Tokamak

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The reaction chamber of the TCV, an experimental tokamak fusion reactor at École polytechnique fédérale de Lausanne, Lausanne, Switzerland which has been used in research since it was completed in 1992. The characteristic torus-shaped chamber is clad with graphite to help withstand the extreme heat. The shape is distorted by the camera's fisheye lens.

A tokamak (Russian: токама́к) is a device that uses a powerful magnetic field to confine plasma in the shape of a torus. The tokamak is one of the several types of magnetic confinement devices being developed to contain the hot plasma needed for producing controlled thermonuclear fusion power. As of 2017, it is the leading candidate for a practical fusion reactor.

Tokamaks were invented in the 1950s by Soviet physicists Igor Tamm and Andrei Sakharov, inspired by an original idea of Oleg Lavrentiev.[1] It had earlier been demonstrated that a stable plasma equilibrium requires magnetic field lines that move around the torus in a helical shape. Earlier devices like the z-pinch and stellarator had attempted this, but demonstrated serious instabilities anyway. It was the development of the concept now known as the safety factor that guided tokamak development; by arranging the reactor so the critical factor q was always greater than 1, the tokamaks strongly suppressed the kink instability that plagued earlier designs.

The first tokamak, T-1, began operation in 1958. By the mid-1960s their performance had improved so much that an initial release of results in 1965 was largely ignored. Lyman Spitzer, inventor of the stellarator, dismissed them out of hand. A second set of results was published in 1968, this time claiming performance far in advance of any other machine. Recognizing these claims might be dismissed as well, the Soviet delegation invited a team from the United Kingdom to verify the result. Their 1969 publication confirmed the dramatic improvements, resulting in a stampede of tokamak construction around the world. The performance was such an advance that the US abandoned the stellarator approach and converted their latest machine to a tokamak.

By the mid-1970s, newer machines had reached all of the conditions needed for practical fusion, although not at the same time and in a single reactor. This led to a new series of machines in the 1980s, notably the Joint European Torus and Tokamak Fusion Test Reactor, with the explicit goal of reaching breakeven. They instead demonstrated a new series of problems that limited their performance and demonstrated that a successful machine would have to be larger and more complex. The designs would be so expensive that they could not be developed by a single country. After an initial agreement between Ronald Reagan and Mikhail Gorbachev in November 1985, the ITER reactor effort developed, and remains the primary international effort to develop practical fusion power. Many smaller designs, and offshoots like the spherical tokamak, continue to be used to investigate performance parameters and other issues.

Etymology

The word tokamak is a transliteration of the Russian word токамак, an acronym of either:

  • "тороидальная камера с магнитными катушками" (toroidal'naya kamera s magnitnymi katushkami) — toroidal chamber with magnetic coils;

or

  • "тороидальная камера с аксиальным магнитным полем" (toroidal'naya kamera s aksial'nym magnitnym polem) — toroidal chamber with axial magnetic field.[2]

History

A USSR stamp, 1987. Tokamak thermonuclear system.

Experimental research of tokamak systems started in 1956 in Kurchatov Institute, Moscow, by a group of Soviet scientists led by Lev Artsimovich. The group constructed the first tokamaks, the most successful of which were the T-3 and its larger version T-4. T-4 was tested in 1968 in Novosibirsk, conducting the first ever quasistationary thermonuclear fusion reaction.[3]

In 1968, at the third IAEA International Conference on Plasma Physics and Controlled Nuclear Fusion Research at Novosibirsk, Soviet scientists announced that they had achieved electron temperatures of over 1000 eV in a tokamak device.[4] British and American scientists met this news with skepticism since they were far from reaching that benchmark; they remained suspicious until laser scattering tests confirmed the findings the next year.[5]

In 1973 design work on JET, the Joint European Torus, began.

In 1978, Bob Guccione, publisher of Penthouse Magazine met Robert Bussard and became the world's biggest and most committed private investor in fusion technology, ultimately putting $20 million ($60 million in 2016 dollars) of his own money into Bussard's Compact Tokamak.[6]

Toroidal design

Tokamak magnetic field and current. Shown is the toroidal field and the coils (blue) that produce it, the plasma current (red) and the poloidal field produced by it, and the resulting twisted field when these are overlaid.

