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Inertial electrostatic confinement

Inertial electrostatic confinement, or IEC, is a class of fusion power devices that use electric fields to confine the plasma rather than the more common approach using magnetic fields found in magnetic confinement fusion (MCF) designs. Most IEC devices directly accelerate their fuel to fusion conditions, thereby avoiding energy losses seen during the longer heating stages of MCF devices. In theory, this makes them more suitable for using alternative aneutronic fusion fuels, which offer a number of major practical benefits and makes IEC devices one of the more widely studied approaches to fusion.

A fusor, exhibiting nuclear fusion in star mode

As the negatively charged electrons and positively charged ions in the plasma move in different directions in an electric field, the field has to be arranged in some fashion so that the two particles remain close together. Most IEC designs achieve this by pulling the electrons or ions across a potential well, beyond which the potential drops and the particles continue to move due to their inertia. Fusion occurs in this lower-potential area when ions moving in different directions collide. Because the motion provided by the field creates the energy levels needed for fusion, not random collisions with the rest of the fuel, the bulk of the plasma does not have to be hot and the systems as a whole work at much lower temperatures and energy levels than MCF devices.

One of the simpler IEC devices is the fusor, which consists of two concentric metal wire spherical grids. When the grids are charged to a high voltage, the fuel gas ionizes. The field between the two then accelerates the fuel inward, and when it passes the inner grid the field drops and the ions continue inward toward the center. If they impact with another ion they may undergo fusion. If they do not, they travel out of the reaction area into the charged area again, where they are re-accelerated inward. Overall the physical process is similar to the colliding beam fusion, although beam devices are linear instead of spherical. Other IEC designs, like the polywell, differ largely in the arrangement of the fields used to create the potential well.

A number of detailed theoretical studies have pointed out that the IEC approach is subject to a number of energy loss mechanisms that are not present if the fuel is evenly heated, or "Maxwellian". These loss mechanisms appear to be greater than the rate of fusion in such devices, meaning they can never reach fusion breakeven and thus be used for power production. These mechanisms are more powerful when the atomic mass of the fuel increases, which suggests IEC also does not have any advantage with aneutronic fuels. Whether these critiques apply to specific IEC devices remains highly contentious.

Mechanism edit

For every volt that an ion is accelerated across, its kinetic energy gain corresponds to an increase of temperature of 11,604 kelvins (K). For example, a typical magnetic confinement fusion plasma is 15 keV, which corresponds to 170 megakelvin (MK). An ion with a charge of one can reach this temperature by being accelerated across a 15,000 V drop. This sort of voltage is easily achieved in common electrical devices; a typical cathode-ray tube operates in this range.

In fusors, the voltage drop is made with a wire cage. However high conduction losses occur in fusors because most ions fall into the cage before fusion can occur. This prevents current fusors from ever producing net power.

 
This is an illustration of the basic mechanism of fusion in fusors. (1) The fusor contains two concentric wire cages. The cathode is inside the anode. (2) Positive ions are attracted to the inner cathode. They fall down the voltage drop. The electric field does work on the ions heating them to fusion conditions. (3) The ions miss the inner cage. (4) The ions collide in the center and may fuse.[1][2]

History edit

1930s edit

Mark Oliphant adapts Cockcroft and Walton's particle accelerator at the Cavendish Laboratory to create tritium and helium-3 by nuclear fusion.[3]

1950s edit

 
This picture shows the anode/cathode design for different IEC concepts and experiments.

Three researchers at LANL including Jim Tuck first explored the idea, theoretically, in a 1959 paper.[4] The idea had been proposed by a colleague.[5] The concept was to capture electrons inside a positive cage. The electrons would accelerate the ions to fusion conditions.

Other concepts were being developed which would later merge into the IEC field. These include the publication of the Lawson criterion by John D. Lawson in 1957 in England.[6] This puts on minimum criteria on power plant designs which do fusion using hot Maxwellian plasma clouds. Also, work exploring how electrons behave inside the biconic cusp, done by Harold Grad group at the Courant Institute in 1957.[7][8] A biconic cusp is a device with two alike magnetic poles facing one another (i.e. north-north). Electrons and ions can be trapped between these.

1960s edit

 
U.S. Patent 3,386,883 - Schematic from Philo Farnsworth 1968 patent. This device has an inner cage to make the field, and four ion guns on the outside.

In his work with vacuum tubes, Philo Farnsworth observed that electric charge would accumulate in regions of the tube. Today, this effect is known as the multipactor effect.[9] Farnsworth reasoned that if ions were concentrated high enough they could collide, and fuse. In 1962, he filed a patent on a design using a positive inner cage to concentrate plasma, in order to achieve nuclear fusion.[10] During this time, Robert L. Hirsch joined the Farnsworth Television labs and began work on what became the fusor. Hirsch patented the design in 1966[11] and published the design in 1967.[12] The Hirsch machine was a 17.8 cm diameter machine with 150 kV voltage drop across it and used ion beams to help inject material.

Simultaneously, a key plasma physics text was published by Lyman Spitzer at Princeton in 1963.[13] Spitzer took the ideal gas laws and adapted them to an ionized plasma, developing many of the fundamental equations used to model a plasma. Meanwhile, magnetic mirror theory and direct energy conversion were developed by Richard F. Post's group at LLNL.[14][15] A magnetic mirror or magnetic bottle is similar to a biconic cusp except that the poles are reversed.

1980s edit

In 1980 Robert W. Bussard developed a cross between a fusor and magnetic mirror, the polywell. The idea was to confine a non-neutral plasma using magnetic fields. This would, in turn, attract ions. This idea had been published previously, notably by Oleg Lavrentiev in Russia.[16][17][18] Bussard patented[19] the design and received funding from Defense Threat Reduction Agency, DARPA and the US Navy to develop the idea.[20]

1990s edit

Bussard and Nicholas Krall published theory and experimental results in the early nineties.[21][22] In response, Todd Rider at MIT, under Lawrence Lidsky developed general models of the device.[23] Rider argued that the device was fundamentally limited. That same year, 1995, William Nevins at LLNL published a criticism of the polywell.[24] Nevins argued that the particles would build up angular momentum, causing the dense core to degrade.

In the mid-nineties, Bussard publications prompted the development of fusors at the University of Wisconsin–Madison and at the University of Illinois at Urbana–Champaign. Madison's machine was first built in 1995.[25] George H. Miley's team at Illinois built a 25 cm fusor which has produced 107 neutrons using deuterium gas[26] and discovered the "star mode" of fusor operation in 1994.[27] The following year, the first "US-Japan Workshop on IEC Fusion" was conducted. This is now the premier conference for IEC researchers. At this time in Europe, an IEC device was developed as a commercial neutron source by Daimler-Chrysler Aerospace under the name FusionStar.[28] In the late nineties, hobbyist Richard Hull began building amateur fusors in his home.[29] In March 1999, he achieved a neutron rate of 105 neutrons per second.[30] Hull and Paul Schatzkin started fusor.net in 1998.[31] Through this open forum, a community of amateur fusioneers have done nuclear fusion using homemade fusors.

