Abstract
The variance and correlation function are calculated for the internal stress field created by point defects situated independently at random lattice points in a crystal. For equal concentration dilatations, the amplitude of the internal stresses in a fcc lattice is several times the amplitude in an fcc lattice. It is shown that the stress field is practically uncorrelated and its probability density function is represented by an Edgeworth asymptotic series. An asymptotic representation of the stress distribution is proposed in the form of a superposition of a discrete stress spectrum and a normally distributed “background.”
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Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 8, pp. 43–47, August, 1982.
The author is deeply indebted to M. A. Shtremel' for steadfast interest in the work and a useful discussion of the results.
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Mel'nichenko, A.S. Random field of internal stresses from point defects in a crystal. Soviet Physics Journal 25, 717–720 (1982). https://doi.org/10.1007/BF00895246
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DOI: https://doi.org/10.1007/BF00895246