Published 2016 | Version v1
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Is spent nuclear fuel immune from delayed hydride cracking during dry storage? An IAEA coordinated research project - 2016-0048

  • 1. Canadian Nuclear Laboratories, Chalk River, Ontario, KOJ1J0 (Canada)
  • 2. A. A. Bochvar High-Technology Scientific Research Institute for Inorganic Materials, Rogova St., 5a, 123098, Moscow (Russian Federation)
  • 3. RATEN, Campului 1, 115400 Mioveni, Arges (Romania)
  • 4. Lithuanian Energy Institute, Breslaujos 3, 44403 Kaunas, Lithuani (Lithuania)
  • 5. Bhabha Atomic Research Centre, Mechanical Metallurgy Division, Materials Group, Mumbai 400 085 (India)
  • 6. Studsvik Nuclear AB, Mechanical Metallurgy Division, SE-611 82, Nykoping (Sweden)
  • 7. Pakistan Institute of Nuclear Science and Technology, PO Nilore, Islamabad (Pakistan)
  • 8. The Energy and Nuclear Research Institute, Materials Science and Technology Center, CP 11049, Sao Paulo S.P. (Brazil)
  • 9. International Atomic Energy Agency, Wagramer Strasse 5, A-1400, Vienna, (Austria)

Description

Delayed hydride cracking (DHC) has been responsible for cracking in zirconium alloy pressure tubes and fuel cladding and is a concern for spent fuel storage. For cracking to start, sufficient hydrogen must be present for hydride to form at a flaw tip and the local tensile stress must be sufficiently large to crack the hydride (a crack will not extend if the threshold in the stress intensity factor, KIH, is not exceeded. A high-temperature limit exists when the yield stress of the cladding alloy becomes too low to crack the hydride. In this paper we describe measurements of KIH and the crack growth rate, V, in unirradiated Zircaloy-4 fuel cladding containing approximately 130 ppm hydrogen in the cold-worked stress-relieved condition representing pressurized water reactors (PWRs) and pressurized heavy-water (PHWR) reactors. Four methods are used to evaluate KIH. The test specimen and fixture used in these methods was the pin-loading tension configuration. The test temperature ranged from 227 to 315 deg. C. The mean value of KIH below 280 deg. C had little temperature dependence; it was about 5.5 MPa√m in the PWR cladding and slightly higher at 7 MPa√m in the PHWR material. At higher test temperatures, KIH increased dramatically to more than 12 MPa√m, whereas the crack growth rate declined toward zero. This behavior suggests that unirradiated Zircaloy-4 fuel cladding is immune from DHC above about 320 deg. C; this temperature may be increased to 360 deg. C by irradiation. The implications for spent fuel storage are that during early storage when the temperatures are high, any flaw will not extend by DHC, whereas at low temperatures, after many years of storage, flaws would have to be very large, approaching through wall, before being extended by DHC. To date, spent nuclear fuel is not known to have failed by DHC during storage, confirming the inference. (authors)

Availability note (English)

Available from doi: http://dx.doi.org/10.1520/STP159720160048

Additional details

Identifiers

Publishing Information

Publisher
ASTM International
Imprint Place
West Conshohocken, PA (United States)
Imprint Pagination
28 p.

Conference

Title
18. International Symposium on Zirconium in the Nuclear Industry
Dates
15-19 May 2016
Place
Hilton Head, SC (United States)

Optional Information

Notes
51 refs.