Phase selection motifs in High Entropy Alloys revealed through combinatorial methods: Large atomic size difference favors BCC over FCC

被引:203
作者
Kube, Sebastian Alexander [1 ]
Sohn, Sungwoo [1 ]
Uhl, David [2 ]
Datye, Amit [1 ]
Mehta, Apurva [3 ]
Schroers, Jan [1 ]
机构
[1] Yale Univ, Dept Mech Engn & Mat Sci, 15 Prospect St,BCT Room 217, New Haven, CT 06511 USA
[2] Southern Connecticut State Univ, Dept Phys, Ctr Nanotechnol, 425 Fitch St, New Haven, CT 06514 USA
[3] SLAC Natl Accelerator Lab, Stanford Synchrotron Radiat Lightsource, 2575 Sandhill Rd, Stanford, CA 94025 USA
基金
美国国家科学基金会;
关键词
High entropy alloys; Combinatorial sputtering; Phase selection; Atomic size difference; SOLID-SOLUTION; MECHANICAL-BEHAVIOR; SINGLE-PHASE; MICROSTRUCTURE; STABILITY; GLASS; PREDICTION; SERRATION; CORROSION; DESIGN;
D O I
10.1016/j.actamat.2019.01.023
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
High Entropy Alloys are inherently complex and span a vast composition space, making their research and discovery challenging. Developing quantitative predictions of their phase selection requires a large quantity of consistently determined experimental data. Here, we use combinatorial methods to fabricate and characterize 2478 quinary alloys based on Al and transition metals. All data are publicly available at http://materialsatlasproject.org/. Phase selection can be predicted for considered alloys when combining the content of FCC/BCC elements and the constituents' atomic size difference. Mining our data reveals that High Entropy Alloys with increasing atomic size difference prefer BCC structure over FCC. This preference is typically overshadowed by other selection motifs, which dominate during close-to equilibrium processing. Not suggested by the Hume-Rothery rules, this preference originates from the ability of the BCC structure to accommodate a large atomic size difference with lower strain energy penalty which can be practically only realized in High Entropy Alloys. (C) 2019 Acta Materialia Inc. Published by Elsevier Ltd.
引用
收藏
页码:677 / 686
页数:10
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