Positively and negatively charged ions and negatively charged electrons in a fusion plasma are at very high temperatures, and have correspondingly large velocities. In order to maintain the fusion process, particles from the hot plasma must be confined in the central region, or the plasma will rapidly cool. Magnetic confinement fusion devices exploit the fact that charged particles in a magnetic field experience a Lorentz force and follow helical paths along the field lines.

Early fusion research devices were variants on the Z-pinch and used electric current to generate a poloidal magnetic field to contain the plasma along a linear axis between two points. Researchers discovered that a simple toroidal field, in which the magnetic field lines run in circles around an axis of symmetry, confines a plasma hardly better than no field at all. This can be understood by looking at the orbits of individual particles. The particles not only spiral around the field lines, they also drift across the field. Since a toroidal field is curved and decreases in strength moving away from the axis of rotation, the ions and the electrons move parallel to the axis, but in opposite directions. The charge separation leads to an electric field and an additional drift, in this case outward (away from the axis of rotation) for both ions and electrons. Alternatively, the plasma can be viewed as a torus of fluid with a magnetic field frozen in. The plasma pressure results in a force that tends to expand the torus. The magnetic field outside the plasma cannot prevent this expansion. The plasma simply slips between the field lines.

For a toroidal plasma to be effectively confined by a magnetic field, there must be a twist to the field lines. There are then no longer flux tubes that simply encircle the axis, but, if there is sufficient symmetry in the twist, flux surfaces. Some of the plasma in a flux surface will be on the outside (larger major radius, or "low-field side") of the torus and will drift to other flux surfaces farther from the circular axis of the torus. Other portions of the plasma in the flux surface will be on the inside (smaller major radius, or "high-field side"). Since some of the outward drift is compensated by an inward drift on the same flux surface, there is a macroscopic equilibrium with much improved confinement. Another way to look at the effect of twisting the field lines is that the electric field between the top and the bottom of the torus, which tends to cause the outward drift, is shorted out because there are now field lines connecting the top to the bottom.

When the problem is considered even more closely, the need for a vertical (parallel to the axis of rotation) component of the magnetic field arises. The Lorentz force of the toroidal plasma current in the vertical field provides the inward force that holds the plasma torus in equilibrium.

Advanced tokamaks

Since about 1990 tokamaks are designed to operate in high-confinement mode to reduce plasma and energy losses.

Advanced or 2nd generation tokamaks generally use a 'C' or 'D' shaped plasma cross-section.

Plasma disruptions

At the necessarily large toroidal currents (15 megaamperes in ITER) the tokamak concept suffers from a fundamental problem of stability. The nonlinear evolution of magnetohydrodynamical instabilities leads to a dramatic quench of the plasma current within milliseconds. Very energetic electrons are created (runaway electrons) and finally a global loss of confinement happens. At that point very intense radiation is inflicted on small areas. This phenomenon is called a major disruption.[7] The occurrence of major disruptions in running tokamaks has always been rather high, of the order of a few percent of the total numbers of the shots. In currently operated tokamaks, the damage is often large but rarely dramatic. In the ITER tokamak, it is expected that the occurrence of a limited number of major disruptions will definitively damage the chamber with no possibility to restore the device.[8][9][10][dubious ][page needed]

A large amplitude of the central current density can also result in internal disruptions, or sawteeth, which do not generally result in termination of the discharge.[11]

Plasma heating

In an operating fusion reactor, part of the energy generated will serve to maintain the plasma temperature as fresh deuterium and tritium are introduced. However, in the startup of a reactor, either initially or after a temporary shutdown, the plasma will have to be heated to its operating temperature of greater than 10 keV (over 100 million degrees Celsius). In current tokamak (and other) magnetic fusion experiments, insufficient fusion energy is produced to maintain the plasma temperature.

