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Reactor Kinetics

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Abstract

The goal of reactor physics is to maintain the reactor in a stable state. Nevertheless, the reactor must be brought to a stable state at full power, starting from a cold shutdown state. Further, a reactivity incident may modify the stable state thus achieved. Reactor kinetics studies the transient time phenomena and is the starting point of studies for reactivity accidents.

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Notes

  1. 1.

    To avoid any confusion with Greek letter, nu (ν) used in the production cross section and the velocity, exceptionally, we use the velocity in non-italics ν as for the remaining equations. Some references use the symbol Λfor the generation time.

  2. 2.

    This analogy means that if all couples had twins at 20, this would be equivalent to have one child at 10, and a second one 10 years later. This example shows that the calculation of the population over a long period is identical in both cases, even if the basic hypothesis is inconsistent.

  3. 3.

    R. B. Roberts, J. R. Hafstad, R. C. Meyer and P. Wang: The delayed neutron emission which accompanies fission of uranium and Thorium, Phys. Rev. 55 (664), March 1939.

  4. 4.

    John Archibald Wheeler (1911–2008). American theoretical physicist. After receiving his PhD from John Hopkins University in 1933, he taught at the University of North Carolina, then, from 1938, at Princeton, becoming one of the youngest professors at this prestigious university. In 1939, together with Niels Bohr he proposed an explanation for nuclear fission. He contributed to the Manhattan Project at the Hanford plutonium-producing reactor site. He predicted xenon poisoning by which reactor start-up could be stopped. Wheeler worked on reactor physics between 1941 and 1945. On returning to Princeton, he worked on quantum gravitation and relativity, and it was he who coined the term “black hole”. He directed the theoretical physics center in Texas in 1976. In 1969 he was awarded the Franklin Medal for his fission theory.

  5. 5.

    R. J. Tuttle: Delayed-neutron data for reactor-physics analysis, Nuclear science and engineering, 56, pp. 37–71 (1975).

  6. 6.

    Lothar Wolfgang Nordheim (1899–1985), a German physicist of Jewish origin, emigrated to the United States in 1934 like many German physicists, due to the rise of Nazism. He taught at Duke University where he spent most of his career as of 1937. He was appointed head of the theoretical physics group of the Clinton laboratories, the ancestor of Oak Ridge National Laboratories in the Manhattan Project. He worked on kinetics problems and explosions in the wake of development of the hydrogen bomb. He also contributed to nuclear shell theory. The Fowler-Nordheim model establishes that the emission of electrons under an electric field at the surface of a metal follows a Fermi-Dirac distribution and obeys the tunneling effect. The latter has many practical applications.

  7. 7.

    This may seem paradoxical in a thermal neutron equation, but it is indeed the prompt neutron lifetime, i.e. the mean time between the birth of a (prompt) neutron and the birth of (prompt) neutrons of the new generation appearing in the equation. The reader should bear in mind the obvious statement that a neutron can only be thermal if it was initially fast.

  8. 8.

    There is (unfortunately) some confusion regarding notation in the references on neutron kinetics, and also on occasion, regarding the numerical values of prompt neutron lifetimes. The following table gives corresponding definitions from the better-known references.

     

    Marguet

    Keepin (1965, p. 166)

    Hetrick (1993, p. 6)

    Ott and Neuhold (1985, p. 24)

    Reuss (2003, p. 119)

    Prompt neutron lifetime in an infinite medium

    \( {\ell}_0=\frac{1}{\rm{v}{\varSigma}_a} \)

     

    \( {\ell}_{\infty }{\displaystyle \begin{array}{c}\\ {}\end{array}} \)

    \( {\ell}_{\infty }{\displaystyle \begin{array}{c}\\ {}\end{array}} \)

     

    Prompt neutron lifetime in a finite medium

    \( {\ell}_{B_g}=\frac{\ell_0}{1+{L}^2{B}_g^2} \)

    \( \ell {\displaystyle \begin{array}{c}\\ {}\end{array}} \)

    \( {\ell}_0{\displaystyle \begin{array}{c}\\ {}\end{array}} \)