2000s edit

Despite demonstration in 2000 of 7200 hours of operation without degradation at high input power as a sealed reaction chamber with automated control the FusionStar project was canceled and the company NSD Ltd was founded. The spherical FusionStar technology was then further developed as a linear geometry system with improved efficiency and higher neutron output by NSD Ltd. which became NSD-Fusion GmbH in 2005.

In early 2000, Alex Klein developed a cross between a polywell and ion beams.[32] Using Gabor lensing, Dr. Klein attempted to focus plasma into non-neutral clouds for fusion. He founded FP generation, which in April 2009 raised $3 million in financing from two venture funds.[33][34] The company developed the MIX and Marble machine, but ran into technical challenges and closed.

In response to Riders' criticisms, researchers at LANL reasoned that a plasma oscillating could be at local thermodynamic equilibrium; this prompted the POPS and Penning trap machines.[35][36] At this time, MIT researchers became interested in fusors for space propulsion[37] and powering space vehicles.[38] Specifically, researchers developed fusors with multiple inner cages. In 2005, Greg Piefer founded Phoenix Nuclear Labs to develop the fusor into a neutron source for the mass production of medical isotopes.[39]

Robert Bussard began speaking openly about the Polywell in 2006.[40] He attempted to generate interest[41] in the research, before passing away from multiple myeloma in 2007.[42] His company was able to raise over ten million in funding from the US Navy in 2008[43][44] and 2009.[45]

2010s edit

Bussard's publications prompted the University of Sydney to start research into electron trapping in polywells in 2010.[46] The group has explored theory,[47] modeled devices,[48] built devices, measured trapping[49] and simulated trapping. These machines were all low power and cost and all had a small beta ratio. In 2010, Carl Greninger founded the northwest nuclear consortium, an organization which teaches nuclear engineering principles to high school students, using a 60 kvolt fusor.[50][51] In 2012, Mark Suppes received attention,[52][53] for a fusor. Suppes also measured electron trapping inside a polywell.[54] In 2013, the first IEC textbook was published by George H. Miley.[55]

2020s edit

Avalanche Energy is a start-up with about $51 million in venture/DOD funding that is working on small (tens of centimetres), modular, fusion batteries producing 5kWe. They are targeting 600 kV for their device to achieve certain design goals. Their Orbitron concept electrostatically (magnetron-augmented) confines ions orbiting around a high voltage (00s of kVs) cathode in a high vacuum environment (p< 10 −8 Torr) surrounded by one or two anode shells separated by a dielectric. Concerns include breakdown of the vacuum/dielectric and insulator surface flashover. Permanent magnet/electromagnet magnetic field generators are arranged coaxially around the anode. The magnetic field strength is targeted to exceed a Hull cut-off condition, ranging from 50-4,000 kV. Candidate ions include protons (m/z=1), deuterium (m/z=2), tritium (m/z=3), lithium-6 (m/z=6), and boron-11 (m/z=11). Recent progress includes successful testing of a 300 kV bushing.[56]

Designs with cage edit

Fusor edit

The best known IEC device is the fusor.[12] This device typically consists of two wire cages inside a vacuum chamber. These cages are referred to as grids. The inner cage is held at a negative voltage against the outer cage. A small amount of fusion fuel is introduced (deuterium gas being the most common). The voltage between the grids causes the fuel to ionize. The positive ions fall down the voltage drop toward the negative inner cage. As they accelerate, the electric field does work on the ions, heating them to fusion conditions. If these ions collide, they can fuse. Fusors can also use ion guns rather than electric grids. Fusors are popular with amateurs,[57] because they can easily be constructed, can regularly produce fusion and are a practical way to study nuclear physics. Fusors have also been used as a commercial neutron generator for industrial applications.[58]

No fusor has come close to producing a significant amount of fusion power. They can be dangerous if proper care is not taken because they require high voltages and can produce harmful radiation (neutrons and X-rays). Often, ions collide with the cages or wall. This conducts energy away from the device limiting its performance. In addition, collisions heat the grids, which limits high-power devices. Collisions also spray high-mass ions into the reaction chamber, pollute the plasma, and cool the fuel.

POPS edit

In examining nonthermal plasma, workers at LANL realized that scattering was more likely than fusion. This was due to the coulomb scattering cross section being larger than the fusion cross section.[59] In response they built POPS,[60][61] a machine with a wire cage, where ions are moving at steady-state, or oscillating around. Such plasma can be at local thermodynamic equilibrium.[62] The ion oscillation is predicted to maintain the equilibrium distribution of the ions at all times, which would eliminate any power loss due to Coulomb scattering, resulting in a net energy gain. Working off this design, researchers in Russia simulated the POPS design using particle-in-cell code in 2009.[63] This reactor concept becomes increasingly efficient as the size of the device shrinks. However, very high transparencies (>99.999%) are required for successful operation of the POPS concept. To this end S. Krupakar Murali et al., suggested that carbon nanotubes can be used to construct the cathode grids.[64] This is also the first (suggested) application of carbon nanotubes directly in any fusion reactor.

Designs with fields edit

Several schemes attempt to combine magnetic confinement and electrostatic fields with IEC. The goal is to eliminate the inner wire cage of the fusor, and the resulting problems.

Polywell edit

The polywell uses a magnetic field to trap electrons. When electrons or ions move into a dense field, they can be reflected by the magnetic mirror effect.[15] A polywell is designed to trap electrons in the center, with a dense magnetic field surrounding them.[49][65][66] This is typically done using six electromagnets in a box. Each magnet is positioned so their poles face inward, creating a null point in the center. The electrons trapped in the center form a "virtual electrode"[67] Ideally, this electron cloud accelerates ions to fusion conditions.[19]

Penning trap edit

 
Penning trap cross-section. Axis is vertical. Electrons orbit the center under DC electrostatic (blue) and DC magnetic (red) confinement. In this diagram the confined particles are positive; to confine electrons, the electrodes' polarities must be swapped.

