Nuclear graphite

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Nuclear graphite is any grade of graphite, usually synthetic graphite, manufactured for use as a moderator or reflector within a nuclear reactor. Graphite is an important material for the construction of both historical and modern nuclear reactors because of its extreme purity and ability to withstand extremely high temperatures.

Contents

Core graphite from the Molten-Salt Reactor Experiment MSRE Core.JPG
Core graphite from the Molten-Salt Reactor Experiment

History

Nuclear fission, the creation of a nuclear chain reaction in uranium, was discovered in 1939 following experiments by Otto Hahn and Fritz Strassman, and the interpretation of their results by physicists such as Lise Meitner and Otto Frisch. [1] [2] Shortly thereafter, word of the discovery spread throughout the international physics community.

In order for the fission process to chain react, the neutrons created by uranium fission must be slowed down by interacting with a neutron moderator (an element with a low atomic weight, that will "bounce", when hit by a neutron) before they will be captured by other uranium atoms. By late 1939, it was generally known that heavy water might be used as a moderator. The highest-purity graphite then commercially available (so called electro-graphite) was dismissed by the Germans and the British as a possible moderator because it contained boron and cadmium impurities. [3] However, graphite of high enough purity was developed in the early 1940's in the United States, and this then was utilized in the first and subsequent nuclear reactors for the Manhattan Project. [4]

In February 1940, using funds that were allocated partly as a result of the Einstein-Szilard letter to President Roosevelt, Leo Szilard purchased several tons of graphite from the Speer Carbon Company and from the National Carbon Company (the National Carbon Division of the Union Carbide and Carbon Corporation in Cleveland, Ohio) for use in Enrico Fermi's first fission experiments, the so-called exponential pile. [5] :190 Fermi writes that "The results of this experiment was [sic] somewhat discouraging" [6] presumably because of the absorption of neutrons by some unknown impurity. [7] :40 So, in December 1940 Fermi and Szilard met with Herbert G. MacPherson and V. C. Hamister at National Carbon to discuss the possible existence of impurities in graphite. [8] :143 During this conversation it became clear that minute quantities of boron impurities were the source of the problem. [4] [9]

As a result of this meeting, over the next two years, MacPherson and Hamister developed thermal and gas extraction purification techniques at National Carbon for the production of boron-free graphite. [9] [10] The resulting product was designated AGOT Graphite ("Acheson Graphite Ordinary Temperature") by National Carbon, and it was "the first true nuclear grade graphite". [11]

During this period, Fermi and Szilard purchased graphite from several manufacturers with various degrees of neutron absorption cross section: AGX graphite from National Carbon Company with 6.68 mb (millibarns) cross section, US graphite from United States Graphite Company with 6.38 mb cross section, Speer graphite from the Speer Carbon Company with 5.51 mb cross section, and when it became available, AGOT graphite from National Carbon, with 4.97 mb cross section. [7] :178 [12] :4 [13] By November 1942 National Carbon had shipped 250 tons of AGOT graphite to the University of Chicago [5] :200 where it became the primary source of graphite to be used in the construction of Fermi's Chicago Pile-1, the first nuclear reactor to generate a sustained chain reaction (December 2, 1942). [7] :295 In early 1943 AGOT graphite was used to build the X-10 Graphite Reactor at Clinton Engineer Works in Tennessee and the first reactors at the Hanford Site in Washington, [12] :5 for the production of plutonium during and after World War II. [9] [11] The AGOT process and its later refinements became standard techniques in the manufacture of nuclear graphite. [12]

The neutron cross section of graphite was investigated during the Second World War in Germany by Walter Bothe, P. Jensen, and Werner Heisenberg. The purest graphite available to them was a product from the Siemens Plania company, which exhibited a neutron absorption cross section of about 6.4 mb [14] :370 to 7.5 mb. [15] Heisenberg therefore decided that graphite would be unsuitable as a moderator in a reactor design using natural uranium. [4] [14] [16] Consequently, the German effort to create a chain reaction involved attempts to use heavy water, an expensive and scarce alternative, made all the more difficult to acquire as a consequence of the Norwegian heavy water sabotage by Norwegian and Allied forces. Writing as late as 1947, Heisenberg still did not understand that the only problem with graphite was the boron impurity. [16]