    \( \ell {\displaystyle \begin{array}{c}\\ {}\end{array}} \)

    \( \theta {\displaystyle \begin{array}{c}\\ {}\end{array}} \)

    Effective prompt neutron lifetime or generation time

    \( \ell =\frac{\ell_{B_g}}{k_{eff}}=\frac{1}{\rm{v}\nu {\varSigma}_f} \)

    \( \Lambda {\displaystyle \begin{array}{c}\\ {}\end{array}} \)

    \( \ell {\displaystyle \begin{array}{c}\\ {}\end{array}} \)

    \( \Lambda {\displaystyle \begin{array}{c}\\ {}\end{array}} \)

    \( \ell {\displaystyle \begin{array}{c}\\ {}\end{array}} \)

  9. 9.

    D. R. Wyman, A. A. Harms, Kinetics of driven multiplying media, Nuclear Science and Engineering, 83, p. 483 (1983).

  10. 10.

    R. C. Greenwood, K. D. Watts: Delayed neutron energy spectra of Br87, Br88, Br89, Br90, I137, I138, I139 and Te136, Nuclear Science and Engineering, Vol. 126, pp. 324–332 (1997).

  11. 11.

    G. Keepin, Progress in Nuclear Energy, Vol. 1, Series 1, Pergamon Press, London (1956).

  12. 12.

    S. Das : The importance of delayed neutrons in nuclear research—a review, Progress in Nuclear Energy, Vol. 28, No. 3, pp. 209–264 (1994). This import journal on delayed neutrons concludes this chapter perfectly. It contains several recent data (particularly on delayed spectra and β eff for several experiments).

  13. 13.

    D. Saphier, D. Ilberg, S. Shalev, S. Yiftah: Evaluated delayed neutron spectra and their importance in reactor calculations, Nuclear Science and Engineering, 62, pp. 660–694 (1977).

  14. 14.

    Véronique Zammit-Averlant : Validation intégrale des estimations du paramètre béta effectif pour les réacteurs MOX et incinérateurs [Integral validation of calculations of the effective beta parameter for MOX reactors and incinerators], thesis at the University of Aix-Marseille (1998).

  15. 15.

    On the different calculation techniques related to reactivity measurements, see Joao Manoel Losada Moreira : Space-time analysis reactivity measurements, PhD at The University of Michigan, 1984.

  16. 16.

    Here we have the exact form of the Weber equation, with the ¼ coefficient. However, (Hetrick 1993) chose to write it without this coefficient, resulting in modified values of α and κ.

  17. 17.

    The first Hermite polynomials are: H 0(x) = 1, H 1(x) = 2x, H 2(x) = 4x 2 − 2, H 3(x) = 8x 3 − 12x. The Hermite functions are orthogonal in L2(): \( \underset{\Re }{\int \limits }{\varphi}_n(x)\kern0.1em {\varphi}_m(x)\kern0.1em dx=0\kern1em n\ne m \).

  18. 18.

    Klaus Fuchs, a German-born British scientist who worked on the Manhattan Project. He was famously tried as a USSR spy and in 1950 he was sentenced to 14 years in prison. (The Rosenbergs were also convicted for espionage and sentenced to the electric chair, despite international protest). He was released after 9 years and immigrated to East Germany.

  19. 19.

    Ajoy K. Ghatak: Non-linear prompt neutron kinetics in multi-group diffusion, theory, PhD thesis, Cornell University (1963). The Nordheim-Fuchs model is thoroughly described. The use of higher modes in plane geometry is worked out to its limits.

  20. 20.

    J. Chernick: The dependence of reactor kinetics on temperature, Rapport BNL-173, 38 pages, 20 décembre 1951.

  21. 21.

    R. T. Ackroyd, G. H. Hinchin, J. E. Mann, J. D. McCullen: Stability considerations in the design of fast reactors, Proc 2nd Conf. on peaceful uses of atomic energy, 1958, Vol 12 p. 230.

  22. 22.

    Tomoaki Suzudo : Reactor noise analysis based on nonlinear dynamic theory—application for power oscillation, Nuclear Science and Engineering, 113 pp. 145–160 (1993).