A Penning trap uses both an electric and a magnetic field to trap particles, a magnetic field to confine particles radially and a quadrupole electric field to confine the particles axially.[68]

In a Penning trap fusion reactor, first the magnetic and electric fields are turned on. Then, electrons are emitted into the trap, caught and measured. The electrons form a virtual electrode similar to that in a polywell, described above. These electrons are intended to then attract ions, accelerating them to fusion conditions.[69]

In the 1990s, researchers at LANL built a Penning trap to do fusion experiments. Their device (PFX) was a small (millimeters) and low power (one fifth of a tesla, less than ten thousand volts) machine.[36]

Marble edit

MARBLE (multiple ambipolar recirculating beam line experiment) was a device which moved electrons and ions back and forth in a line.[34] Particle beams were reflected using electrostatic optics.[70] These optics made static voltage surfaces in free space.[citation needed] Such surfaces reflect only particles with a specific kinetic energy, while higher-energy particles can traverse these surfaces unimpeded, although not unaffected. Electron trapping and plasma behavior was measured by Langmuir probe.[34] Marble kept ions on orbits that do not intersect grid wires—the latter also improves the space charge limitations by multiple nesting of ion beams at several energies.[71] Researchers encountered problems with ion losses at the reflection points. Ions slowed down when turning, spending much time there, leading to high conduction losses.[72]

MIX edit

The multipole ion-beam experiment (MIX) accelerated ions and electrons into a negatively charged electromagnet.[32] Ions were focused using Gabor lensing. Researcher had problems with a very thin ion-turning region very close to a solid surface[32] where ions could be conducted away.

Magnetically insulated edit

Devices have been proposed where the negative cage is magnetically insulated from the incoming plasmas.[73]

General criticism edit

In 1995, Todd Rider critiqued all fusion power schemes using plasma systems not at thermodynamic equilibrium.[23] Rider assumed that plasma clouds at equilibrium had the following properties:

  • They were quasineutral, where the positives and negatives are equally mixed together.[23]
  • They had evenly mixed fuel.[23]
  • They were isotropic, meaning that its behavior was the same in any given direction.[23]
  • The plasma had a uniform energy and temperature throughout the cloud.[23]
  • The plasma was an unstructured Gaussian sphere.

Rider argued that if such system was sufficiently heated, it could not be expected to produce net power, due to high X-ray losses.

Other fusion researchers such as Nicholas Krall,[74] Robert W. Bussard,[67] Norman Rostoker, and Monkhorst disagreed with this assessment. They argue that the plasma conditions inside IEC machines are not quasineutral and have non-thermal energy distributions.[75] Because the electron has a mass and diameter much smaller than the ion, the electron temperature can be several orders of magnitude different than the ions. This may allow the plasma to be optimized, whereby cold electrons would reduce radiation losses and hot ions would raise fusion rates.[41]

Thermalization edit

 
This is an energy distribution comparison of thermalized and non-thermalized ions

The primary problem that Rider has raised is the thermalization of ions. Rider argued that, in a quasineutral plasma where all the positives and negatives are distributed equally, the ions will interact. As they do, they exchange energy, causing their energy to spread out (in a Wiener process) heading to a bell curve (or Gaussian function) of energy. Rider focused his arguments within the ion population and did not address electron-to-ion energy exchange or non-thermal plasmas.

This spreading of energy causes several problems. One problem is making more and more cold ions, which are too cold to fuse. This would lower output power. Another problem is higher energy ions which have so much energy that they can escape the machine. This lowers fusion rates while raising conduction losses, because as the ions leave, energy is carried away with them.

Radiation edit

Rider estimated that once the plasma is thermalized the radiation losses would outpace any amount of fusion energy generated. He focused on a specific type of radiation: X-ray radiation. A particle in a plasma will radiate light anytime it speeds up or slows down. This can be estimated using the Larmor formula. Rider estimated this for D–T (deuterium–tritium fusion), D–D (deuterium fusion), and D–He3 (deuterium–helium 3 fusion), and that breakeven operation with any fuel except D–T is difficult.[23]

Core focus edit

In 1995, Nevins argued that such machines would need to expend a great deal of energy maintaining ion focus in the center. The ions need to be focused so that they can find one another, collide, and fuse. Over time the positive ions and negative electrons would naturally intermix because of electrostatic attraction. This causes the focus to be lost. This is core degradation. Nevins argued mathematically, that the fusion gain (ratio of fusion power produced to the power required to maintain the non-equilibrium ion distribution function) is limited to 0.1 assuming that the device is fueled with a mixture of deuterium and tritium.[24]

The core focus problem was also identified in fusors by Tim Thorson at the University of Wisconsin–Madison during his 1996 doctoral work.[1] Charged ions would have some motion before they started accelerating in the center. This motion could be a twisting motion, where the ion had angular momentum, or simply a tangential velocity. This initial motion causes the cloud in the center of the fusor to be unfocused.

Brillouin limit edit

In 1945, Columbia University professor Léon Brillouin, suggested that there was a limit to how many electrons one could pack into a given volume.[76] This limit is commonly referred to as the Brillouin limit or Brillouin density,[77] this is shown below.[36]

 

Where B is the magnetic field,   the permeability of free space, m the mass of confined particles, and c the speed of light. This may limit the charge density inside IEC devices.

Commercial applications edit

Since fusion reactions generates neutrons, the fusor has been developed into a family of compact sealed reaction chamber neutron generators[78] for a wide range of applications that need moderate neutron output rates at a moderate price. Very high output neutron sources may be used to make products such as molybdenum-99[39] and nitrogen-13, medical isotopes used for PET scans.[79]

Devices edit

Government and commercial edit

  • Los Alamos National Laboratory Researchers developed[80] POPS and Penning trap[35]
  • Turkish Atomic Energy Authority In 2013 this team built a 30 cm fusor at the Saraykoy Nuclear Research and Training center in Turkey. This fusor can reach 85 kV and do deuterium fusion, producing 2.4×104 neutrons per second.[81]
  • ITT Corporation Hirschs original machine was a 17.8 cm diameter machine with 150 kV voltage drop across it.[12] This machine used ion beams.
  • Phoenix Nuclear Labs has developed a commercial neutron source based on a fusor, achieving 3×1011 neutrons per second with the deuterium-deuterium fusion reaction for 132 hours of continuous operation.[39]
  • Energy Matter Conversion Inc Is a company in Santa Fe which has developed large high powered polywell devices for the US Navy.
  • NSD-Gradel-Fusion sealed IEC neutron generators for DD (2.5 MeV) or DT (14 MeV) with a range of maximum outputs are manufactured by Gradel sárl in Luxembourg.[78]
  • Atomic Energy Organization of Iran Researchers at Shahid Beheshti University in Iran have built a 60 cm diameter fusor which can produce 2×107 neutrons per second at 80 kilovolts using deuterium gas.[82]
  • Avalanche Energy has received $5 million in venture capital to build their prototype.[83]
  • CPP-IPR in India, has achieved a significant milestone by pioneering the development of India's first Inertial Electrostatic Confinement Fusion (IECF) neutron source. The device is capable of reaching an energy potential of -92kV. It can generate an neutron yield of up to 107 neutrons per second by deuterium fusion. The primary objective of this program is to propel the advancement of portable and handheld neutron sources, characterized by both linear and spherical geometries.[84]

