TY - JOUR
T1 - Aluminum alloying effects on lattice types, microstructures, and mechanical behavior of high-entropy alloys systems
AU - Tang, Zhi
AU - Gao, Michael C.
AU - Diao, Haoyan
AU - Yang, Tengfei
AU - Liu, Junpeng
AU - Zuo, Tingting
AU - Zhang, Yong
AU - Lu, Zhaoping
AU - Cheng, Yongqiang
AU - Zhang, Yanwen
AU - Dahmen, Karin A.
AU - Liaw, Peter K.
AU - Egami, Takeshi
N1 - Funding Information:
Zhi Tang, Tengfei Yang, Yanwen Zhang, and Takeshi Egami acknowledge the financial support from the Department of Energy (DOE), Office of Nuclear Energy’s Nuclear Energy University Program (NEUP) grant 00119262, with Drs. R.O. Jensen, L. Tian, and S. Lesica as program managers. Michael C. Gao acknowledges support of the Innovative Processing and Technologies Program of the National Energy Technology Laboratory’s (NETL) Strategic Center for Coal under the RES contract DE-FE-0004000. Haoyan Diao and Peter K. Liaw would like to acknowledge the DOE, Office of Fossil Energy, National Energy Technology Laboratory (DE-FE-0008855), with Mr. V. Cedro as program manager. Yongqiang Cheng is supported by the Scientific User Facilities Division, Office of Basic Energy Sciences, DOE. Karin A. Dahmen and Peter K. Liaw thank the support from the project of DE-FE-0011194 with the program manager, Dr. S. Markovich.
PY - 2013/12
Y1 - 2013/12
N2 - The crystal lattice type is one of the dominant factors for controlling the mechanical behavior of high-entropy alloys (HEAs). For example, the yield strength at room temperature varies from 300 MPa for the face-centered-cubic (fcc) structured alloys, such as the CoCrCuFeNiTi x system, to about 3,000 MPa for the body-centered-cubic (bcc) structured alloys, such as the AlCoCrFeNiTi x system. The values of Vickers hardness range from 100 to 900, depending on lattice types and microstructures. As in conventional alloys with one or two principal elements, the addition of minor alloying elements to HEAs can further alter their mechanical properties, such as strength, plasticity, hardness, etc. Excessive alloying may even result in the change of lattice types of HEAs. In this report, we first review alloying effects on lattice types and properties of HEAs in five Al-containing HEA systems: Al x CoCrCuFeNi, Al x CoCrFeNi, Al x CrFe1.5MnNi0.5, Al x CoCrFeNiTi, and Al x CrCuFeNi2. It is found that Al acts as a strong bcc stabilizer, and its addition enhances the strength of the alloy at the cost of reduced ductility. The origins of such effects are then qualitatively discussed from the viewpoints of lattice-strain energies and electronic bonds. Quantification of the interaction between Al and 3d transition metals in fcc, bcc, and intermetallic compounds is illustrated in the thermodynamic modeling using the CALculation of PHAse Diagram method.
AB - The crystal lattice type is one of the dominant factors for controlling the mechanical behavior of high-entropy alloys (HEAs). For example, the yield strength at room temperature varies from 300 MPa for the face-centered-cubic (fcc) structured alloys, such as the CoCrCuFeNiTi x system, to about 3,000 MPa for the body-centered-cubic (bcc) structured alloys, such as the AlCoCrFeNiTi x system. The values of Vickers hardness range from 100 to 900, depending on lattice types and microstructures. As in conventional alloys with one or two principal elements, the addition of minor alloying elements to HEAs can further alter their mechanical properties, such as strength, plasticity, hardness, etc. Excessive alloying may even result in the change of lattice types of HEAs. In this report, we first review alloying effects on lattice types and properties of HEAs in five Al-containing HEA systems: Al x CoCrCuFeNi, Al x CoCrFeNi, Al x CrFe1.5MnNi0.5, Al x CoCrFeNiTi, and Al x CrCuFeNi2. It is found that Al acts as a strong bcc stabilizer, and its addition enhances the strength of the alloy at the cost of reduced ductility. The origins of such effects are then qualitatively discussed from the viewpoints of lattice-strain energies and electronic bonds. Quantification of the interaction between Al and 3d transition metals in fcc, bcc, and intermetallic compounds is illustrated in the thermodynamic modeling using the CALculation of PHAse Diagram method.
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U2 - 10.1007/s11837-013-0776-z
DO - 10.1007/s11837-013-0776-z
M3 - Article
AN - SCOPUS:84890543052
SN - 1047-4838
VL - 65
SP - 1848
EP - 1858
JO - JOM
JF - JOM
IS - 12
ER -