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Acta Metall Sin  2022, Vol. 58 Issue (5): 649-659    DOI: 10.11900/0412.1961.2021.00192
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Mechanism of Dynamic Strain-Induced Ferrite Transformation in a 3Mn-0.2C Medium Mn Steel
SUN Yi1,2, ZHENG Qinyuan2,3, HU Baojia2,3, WANG Ping1(), ZHENG Chengwu2,3(), LI Dianzhong2,3
1.Key Laboratory of Electromagnetic Processing of Materials, Ministry of Education, Northeastern University, Shenyang 110819, China
2.Shenyang National Laboratory for Materials Science, Institute of Metal Research, Chinese Academy of Sciences, Shenyang 110016, China
3.School of Materials Science and Engineering, University of Science and Technology of China, Shenyang 110016, China
Cite this article: 

SUN Yi, ZHENG Qinyuan, HU Baojia, WANG Ping, ZHENG Chengwu, LI Dianzhong. Mechanism of Dynamic Strain-Induced Ferrite Transformation in a 3Mn-0.2C Medium Mn Steel. Acta Metall Sin, 2022, 58(5): 649-659.

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Abstract  

Medium Mn steels (MMSs) have Mn contents of 3%-12% (mass fraction), and have been energetically investigated as the most promising candidates of the third-generation advanced high-strength steel. Their phase transformations and microstructures during various heat treatments and thermomechanical processes have received wide attention with the purpose to achieve an optimal balance of cost-efficient alloying compositions and mechanical properties. The aim of this work is to investigate the microstructural behavior of deformation-induced ferrite transformation (DIFT), starting from austenite, which occurs in MMS. Then, improved understandings of the formation of ultrafine ferrite via the DIFT and conservation of this microstructure during the post-deformation period can be obtained. For this purpose, a 3Mn-0.2C MMS with lower contents of alloying elements was selected. Microstructures and alloying element distributions of the thermomechanically processed samples were analyzed via EBSD and EPMA. The results showed that the DIFT occurred in the thermomechanically processed 3Mn-0.2C MMS in the α + γ region. Characteristic multiphase microstructures consisting isolated martensite and fine-grained equiaxed ferrite concomitant with fine islands of retained austenite dispersed between ferrite grains can be obtained. During the DIFT, the enhanced nucleation of ferrite at α/γ interfaces can not only increase the ferrite nucleation density but also facilitate extensive impingement among the neighboring grains. Formation of ultrafine ferrite via the DIFT in MMS can be interpreted in terms of unsaturated nucleation and limited growth. In addition, partitioning of Mn between the ultrafine ferrite and austenite is accelerated during the DIFT such that a large number of Mn-enriched fine islands of austenite are left untransformed at the α/α grain boundaries or at triple junctions. These islands of austenite are considered to play critical roles not only for obtaining retained austenite at room temperature but also for conserving the ultrafine microstructure of the DIFT during the post-deformation processing.

Key words:  hot deformation      ultra-fine grained ferrite      Mn partitioning      deformation induced ferrite transformation      medium Mn steel     
Received:  07 May 2021     
ZTFLH:  TG142.1  
Fund: National Natural Science Foundation of China(52071322);National Natural Science Foundation of China(51771192);National Natural Science Foundation of China(U1708252)
About author:  WANG Ping, professor, Tel: (024)83684630, E-mail: wping@epm.neu.edu.cn
ZHENG Chengwu, associate professor, Tel: (024)23971973, E-mail: cwzheng@imr.ac.cn

URL: 

https://www.ams.org.cn/EN/10.11900/0412.1961.2021.00192     OR     https://www.ams.org.cn/EN/Y2022/V58/I5/649

Fig.1  Schematics showing the thermal-mechanical cycles used for the deformation induced ferrite transformation (a) and the isothermal ferrite transformation (b) of the 3Mn-0.2C medium Mn steel (MMS) (Ae3 is the highest temperature at which ferrite and austenite phases can coexist in equilibrium. Ae1 is the lowest temperature at which ferrite, cementite, and austenite phases can coexist in equilibrium in the steel)
Fig.2  True stress-true strain curve of the 3Mn-0.2C MMS (a) and corresponding EBSD maps at strains of ε = 0.22 (b), 0.51 (c), and 0.92 (d) at temperature of T = 660oC and strain rate of ε˙ = 0.001 s-1 (The green and blue lines in Figs.2b~d represent boundaries with 2° ≤ θ < 15° and θ ≥ 15°, respectively. θ is misorientation angle of the boundary. M—martensite, α—ferrite)
Fig.3  SEM images of 3Mn-0.2C MMS soaking at T = 660oC for 1800 s (a) and deformed to ε = 0.51 with ε˙ = 0.001 s-1 at T = 660oC (b) (RA—retained austenite)
Fig.4  EBSD images of the 3Mn-0.2C MMS at ε = 0.22 (a), 0.51 (b), and 0.92 (c) with the hot deformation under T = 660oC and ε˙ = 0.001 s-1 (The yellow arrows in Fig.4b indicate the ferrite grains formed along the intragranular deformation bands. The green and blue lines in the figures represent boundaries with 2° ≤ θ < 15° and θ ≥ 15°, respectively)
Fig.5  SEM image of the 3Mn-0.2C MMS deformed to ε = 0.92 under T = 660oC and ε˙ = 0.001 s-1, and the associated alloying elements distributions of C, Si, and Mn
Fig. 6  EBSD images of the 3Mn-0.2C MMS deformed to ε = 0.92 under T = 660oC and ε˙ = 0.001 s-1 (a), and the 3Mn-0.2C MMS continuously soaked for 1000 s after deformation at the same temperature (b) (The green and blue lines in the figures represent boundaries with 2° ≤ θ < 15° and θ ≥ 15°, respectively)
Fig.7  SEM images and the distributions of Mn of the 3Mn-0.2C MMS deformed to ε = 0.92 under T = 660oC and ε˙ = 0.001 s-1 (a), and the 3Mn-0.2C MMS continuously soaked for 1000 s after deformation at the same temperature (b)
Fig.8  EBSD images of the 3Mn-0.2C MMS deformed to ε = 0.92 at T = 660oC with ε˙ = 0.1 s-1 (a), 0.01 s-1 (b), and 0.001 s-1 (c) (The green and blue lines in the figures represent boundaries with 2° ≤ θ < 15° and θ ≥ 15°, respectively)
Fig.9  SEM images and the distributions of C and Mn of the 3Mn-0.2C MMS deformed to ε = 0.92 at T = 660oC with ε˙ = 0.1 s-1 (a), 0.01 s-1 (b), and 0.001 s-1 (c)
Fig.10  Schematics of the microstructure evolution during the deformation induced ferrite transformation of the medium Mn steel (a-d)
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