Universities edit

  • Tokyo Institute of Technology has four IEC devices of different shapes: a spherical machine, a cylindrical device, a co-axial double cylinder and a magnetically assisted device.[85]
  • University of Wisconsin–Madison – A group at Wisconsin–Madison has several large devices, since 1995.[86]
  • University of Illinois at Urbana–Champaign – The fusion studies laboratory has built a ~25 cm fusor which has produced 107 neutrons using deuterium gas.[26]
  • Massachusetts Institute of Technology – For his doctoral thesis in 2007, Carl Dietrich built a fusor and studied its potential use in spacecraft propulsion.[87] Also, Thomas McGuire studied multiple well fusors for applications in spaceflight.[87]
  • University of Sydney has built several IEC devices and also low power, low beta ratio polywells. The first was constructed of Teflon rings and was about the size of a coffee cup. The second has ~12" diameter full casing, metal rings.
  • Eindhoven Technical University[88]
  • Amirkabir University of Technology and Atomic Energy Organization of Iran have investigated the effect of strong pulsed magnetic fields on the neutron production rate of IEC device. Their study showed that by 1-2 Tesla magnetic field it is possible to increase the discharge current and neutron production rate more than ten times with respect to the ordinary operation.[89]
  • The Institute of Space Systems at the University of Stuttgart, is developing IEC devices for plasma physics research and also as an electric propulsion device, the IECT (Inertial Electrostatic Confinement Thruster).[90][91][92]

See also edit

Patents edit

  • P.T. Farnsworth, U.S. Patent 3,258,402, June 1966 (Electric discharge — Nuclear interaction)
  • P.T. Farnsworth, U.S. Patent 3,386,883. June 1968 (Method and apparatus)
  • Hirsch, Robert, U.S. Patent 3,530,036. September 1970 (Apparatus)
  • Hirsch, Robert, U.S. Patent 3,530,497. September 1970 (Generating apparatus — Hirsch/Meeks)
  • Hirsch, Robert, U.S. Patent 3,533,910. October 1970 (Lithium-Ion source)
  • Hirsch, Robert, U.S. Patent 3,655,508. April 1972 (Reduce plasma leakage)
  • Hirsch, Robert, U.S. Patent 3,664,920. May 1972 (Electrostatic containment)
  • R.W. Bussard, "Method and apparatus for controlling charged particles", U.S. Patent 4,826,646, May 1989 (Method and apparatus — Magnetic grid fields)
  • R.W. Bussard, "Method and apparatus for creating and controlling nuclear fusion reactions", U.S. Patent 5,160,695, November 1992 (Method and apparatus — Ion acoustic waves)
  • S.T. Brookes, "Nuclear fusion reactor", UK patent GB2461267, May 2012
  • T.V. Stanko, "Nuclear fusion device", UK patent GB2545882, July 2017

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External links edit

  • Polywell Fusion: Electrostatic Fusion in a Magnetic Cusp, talk at Microsoft Research
  • University of Wisconsin-Madison IEC homepage
  • From Proceedings of the 1999 Fusion Summer Study (Snowmass, Colorado):
    • Summary of Physics Aspects of Some Emerging Concepts 2006-03-14 at the Wayback Machine
    • Inertial-Electrostatic Confinement (IEC) of a Fusion Plasma with Grids 2006-03-14 at the Wayback Machine
  • Fusion from Television? (American Scientist Magazine, July-August 1999) 2017-06-04 at the Wayback Machine
  • Should Google Go Nuclear? Clean, cheap, nuclear power (no, really) 2007-11-10 at the Wayback Machine
  • NSD-Gradel-Fusion, NSD-Gradel-Fusion (Luxembourg)

