The DinoFusion thermodynamic process uses cool water and a wall of steam to emulate the containment force of gravity in a natural star. 

After ignition, the heat from the fusion plasma core can only push the wall of steam out so far, beyond which it cannot evaporate any more heavy water. 

Thermal Barrier 

The thermodynamic cycle of this system mimics astrophysical plasma behaviors by containing the plasma core within a dynamically formed self-regulating [thermal barrier] atmosphere. This thermal barrier acts like gravity by preventing the plasma core from expanding uncontrollably. It also creates a safe cool temperature region within the heavy water for plasma support devices such as fuel injectors, plasma heating devices, magnetic coils, transmutation chambers and energy capture mechanisms. The fuel injection system can be placed close to the plasma core within the steam or boiling heavy water layer which is always around 100 degrees Celsius. 

 Plasma Ball Rotation 

The plasma core rotates about its north-south axis for stability. In our sample power generator, the entire main chamber rotates to create an area of gas surrounded by heavy water on all sides.  It utilizes centrifugal force to pin the water against the chamber walls with a parabola of water at the bottom, creating a gas gap in the center for the initial ignition and expansion of the plasma. Heavy water streams in from above during ignition so that the entire sphere of steam is created at once around the fusion plasma core. This reactor leverages the gas gap to absorb shockwaves from ignition while integrating with the surrounding water. 

After ignition the fusion plasma continues to rotate about its axis, frictionless within a sheath of steam.  The fuel is positive and negatively charged prior to injection into the plasma core to maintain the rotation.  The AI control software can increase or decrease the rate of rotation of the plasma but generally matches the rotation rate of the surrounding heavy water. This rotation creates a magnetic field similar to Earth’s. This magnetic field is enhanced in several ways. A current runs through the center of the axis. Magnetohydrodynamics (MHD) of the main chamber and liquid flowing around the plasma reinforces the magnetic field. The rotation also evenly distributes the density within the fusion plasma sphere to enhance stability. The rotation also creates a gyroscopic effect which offers stability but must be balanced not to exceed a threshold.  

 Gas Gap (Pre-Ignition Mode) 

As the main chamber rotates it utilizes centrifugal force to control water pressure against the plasma core, creating a gas gap in the center for the initial ignition and expansion of the fusion plasma. This reactor leverages the gas gap to absorb shockwaves from ignition and to provide a buffer for atmosphere generation.  This system does not rely on magnetic fields alone for containment or to maintain pressure, but all types of magnetic devices can be placed within the heavy water close to the plasma core if additional control is required. This system does not require RF, microwave or other additional heating methods but they too can be placed close to the plasma core if needed.

 Plasma Core Control (Operation Mode) 

This reactor design enables operators to regulate the size and type of fusion plasma. It can transition the plasma between deuterium-tritium, to Hybrid (Deuterium-Helium3).  It can then gradually transition to a Helium3 only aneutronic fusion plasma. However, as we get closer to a purely aneutronic fusion plasma core, the hot zone max temperature rises dramatically.

 Sample Generator – Cylindrical Main Chamber Rotation 

One configuration of a DinoFusion generator is composed of a cylindrical main chamber that holds the entire reactor core. 

The chamber is filled with heavy water liquid with a fusion plasma suspended in the center. The Reactor Core is completely contained in the main chamber. 

The fusion plasma, the plasma support structure and sub-chambers for transmutation. 

As the main chamber rotates, the plasma ball, the heavy water and the thermal barrier are all rotating.  When using a cylindrical main chamber, the axis of rotation will be the center of the circular cross-section.  The rotating materials in the chamber reinforce the magnetohydrodynamic effect on the rotating plasma core.  The walls of the main chamber will consist of heavier transmutable elements which have a larger magnetic (MHD) influence on the rotation of the plasma.  

No new technology is required for the implementation of this invention, and it is much less expensive to build than any existing design. This artificial star can be ignited using any one of multiple existing methods of fusion ignition.  Our sample power generator (below) uses the z-pinch method [which must be slightly modified].  We create a large plasma ball with a 3.5-meter radius starting with a small z-pinch ignition from a 30 M Amp system. This is proven mathematically in the “Formulas Addendum” document. The construction of this nuclear fusion reactor is much less expensive than a tokomak-style or any other reactor design.