Ohmic heating ~ inductive mode

Since the plasma is an electrical conductor, it is possible to heat the plasma by inducing a current through it; in fact, the induced current that heats the plasma usually provides most of the poloidal field. The current is induced by slowly increasing the current through an electromagnetic winding linked with the plasma torus: the plasma can be viewed as the secondary winding of a transformer. This is inherently a pulsed process because there is a limit to the current through the primary (there are also other limitations on long pulses). Tokamaks must therefore either operate for short periods or rely on other means of heating and current drive. The heating caused by the induced current is called ohmic (or resistive) heating; it is the same kind of heating that occurs in an electric light bulb or in an electric heater. The heat generated depends on the resistance of the plasma and the amount of electric current running through it. But as the temperature of heated plasma rises, the resistance decreases and ohmic heating becomes less effective. It appears that the maximum plasma temperature attainable by ohmic heating in a tokamak is 20-30 million degrees Celsius. To obtain still higher temperatures, additional heating methods must be used.

Neutral-beam injection

Neutral-beam injection involves the introduction of high energy (rapidly moving) atoms (molecules) into an ohmically heated, magnetically confined plasma within the tokamak. The high energy atoms (molecules) originate as ions in an arc chamber before being extracted through a high voltage grid set. The term "ion source" is used to generally mean the assembly consisting of a set of electron emitting filaments, an arc chamber volume, and a set of extraction grids. The extracted ions travel through a neutralizer section of the beamline where they gain enough electrons to become neutral atoms (molecules) but retain the high velocity imparted to them from the ion source. Once the neutral beam enters the tokamak, interactions with the main plasma ions occur which significantly heat the bulk plasma and bring it closer to fusion-relevant temperatures. Ion source extraction voltages are typically of the order 50-100 kV, and high voltage, negative ion sources (-1 MV) are being developed for ITER. The ITER Neutral Beam Test Facility in Padova will be the first ITER facility to start operation.[12] While neutral beam injection is used primarily for plasma heating, it can also be used as a diagnostic tool and in feedback control by making a pulsed beam consisting of a string of brief 2-10 ms beam blips. Deuterium is a primary fuel for neutral beam heating systems and hydrogen and helium are sometimes used for selected experiments.

Magnetic compression

A gas can be heated by sudden compression. In the same way, the temperature of a plasma is increased if it is compressed rapidly by increasing the confining magnetic field. In a tokamak system this compression is achieved simply by moving the plasma into a region of higher magnetic field (i.e., radially inward). Since plasma compression brings the ions closer together, the process has the additional benefit of facilitating attainment of the required density for a fusion reactor.

Set of hyperfrequency tubes (84 GHz and 118 GHz) for plasma heating by electron cyclotron waves on the Tokamak à Configuration Variable (TCV). Courtesy of SPC-EPFL.

Radio-frequency heating

High-frequency electromagnetic waves are generated by oscillators (often by gyrotrons or klystrons) outside the torus. If the waves have the correct frequency (or wavelength) and polarization, their energy can be transferred to the charged particles in the plasma, which in turn collide with other plasma particles, thus increasing the temperature of the bulk plasma. Various techniques exist including electron cyclotron resonance heating (ECRH) and ion cyclotron resonance heating. This energy is usually transferred by microwaves.

Tokamak particle inventory

Plasma discharges within the tokamak's vacuum chamber consist of energized ions and atoms and the energy from these particles eventually reaches the inner wall of the chamber through radiation, collisions, or lack of confinement. The inner wall of the chamber is water-cooled and the heat from the particles is removed via conduction through the wall to the water and convection of the heated water to an external cooling system.

Turbomolecular or diffusion pumps allow for particles to be evacuated from the bulk volume and cryogenic pumps, consisting of a liquid helium-cooled surface, serve to effectively control the density throughout the discharge by providing an energy sink for condensation to occur. When done correctly, the fusion reactions produce large amounts of high energy neutrons. Being electrically neutral and relatively tiny, the neutrons are not affected by the magnetic fields nor are they stopped much by the surrounding vacuum chamber.

The neutron flux is reduced significantly at a purpose-built neutron shield boundary that surrounds the tokamak in all directions. Shield materials vary, but are generally materials made of atoms which are close to the size of neutrons because these work best to absorb the neutron and its energy. Good candidate materials include those with much hydrogen, such as water and plastics. Boron atoms are also good absorbers of neutrons. Thus, concrete and polyethylene doped with boron make inexpensive neutron shielding materials.