After testing indigenous electro-graphite, Soviet scientists were able to procure and test American Acheson Graphite in 1943 and subsequently reproduced the technology. [17]

Graphite has also recently been used in nuclear fusion reactors such as the Wendelstein 7-X. As of experiments published in 2019, graphite in elements of the stellarator's wall and a graphite island divertor have greatly improved plasma performance within the device, yielding better control over impurity and heat exhaust, and long high-density discharges. [18]

Wigner effect

In December 1942 Eugene Wigner suggested [19] that neutron bombardment might introduce dislocations and other damage in the molecular structure of materials such as the graphite moderator in a nuclear reactor. The resulting buildup of energy in the material became a matter of concern [11] :5 The possibility was suggested that graphite bars might fuse together as chemical bonds at the surface of the bars when opened and closed again. Even the possibility that the graphite parts might very quickly break into small pieces could not be ruled out. However, the first power-producing reactors (X-10 Graphite Reactor and Hanford B Reactor) had to be built without such knowledge. Cyclotrons, which were the only fast neutron sources available, would take several months to produce neutron irradiation equivalent to one day in B Reactor.

This was the starting point for large-scale research programmes to investigate the property changes from fast particle radiation and to predict their influence on the safety and the lifetime of graphite reactors to be built. Influences of fast neutron radiation material properties have been observed many times and in many countries after the first results emerged from the X-10 Graphite Reactor in 1944.

Specific changes to graphite when irradiated include:

As the state of nuclear graphite in active reactors can only be determined at routine inspections, about every 18 months mathematical modelling of the nuclear graphite as it approaches end-of-life is important. However as only surface features can be inspected and the exact time of changes is not known, reliability modelling is especially difficult. [20] Although catastrophic behaviour such as fusion or crumbling of graphite pieces has never occurred, large changes in many properties do result from fast neutron irradiation which need to be taken into account when graphite components of nuclear reactors are designed. Although not all effects are well understood yet, more than 100 graphite reactors have successfully operated for decades since the 1940s. In the 2010s, the collection of new material property data has improved knowledge significantly. [21] [22]

Manufacture

Reactor-grade graphite must be free of neutron absorbing materials, especially boron, which has a large neutron capture cross section. Boron sources in graphite include the raw materials, the packing materials used in baking the product, and even the choice of soap (for example, borax) used to launder the clothing worn by workers in the machine shop. [12] :80 Boron concentration in thermally purified graphite (such as AGOT graphite) can be less than 0.4 ppm, [12] :81 and in chemically purified nuclear graphite it is less than 0.06 ppm. [12] :47

Nuclear graphite for the UK Magnox reactors was manufactured from petroleum coke mixed with coal-based binder pitch heated and extruded into billets, and then baked at 1,000 °C for several days. To reduce porosity and increase density, the billets were impregnated with coal tar at high temperature and pressure before a final bake at 2,800 °C. Individual billets were then machined into the final required shapes. [23]

Accidents in graphite-moderated reactors

There have been two major accidents in graphite-moderated reactors, the Windscale fire and the Chernobyl disaster.

In the Windscale fire, an untested annealing process for the graphite was used, causing overheating in unmonitored areas of the core and leading directly to the ignition of the fire. The material that ignited was the canisters of metallic uranium fuel within the reactor. When the fire was extinguished, it was found that the only areas of the graphite moderator to have incurred thermal damage were those that had been close to the burning fuel canisters. [24] [25]

In the Chernobyl disaster, the moderator was not responsible for the primary event. Instead, a massive power excursion (exacerbated by the high and positive void coefficient of the RBMK as it was designed and used at the time) during a mishandled test caused the catastrophic failure of the reactor vessel and a near-total loss of coolant supply. The result was that the fuel rods rapidly melted and flowed together while in an extremely high power state, causing a small portion of the core to reach a state of runaway prompt criticality and leading to a massive energy release, [26] resulting in the explosion of the reactor core and the destruction of the reactor building. The massive energy release during the primary event superheated the graphite moderator, and the disruption of the reactor vessel and building allowed the superheated graphite to come into contact with atmospheric oxygen. As a result, the graphite moderator caught fire, sending a plume of highly radioactive fallout into the atmosphere and over a very widespread area. [27]

