2021
DOI: 10.1016/j.matlet.2021.130735
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A new fcc-bcc orientation relationship observed in the strain-induced martensitic transformation of an austenitic stainless steel

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Cited by 14 publications
(2 citation statements)
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“…In particular, the (1 1 1)γ was intensively converted to (1 1 0)α 0 , which is consistent with the relationship established early on by Kurdjumov-Sachs (K-S) for the martensite transformation in the iron alloy. [17] However, the transformation rate differed depending on the tensile direction and temperature conditions. Results from the peak-intensity variations of each phase, the α 0 -martensite formed faster when it was tensile along the RD or at cryogenic temperatures.…”
Section: Microstructural Evolutions During Tensile Deformationmentioning
confidence: 99%
“…In particular, the (1 1 1)γ was intensively converted to (1 1 0)α 0 , which is consistent with the relationship established early on by Kurdjumov-Sachs (K-S) for the martensite transformation in the iron alloy. [17] However, the transformation rate differed depending on the tensile direction and temperature conditions. Results from the peak-intensity variations of each phase, the α 0 -martensite formed faster when it was tensile along the RD or at cryogenic temperatures.…”
Section: Microstructural Evolutions During Tensile Deformationmentioning
confidence: 99%
“…The deformation-induced martensitic transformation is influenced by many factors, such as: temperature, the degree and method of deformation, as well as the chemical composition, size and crystallographic orientation of the austenite grain [20,21]. The instability of austenite depends on the stacking fault energy (SFE), which is influenced by the chemical composition and temperature [22][23][24]. If the steel was deformed below the temperature M d30/50 then a phase transformation induced by deformation took place in the steel.…”
Section: Introductionmentioning
confidence: 99%