Modeling dislocation interactions with grain boundaries in lath martensitic steels

dc.contributor.authorAbou Ali Modad, Ossama
dc.contributor.authorShehadeh, Mutasem A.
dc.contributor.departmentDepartment of Mechanical Engineering
dc.contributor.facultyMaroun Semaan Faculty of Engineering and Architecture (MSFEA)
dc.contributor.institutionAmerican University of Beirut
dc.date.accessioned2025-01-24T11:33:28Z
dc.date.available2025-01-24T11:33:28Z
dc.date.issued2023
dc.description.abstractMartensitic steels are widely used as a structural material in critical components of fossil fuel and nuclear power plants, such as boilers, pipes, and fittings. Martensitic steels are known to have a hierarchical microstructure that follows the Kurdjumov–Sachs (K–S) orientation relationship, where a prior austenite grain is composed of packets separated by high angle grain boundaries or packet boundaries, which are, in turn, divided into blocks or variants segregated by high angle grain boundaries called block boundaries. Blocks themselves are an agglomeration of laths divided by low angle grain boundaries named lath boundaries which have precipitates scattered on them. This work seeks to examine, using a couple dislocation dynamics—continuum mechanics approach called multiscale dislocation dynamics plasticity (MDDP), the interactions between dislocations and packet, block, lath boundaries, and precipitates under uniaxial tension loading and their effect on the mechanical response of the material. The simulations are conducted at a strain rate of 105 s−1 at room temperature. The main crystallographic features that arise during the deformation process were extracted and analyzed in terms of their contribution to the mechanical response of the material. The orientation relationship governing the microstructure of martensitic steels, namely, the K–S orientation relationship, was incorporated in MDDP in an effort to accurately capture the deformation behavior of the material in question. The strength of lath martensitic steel was analyzed as a function of the lath width, block size, and packet size to determine the appropriate effective grain size. © 2023, The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature.
dc.identifier.doihttps://doi.org/10.1007/s10853-023-09084-0
dc.identifier.eid2-s2.0-85179945590
dc.identifier.urihttp://hdl.handle.net/10938/27988
dc.language.isoen
dc.publisherSpringer
dc.relation.ispartofJournal of Materials Science
dc.sourceScopus
dc.subjectContinuum mechanics
dc.subjectFossil fuel power plants
dc.subjectFossil fuels
dc.subjectGrain boundaries
dc.subjectMartensitic stainless steel
dc.subjectMicrostructure
dc.subjectNuclear fuels
dc.subjectNuclear power plants
dc.subjectCritical component
dc.subjectDislocation dynamics
dc.subjectDislocation interaction
dc.subjectDynamic plasticity
dc.subjectGrain-boundaries
dc.subjectHigh angle grain boundaries
dc.subjectKurdjumov-sachs orientation relationships
dc.subjectLath boundary
dc.subjectLath martensitic steels
dc.subjectMechanical response
dc.subjectStrain rate
dc.titleModeling dislocation interactions with grain boundaries in lath martensitic steels
dc.typeArticle

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