Pshenichnikov, A.

Stuckert, J.

English

KITopen

KIT – University of the State of Baden-Württemberg and National Large-scale Research Center of the Helmholtz Association Institute for Applied Materials, IAM-WPT, Program NUKLEAR www.kit.edu   Overview of investigations on bulk distribution of hydrogen absorbed by zirconium alloys A. Pshenichnikov, J. Stuckert QWS18, Karlsruhe 2012 2 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Hydride formation Mechanisms of hydrogen absorption Mechanisms of embrittlement Application to the results of QUENCH-LOCA tests Objectives 3 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop M5 cladding pre-hydrided from outer side to 1700 wppm at 800°C: double rupture during tensile test  optical microscopy: no visible hydrides QUENCH-L0 (Zry-4), rod#2: brittle double rupture during tensile tests, fracture stress 400 MPa, elongation 1%; to comparison rupture after necking: fract. elong. 10%  optical microscopy of hydrogen enriched band: no visible hydrides TEM image of inhomogeneities in the hydrogen enriched band Embrittlement of hydrogenated cladding  4 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Known phases  of Zr – H system 5 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Volume of Zr and ZrHx structures after  E. A. Gulbransen and K. F. Andrew // J. Electrochem. Soc. 1954, V.101(9), P. 474-480. Zirconium – hydrogen phase diagram Beck R.L. // ASM Trans. Q.,55 (1962) 542-555. Zr – H phases  “Hydrogen cannot be kept in supersaturated solution by quenching”. S.R. MacEwen et al., Acta Metal. 33 (1985) 753–757. „γ – phase is metastable”.  B. Nath // Journal of Nuclear Materials 58 (1975) 153-162. G. Hägg, Zeitschrift für Physikalische Chemie, 11, 439 (1930) 6 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop ZrHx  structures γ - phase  δ - phase  ε - phase  Stoichiometric ratio x=1 x = 1.5–1.65  x = 1.75–2 atom positions in tetragonal cell occupied*  1/2 3/4  4/4 Stability metastable  (stable only in high purity Zr**) equilibrium equilibrium Usually in presence of stabilizers** β-stabilizers (Nb, H…) α-stabilizers (Sn, Hf, O…) ------- Cluster model of Zirconium hydride crystal structure  S. Yamanaka et al. // Journal of Alloys and Compounds 330 –332 (2002) 313 - 317. ___________ * V. Perovic  et al. // Acta metallurgica V.31, No.9 1381-1391. ** L. Lanzani, M. Ruch // Journal of Nuclear Materials 324 (2004) 165-176.  7 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Recent investigation on Zr hydrides HREM-image of zirconium hydride A.T.W. Barrow, A. Korinek , M.R. Daymond // Journal of Nuclear Materials 432 (2013) 366–370. Zr-matrix/hydride interface image with the diagramm of plasmon energy vs distance -Zr Nano-beam electron diffraction results: the volume misfit associated with precipitation results in elastic strains that are 4 times greater in the matrix than the hydride. Electron energy loss spectroscopy 8 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop How hydrogen penetrates into metal? 9 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Penetration of H into Zr Penetration   ~  𝑃𝐻𝐻∗𝑒𝑇𝑑 Presence of water vapor will greatly reduce penetration of hydrogen because of reducing vacancy concentration. T. Smith // Journal of nuclear materials 18 (1966) 323-336.  Hydrogen can permeate oxide layer in several days. M.B. Elmoselhi // Journal of Alloys and Compounds 231 (1995) 716-721. Oxide is penetrable via lattice interstitial diffusion, crystallites boundaries and line defects. There is no evidence that hydrogen can pass trough oxide layer by those mechanisms. The only possibility is due to microcracks. He proposed the mechanism of „steam depletion“ on the bottom of the crack. Oxide layer cannot grow dick under this conditions. Such cracks become the way of hydrogen penetration. B. Cox // Journal of Nuclear Materials 264 (1999) 283-294. Oxide – induced stress is sufficient since the volume during Zr oxidation into ZrO2 expands 1,56 times. Under these conditions cracks can easily pass through oxide layer and penetrate into metal, which is the perfect way for hydrogen uptake. Chung H.M. // Proc. Of Intern. Meeting on LWR Fuel Performance, 2000, USA, 325-344. Two opinions 10 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Oxide-induced stresses cause cracks  H2 H2O H2 Scheme for  Chung H.M. // Proc. Of Intern. Meeting on LWR Fuel Performance, 2000, USA, 325-344. Pure metal region H2O 11 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop In-situ diffusion experiments at 1173 K One-dimensional diffusion of the hydrogen in Zry-4 and the hydrogen uptake during steam oxidation by means of neutron radiography was studied. The authors found that when oxide scale at the left side of cylinder was removed a rapid hydrogen absorption took place at this site. Oxidised sides were not penetrable for hydrogen. M. Grosse et al. // Nuclear Instruments and Methods in Physics Research A 651 (2011) 253–257. 