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<span class="mw-page-title-main">Enrico Fermi</span> Italian-American physicist (1901–1954)

Enrico Fermi was an Italian and naturalized American physicist, renowned for being the creator of the world's first artificial nuclear reactor, the Chicago Pile-1, and a member of the Manhattan Project. He has been called the "architect of the nuclear age" and the "architect of the atomic bomb". He was one of very few physicists to excel in both theoretical physics and experimental physics. Fermi was awarded the 1938 Nobel Prize in Physics for his work on induced radioactivity by neutron bombardment and for the discovery of transuranium elements. With his colleagues, Fermi filed several patents related to the use of nuclear power, all of which were taken over by the US government. He made significant contributions to the development of statistical mechanics, quantum theory, and nuclear and particle physics.

<span class="mw-page-title-main">Nuclear fission</span> Nuclear reaction splitting an atom into multiple parts

Nuclear fission is a reaction in which the nucleus of an atom splits into two or more smaller nuclei. The fission process often produces gamma photons, and releases a very large amount of energy even by the energetic standards of radioactive decay.

<span class="mw-page-title-main">Nuclear chain reaction</span> When one nuclear reaction causes more

In nuclear physics, a nuclear chain reaction occurs when one single nuclear reaction causes an average of one or more subsequent nuclear reactions, thus leading to the possibility of a self-propagating series or "positive feedback loop" of these reactions. The specific nuclear reaction may be the fission of heavy isotopes. A nuclear chain reaction releases several million times more energy per reaction than any chemical reaction.

<span class="mw-page-title-main">Nuclear reactor</span> Device for controlled nuclear reactions

A nuclear reactor is a device used to initiate and control a fission nuclear chain reaction. Nuclear reactors are used at nuclear power plants for electricity generation and in nuclear marine propulsion. When a fissile nucleus like uranium-235 or plutonium-239 absorbs a neutron, it splits into lighter nuclei, releasing energy, gamma radiation, and free neutrons, which can induce further fission in a self-sustaining chain reaction. The process is carefully controlled using control rods and neutron moderators to regulate the number of neutrons that continue the reaction, ensuring the reactor operates safely, although inherent control by means of delayed neutrons also plays an important role in reactor output control. The efficiency of nuclear fuel is much higher than fossil fuels; the 5% enriched uranium used in the newest reactors has an energy density 120,000 times higher than coal.

<span class="mw-page-title-main">Leo Szilard</span> Hungarian-American physicist and inventor (1898–1964)

Leo Szilard was a Hungarian-born physicist, biologist and inventor who made numerous important discoveries in nuclear physics and the biological sciences. He conceived the nuclear chain reaction in 1933, and patented the idea in 1936. In late 1939 he wrote the letter for Albert Einstein's signature that resulted in the Manhattan Project that built the atomic bomb, and then in 1944 wrote the Szilard petition asking President Truman to demonstrate the bomb without dropping it on civilians. According to György Marx, he was one of the Hungarian scientists known as The Martians.

<span class="mw-page-title-main">Pebble-bed reactor</span> Type of very-high-temperature reactor

The pebble-bed reactor (PBR) is a design for a graphite-moderated, gas-cooled nuclear reactor. It is a type of very-high-temperature reactor (VHTR), one of the six classes of nuclear reactors in the Generation IV initiative.

<span class="mw-page-title-main">Neutron moderator</span> Substance that slows down particles with no electric charge

In nuclear engineering, a neutron moderator is a medium that reduces the speed of fast neutrons, ideally without capturing any, leaving them as thermal neutrons with only minimal (thermal) kinetic energy. These thermal neutrons are immensely more susceptible than fast neutrons to propagate a nuclear chain reaction of uranium-235 or other fissile isotope by colliding with their atomic nucleus.

