Extraordinary creep resistance in a non-equiatomic high-entropy alloy from the optimum solid-solution strengthening and stress-assisted precipitation process

被引:32
作者
Chen, Shuying [1 ]
Qiao, Jingbo [1 ]
Diao, Haoyan [2 ]
Yang, Tengfei [3 ]
Poplawsky, Jonathan [4 ]
Li, Weidong [2 ]
Meng, Fanchao [1 ]
Tong, Yang [1 ]
Jiang, Liang [1 ]
Liaw, Peter K. [2 ]
Gao, Yanfei [2 ]
机构
[1] Yantai Univ, Inst Adv Studies Precis Mat, Yantai 264005, Peoples R China
[2] Univ Tennessee, Dept Mat Sci & Engn, Knoxville, TN 37996 USA
[3] Hunan Univ, Coll Mat Sci & Engn, Changsha 410082, Peoples R China
[4] Oak Ridge Natl Lab, Ctr Nanophases Mat Sci, Oak Ridge, TN 37831 USA
基金
中国国家自然科学基金; 美国国家科学基金会;
关键词
High -entropy alloy; Creep resistance; Stress -assisted precipitation process; TEMPERATURE DEFORMATION MECHANISMS; HIGH-DUCTILITY; BEHAVIOR; AL; MICROSTRUCTURE; STABILITY; MAPS;
D O I
10.1016/j.actamat.2022.118600
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Improving creep resistance has commonly been achieved by the optimization of alloy design that results into strong solid-solution strengthening and/or coherent precipitates for dislocation blockage. High-entropy alloys (HEAs), despite their single-phase solid-solution nature, only exhibit creep properties that are comparable to precipitate-strengthened ferritic alloys. Moreover, many HEAs are found to be plagued with many incoherent second phases after long-term annealing, which reduces the lifetime and thus prohibits their usage at elevated temperatures. The present work demonstrates the extraordinary creep resistance of a non-equiatomic Al0.3CoCrFeNi HEA, in which the creep strain rate is found to be several orders of magnitude lower than the Cantor alloy and its subsets. Using a suite of characterization tools such as atom probe tomography (APT) and transmission electron microscopy (TEM), it was shown that a B2 precipitate phase that has been widely seen during annealing is suppressed during the early stage of the creep deformation. Currently, metastable and coherent L1(2) precipitates emerge and provide significant creep strengthening. This observation is rationalized by the coupling between the applied stress and the lattice mismatch. In the range of 973 similar to 1033 K, the stress exponent and activation energy were determined to be 3-6.53 and 390-548.2 kJ center dot mol(-1), respectively. The creep lifetime, on the other hand, is comparable to Cantor subset alloys because the precipitate free zone near the grain boundaries does not provide sufficient constraint for the grain boundary cavity growth. The present work pro-vides a pathway to design novel HEAs with improved creep resistance.
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页数:17
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