FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2024584942> ?p ?o ?g. }

• W2024584942 endingPage "15" @default.
• W2024584942 startingPage "1" @default.
• W2024584942 abstract "Consider a magnesium bicrystal created from two single crystal lattices referred to as black and white. The bicrystal abuts a basal plane of the black crystal with a first-order prismatic plane of the white crystal. At zero stress, the boundary relaxes by developing coherent terraces, while two types of disconnection dipoles and a misfit dislocation above each dipole nucleate, in combination, to remove the attendant long-range elastic strains and maximize local coherency. When the bicrystal is stretched normal to its semicoherent interface, stress motivates the misfit dislocation at the far side of the boundary to glide and annihilate at the triple point. The removal of this bounding misfit dislocation allows the positive step of the disconnection dipole to conservatively move away. The negative step of this dipole, however, remains sessile at the grain boundary as it cannot glide conservatively. This sessile step facilitates nucleation of a new disconnection dipole. The first process of disconnection dipole widening then repeats, and the new residual negative step coalesces with the first one to form a novel disconnection of double step height. The whole process cycles once more, and two of these double-height disconnections pile-up at the boundary. The pile-up quickly relaxes into a coherent boundary along the {1 0 1¯ 2} plane; a {1 0 1¯ 2} twin facet thus nucleates, and a disclination dipole arises to bound the twin facet at the two junctions. Soon thereafter, the lower disclination, at the opposite side from where the misfit was removed, begins emitting twinning disconnections toward the upper disclination. These twinning disconnections caused their source junction to recede in favor of an overwhelming lengthening of the twin facet. All twinning disconnections end up moving through the upper disclination, thereby undergoing a dislocation transformation event. The new transformed disconnection glides freely along the remaining basal-prismatic boundary segment, and enables this boundary to be dragged with the propagating twin facet. This steady stage proceeds until the entire bicrystal transforms in to a single twinned crystal. This paper examines the fundamentals of these twin nucleation mechanisms at the grain boundary on the basis of the interfacial defect theory advanced by Pond and co-workers [1], [2]. It introduces an important twin nucleation mechanism with dynamics of twin faceting in relation to an important asymmetric low-energy boundary in hexagonal close-packed materials." @default.
• W2024584942 created "2016-06-24" @default.
• W2024584942 creator A5004607212 @default.
• W2024584942 creator A5044815336 @default.
• W2024584942 date "2014-01-01" @default.
• W2024584942 modified "2023-10-05" @default.
• W2024584942 title "The roles of grain boundary dislocations and disclinations in the nucleation of {102} twinning" @default.
• W2024584942 cites W1030537428 @default.
• W2024584942 cites W1963945208 @default.
• W2024584942 cites W1964127217 @default.
• W2024584942 cites W1970486977 @default.
• W2024584942 cites W1992652129 @default.
• W2024584942 cites W1998522395 @default.
• W2024584942 cites W2007836519 @default.
• W2024584942 cites W2008169672 @default.
• W2024584942 cites W2010356892 @default.
• W2024584942 cites W2014272734 @default.
• W2024584942 cites W2019285109 @default.
• W2024584942 cites W2019465613 @default.
• W2024584942 cites W2022343478 @default.
• W2024584942 cites W2022854772 @default.
• W2024584942 cites W2026831094 @default.
• W2024584942 cites W2038937373 @default.
• W2024584942 cites W2049233869 @default.
• W2024584942 cites W2050322282 @default.
• W2024584942 cites W2053144336 @default.
• W2024584942 cites W2053609266 @default.
• W2024584942 cites W2063183347 @default.
• W2024584942 cites W2063901874 @default.
• W2024584942 cites W2090945188 @default.
• W2024584942 cites W2129236398 @default.
• W2024584942 cites W2161627685 @default.
• W2024584942 cites W2963105053 @default.
• W2024584942 cites W2988745324 @default.