<span class="mw-page-title-main">Neutron radiation</span> Ionizing radiation that presents as free neutrons

Neutron radiation is a form of ionizing radiation that presents as free neutrons. Typical phenomena are nuclear fission or nuclear fusion causing the release of free neutrons, which then react with nuclei of other atoms to form new nuclides—which, in turn, may trigger further neutron radiation. Free neutrons are unstable, decaying into a proton, an electron, plus an electron antineutrino. Free neutrons have a mean lifetime of 887 seconds.

<span class="mw-page-title-main">Chicago Pile-1</span> Worlds first human-made nuclear reactor

Chicago Pile-1 (CP-1) was the world's first artificial nuclear reactor. On 2 December 1942, the first human-made self-sustaining nuclear chain reaction was initiated in CP-1 during an experiment led by Enrico Fermi. The secret development of the reactor was the first major technical achievement for the Manhattan Project, the Allied effort to create nuclear weapons during World War II. Developed by the Metallurgical Laboratory at the University of Chicago, CP-1 was built under the west viewing stands of the original Stagg Field. Although the project's civilian and military leaders had misgivings about the possibility of a disastrous runaway reaction, they trusted Fermi's safety calculations and decided they could carry out the experiment in a densely populated area. Fermi described the reactor as "a crude pile of black bricks and wooden timbers".

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<span class="mw-page-title-main">Metallurgical Laboratory</span> Former laboratory at the University of Chicago, part of the Manhattan Project

The Metallurgical Laboratory was a scientific laboratory from 1942 to 1946 at the University of Chicago. It was established in February 1942 and became the Argonne National Laboratory in July 1946.

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<span class="mw-page-title-main">Einstein–Szilard letter</span> 1939 letter to U.S. president Franklin D. Roosevelt

The Einstein–Szilard letter was a letter written by Leo Szilard and signed by Albert Einstein on August 2, 1939, that was sent to President of the United States Franklin D. Roosevelt. Written by Szilard in consultation with fellow Hungarian physicists Edward Teller and Eugene Wigner, the letter warned that Germany might develop atomic bombs and suggested that the United States should start its own nuclear program. It prompted action by Roosevelt, which eventually resulted in the Manhattan Project, the development of the first atomic bombs, and the use of these bombs on the cities of Hiroshima and Nagasaki.

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<span class="mw-page-title-main">Graphite-moderated reactor</span> Type of nuclear reactor

A graphite-moderated reactor is a nuclear reactor that uses carbon as a neutron moderator, which allows natural uranium to be used as nuclear fuel.