Once freed, the neutron has a relatively short half-life of about 10 minutes before it decays into a proton and electron with the emission of energy. When the time comes to actually try to make electricity from a tokamak-based reactor, some of the neutrons produced in the fusion process would be absorbed by a liquid metal blanket and their kinetic energy would be used in heat-transfer processes to ultimately turn a generator.

Experimental tokamaks

Currently in operation

(in chronological order of start of operations)

Alcator C-Mod

Previously operated

The control room of the Alcator C tokamak at the MIT Plasma Science and Fusion Center, in about 1982–1983.

Planned

  • ITER, international project in Cadarache, France; 500 MW; construction began in 2010, first plasma expected in 2020.[27]
  • DEMO; 2000 MW, continuous operation, connected to power grid. Planned successor to ITER; construction to begin in 2024 according to preliminary timetable.
  • CFETR, also known as "China Fusion Engineering Test Reactor"; 200 MW; Next generation Chinese fusion reactor, is a new tokamak device.[28][29][30][31]

See also

Notes

  1. ^ Bondarenko B D "Role played by O. A. Lavrent'ev in the formulation of the problem and the initiation of research into controlled nuclear fusion in the USSR" Phys. Usp. 44 844 (2001) available online
  2. ^ "Tokamak - Definition of tokamak by Merriam-Webster". merriam-webster.com. 
  3. ^ Great Soviet Encyclopedia, 3rd edition, entry on "Токамак", available online here [1]
  4. ^ "Measurement of the electron temperature by Thomson scattering in tokamak T3". Nature. 1969. 
  5. ^ Peacock, N. J.; Robinson, D. C.; Forrest, M. J.; Wilcock, P. D.; Sannikov, V. V. (1969). "Measurement of the Electron Temperature by Thomson Scattering in Tokamak T3". Nature. 224 (5218): 488–490. Bibcode:1969Natur.224..488P. doi:10.1038/224488a0. 
  6. ^ Penthouse founder had invested his fortune in fusion, ITER News Oct 25, 2010
  7. ^ Kruger, S. E.; Schnack, D. D.; Sovinec, C. R., (2005). "Dynamics of the Major Disruption of a DIII-D Plasma". Phys. Plasmas 12, 056113. doi:10.1063/1.1873872.
  8. ^ Wurden, G., (2011) International Workshop "MFE Roadmapping in the ITER Era", Princeton
  9. ^ Baylor, L. R.; Combs, S. K.; Foust, C. R.; Jernigan, T.C.; Meitner, S. J.; Parks, P. B.; Caughman, J. B.; Fehling, D. T.; Maruyama, S.; Qualls, A. L.; Rasmussen, D. A.; Thomas, C. E., (2009). "Pellet Fuelling, ELM Pacing and Disruption Mitigation Technology Development for ITER". Nucl. Fusion 49 085013. doi:10.1088/0029-5515/49/8/085013. >
  10. ^ Thornton, A. J.; Gibsonb, K. J.; Harrisona, J. R.; Kirka, A.; Lisgoc, S. W.; Lehnend, M.; Martina, R.;, Naylora, G.; Scannella, R.; Cullena, A. and MAST Team Thornton, A., (2011). "Disruption mitigation studies on the Mega Amp Spherical Tokamak (MAST)". Journal Nucl. Mat. 415, 1, Supplement, 1, S836-S840. doi:10.1016/j.jnucmat.2010.10.029.
  11. ^ Goeler, V. et al. (1974). Studies of internal disruptions and m= 1 oscillations in tokamak discharges with soft—x-ray techniques, Physical Review Letters, vol. 20, p. 1201.
  12. ^ https://www.igi.cnr.it/www/sites/default/files/home201511/SchedaNBTF_MIUR_EN.pdf
  13. ^ Vojtěch Kusý. "GOLEM @ FJFI.CVUT". cvut.cz. 
  14. ^ a b "Tokamak Department, Institute of Plasma Physics". cas.cz. Archived from the original on 2015-09-01. 
  15. ^ History of Golem
  16. ^ Tore Supra Archived November 15, 2012, at the Wayback Machine.
  17. ^ DIII-D (video)
  18. ^ EMazzitelli, Giuseppe. "ENEA-Fusion: FTU". www.fusione.enea.it. 
  19. ^ "Centro de Fusão Nuclear". utl.pt. 
  20. ^ Fusion Research: Australian Connections, Past and Future B. D. Blackwell, (1) M.J. Hole, J. Howard and J. O'Connor
  21. ^ "Pegasus Toroidal Experiment". wisc.edu. 
  22. ^ "Tokamak". Pprc.srbiau.ac.ir. Retrieved 2012-06-28. 
  23. ^ a b Tokamak. "Tokamak Energy – About Us". tokamakenergy.co.uk. 
  24. ^ http://adsabs.harvard.edu/abs/1979SAJSc..75..155D
  25. ^ Ramos, J.; Meléndez, L.; et al. (1983). "Diseño del Tokamak Novillo" (PDF). Rev. Mex. Fís. 29 (4): 551–592. 
  26. ^ "MIT Plasma Science & Fusion Center: research>alcator>". mit.edu. Archived from the original on 2015-07-09. 
  27. ^ "ITER & Beyond. The Phases of ITER". Archived from the original on 22 September 2012. Retrieved 12 September 2012. 
  28. ^ http://www-naweb.iaea.org/napc/physics/meetings/TM45256/talks/Gao.pdf
  29. ^ "Concept design of CFETR superconducting magnet system based on different maintenance ports". Fusion Engineering and Design. 88: 2960–2966. doi:10.1016/j.fusengdes.2013.06.008. 
  30. ^ Song, Yun Tao; et al. (2014). "Concept Design of CFETR Tokamak Machine". IEEE Transactions on Plasma Science. 42 (3): 503–509. Bibcode:2014ITPS...42..503S. doi:10.1109/TPS.2014.2299277. 
  31. ^ http://aries.ucsd.edu/LIB/MEETINGS/1302-USJ-PPS/Ye.pdf

