New expressions for the diffraction elastic constants are presented for a cubic polycrystal that is statistically homogeneous, isotropic and disordered. The results are an extension of the theory of statistical continuum mechanics and differ from a previous derivation given by Bollenrath, Hauk, & Müller [ Z Metallkde (1967), 58 , 76–82].
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R. de Wit (1997) studied this question.
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