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Using L. S. Pontryagin's maximum principle in minimum-critical-size and maximum-power reactor problems

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Abstract

L. S. Pontryagin's maximum principle is used for solving problems in which it is necessary to find the minimum critical size of a reactor for a given power or to find the maximum power for a given critical size . Recently Pontryagin's maximum principle [1] has been successfully used both for determining the optimum transient conditions for reactors [2, 4] and for finding the optimum spatial arrangement for reactors with prescribed physical characteristics [1]. In the present study this principle is used in two otherproblems encountered in the theory of reactor design.

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Literature Cited

  1. L. S. Pontryagin et al., Mathematical Theory of Optimal Processes [in Russian], Moscow, Fizmatgiz (1961).

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  2. Joshikumi Shinohara and Jean Valat, C. r. Acad. Sci.,259 Groupe 6 (1964).

  3. Z. Rosztoczy and L. Weaver, Nucl. Sci. Eng.20, 318 (1964).

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  4. J. Roberts and H. Smith, Nucl. Sci. Eng.,22, 470 (1965).

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  5. B. P. Kochurov, Atomnaya Énergiya,20, 243 (1966).

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  6. A. D. Galanin, Theory of Thermal-Neutron Nuclear Reactors [in Russian], Moscow, Atomizdat (1959).

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Translated from Atomnaya Énergiya, Vol.22, No.1, pp.6–10, January, 1967.

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Zaritskaya, T.S., Rudik, A.P. Using L. S. Pontryagin's maximum principle in minimum-critical-size and maximum-power reactor problems. At Energy 22, 5–9 (1967). https://doi.org/10.1007/BF01225384

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  • DOI: https://doi.org/10.1007/BF01225384

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