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References

  1. Roberts, R. B.; Kuiper, J. B. H. (1939), "Uranium and Atomic Power", Journal of Applied Physics, 10 (9): 612–614, Bibcode:1939JAP....10..612R, doi:10.1063/1.1707351
  2. "Manhattan Project: The Discovery of Fission, 1938-1939". www.osti.gov. Retrieved 2022-12-01.
  3. Dahl, Per F. (1999). Heavy Water and the Wartime Race for Nuclear Energy. CRC Press. ISBN   978-0-7503-0633-1.
  4. 1 2 3 Bethe, Hans (2000), "The German Uranium Project", Physics Today, 53 (7), American Institute of Physics: 34–36, Bibcode:2000PhT....53g..34B, doi:10.1063/1.1292473
  5. 1 2 Salvetti, Carlo (2001). "Fermi's Pile". In C. Bernardini and L. Bonolis (ed.). Enrico Fermi: His work and legacy. New York N. Y.: Springer Verlag. pp.  177–203. ISBN   3540221417.
  6. Fermi, Enrico (1946), "Development of the First chain reacting pile", Proceedings of the American Philosophical Society, 90 (1): 2024
  7. 1 2 3 Fermi, Enrico (1965). Collected Papers. Vol. 2. University of Chicago Press.
  8. Szilard, Gertrude; Weart, Spencer (1978). Leo Szilard: His Version of the Facts. Vol. II. MIT Press. ISBN   0262191687.
  9. 1 2 3 Weinberg, Alvin (1994), "Herbert G. MacPherson", Memorial Tributes, vol. 7, National Academy of Engineering Press, pp. 143–147, doi:10.17226/4779, ISBN   978-0-309-05146-0
  10. Currie, L. M.; Hamister, V. C.; MacPherson, H. G. (1955). The Production and Properties of Graphite for Reactors. National Carbon Company.
  11. 1 2 3 Eatherly, W. P. (1981), "Nuclear graphite - the first years", Journal of Nuclear Materials, 100 (1–3): 55–63, Bibcode:1981JNuM..100...55E, doi:10.1016/0022-3115(81)90519-5
  12. 1 2 3 4 5 6 Nightingale, R. E. (1962). Nuclear Graphite. Division of Technical Information, United States Atomic Energy Commission. Academic Press. ISBN   0125190506.
  13. Haag, G. 2005, Properties of ATR-2E Graphite and Property Changes due to Fast Neutron Irradiation, FZ-Juelich, Juel-4813.
  14. 1 2 Hentschel, Klaus (ed.); Hentschel, Anne M. (translator) (1996), "Document 115", Physics and National Socialism: An Anthology of Primary Sources (English translation of Heisenberg 1947), Birkhäuser, pp. 361–379, ISBN   978-3-0348-0202-4 {{citation}}: |first1= has generic name (help)
  15. Haag, 2005.
  16. 1 2 Heisenberg, Werner (16 August 1947), "Research in Germany on the Technical Applications of Atomic Energy", Nature, 160 (4059): 211–215, Bibcode:1947Natur.160..211H, doi:10.1038/160211a0, PMID   20256200, S2CID   4077785
  17. https://club.nrcki.ru/sekretnayavoyna/reshauchiy1943
  18. Klinger, T.; et al. (2019). "Overview of First Wendelstein 7-X High-Performance Operation". Nuclear Fusion. 59 (11): 112004. Bibcode:2019NucFu..59k2004K. doi: 10.1088/1741-4326/ab03a7 . hdl: 2434/653115 .
  19. Fermi, Enrico (1942), "Report for Month Ending December 15, 1942, Physics Division", United States Atomic Energy Commission report CP-387
  20. Philip Maul; Peter Robinson; Jenny Burrowand; Alex Bond (June 2017). "Cracking in Nuclear Graphite" (PDF). Mathematics Today. Retrieved 10 March 2019.
  21. Arregui Mena, J.D.; et al. (2016). "Spatial variability in the mechanical properties of Gilsocarbon" (PDF). Carbon. 110: 497–517. doi:10.1016/j.carbon.2016.09.051. S2CID   137890948.
  22. Arregui Mena, J.D.; et al. (2018). "Characterisation of the spatial variability of material properties of Gilsocarbon and NBG-18 using random fields" (PDF). Journal of Nuclear Materials. 511: 91–108. Bibcode:2018JNuM..511...91A. doi: 10.1016/j.jnucmat.2018.09.008 . S2CID   105291655.
  23. Gareth B. Neighbour (2007). Management of ageing in graphite reactor cores. Royal Society of Chemistry. ISBN   978-0-85404-345-3 . Retrieved 2009-06-15.
  24. "Meeting of RG2 with Windscale Pile 1 Decommissioning Project Team" (PDF). Nuclear Safety Advisory Committee. 2005-09-29. NuSAC(2005)P 18. Retrieved 2008-11-26.
  25. Marsden, B.J.; Preston, S.D.; Wickham, A.J. (8–10 September 1997). "Evaluation of graphite safety issues for the British production piles at Windscale]". AEA Technology . IAEA. IAEA-TECDOC—1043. Archived from the original on 12 October 2008. Retrieved 13 November 2010.
  26. Pakhomov, Sergey A.; Dubasov, Yuri V. (2009). "Estimation of Explosion Energy Yield at Chernobyl NPP Accident". Pure and Applied Geophysics. 167 (4–5): 575. Bibcode:2010PApGe.167..575P. doi: 10.1007/s00024-009-0029-9 .
  27. "Frequently Asked Chernobyl Questions". International Atomic Energy Agency – Division of Public Information. May 2005. Archived from the original on 23 February 2011. Retrieved 23 March 2011.