2019
DOI: 10.1007/s10853-019-03716-0
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Screw dislocation–spherical void interactions in fcc metals and their dependence on stacking fault energy

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Cited by 20 publications
(4 citation statements)
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“…The work in Cu is not applicable for austenitic stainless steels due to an alternate stacking fault energy (SFE) and shear modulus. There are many atomic-scale simulations on the interactions of dislocations and defects, e.g., dislocation loops and voids, in austenitic stainless steels [18][19][20][21]. However, studies on the interactions between dislocations and SFTs in austenitic stainless steels are limited or not available, and the interactions between dislocations and SFTs contribute to irradiation hardening is unclear.…”
Section: Introductionmentioning
confidence: 99%
“…The work in Cu is not applicable for austenitic stainless steels due to an alternate stacking fault energy (SFE) and shear modulus. There are many atomic-scale simulations on the interactions of dislocations and defects, e.g., dislocation loops and voids, in austenitic stainless steels [18][19][20][21]. However, studies on the interactions between dislocations and SFTs in austenitic stainless steels are limited or not available, and the interactions between dislocations and SFTs contribute to irradiation hardening is unclear.…”
Section: Introductionmentioning
confidence: 99%
“…When the cathode current density was 500 A/m 2 , and the anode was 1000 A/m 2 , the macroscopic surface morphology of manganese metal was uneven and had many protrudes, with noticeable dendritic crystals at the edges. This may have been caused by the mechanism of "helical dislocation growth" 20,21 , and excessive current density caused crystals to deposit along the dislocation line and develop dendrites. Such "outburst growth" dendrites will increase the effective area of the cathode plate but reduce the actual current density and hydrogen overpotential, affecting the cathode's manganese production rate.…”
Section: Accepted M Manuscriptmentioning
confidence: 99%
“…Via MD simulations, researchers measured dislocation mobility in face-centered cubic (FCC) [26][27][28][29][30][31][32], body-centered cubic (BCC) [25,[33][34][35][36] and hexagonal close-packed (HCP) [37][38][39] metals. MD simulations are also carried out to explain the interactions between dislocations and different obstacles, such as dislocation-void interaction [40][41][42][43], dislocation-precipitate interaction [44][45][46][47] and dislocation-GB interaction [48][49][50][51].…”
Section: Introductionmentioning
confidence: 99%
“…In many of the MD simulations mentioned above, researchers utilized various model settings, choices usually driven by technical development or particular research goals. For example, over the years, newer formulations of interatomic potentials for copper have been tested via investigations of dislocation dynamics [43,[52][53][54][55]. Among these interatomic potentials, the intrinsic stacking fault energy varies, leading to discrepancies associated with dissociated core width, mobility, and reactions involving dislocations.…”
Section: Introductionmentioning
confidence: 99%