References

  • Braams, C.M. & Stott, P.E. (2002). Nuclear Fusion: Half a Century of Magnetic Confinement Research. Institute of Physics Publishing. ISBN 0-7503-0705-6. 
  • Dolan, Thomas J. (1982). Fusion Research, Volume 1 - Principles. Pergamon Press. LCC QC791.D64. 
  • Nishikawa, K. & Wakatani, M. (2000). Plasma Physics. Springer-Verlag. ISBN 3-540-65285-X. 
  • Raeder, J.; et al. (1986). Controlled Nuclear Fusion. John Wiley & Sons. ISBN 0-471-10312-8. 
  • Wesson, John (2000). The Science of JET (PDF). 
  • Wesson, John; et al. (2004). Tokamaks. Oxford University Press. ISBN 0-19-850922-7. 

External links

  • CCFE - site from the UK fusion research centre CCFE.
  • Int'l Tokamak research - various that relate to ITER
  • Plasma Science - site on tokamaks from the French CEA.
  • Fusion Programs at General Atomics, including the DIII-D National Fusion Facility, an experimental tokamak.
  • General Atomics DIII-D Program
  • Fusion and Plasma Physics Seminar at MIT OCW
  • Unofficial ITER fan club, Club for fans of the biggest tokamak planned to be built in near future.
  • www.tokamak.info Extensive list of current and historic tokamaks from around the world.
  • SSTC-1 Overview video of a small scale tokamak concept.
  • SSTC-2 on YouTube Section View Video of a small scale tokamak concept.
  • SSTC-3 on YouTube Fly Through Video of a small scale tokamak concept.
  • LAP_Tokamak_Development Information on conditions necessary for nuclear reaction in a tokamak reactor
  • A. P. Frass (1973). "Engineering Problems In The Design Of Controlled Thermonuclear Reactors" (PDF). Oak Ridge National Laboratory. Retrieved September 2013.  Check date values in: |access-date= (help)
  • Observer Newspaper Article on Tokomak Nuclear fusion and the promise of a brighter tomorrow
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