2012
DOI: 10.1016/j.scriptamat.2011.10.009
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Continuum modeling of dislocation starvation and subsequent nucleation in nano-pillar compressions

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Cited by 26 publications
(8 citation statements)
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“…This microstructure results in a dramatically different stress-strain response as compared to the system with curved dislocations: because we have neither an increase in density nor a line tension one can only observe a linear hardening (regime II) which -regardless the boundary condition -is followed by a nearly elastic regime III where the stresses are considerably different from those reached for the system with dislocation loops. The loss of dislocations through surfaces (and ultimately the 'dislocation starvation') has been experimentally observed in nano/micro pillar compression tests (Shan et al, 2008;Jerusalem et al, 2012) as well. This starvation effect also gave rise to a second elastic regime as observed in our edge dislocation system.…”
Section: Study 1: the Influence Of Boundary Conditions (Case 1)mentioning
confidence: 94%
“…This microstructure results in a dramatically different stress-strain response as compared to the system with curved dislocations: because we have neither an increase in density nor a line tension one can only observe a linear hardening (regime II) which -regardless the boundary condition -is followed by a nearly elastic regime III where the stresses are considerably different from those reached for the system with dislocation loops. The loss of dislocations through surfaces (and ultimately the 'dislocation starvation') has been experimentally observed in nano/micro pillar compression tests (Shan et al, 2008;Jerusalem et al, 2012) as well. This starvation effect also gave rise to a second elastic regime as observed in our edge dislocation system.…”
Section: Study 1: the Influence Of Boundary Conditions (Case 1)mentioning
confidence: 94%
“…В англоязычной литературе такой режим получил образное название " дислокационный голод" (dislocation starvation) [89,103,104,307]. Подобный режим наблюдался во многих ГЦК и ОЦК материалах при D < 1 µm [308][309][310]. В результате на столбиках из отожженного монокристаллического Mo диаметром ∼ 100 nm с полусферической вершиной, вырезанных из массива c помощью FIB и продеформированных в таком режиме in situ в колонне ТЕМ, достигался предел текучести, близкий или равный теоретическому пределу прочности τ th [309].…”
Section: размерные эффекты природа деформации и разрушения в наношкалеunclassified
“…Some attempts have been made to directly correlate appropriate constitutive models to finite element (FE) analysis that can handle complex geometry easily, apply boundary conditions accurately and compute efficiently. In most cases, FE simulations using the phenomenological (Jérusalem et al, 2012;Maaß et al, 2009;Raabe et al, 2007;Zhang and Shang, 2014) and dislocation-based crystal plasticity theories (Hurtado and Ortiz, 2012;Kuroda, 2013) are employed to study micropillar plasticity because they can analyze microscopic heterogeneity associated with plastic deformation in materials and address the issue of high strain rate in dislocation dynamics simulations.…”
Section: Introductionmentioning
confidence: 99%
“…Some FE analyses using crystal plasticity models have already been employed to study size-dependent flow strength (Hurtado and Ortiz, 2012), microplastic deformation mode (Kuroda, 2013) and smoother transition to plasticity observed in micro-compression tests (Jérusalem et al, 2012). A general introduction of strain bursts into the crystal plasticity finite element framework that is capable of capturing the strain bursts in the macroscopic stressstrain behavior of single crystalline micropillar compressions, has been described in Zhang and Shang (2014).…”
Section: Introductionmentioning
confidence: 99%