inertial, electrostatic, confinement, class, fusion, power, devices, that, electric, fields, confine, plasma, rather, than, more, common, approach, using, magnetic, fields, found, magnetic, confinement, fusion, designs, most, devices, directly, accelerate, the. Inertial electrostatic confinement or IEC is a class of fusion power devices that use electric fields to confine the plasma rather than the more common approach using magnetic fields found in magnetic confinement fusion MCF designs Most IEC devices directly accelerate their fuel to fusion conditions thereby avoiding energy losses seen during the longer heating stages of MCF devices In theory this makes them more suitable for using alternative aneutronic fusion fuels which offer a number of major practical benefits and makes IEC devices one of the more widely studied approaches to fusion A fusor exhibiting nuclear fusion in star modeAs the negatively charged electrons and positively charged ions in the plasma move in different directions in an electric field the field has to be arranged in some fashion so that the two particles remain close together Most IEC designs achieve this by pulling the electrons or ions across a potential well beyond which the potential drops and the particles continue to move due to their inertia Fusion occurs in this lower potential area when ions moving in different directions collide Because the motion provided by the field creates the energy levels needed for fusion not random collisions with the rest of the fuel the bulk of the plasma does not have to be hot and the systems as a whole work at much lower temperatures and energy levels than MCF devices One of the simpler IEC devices is the fusor which consists of two concentric metal wire spherical grids When the grids are charged to a high voltage the fuel gas ionizes The field between the two then accelerates the fuel inward and when it passes the inner grid the field drops and the ions continue inward toward the center If they impact with another ion they may undergo fusion If they do not they travel out of the reaction area into the charged area again where they are re accelerated inward Overall the physical process is similar to the colliding beam fusion although beam devices are linear instead of spherical Other IEC designs like the polywell differ largely in the arrangement of the fields used to create the potential well A number of detailed theoretical studies have pointed out that the IEC approach is subject to a number of energy loss mechanisms that are not present if the fuel is evenly heated or Maxwellian These loss mechanisms appear to be greater than the rate of fusion in such devices meaning they can never reach fusion breakeven and thus be used for power production These mechanisms are more powerful when the atomic mass of the fuel increases which suggests IEC also does not have any advantage with aneutronic fuels Whether these critiques apply to specific IEC devices remains highly contentious Contents 1 Mechanism 2 History 2 1 1930s 2 2 1950s 2 3 1960s 2 4 1980s 2 5 1990s 2 6 2000s 2 7 2010s 2 8 2020s 3 Designs with cage 3 1 Fusor 3 2 POPS 4 Designs with fields 4 1 Polywell 4 2 Penning trap 4 3 Marble 4 4 MIX 4 5 Magnetically insulated 5 General criticism 5 1 Thermalization 5 2 Radiation 5 3 Core focus 5 4 Brillouin limit 6 Commercial applications 7 Devices 7 1 Government and commercial 7 2 Universities 8 See also 9 Patents 10 References 11 External linksMechanism editFor every volt that an ion is accelerated across its kinetic energy gain corresponds to an increase of temperature of 11 604 kelvins K For example a typical magnetic confinement fusion plasma is 15 keV which corresponds to 170 megakelvin MK An ion with a charge of one can reach this temperature by being accelerated across a 15 000 V drop This sort of voltage is easily achieved in common electrical devices a typical cathode ray tube operates in this range In fusors the voltage drop is made with a wire cage However high conduction losses occur in fusors because most ions fall into the cage before fusion can occur This prevents current fusors from ever producing net power nbsp This is an illustration of the basic mechanism of fusion in fusors 1 The fusor contains two concentric wire cages The cathode is inside the anode 2 Positive ions are attracted to the inner cathode They fall down the voltage drop The electric field does work on the ions heating them to fusion conditions 3 The ions miss the inner cage 4 The ions collide in the center and may fuse 1 2 History edit1930s edit Mark Oliphant adapts Cockcroft and Walton s particle accelerator at the Cavendish Laboratory to create tritium and helium 3 by nuclear fusion 3 1950s edit nbsp This picture shows the anode cathode design for different IEC concepts and experiments Three researchers at LANL including Jim Tuck first explored the idea theoretically in a 1959 paper 4 The idea had been proposed by a colleague 5 The concept was to capture electrons inside a positive cage The electrons would accelerate the ions to fusion conditions Other concepts were being developed which would later merge into the IEC field These include the publication of the Lawson criterion by John D Lawson in 1957 in England 6 This puts on minimum criteria on power plant designs which do fusion using hot Maxwellian plasma clouds Also work exploring how electrons behave inside the biconic cusp done by Harold Grad group at the Courant Institute in 1957 7 8 A biconic cusp is a device with two alike magnetic poles facing one another i e north north Electrons and ions can be trapped between these 1960s edit nbsp U S Patent 3 386 883 Schematic from Philo Farnsworth 1968 patent This device has an inner cage to make the field and four ion guns on the outside In his work with vacuum tubes Philo Farnsworth observed that electric charge would accumulate in regions of the tube Today this effect is known as the multipactor effect 9 Farnsworth reasoned that if ions were concentrated high enough they could collide and fuse In 1962 he filed a patent on a design using a positive inner cage to concentrate plasma in order to achieve nuclear fusion 10 During this time Robert L Hirsch joined the Farnsworth Television labs and began work on what became the fusor Hirsch patented the design in 1966 11 and published the design in 1967 12 The Hirsch machine was a 17 8 cm diameter machine with 150 kV voltage drop across it and used ion beams to help inject material Simultaneously a key plasma physics text was published by Lyman Spitzer at Princeton in 1963 13 Spitzer took the ideal gas laws and adapted them to an ionized plasma developing many of the fundamental equations used to model a plasma Meanwhile magnetic mirror theory and direct energy conversion were developed by Richard F Post s group at LLNL 14 15 A magnetic mirror or magnetic bottle is similar to a biconic cusp except that the poles are reversed 1980s edit In 1980 Robert W Bussard developed a cross between a fusor and magnetic mirror the polywell The idea was to confine a non neutral plasma using magnetic fields This would in turn attract ions This idea had been published previously notably by Oleg Lavrentiev in Russia 16 17 18 Bussard patented 19 the design and received funding from Defense Threat Reduction Agency DARPA and the US Navy to develop the idea 20 1990s edit Bussard and Nicholas Krall published theory and experimental results in the early nineties 21 22 In response Todd Rider at MIT under Lawrence Lidsky developed general models of the device 23 Rider argued that the device was fundamentally limited That same year 1995 William Nevins at LLNL published a criticism of the polywell 24 Nevins argued that the particles would build up angular momentum causing the dense core to degrade In the mid nineties Bussard publications prompted the development of fusors at the University of Wisconsin Madison and at the University of Illinois at Urbana Champaign Madison s machine was first built in 1995 25 George H Miley s team at Illinois built a 25 cm fusor which has produced 107 neutrons using deuterium gas 26 and discovered the star mode of fusor operation in 1994 27 The following year the first US Japan Workshop on IEC Fusion was conducted This is now the premier conference for IEC researchers At this time