2020
DOI: 10.1016/j.mtla.2020.100667
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Influence of nanovoids in the hydrogen embrittlement fracture of Al–Zn–Mg–Cu alloys

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Cited by 14 publications
(6 citation statements)
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“…Furthermore, the growth or merging of nanovoids caused by hydrogen is not seen even before fracture, suggesting that nanovoids do not play a dominant role in inducing quasicleavage cracks in Al-Zn-Mg-Cu aluminum alloys 2 . In addition, neither growth nor coalescence of hydrogen-induced nanovoids are observed even just before fracture, indicating that nanovoids do not behave as the dominant factor of hydrogen-induced quasicleavage cracks in Al-Zn-Mg-Cu aluminum alloys 64,65 . For grain boundaries, it has been reported that if large amounts of hydrogen are enriched at the aluminum grain boundary, hydrogen-induced debonding can occur, analogous to the precipitate interface 29 .…”
Section: 𝜃 T 𝑖 1 − 𝜃 Tmentioning
confidence: 94%
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“…Furthermore, the growth or merging of nanovoids caused by hydrogen is not seen even before fracture, suggesting that nanovoids do not play a dominant role in inducing quasicleavage cracks in Al-Zn-Mg-Cu aluminum alloys 2 . In addition, neither growth nor coalescence of hydrogen-induced nanovoids are observed even just before fracture, indicating that nanovoids do not behave as the dominant factor of hydrogen-induced quasicleavage cracks in Al-Zn-Mg-Cu aluminum alloys 64,65 . For grain boundaries, it has been reported that if large amounts of hydrogen are enriched at the aluminum grain boundary, hydrogen-induced debonding can occur, analogous to the precipitate interface 29 .…”
Section: 𝜃 T 𝑖 1 − 𝜃 Tmentioning
confidence: 94%
“…Holding time is a parameter that can be considered equivalent to the strain rate in slow strain rate tensile testing, and the effect of increased holding time is interpreted as a decrease in the strain rate. Hydrogen repartitioning or hydrogen invasion from outside the specimen occurs during the tensile deformation process [65][66][67] , making hydrogen embrittlement more pronounced at longer holding times (lower strain rates). This phenomenon occurs due to the complicated superposition of the formation of local stress gradients, changes in hydrogen trap site density due to loading, hydrogen diffusion during deformation, and hydrogen invasion caused by the fracture of the passive film on the aluminum surface.…”
Section: 𝜃 T 𝑖 1 − 𝜃 Tmentioning
confidence: 99%
“…Details of the quantification of the trap site densities are available elsewhere. 13,16,21,41) The number of hydrogen atoms that a trap site can trap per unit number, unit length, unit area, and unit volume (herein called the hydrogen trap interval) has been reported using first-principles calculations. 13,19,3036) The reported hydrogen trap intervals are 1.0 atomH/atom for the solute Mg atoms, 32) 1.0 atomH/nm for the edge dislocation, 31) 1.2 atomH/nm for the screw dislocation, 31) 8 atomH/vacancy for the vacancy, 34) 21.9 atomH/nm 2 for the grain boundary, 33) 17.1 atomH/nm 2 for the coherent interface of the MgZn 2 precipitate, 13,35) 5.6 atomH/nm 2 for the semi-coherent interface the MgZn 2 precipitate, 36) 13.2 atomH/nm 3 for the Al 7 Cu 2 Fe particle, 19) and also 20 atomH/nm 2 for the micropore.…”
Section: Hydrogen Partitioning Behaviormentioning
confidence: 99%
“…In the localized deformation region, it was reported that the number of vacancies increased approximately 10 4 times while that of dislocations increased approximately several times due to deformation. 6,22) In addition, the hydrogen binding energy of dislocation is 16.4 kJ/mol, and this value is relatively low for the trapping sites in aluminum. 23) Since the binding energy of vacancies is 28 kJ/mol and higher than the value for dislocation, the accumulated hydrogen is preferentially repartitioned to vacancy.…”
Section: Effect Of the Mechanical And Microstructural Factors On Hydrogen Accumulationmentioning
confidence: 99%