This system essentially creates a classical physics steam engine generator “wrapper” around a quantum-level nuclear physics reactor core. This allows us to reduce a complex fusion reactor to a simple “Plasma Ball”.  All the complexity of supporting the plasma is contained and controlled by AI software which is continuously monitoring and modifying the plasma attributes.  

Fuel parameters such as injection speed and electrical charge and direction are modified in real-time with nanosecond precision. Note: At higher temperatures [over 700 million Kelvin] there is a risk to the molecular stability of the heavy water breaks down.  It is necessary to modify the heavy water to prevent a catastrophic uncontrolled runaway fusion reaction.  See “Heavy Water Doping” section for details. Heavy water doping is necessary for boron-proton fully aneutronic fusion reactions. 

A side-effect of failed ignition attempts is that each attempt is highly profitable whether it is successful or not.  Since we require a large plasma ball [to create a large hot zone], there are massive amounts of neutron and alpha particle emissions. The rotating chamber allows us to capture 99% of the neutrons before reaching the chamber walls via Coriolis effect and the large chamber. Lithium blankets will yield high-value gases such as tritium and helium-3 which can be utilized for future experiments or sold for profit. Valuable solids such as Rhodium and Platinum can be created to pay for the next experiments, while the fuel gases are saved for future experiments.  Is never achieved.

The system is modular, allowing scalable designs from small mobile power plants to full-scale commercial reactors.  It supports a closed-loop energy cycle, reprocessing fusion byproducts for sustained operation and reducing waste.

Perhaps the best feature of this design is that all the parts of this reactor can be purchased for a relatively low cost, and a test site can be constructed within a year or two, once approved.  The site would be profitable almost immediately after it is fully built.

Magnetic Fields 

A Magnetic Bottle is implemented to work with the magnetic fields of the dipole magnetism of the artificial star. The poloidal magnetic fields work to contain the toroidal fields generated from the rotating plasma.

A magnetic mirror configuration is used to funnel steam out through the north and south pole exits. See sample generator section.  Due to the cool temperatures so close to the plasma core, the first reactor will serve as a testbed for various low-cost options of refining control of the plasma ball. The novel approach to managing extreme temperatures by suspending the plasma in heavy water, opens many options to add a variety of low-cost plasma-control magnetic devices. 

In this design, the magnetic mirror and magnetic bottle forces confine the fusion plasma. 

The rotating electrically charged plasma creates a dipole magnet—this associated with additional magnetic forces can create a bottle effect such that the plasma cannot move left or right in any significant way.

Additional magnetic fields are deployed as dynamically reinforcing, trimming, shaping, and stabilizing the naturally formed plasma sphere. The overall strategy is to emulate astrophysical objects like stars, pulsars, and magnetospheres, where magnetic fields arise from internal currents, rotation, and charged fluid motion. However, the same magnetic fields are available to exploit for further control. The first reactor configuration is designed to have as many controls as feasible.  They may be turned on only when or if needed.

In the attached sample cylindrical reactor design, a magnetic mirror is implemented to channel the supercritical heavy water steam through the north and south pole exits to generate electricity. In the comet-style configuration it might not be necessary.

The plasma ball is designed to rotate and generate a weak magnetosphere.  A current is run through the north-south pole axis, and the metal chamber and rotating fluid reinforce the magnetic field via MHD.  This magnetosphere will work with outer magnetic fields to further stabilize and confine the fusion plasma core.

Some of the magnetic forces that can be implemented are:

- Axial Plasma Current 

– Core Toroidal Field

- Magnetic Mirror Fields 

– Polar Magnetic Brakes

- Equatorial Magnetic Coils 

– Passive Field Shaping

- Chamber-Induced Eddy Currents 

– Reflective Magnetic Casing

-  Helicity Injection 

– Magnetic Topology Self-Organization

- AI-Guided Magnetic Feedback Loop

The paradigm is to deploy multiple techniques to generate, enhance, and control magnetic fields using minimal energy expenditure and maximum synergy with the reactor’s own geometry, rotation, and hydrodynamics. Plasma behavior is often counterintuitive. It may require AI control software to predict response behavior based on patterns based on real-time and empirical feedback.