in Europe an IEC device was developed as a commercial neutron source by Daimler Chrysler Aerospace under the name FusionStar 28 In the late nineties hobbyist Richard Hull began building amateur fusors in his home 29 In March 1999 he achieved a neutron rate of 105 neutrons per second 30 Hull and Paul Schatzkin started fusor net in 1998 31 Through this open forum a community of amateur fusioneers have done nuclear fusion using homemade fusors 2000s edit Despite demonstration in 2000 of 7200 hours of operation without degradation at high input power as a sealed reaction chamber with automated control the FusionStar project was canceled and the company NSD Ltd was founded The spherical FusionStar technology was then further developed as a linear geometry system with improved efficiency and higher neutron output by NSD Ltd which became NSD Fusion GmbH in 2005 In early 2000 Alex Klein developed a cross between a polywell and ion beams 32 Using Gabor lensing Dr Klein attempted to focus plasma into non neutral clouds for fusion He founded FP generation which in April 2009 raised 3 million in financing from two venture funds 33 34 The company developed the MIX and Marble machine but ran into technical challenges and closed In response to Riders criticisms researchers at LANL reasoned that a plasma oscillating could be at local thermodynamic equilibrium this prompted the POPS and Penning trap machines 35 36 At this time MIT researchers became interested in fusors for space propulsion 37 and powering space vehicles 38 Specifically researchers developed fusors with multiple inner cages In 2005 Greg Piefer founded Phoenix Nuclear Labs to develop the fusor into a neutron source for the mass production of medical isotopes 39 Robert Bussard began speaking openly about the Polywell in 2006 40 He attempted to generate interest 41 in the research before passing away from multiple myeloma in 2007 42 His company was able to raise over ten million in funding from the US Navy in 2008 43 44 and 2009 45 2010s edit Bussard s publications prompted the University of Sydney to start research into electron trapping in polywells in 2010 46 The group has explored theory 47 modeled devices 48 built devices measured trapping 49 and simulated trapping These machines were all low power and cost and all had a small beta ratio In 2010 Carl Greninger founded the northwest nuclear consortium an organization which teaches nuclear engineering principles to high school students using a 60 kvolt fusor 50 51 In 2012 Mark Suppes received attention 52 53 for a fusor Suppes also measured electron trapping inside a polywell 54 In 2013 the first IEC textbook was published by George H Miley 55 2020s edit Avalanche Energy is a start up with about 51 million in venture DOD funding that is working on small tens of centimetres modular fusion batteries producing 5kWe They are targeting 600 kV for their device to achieve certain design goals Their Orbitron concept electrostatically magnetron augmented confines ions orbiting around a high voltage 00s of kVs cathode in a high vacuum environment p lt 10 8 Torr surrounded by one or two anode shells separated by a dielectric Concerns include breakdown of the vacuum dielectric and insulator surface flashover Permanent magnet electromagnet magnetic field generators are arranged coaxially around the anode The magnetic field strength is targeted to exceed a Hull cut off condition ranging from 50 4 000 kV Candidate ions include protons m z 1 deuterium m z 2 tritium m z 3 lithium 6 m z 6 and boron 11 m z 11 Recent progress includes successful testing of a 300 kV bushing 56 Designs with cage editFusor edit The best known IEC device is the fusor 12 This device typically consists of two wire cages inside a vacuum chamber These cages are referred to as grids The inner cage is held at a negative voltage against the outer cage A small amount of fusion fuel is introduced deuterium gas being the most common The voltage between the grids causes the fuel to ionize The positive ions fall down the voltage drop toward the negative inner cage As they accelerate the electric field does work on the ions heating them to fusion conditions If these ions collide they can fuse Fusors can also use ion guns rather than electric grids Fusors are popular with amateurs 57 because they can easily be constructed can regularly produce fusion and are a practical way to study nuclear physics Fusors have also been used as a commercial neutron generator for industrial applications 58 No fusor has come close to producing a significant amount of fusion power They can be dangerous if proper care is not taken because they require high voltages and can produce harmful radiation neutrons and X rays Often ions collide with the cages or wall This conducts energy away from the device limiting its performance In addition collisions heat the grids which limits high power devices Collisions also spray high mass ions into the reaction chamber pollute the plasma and cool the fuel POPS edit In examining nonthermal plasma workers at LANL realized that scattering was more likely than fusion This was due to the coulomb scattering cross section being larger than the fusion cross section 59 In response they built POPS 60 61 a machine with a wire cage where ions are moving at steady state or oscillating around Such plasma can be at local thermodynamic equilibrium 62 The ion oscillation is predicted to maintain the equilibrium distribution of the ions at all times which would eliminate any power loss due to Coulomb scattering resulting in a net energy gain Working off this design researchers in Russia simulated the POPS design using particle in cell code in 2009 63 This reactor concept becomes increasingly efficient as the size of the device shrinks However very high transparencies gt 99 999 are required for successful operation of the POPS concept To this end S Krupakar Murali et al suggested that carbon nanotubes can be used to construct the cathode grids 64 This is also the first suggested application of carbon nanotubes directly in any fusion reactor Designs with fields editSeveral schemes attempt to combine magnetic confinement and electrostatic fields with IEC The goal is to eliminate the inner wire cage of the fusor and the resulting problems Polywell edit The polywell uses a magnetic field to trap electrons When electrons or ions move into a dense field they can be reflected by the magnetic mirror effect 15 A polywell is designed to trap electrons in the center with a dense magnetic field surrounding them 49 65 66 This is typically done using six electromagnets in a box Each magnet is positioned so their poles face inward creating a null point in the center The electrons trapped in the center form a virtual electrode 67 Ideally this electron cloud accelerates ions to fusion conditions 19 Penning trap edit nbsp Penning trap cross section Axis is vertical Electrons orbit the center under DC electrostatic blue and DC magnetic red confinement In this diagram the confined particles are positive to confine electrons the electrodes polarities must be swapped A Penning trap uses both an electric and a magnetic field to trap particles a magnetic field to confine particles radially and a quadrupole electric field to confine the particles axially 68 In a Penning trap fusion reactor first the magnetic and electric fields are turned on Then electrons are emitted into the trap caught and measured The electrons form a virtual electrode similar to that in a polywell described above These electrons are intended to then attract ions accelerating them to fusion conditions 69 In the 1990s researchers at LANL built a Penning trap to do fusion experiments Their device PFX was a small millimeters and low power one fifth of a tesla less than ten thousand volts machine 36 Marble edit MARBLE multiple ambipolar recirculating beam line experiment was a device which moved electrons and ions back and forth in a line 34 Particle beams were reflected using electrostatic optics 70 These optics made static voltage surfaces in free space citation needed Such surfaces reflect only particles with a specific kinetic energy while higher energy particles can traverse these surfaces unimpeded although not unaffected Electron trapping and plasma behavior was measured by Langmuir