2020
DOI: 10.22226/2410-3535-2020-4-537-542
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On the common topological conditions for shear-coupled twin boundary migration in bcc and hcp metals

Abstract: The most abundant deformation twins in metals with hcp and bcc crystallographic structures, i. e. (10-12) and (112) respectively, proceed with the same mechanism of deformation under an applied shear stress, i. e. shear-coupled twin boundary migration. Despite the differences in the atomic structure and degrees of symmetry of bcc and hcp crystals, the topological aspects that rule the processes of growth and shrinkage of these deformation twins are equivalent. In this paper, we revisit the atomic level process… Show more

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Cited by 8 publications
(10 citation statements)
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“…More generally, real GBs are rarely symmetric nor flat, nor do they have a pure tilt or pure twist character, and even without preliminary deformation, they contain disconnections of various characters [53]. This defect has been known for decades in phase transformation and twinning [66][67][68][69], but has only recently been considered as the basic brick of shear-coupled GB migration [70][71][72], in metals with bcc and hcp structures too [73,74]. One reason for this late acceptance is that the observation of moving disconnections is complicated experimentally, as in-situ TEM is almost the only way to do it [75] and that many atomistic simulations considered perfect GBs where the disconnection nucleation step overshadows the other mechanisms such as their propagation.…”
Section: Discussionmentioning
confidence: 99%
“…More generally, real GBs are rarely symmetric nor flat, nor do they have a pure tilt or pure twist character, and even without preliminary deformation, they contain disconnections of various characters [53]. This defect has been known for decades in phase transformation and twinning [66][67][68][69], but has only recently been considered as the basic brick of shear-coupled GB migration [70][71][72], in metals with bcc and hcp structures too [73,74]. One reason for this late acceptance is that the observation of moving disconnections is complicated experimentally, as in-situ TEM is almost the only way to do it [75] and that many atomistic simulations considered perfect GBs where the disconnection nucleation step overshadows the other mechanisms such as their propagation.…”
Section: Discussionmentioning
confidence: 99%
“…Besides the low formation energy of the {112} tilt GB, a relevant feature of this GB for the accommodation of plastic deformation is the existence of highly glissile EDiscs responsible for the shear-coupled GB migration [17,18,24,25]. The critical resolved shear stress of the EDisc is about 20 MPa [54] in Fe.…”
Section: B Elementary Disconnections At the (112) Gbmentioning
confidence: 99%
“…(i) The dislocation at the GB undergoes a variety of feasible processes. The possible reactions of the dislocation present a gradation of complexity, ranging from transmission with a small resistance keeping the same Burgers vector [16] to full absorption by the GB [17,18]. In intermediate situations, the dislocation is partially transmitted, leaving a residual defect at the GB, which is necessary to account for Burgers vector conservation [19].…”
Section: Introductionmentioning
confidence: 99%
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“…Among the variety of disconnections, we define as EDisc the glissile ones that have a Bv parallel to the interfaces [51]. They are responsible for the SCGBM [31,40,49,51,[56][57][58][59]. Thus, the effectiveness of the accommodation of plastic deformation depends on the creation of disconnections, its glissile character and the interaction of these disconnections with other defects located on the GB.…”
Section: Grain Boundaries Under Plastic Deformation Shear-coupled Gb ...mentioning
confidence: 99%