TY - JOUR
T1 - In situ neutron diffraction unravels deformation mechanisms of a strong and ductile FeCrNi medium entropy alloy
AU - Tang, L.
AU - Jiang, F. Q.
AU - Wróbel, J. S.
AU - Liu, B.
AU - Kabra, S.
AU - Duan, R. X.
AU - Luan, J. H.
AU - Jiao, Z. B.
AU - Attallah, M. M.
AU - Nguyen-Manh, D.
AU - Cai, B.
N1 - Funding Information:
The authors thank ISIS neutron and muon source (the Rutherford Appleton Laboratory, UK) for providing the beamtime (RB1810732 and RB1920111) and staff at ENGIN-X beamline for support. Atom probe tomography research was conducted by Dr. J.H. Luan and Dr. Z.B. Jiao at the Inter-University 3D Atom Probe Tomography Unit of City University of Hong Kong, which is supported by the CityU grant 9360161 and RGC grant 25202719. DNM's work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programs 2014–2018 and 2019–2020 under Grant Agreement No. 633053 and from the RCUK Energy Programme [Grant No. EP/T012250/1]. We also acknowledge funding from the European Research Council (ERC) under the European Union's Horizon 2020 research and innovation program (grant agreement No. 714697). The views and opinions expressed herein do not necessarily reflect those of the European Commission. DNM and JSW acknowledge the support from high-performing computing facility MARCONI (Bologna, Italy) provided by EUROfusion. The work at Warsaw University of Technology has been carried out as a part of an international project co-financed from the funds of the program of the Polish Minister of Science and Higher Education entitled "PMW" in 2019, Agreement No. 5018 / H2020-Euratom / 2019/2. The simulations were also carried out with the support of the Interdisciplinary center for Mathematical and Computational Modeling (ICM), University of Warsaw, under grant No. GB79–6.
Funding Information:
The authors thank ISIS neutron and muon source (the Rutherford Appleton Laboratory, UK) for providing the beamtime (RB1810732 and RB1920111) and staff at ENGIN-X beamline for support. Atom probe tomography research was conducted by Dr. J.H. Luan and Dr. Z.B. Jiao at the Inter-University 3D Atom Probe Tomography Unit of City University of Hong Kong, which is supported by the CityU grant 9360161 and RGC grant 25202719. DNM's work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programs 2014?2018 and 2019?2020 under Grant Agreement No. 633053 and from the RCUK Energy Programme [Grant No. EP/T012250/1]. We also acknowledge funding from the European Research Council (ERC) under the European Union's Horizon 2020 research and innovation program (grant agreement No. 714697). The views and opinions expressed herein do not necessarily reflect those of the European Commission. DNM and JSW acknowledge the support from high-performing computing facility MARCONI (Bologna, Italy) provided by EUROfusion. The work at Warsaw University of Technology has been carried out as a part of an international project co-financed from the funds of the program of the Polish Minister of Science and Higher Education entitled "PMW" in 2019, Agreement No. 5018 / H2020-Euratom / 2019/2. The simulations were also carried out with the support of the Interdisciplinary center for Mathematical and Computational Modeling (ICM), University of Warsaw, under grant No. GB79?6.
Publisher Copyright:
© 2022
PY - 2022/7/20
Y1 - 2022/7/20
N2 - We investigated the mechanical and microstructural responses of a high-strength equal-molar medium entropy FeCrNi alloy at 293 and 15 K by in situ neutron diffraction testing. At 293 K, the alloy had a very high yield strength of 651 ± 12 MPa, with a total elongation of 48% ± 5%. At 15 K, the yield strength increased to 1092 ± 22 MPa, but the total elongation dropped to 18% ± 1%. Via analyzing the neutron diffraction data, we determined the lattice strain evolution, single-crystal elastic constants, stacking fault probability, and estimated stacking fault energy of the alloy at both temperatures, which are the critical parameters to feed into and compare against our first-principles calculations and dislocation-based slip system modeling. The density functional theory calculations show that the alloy tends to form short-range order at room temperatures. However, atom probe tomography and atomic-resolution transmission electron microscopy did not clearly identify the short-range order. Additionally, at 293 K, experimental measured single-crystal elastic constants did not agree with those determined by first-principles calculations with short-range order but agreed well with the values from the calculation with the disordered configuration at 2000 K. This suggests that the alloy is at a metastable state resulted from the fabrication methods. In view of the high yield strength of the alloy, we calculated the strengthening contribution to the yield strength from grain boundaries, dislocations, and lattice distortion. The lattice distortion contribution was based on the Varenne-Luque-Curtine strengthening theory for multi-component alloys, which was found to be 316 MPa at 293 K and increased to 629 MPa at 15 K, making a significant contribution to the high yield strength. Regarding plastic deformation, dislocation movement and multiplication were found to be the dominant hardening mechanism at both temperatures, whereas twinning and phase transformation were not prevalent. This is mainly due to the high stacking fault energy of the alloy as estimated to be 63 mJm−2 at 293 K and 47 mJm−2 at 15 K. This work highlights the significance of lattice distortion and dislocations played in this alloy, providing insights into the design of new multi-component alloys with superb mechanical performance for cryogenic applications.
AB - We investigated the mechanical and microstructural responses of a high-strength equal-molar medium entropy FeCrNi alloy at 293 and 15 K by in situ neutron diffraction testing. At 293 K, the alloy had a very high yield strength of 651 ± 12 MPa, with a total elongation of 48% ± 5%. At 15 K, the yield strength increased to 1092 ± 22 MPa, but the total elongation dropped to 18% ± 1%. Via analyzing the neutron diffraction data, we determined the lattice strain evolution, single-crystal elastic constants, stacking fault probability, and estimated stacking fault energy of the alloy at both temperatures, which are the critical parameters to feed into and compare against our first-principles calculations and dislocation-based slip system modeling. The density functional theory calculations show that the alloy tends to form short-range order at room temperatures. However, atom probe tomography and atomic-resolution transmission electron microscopy did not clearly identify the short-range order. Additionally, at 293 K, experimental measured single-crystal elastic constants did not agree with those determined by first-principles calculations with short-range order but agreed well with the values from the calculation with the disordered configuration at 2000 K. This suggests that the alloy is at a metastable state resulted from the fabrication methods. In view of the high yield strength of the alloy, we calculated the strengthening contribution to the yield strength from grain boundaries, dislocations, and lattice distortion. The lattice distortion contribution was based on the Varenne-Luque-Curtine strengthening theory for multi-component alloys, which was found to be 316 MPa at 293 K and increased to 629 MPa at 15 K, making a significant contribution to the high yield strength. Regarding plastic deformation, dislocation movement and multiplication were found to be the dominant hardening mechanism at both temperatures, whereas twinning and phase transformation were not prevalent. This is mainly due to the high stacking fault energy of the alloy as estimated to be 63 mJm−2 at 293 K and 47 mJm−2 at 15 K. This work highlights the significance of lattice distortion and dislocations played in this alloy, providing insights into the design of new multi-component alloys with superb mechanical performance for cryogenic applications.
KW - Cryogenic temperature
KW - Medium entropy alloy
KW - Multi-component alloy
KW - Neutron diffraction
UR - http://www.scopus.com/inward/record.url?scp=85123990420&partnerID=8YFLogxK
U2 - 10.1016/j.jmst.2021.10.034
DO - 10.1016/j.jmst.2021.10.034
M3 - Journal article
AN - SCOPUS:85123990420
SN - 1005-0302
VL - 116
SP - 103
EP - 120
JO - Journal of Materials Science and Technology
JF - Journal of Materials Science and Technology
ER -