probe 34 Marble kept ions on orbits that do not intersect grid wires the latter also improves the space charge limitations by multiple nesting of ion beams at several energies 71 Researchers encountered problems with ion losses at the reflection points Ions slowed down when turning spending much time there leading to high conduction losses 72 MIX edit The multipole ion beam experiment MIX accelerated ions and electrons into a negatively charged electromagnet 32 Ions were focused using Gabor lensing Researcher had problems with a very thin ion turning region very close to a solid surface 32 where ions could be conducted away Magnetically insulated edit Devices have been proposed where the negative cage is magnetically insulated from the incoming plasmas 73 General criticism editIn 1995 Todd Rider critiqued all fusion power schemes using plasma systems not at thermodynamic equilibrium 23 Rider assumed that plasma clouds at equilibrium had the following properties They were quasineutral where the positives and negatives are equally mixed together 23 They had evenly mixed fuel 23 They were isotropic meaning that its behavior was the same in any given direction 23 The plasma had a uniform energy and temperature throughout the cloud 23 The plasma was an unstructured Gaussian sphere Rider argued that if such system was sufficiently heated it could not be expected to produce net power due to high X ray losses Other fusion researchers such as Nicholas Krall 74 Robert W Bussard 67 Norman Rostoker and Monkhorst disagreed with this assessment They argue that the plasma conditions inside IEC machines are not quasineutral and have non thermal energy distributions 75 Because the electron has a mass and diameter much smaller than the ion the electron temperature can be several orders of magnitude different than the ions This may allow the plasma to be optimized whereby cold electrons would reduce radiation losses and hot ions would raise fusion rates 41 Thermalization edit nbsp This is an energy distribution comparison of thermalized and non thermalized ionsThe primary problem that Rider has raised is the thermalization of ions Rider argued that in a quasineutral plasma where all the positives and negatives are distributed equally the ions will interact As they do they exchange energy causing their energy to spread out in a Wiener process heading to a bell curve or Gaussian function of energy Rider focused his arguments within the ion population and did not address electron to ion energy exchange or non thermal plasmas This spreading of energy causes several problems One problem is making more and more cold ions which are too cold to fuse This would lower output power Another problem is higher energy ions which have so much energy that they can escape the machine This lowers fusion rates while raising conduction losses because as the ions leave energy is carried away with them Radiation edit Rider estimated that once the plasma is thermalized the radiation losses would outpace any amount of fusion energy generated He focused on a specific type of radiation X ray radiation A particle in a plasma will radiate light anytime it speeds up or slows down This can be estimated using the Larmor formula Rider estimated this for D T deuterium tritium fusion D D deuterium fusion and D He3 deuterium helium 3 fusion and that breakeven operation with any fuel except D T is difficult 23 Core focus edit In 1995 Nevins argued that such machines would need to expend a great deal of energy maintaining ion focus in the center The ions need to be focused so that they can find one another collide and fuse Over time the positive ions and negative electrons would naturally intermix because of electrostatic attraction This causes the focus to be lost This is core degradation Nevins argued mathematically that the fusion gain ratio of fusion power produced to the power required to maintain the non equilibrium ion distribution function is limited to 0 1 assuming that the device is fueled with a mixture of deuterium and tritium 24 The core focus problem was also identified in fusors by Tim Thorson at the University of Wisconsin Madison during his 1996 doctoral work 1 Charged ions would have some motion before they started accelerating in the center This motion could be a twisting motion where the ion had angular momentum or simply a tangential velocity This initial motion causes the cloud in the center of the fusor to be unfocused Brillouin limit edit In 1945 Columbia University professor Leon Brillouin suggested that there was a limit to how many electrons one could pack into a given volume 76 This limit is commonly referred to as the Brillouin limit or Brillouin density 77 this is shown below 36 N B 2 2 m 0 m c 2 displaystyle N frac B 2 2 mu 0 mc 2 nbsp Where B is the magnetic field m 0 displaystyle mu 0 nbsp the permeability of free space m the mass of confined particles and c the speed of light This may limit the charge density inside IEC devices Commercial applications editSince fusion reactions generates neutrons the fusor has been developed into a family of compact sealed reaction chamber neutron generators 78 for a wide range of applications that need moderate neutron output rates at a moderate price Very high output neutron sources may be used to make products such as molybdenum 99 39 and nitrogen 13 medical isotopes used for PET scans 79 Devices editGovernment and commercial edit Los Alamos National Laboratory Researchers developed 80 POPS and Penning trap 35 Turkish Atomic Energy Authority In 2013 this team built a 30 cm fusor at the Saraykoy Nuclear Research and Training center in Turkey This fusor can reach 85 kV and do deuterium fusion producing 2 4 104 neutrons per second 81 ITT Corporation Hirschs original machine was a 17 8 cm diameter machine with 150 kV voltage drop across it 12 This machine used ion beams Phoenix Nuclear Labs has developed a commercial neutron source based on a fusor achieving 3 1011 neutrons per second with the deuterium deuterium fusion reaction for 132 hours of continuous operation 39 Energy Matter Conversion Inc Is a company in Santa Fe which has developed large high powered polywell devices for the US Navy NSD Gradel Fusion sealed IEC neutron generators for DD 2 5 MeV or DT 14 MeV with a range of maximum outputs are manufactured by Gradel sarl in Luxembourg 78 Atomic Energy Organization of Iran Researchers at Shahid Beheshti University in Iran have built a 60 cm diameter fusor which can produce 2 107 neutrons per second at 80 kilovolts using deuterium gas 82 Avalanche Energy has received 5 million in venture capital to build their prototype 83 CPP IPR in India has achieved a significant milestone by pioneering the development of India s first Inertial Electrostatic Confinement Fusion IECF neutron source The device is capable of reaching an energy potential of 92kV It can generate an neutron yield of up to 107 neutrons per second by deuterium fusion The primary objective of this program is to propel the advancement of portable and handheld neutron sources characterized by both linear and spherical geometries 84 Universities edit Tokyo Institute of Technology has four IEC devices of different shapes a spherical machine a cylindrical device a co axial double cylinder and a magnetically assisted device 85 University of Wisconsin Madison A group at Wisconsin Madison has several large devices since 1995 86 University of Illinois at Urbana Champaign The fusion studies laboratory has built a 25 cm fusor which has produced 107 neutrons using deuterium gas 26 Massachusetts Institute of Technology For his doctoral thesis in 2007 Carl Dietrich built a fusor and studied its potential use in spacecraft propulsion 87 Also Thomas McGuire studied multiple well fusors for applications in spaceflight 87 University of Sydney has built several IEC devices and also low power low beta ratio polywells The first was constructed of Teflon rings and was about the size of a coffee cup The second has 12 diameter full casing metal rings Eindhoven Technical University 88 Amirkabir University of Technology and Atomic Energy Organization of Iran have investigated the effect of strong pulsed magnetic fields on the neutron production rate of IEC device Their study showed that by 1 2 Tesla magnetic field it is possible