12 mm No oxide here 12 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Hydride precipitation and dissolution.  Which factors influence hydride formation? 13 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Effect of various factors B. Nath et. al // Journal of Nuclear Materials 58 (1975) 153-162. Hydrogen concentration Cooling rate γ-hydride region  small size Presence of the Ni containing phase causes an increase in the hydrogen uptake during the early period of oxidation.  B. Cox // Journal of Alloys and Compounds 256 (1997) 244-246. Non-oxidized intermetallic particles allow hydrogen to penetrate easier into Zr matrix. B. A. Kalin and A. A. Shmakov // Materialovedenie 10 (2005) 50-56. 5) Oxygen is the most important one for hydride precipitation at low hydrogen concentrations. C. D. Cann, M.P. Puls //Journal of Nuclear Materials 126 (1984) 197-205. 3) Hydrogen concentration vs. cooling rate 4) Secondary phase particles 1) Stress gradient  inhomogeneous hydride precipitation 2) Tensile stress   improves easier hydride precipitation  A. Akhtar // J. of Nucl.  Mater. 64 (1977) 86-92. J. E. Bailey // Acta Metallurgica, 11 (1963) 267-280. 104 K/s 700 ppm 14 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Hydrides precipitation and dissolution Transformation of Zr solid solution into hydride is believed to be a Bainitic type of reaction J. S. Bradbrook // Journal of Nuclear Materials 42 (1972) 142-160. This mechanism was supported by G.J.C. Carpenter, C.E. Ells, A. Akhtar, V. Perovic in their works. Phase diagram from the paper of G. Libowitz //  Journal of Nuclear Materials 5 (1962) 228-233. Prismatic plane 101�0  direction 112�0  J. E. Bailey // Acta Metallurgica, 11, (1963) 267-280. The plane for hydride precipitation is prismatic 101�0 . J. P. Langeron and P. Lehr // Rev. Métall, 60 (1958) 901. A. Akhtar // Journal of Nuclear Materials 64 (1977) 86-92. 15 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Size of hydrides Hydride orientation of “macrohydrides” slip direction The microscopic hydrides in the material is of 20-80 nm thick and 100-500 nm long.  Usual macroscopic hydrides are not less than 100-200 nm thick and 2,000- 10,000 nm long.  Chung H.M. // Proc. Of Intern. Meeting on LWR Fuel Performance, 2000, USA, 325-344. Hydride orientation  of “microhydrides”  slip direction In 1968 it was established by Westlake D.G. that predominant habit of δ− and γ – zirconium hydrides in zirconium alloys is not prismatic but on the near-basal, hexagonal-close-packed (hcp) a-Zr {101�7} planes (14° from the {0001}). Westlake D.G. // J. of Nucl. Mater. 26, 208 (1968). Later it was supported by Weatherly G.C. Acta Metall. 29, 501–512 (1981).  Hydride  needle  More details about orientation of hydrides in review of D. L. Douglass D.L. Douglass The Metallurgy of Zirconium, Wien : IAEA, 1971. 16 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Hydride precipitation and dissolution in Zry-4 In situ synchrotron diffraction study supports the theory of B.W. Leitch and S.-Q. Shi (Modelling Simul. Mater. Sci. Eng. 4 (1996) 281–292) that the combination of surface energy, elastic and plastic strains generated around the hydrides during their formation are responsible for the irreversible behavior and the supersaturation of the solid solution. O. Zanellato et al. // Journal of Nuclear Materials 420 (2012) 537–547. Thermal history of  a sample has an effect on Terminal Solid Solubility during precipitation. Z.L. Pan et al. // Journal of Nuclear Materials 228 (1990) 227-237. 17 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Mechanical properties of hydrides 18 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Mechanical properties of hydrides  The microhardness of zirconium hydrides  K.G. Barraclough and C.J. Beevers //  J. of Nucl. Mater. 34 (1970) 125-134. M.P. Puls et al. // Journal of Nuclear Materials 336 (2005) 73–80. E(25°C) = 90 GPa (δ-phase); 50 Gpa (ε-phase) 19 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Hydride blisters under tension: brittle rupture 50 mkm depth blister fractured at 25 °C 100 mkm depth blister fractured at  300 °C O.N. Pierron et al. // Journal of Nuclear Materials 322 (2003) 21–35. 