• W2024584942 cites W4211105458 @default.
• W2024584942 cites W4232986181 @default.
• W2024584942 cites W4252376781 @default.
• W2024584942 doi "https://doi.org/10.1016/j.actamat.2013.09.012" @default.
• W2024584942 hasPublicationYear "2014" @default.
• W2024584942 type Work @default.
• W2024584942 sameAs 2024584942 @default.
• W2024584942 citedByCount "143" @default.
• W2024584942 countsByYear W20245849422014 @default.
• W2024584942 countsByYear W20245849422015 @default.
• W2024584942 countsByYear W20245849422016 @default.
• W2024584942 countsByYear W20245849422017 @default.
• W2024584942 countsByYear W20245849422018 @default.
• W2024584942 countsByYear W20245849422019 @default.
• W2024584942 countsByYear W20245849422020 @default.
• W2024584942 countsByYear W20245849422021 @default.
• W2024584942 countsByYear W20245849422022 @default.
• W2024584942 countsByYear W20245849422023 @default.
• W2024584942 crossrefType "journal-article" @default.
• W2024584942 hasAuthorship W2024584942A5004607212 @default.
• W2024584942 hasAuthorship W2024584942A5044815336 @default.
• W2024584942 hasConcept C121332964 @default.
• W2024584942 hasConcept C13274807 @default.
• W2024584942 hasConcept C159122135 @default.
• W2024584942 hasConcept C159985019 @default.
• W2024584942 hasConcept C173523689 @default.
• W2024584942 hasConcept C17744445 @default.
• W2024584942 hasConcept C185592680 @default.
• W2024584942 hasConcept C192562407 @default.
• W2024584942 hasConcept C199539241 @default.
• W2024584942 hasConcept C26873012 @default.
• W2024584942 hasConcept C2780371621 @default.
• W2024584942 hasConcept C32418499 @default.
• W2024584942 hasConcept C47908070 @default.
• W2024584942 hasConcept C61048295 @default.
• W2024584942 hasConcept C62520636 @default.
• W2024584942 hasConcept C6840138 @default.
• W2024584942 hasConcept C8010536 @default.
• W2024584942 hasConcept C87976508 @default.
• W2024584942 hasConcept C97355855 @default.
• W2024584942 hasConceptScore W2024584942C121332964 @default.
• W2024584942 hasConceptScore W2024584942C13274807 @default.
• W2024584942 hasConceptScore W2024584942C159122135 @default.
• W2024584942 hasConceptScore W2024584942C159985019 @default.
• W2024584942 hasConceptScore W2024584942C173523689 @default.
• W2024584942 hasConceptScore W2024584942C17744445 @default.
• W2024584942 hasConceptScore W2024584942C185592680 @default.
• W2024584942 hasConceptScore W2024584942C192562407 @default.
• W2024584942 hasConceptScore W2024584942C199539241 @default.
• W2024584942 hasConceptScore W2024584942C26873012 @default.
• W2024584942 hasConceptScore W2024584942C2780371621 @default.
• W2024584942 hasConceptScore W2024584942C32418499 @default.
• W2024584942 hasConceptScore W2024584942C47908070 @default.
• W2024584942 hasConceptScore W2024584942C61048295 @default.
• W2024584942 hasConceptScore W2024584942C62520636 @default.
• W2024584942 hasConceptScore W2024584942C6840138 @default.
• W2024584942 hasConceptScore W2024584942C8010536 @default.
• W2024584942 hasConceptScore W2024584942C87976508 @default.
• W2024584942 hasConceptScore W2024584942C97355855 @default.
• W2024584942 hasLocation W20245849421 @default.
• W2024584942 hasOpenAccess W2024584942 @default.
• W2024584942 hasPrimaryLocation W20245849421 @default.
• W2024584942 hasRelatedWork W1575356166 @default.
• W2024584942 hasRelatedWork W1965067054 @default.

• next