to increase the discharge current and neutron production rate more than ten times with respect to the ordinary operation 89 The Institute of Space Systems at the University of Stuttgart is developing IEC devices for plasma physics research and also as an electric propulsion device the IECT Inertial Electrostatic Confinement Thruster 90 91 92 See also edit nbsp Nuclear technology portalFusor List of fusion experiments List of plasma physics articles Northwest Nuclear Consortium Philo Farnsworth Phoenix Nuclear labs Polywell Robert Bussard Taylor WilsonPatents editP T Farnsworth U S Patent 3 258 402 June 1966 Electric discharge Nuclear interaction P T Farnsworth U S Patent 3 386 883 June 1968 Method and apparatus Hirsch Robert U S Patent 3 530 036 September 1970 Apparatus Hirsch Robert U S Patent 3 530 497 September 1970 Generating apparatus Hirsch Meeks Hirsch Robert U S Patent 3 533 910 October 1970 Lithium Ion source Hirsch Robert U S Patent 3 655 508 April 1972 Reduce plasma leakage Hirsch Robert U S Patent 3 664 920 May 1972 Electrostatic containment R W Bussard Method and apparatus for controlling charged particles U S Patent 4 826 646 May 1989 Method and apparatus Magnetic grid fields R W Bussard Method and apparatus for creating and controlling nuclear fusion reactions U S Patent 5 160 695 November 1992 Method and apparatus Ion acoustic waves S T Brookes Nuclear fusion reactor UK patent GB2461267 May 2012 T V Stanko Nuclear fusion device UK patent GB2545882 July 2017References edit a b Thorson Timothy A 1996 Ion flow and fusion reactivity characterization of a spherically convergent ion focus Ph D University of Wisconsin Madison OCLC 615996599 Thorson T A Durst R D Fonck R J Sontag A C 17 July 1997 Fusion reactivity characterization of a spherically convergent ion focus Nuclear Fusion International Atomic Energy Agency published April 1998 38 4 495 507 Bibcode 1998NucFu 38 495T doi 10 1088 0029 5515 38 4 302 S2CID 250841151 Oliphant M L E Harteck P Rutherford L 1934 05 01 Transmutation Effects Observed with Heavy Hydrogen Proceedings of the Royal Society A Mathematical Physical and Engineering Sciences The Royal Society 144 853 692 703 Bibcode 1934RSPSA 144 692O doi 10 1098 rspa 1934 0077 ISSN 1364 5021 Elmore William C Tuck James L Watson Kenneth M 1959 On the Inertial Electrostatic Confinement of a Plasma Physics of Fluids AIP Publishing 2 3 239 Bibcode 1959PhFl 2 239E doi 10 1063 1 1705917 ISSN 0031 9171 W H Wells Bendix Aviation Corporation private communication 1954 Some Criteria for a Power Producing Thermonuclear Reactor J D Lawson Atomic Energy Research Establishment Harwell Berks 2 November 1956 Grad H Theory of Cusped Geometries I General Survey NYO 7969 Inst Math Sci N Y U December 1 1957 Berkowitz J Theory of Cusped Geometries II Particle Losses NYO 2530 Inst Math Sci N Y U January 6 1959 Cartlidge Edwin The Secret World of Amateur Fusion Physics World March 2007 IOP Publishing Ltd pp 10 11 ISSN 0953 8585 US Patent 3 258 402 June 28 1966 US Patent 3 386 883 June 4 1968 a b c Hirsch Robert L 1967 Inertial Electrostatic Confinement of Ionized Fusion Gases Journal of Applied Physics 38 7 4522 4534 Bibcode 1967JAP 38 4522H doi 10 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Retrieved 2020 09 09 Inertial Electrostatic Confinement Project University of Wisconsin Madison iec neep wisc edu Archived from the original on 2014 02 02 Retrieved 2023 02 09 a b Miley George H 1999 A portable neutron tunable X ray source based on inertial electrostatic confinement Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment Elsevier BV 422 1 3 16 20 Bibcode 1999NIMPA 422 16M doi 10 1016 s0168 9002 98 01108 5 ISSN 0168 9002 Miley Abstract Accomplishments www avrc com Miley abstract accomplishments doc Miley George H Sved J 2000 The IEC star mode fusion neutron source for NAA status and next step designs Appl Radiat Isot 53 4 5 779 83 doi 10 1016 s0969 8043 00 00215 3 PMID 11003520 Living with a nuclear reactor The Wall Street Journal interview with Sam Schechner https www youtube com watch v LJL3RQ4I iE Archived 2016 07 22 at the Wayback Machine The Neutron Club Richard Hull Accessed 6 9 2011 https 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on 2014 02 03 Retrieved 2014 01 28 Inertial Electrostatic Confinement IEC Fusion fundamentals and applications ISBN 978 1 4614 9337 2 Print 978 1 4614 9338 9 published December 26 2013 Wang Brian 2023 02 08 Avalanche Energy Making Technical Progress to a Lunchbox Size Nuclear Fusion Device NextBigFuture com Retrieved 2023 02 09 The Open Source Fusor Research Consortium fusor net Archived from the original on September 4 2020 Retrieved January 7 2014 Since its inception in 1998 Fusor net has provided valuable educational resources for hundreds of amateur scientists around the world There is absolutely no cost to users for these abundant resources Oldenburg awesome Webdesign Bremen Gradel Neutron generators of the latest technology with multiple possible applications nsd fusion com Archived from the original on 2020 10 20 Retrieved 2014 01 09 Evstatiev E G Nebel R A Chacon L Park J Lapenta G 2007 Space charge neutralization in inertial electrostatic con nement plasmas Phys Plasmas 14 4 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electrostatic confinement devices Physics of Plasmas AIP Publishing 5 7 2498 2503 Bibcode 1998PhPl 5 2498B doi 10 1063 1 872933 ISSN 1070 664X Bolukdemir A S Akgun Y Alacakir A 2013 05 23 Preliminary Results of Experimental Studies from Low Pressure Inertial Electrostatic Confinement Device Journal of Fusion Energy Springer Science and Business Media LLC 32 5 561 565 Bibcode 2013JFuE 32 561B doi 10 1007 s10894 013 9607 z ISSN 0164 0313 S2CID 120272975 Experimental Study of the Iranian Inertial Electrostatic Confinement Fusion Device as a Continuous Neutron Generator V Damideh Journal of Fusion Energy June 11 2011 Wesoff Eric 26 May 2022 This tiny fusion reactor is made out of commercially available parts Canary Media Archived from the original on 26 May 2022 Retrieved 27 May 2022 1 Overview of IEC Research at Tokyo Tech Eiki Hotta 15th annual US Japan IEC workshop October 7 2013 http www iae kyoto u ac jp beam iec2013 presentation 1 2 pdf Archived 2013 12 21 at the Wayback Machine R P Ashley G L Kulcinski J F Santarius S K Murali G Piefer 18th IEEE NPSS Symposium on Fusion Engineering IEEE 99CH37050 1999 a b Improving Particle Confinement in Inertial Electrostatic Fusion for Spacecraft Power and Propulsion submitted to the Department of Aeronautics and Astronautics Carl Dietrich February 2007 Fusor of the TU E Fusion Group Archived from the original on 2014 08 12 Retrieved 2014 07 23 Zaeem Alireza Asle Ghafoorifard Hassan Sadighzadeh Asghar 2019 Discharge current enhancement in inertial electrostatic confinement fusion by impulse high magnetic field Vacuum Elsevier BV 166 286 291 Bibcode 2019Vacuu 166 286Z doi 10 1016 j vacuum 2019 05 012 ISSN 0042 207X S2CID 164364500 Chan Yung An Herdrich Georg 2019 Jet extraction and characterization in an inertial electrostatic confinement device Vacuum Elsevier BV 167 482 489 Bibcode 2019Vacuu 167 482C doi 10 1016 j vacuum 2018 07 053 S2CID 104748598 Chan Yung An Herdrich Georg 2019 Influence of Cathode Dimension on Discharge Characteristics of Inertial Electrostatic Confinement Thruster International Electric Propulsion Conference 2019 IEPC 2019 292 Inertial Electrostatic Confinement Thruster IECT English shop Cuvillier Verlag cuvillier de Retrieved 2023 05 16 External links editPolywell Fusion Electrostatic Fusion in a Magnetic Cusp talk at Microsoft Research University of Wisconsin Madison IEC homepage IEC Overview From Proceedings of the 1999 Fusion Summer Study Snowmass Colorado Summary of Physics Aspects of Some Emerging Concepts Archived 2006 03 14 at the Wayback Machine Inertial Electrostatic Confinement IEC of a Fusion Plasma with Grids Archived 2006 03 14 at the Wayback Machine Fusion from Television American Scientist Magazine July August 1999 Archived 2017 06 04 at the Wayback Machine Should Google Go Nuclear Clean cheap nuclear power no really Archived 2007 11 10 at the Wayback Machine NSD Gradel Fusion NSD Gradel Fusion Luxembourg Retrieved from https en wikipedia org w index php title 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