20 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Mechanisms of embrittlement In general for the loss of ductility the following factors are necessary: Hydrogen concentration, temperature, size and morphology of hydrides and their orientation with respect to applied stress. B. A. Kalin and A. A. Shmakov // Materialovedenie 10 (2005) 50-56.  1) Mechanism was proposed by Beevers С. J. (Beevers С. J. On the fracture of zirconium containing zirconum hydride  precipitates.— Electrochem. Technol., 1966, v. 4, p. 222.): • Stage 1: Crack starts in brittle hydride phase; • Stage 2: From brittle phase crack propagates into metal; • Stage 3: Crack continues to grow in metal. 2) In 2000 Hee M. Chung had proposed another mechanism (Chung H.M. // Proc. Of Intern. Meeting on LWR Fuel Performance, 2000, USA, 325-344). The main idea is that hydrides are ductile during operation temperatures of nuclear reactor. He had observed many dislocations around the hydride region. Plastic deformation that occurs at the hydride/metal interface is the key factor for the degradation of mechanical properties. But anyway the fracture can be either brittle or ductile in this case.  21 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Mechanisms of embrittlement The mechanism of Beevers С. J. was clearly in situ demonstrated by G. Bertolino (G. Bertolino et al. / Journal of Nuclear Materials 322 (2003) 57–65). Under tensile stress the crack at first occurs in hydride phase and then easily penetrates to the metal matrix. If hydrides are oriented normal to tensile stress (parallel to crack direction) the process goes much easier. Hydrides themselves prepare the future path for the crack before it comes. That is why one needs much lower stress to destroy material. 22 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Recent studies on the problem of DHC The book of Manfred P. Puls (Atomic Energy of Canada Limited).  The Effect of Hydrogen and Hydrides on the Integrity of Zirconium Alloy Components. Delayed Hydride Cracking. Springer-Verlag London 2012.  The book provides more detailed descriptions of the current theoretical and experimental foundations of the properties and behavior of hydrogen, hydrides, and DHC in zirconium and its alloys than is usually found in individual papers in the literature.  M.P. Puls mentioned however, that: “Even in this seemingly obvious case it is not entirely clear why and how fracture of a localized hydrided region under high tensile stresses occurs since the hydrides have positive transformation strains that create large compressive stresses inside them that could potentially shield them from any externally applied high local tensile stresses”.  He actually asks the previous authors why their mechanism works!!! 23 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Conclusion • Zr-H system has  δ and  ε stable phases. γ – phase is metastable. • Oxide scale is not permeable by  hydrogen during short-time periods such as 1 hour. It seems to be penetrable during several days period. Because of this there are two controversal opinions on the penetration mechanism. • External stresses, heat treatment, intermetallic particles and oxygen have very strong effect on the hydrogen uptake and hydride formation. • Hydrides precipitate in the direction of primary slip plane in the main slip direction, which can obstruct the plastic deformation of zirconium alloy and should be the main cause of embrittlement. • The mechanical parameters (E module, micro harness, yield strength) of the solid hydride specimens remain almost the same as those of the original tube material for hydrogen compositions up to about ZrH1.6. The value of these parameters starts to drop when δ - hydride becomes the major phase and reaches minimum levels for ε - hydrides. Specimens consisting mostly or only of the δ - hydride phase have the highest yield strength and lowest ductility. With the increase of temperature the ductility of hydrided alloy can partly recover. • Two mechanisms of embrittlement due to hydrogen were described in literature (1. crack initiation inside hydride; 2. plastic deformation of matrix surrounding hydride) but the nature of embrittlement remains unclear. 24 20.11.2012 A. Pshenichnikov – hydrogen in Zr 18th QUENCH-Workshop Thank you for your attention! 

Overview of investigations on bulk distribution of hydrogen absorbed by zirconium alloys

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Overview of investigations on bulk distribution of hydrogen absorbed by zirconium alloys

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