  23. 23.

    A.S. Thompson, B.R. Thompson , A model of reactor kinetics, Nuclear science and engineering, 100, pp. 783–88 (1988).

  24. 24.

    Several such applications are described in: Progress in Nuclear Energy, Vol. 29, No 3–4 (1995).

  25. 25.

    On Poisson distribution, see (Ross 1992).

  26. 26.

    Jean Tachon: Etude neutronique d’une pile à neutrons thermiques au plutonium «Proserpine»: corrélations entre neutrons dans une réaction en chaîne [Neutron study of the Proserpine plutonium thermal neutron reactor: correlations between neutrons in a chain reaction], PhD thesis, Science Faculty of Paris, 1960.

  27. 27.

    R. P. Feyman, F. de Hoffmann, H. Serber: Statistical fluctuations in the water boiler and the dispersion of neutrons emitted per fission, Los Alamos Scientific Laboratory report LA-101 (1944).

  28. 28.

    Gregory D. Springs : The reactor noise threshold, Nuclear Science and Engineering, 116, pp. 67–72 (1994). The author precisely defines the limit that must not be exceeded in order for the measurement to be useful. For a critical PWR with a prompt neutron lifetime of 10−3 s, the limit of 0.00025 W is found. This can be measured (with difficulty!) in an industrial reactor (fission power is largely exceeded by residual power). For an over-critical stable reactor, this constraint is less strict. For a stable sub-critical reactor, the criterion depends on the source.

  29. 29.

    Bruno Rossi (1905–1993) studied in Padua and Bologna. He received his PhD in Physics in 1937 and worked in Florence and Padua, before leaving Italy in 1938 for Denmark and subsequently moving to Great Britain. In the United States, he worked on the Manhattan project as co-director of the detectors group, and was in charge of instrumentation for physics testing of the atomic bomb. From 1946, he taught physics at MIT, where he became a worldwide expert in cosmic rays. At the end of his career, he was working on plasma physics and astrophysics.

  30. 30.

    Gregory D. Springs : Two Rossi − α techniques for measuring the effective delayed neutron fraction, Nuclear Science and Engineering, 112, pp. 161–172 (1993).

  31. 31.

    Andrey Andreyevitch Markov (1856–1922) was a Russian mathematician and a student of Tchebychev at the University of St Petersburg. He became a member of the science academy of the same city in 1886. He is the author of several major works in probability theory, particularly Markov inequality: if X is a real discrete random variable with values in R +, then P(X ≥ a) ≤ E(X)/a where E(X) is the expected value of X. More generally, when X is a random numerical variable and a strictly positive increasing function, then for any a > 0: P(X ≥ a) ≤ E(φ(X))/φ(a). A Markov process is a random finite state without past memory where the next state in the process depends solely on its present state. To simplify, only the present state and not past states, influences the future. It should be noted that his son, also named Andrey, was also a prominent Russian mathematician.

  32. 32.

    Williams (1974) used a mean fission time defined by τ f  = 1/(vΣ f ), which can be related to the generation time by \( {\tau}_f=\overline{\nu\;}\ell \). Here, the choice was made so as to avoid new definitions of the lifetime, which could prove confusing.

  33. 33.

    E. D. Courant , P. R. Wallace , Fluctuations of the number of neutrons in a pile, Phys. Rev. Vol 72, December 1947.

  34. 34.

    André Brillon: Le bruit neutronique [Neutron background noise], Bulletin de la Direction des Etudes et Recherches d’EDF, Epure n°17, pp. 3–13, Janvier 1988, from which the illustration is taken.

  35. 35.

    On spectral analysis, the lecture of (Kay 1988) is very helpful.

  36. 36.

    I. Pazsit, O. Glöckler: On the neutron noise diagnostics of pressurized water reactor control rod vibrations: III Application at a power plant, Nuclear science and engineering, 99, pp. 313–328 (1988).

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Marguet, S. (2017). Reactor Kinetics. In: The Physics of Nuclear Reactors. Springer, Cham. https://doi.org/10.1007/978-3-319-59560-3_17

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