Johnson-Mehl-Avrami-Kolmogorov (JMAK-type) Analysis of Deformation-Induced Martensitic Transformation in AISI 304L Stainless Steel
Sohrabi, Mohammad Javad; Mirzadeh, Hamed; Sadeghpour, Saeed; Mahmudi, Reza
Sohrabi, Mohammad Javad
Mirzadeh, Hamed
Sadeghpour, Saeed
Mahmudi, Reza
Iran University of Science & Technology
Sohrabi M J, Mirzadeh H, Sadeghpour S, Mahmudi R. Johnson–Mehl–Avrami–Kolmogorov (JMAK-type) Analysis of Deformation-Induced Martensitic Transformation in AISI 304L Stainless Steel. IJMSE 2023; 20 (4) :1-9 URL: http://ijmse.iust.ac.ir/article-1-3335-en.html
https://creativecommons.org/licenses/by-nc/4.0/
This work is licensed under a Creative Commons Attribution-NonCommercial 4.0 International License.
https://creativecommons.org/licenses/by-nc/4.0/
This work is licensed under a Creative Commons Attribution-NonCommercial 4.0 International License.
https://creativecommons.org/licenses/by-nc/4.0/
Julkaisun pysyvä osoite on
https://urn.fi/URN:NBN:fi:oulu-202404172814
https://urn.fi/URN:NBN:fi:oulu-202404172814
Tiivistelmä
Abstract
Deformation -induced α΄ -martensite generally forms at shear bands in the coarse -grained austenite, while it nucleates at grain boundaries in the ultrafine -grained (UFG) austenite. The available kinetics models are related to the nucleation on the shear band intersections. Hence, their application to investigating the kinetics of α΄ -martensite formation for the UFG regime cannot be justified. Accordingly, in the present work, the general Johnson –Mehl–Avrami– Kolmogorov (JMAK-type) model was implemented for comparing the kinetics of α΄ -martensite formation in the UFG and coarse -grained regimes using an AISI 304L stainless steel. On the experimental front, the X-ray diffraction (XRD) patterns and the electron backscattered diffraction (EBSD) maps were used for phase and microstructural analyses, respectively. It was revealed that the simple JMAK-type model, by considering the dependency of the volume fraction of α΄ -martensite on the strain, is useful for modelling the experimental data, predicting the nucleation sites based on the theoretical Avrami exponents, and characterizing the transformation kinetics at low and high strains.
Deformation -induced α΄ -martensite generally forms at shear bands in the coarse -grained austenite, while it nucleates at grain boundaries in the ultrafine -grained (UFG) austenite. The available kinetics models are related to the nucleation on the shear band intersections. Hence, their application to investigating the kinetics of α΄ -martensite formation for the UFG regime cannot be justified. Accordingly, in the present work, the general Johnson –Mehl–Avrami– Kolmogorov (JMAK-type) model was implemented for comparing the kinetics of α΄ -martensite formation in the UFG and coarse -grained regimes using an AISI 304L stainless steel. On the experimental front, the X-ray diffraction (XRD) patterns and the electron backscattered diffraction (EBSD) maps were used for phase and microstructural analyses, respectively. It was revealed that the simple JMAK-type model, by considering the dependency of the volume fraction of α΄ -martensite on the strain, is useful for modelling the experimental data, predicting the nucleation sites based on the theoretical Avrami exponents, and characterizing the transformation kinetics at low and high strains.
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