First-principles study of the phase stability and the mechanical properties of W-Ta and W-Re alloys
Source abstract
Abstract
The phase stability and mechanical properties of binary W1−xTax and W1−xRex alloys were investigated using the full-potential augmented plane-wave method. The special quasirandom structures(SQSs) of these alloys are mechanically stable due to all of the positive elastic constants and negative binding energies. The binding energies of both the W1−xTax and W1−xRex alloys also exhibit energy favorable asymmetry toward the W-rich side. In addition, the bulk modulus of the W1−xTax alloys decrease gradually with the increase of the Ta concentration, while those of the W1−xRex alloys increase gradually with the increase of the Re concentration. Consequently, the bulk modulus of W metal can be improved by doping with Re, implying that the resistance to deformation is enhanced. Based on the mechanical characteristic G/B and Poisson's ratio ν, both the W1−xTax and W1−xRex alloys are regarded as being ductile materials, the ductility of which improves with the increase of Ta or Re.
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Research context
OpenAlex topics: Metal and Thin Film Mechanics · Intermetallics and Advanced Alloy Properties · Fusion materials and technologies
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Chinese Academy of Sciences 1 Key Laboratory for Materials Physics, Institute of Solid State Physics, , Hefei, 230031, China
University of Science and Technology of China 2 , Hefei, 230026, China
Chinese Academy of Sciences 3 Computer Network Information Center (CNIC), Beijing 100190, P.O. Box 349, China
Funding
NSFC
References (28)
Show source-provided references
1. J. Nucl. Mater · 2000 · 278 · 27310.1016/S0022-3115(99)00241-X ↗
2. Fusion Eng. Des · 2009 · 84 · 19410.1016/j.fusengdes.2009.02.028 ↗
3. J. Nucl. Mater · 2004 · 66–73 · 329
4. Int. J. Thermophys · 2009 · 30 · 193110.1007/s10765-009-0660-9 ↗
5. Mater. Lett · 2001 · 51 · 42010.1016/S0167-577X(01)00330-5 ↗
6. Phys. Rev. B · 2008 · 77 · 10420310.1103/PhysRevB.77.104203 ↗
7. Phys. Rev. B · 2001 · 64 · 08511210.1103/PhysRevB.64.085112 ↗
8. Phys. Rev. B · 2004 · 69 · 21420210.1103/PhysRevB.69.214202 ↗
9. Phys. Rev. B · 2005 · 72 · 115163
10. Phys. Rev. B · 2001 · 84 · 10411510.1103/PhysRevB.84.104115 ↗
11. Philos. Mag · 2007 · 87 · 258910.1080/14786430701253197 ↗
12. Phys. Rev. Lett · 1990 · 65 · 35310.1103/PhysRevLett.65.353 ↗
13. Phys. Rev. B · 2007 · 75 · 20520910.1103/PhysRevB.75.205209 ↗
14. Comput. Phys. Commun · 1990 · 59 · 39910.1016/0010-4655(90)90187-6 ↗
15. Phys. Rev. Lett · 1980 · 45 · 81110.1103/PhysRevLett.45.811 ↗
16. Phys. Rev. B · 1951 · 81 · 98810.1103/PhysRev.81.988 ↗
17. Phys. Rev. B · 2006 · 74 · 02420410.1103/PhysRevB.74.024204 ↗
18. Phys. Rev. B · 2007 · 76 · 14420410.1103/PhysRevB.76.144204 ↗
19. J. Appl. Phys · 1938 · 9 · 27910.1063/1.1710417 ↗
20. J. Appl. Phys · 1968 · 39 · 378010.1063/1.1656855 ↗
21. J. Alloy Phase Diagrams · 1987 · 3 · 1
22. Phys. Rev. B · 1993 · 48 · 584410.1103/PhysRevB.48.5844 ↗
23. Phys. Rev. Lett · 1997 · 79 · 207310.1103/PhysRevLett.79.2073 ↗
24. Phys. Rev. B · 1974 · 9 · 142110.1103/PhysRevB.9.1421 ↗
25. Phys. Rev. B · 1995 · 51 · 1743110.1103/PhysRevB.51.17431 ↗
26. Phys. Rev. B · 2005 · 71 · 09420610.1103/PhysRevB.71.094206 ↗
27. Philos. Mag · 1954 · 45 · 82310.1080/14786440808520496 ↗
28. Mater. Trans. JIM · 1990 · 31 · 43510.2320/matertrans1989.31.435 ↗