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DHC Initiation at Volumetric Flaws

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Part of the book series: Engineering Materials ((ENG.MAT.))

Abstract

Threshold conditions for DHC initiation at volumetric flaws—which require a different treatment than is appropriate for DHC initiation at cracks—is summarized in this chapter. The initial approach, based on a peak stress threshold criterion, resulted in this threshold decreasing with the number of reactor shutdown cycles. This was found to be too restrictive on reactor operation. Moreover, the method did not have an explicit dependence on flaw geometry (root radius) nor could it readily be used to assess the DHC initiation potential of sharp secondary flaws at the root of blunt flaws. The hydride process zone model that was developed to eliminate these deficiencies of the peak threshold stress model is described in this chapter. Details of the validation procedures of the engineering process zone model in relation to the experimental data base for DHC initiation from blunt flaws in unirradiated and pre-irradiated Zr–2.5Nb pressure tube material are given.

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Notes

  1. 1.

    This expression was not actually given in the original derivation but follows from standard fracture mechanics theory for a strip-yield model.

  2. 2.

    The notation for the hydrided region’s stress and relative displacement at the flaw tip (\( p_{ * } \) and \( v_{ * } \), respectively) used in Smith’s paper is different from what is used here. The notation has been changed to be consistent with Smith’s later notation for these parameters.

  3. 3.

    These two values are presently considered as the nominal lower bound values for \( K_{IH} \) and \( p_{c} \) for use in assessment methodologies.

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Correspondence to Manfred P Puls .

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© 2012 Springer-Verlag London

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Puls, M.P. (2012). DHC Initiation at Volumetric Flaws. In: The Effect of Hydrogen and Hydrides on the Integrity of Zirconium Alloy Components. Engineering Materials. Springer, London. https://doi.org/10.1007/978-1-4471-4195-2_11

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  • DOI: https://doi.org/10.1007/978-1-4471-4195-2_11

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