Making an Ultra‐Ductile Laminate Medium Entropy Alloy by Pressure Thermal Treatment
Source abstract
Abstract
Abstract Innovations in either high‐performance materials or microstructures by conventional processing methods are often challenging to achieve without a synergistic combination. The perfect combination of pressure and temperature offers a great prospect for altering the microstructure that would permit achieving the extreme properties in functional and structural materials. Here, pressure thermal treatment is used to make a laminate medium‐entropy alloy that exhibits a combination of a large fracture elongation of ≈122 percent and a high fracture strength of ≈900 megapascals. The high tensile ductility stems from the strong synergistic effects of the laminate structures with low‐energy interfaces. Consequently, versatile dislocation configurations and deformation twinning are sequentially stimulated, effectively improving the alloy's ability to accommodate plastic deformation. This unique laminate structure with the low‐energy interface obtained from pressure thermal treatment offers a paradigm for developing hierarchically metallic materials with exceptional mechanical properties.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: High Entropy Alloys Studies · High-Temperature Coating Behaviors · Metal and Thin Film Mechanics
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Center for High Pressure Science and Technology, College of Energy Engineering Zhejiang University Hangzhou 310007 China
Faculty of Arts and Sciences Beijing Normal University Zhuhai 519080 China
School of Materials Science and Engineering Xiangtan University Xiangtan 411199 China
Funding
National Natural Science Foundation of China · China Postdoctoral Science Foundation
References (53)
Show source-provided references
1. 10.1038/ncomms458010.1038/ncomms4580 ↗
2. 10.1038/s41467-023-35863-z10.1038/s41467-023-35863-z ↗
3. 10.1038/nmat311510.1038/nmat3115 ↗
4. 10.1088/0370-1301/64/9/30310.1088/0370-1301/64/9/303 ↗
5. 10.1126/science.115610110.1126/science.1156101 ↗
6. 10.1038/nature0892910.1038/nature08929 ↗
7. 10.1038/nature2169110.1038/nature21691 ↗
8. 10.1038/s41467-023-40580-810.1038/s41467-023-40580-8 ↗
9. 10.1038/s41467-022-32134-110.1038/s41467-022-32134-1 ↗
10. 10.1002/adma.20240545910.1002/adma.202405459 ↗
11. 10.1016/j.mattod.2017.02.00310.1016/j.mattod.2017.02.003 ↗
12. 10.1016/j.pmatsci.2017.04.01310.1016/j.pmatsci.2017.04.013 ↗
13. 10.1038/s41578-020-0212-210.1038/s41578-020-0212-2 ↗
14. 10.1038/s41467-022-30873-910.1038/s41467-022-30873-9 ↗
15. 10.1016/j.ijplas.2019.07.01910.1016/j.ijplas.2019.07.019 ↗
16. Wu X. · Appl. Phys. Sci. · 2015 · 112
17. 10.1016/j.mattod.2018.03.00610.1016/j.mattod.2018.03.006 ↗
18. 10.1016/j.ijplas.2012.10.00310.1016/j.ijplas.2012.10.003 ↗
19. Cheng Z. · Science · 2018 · 362
20. 10.1016/j.jmst.2021.09.05810.1016/j.jmst.2021.09.058 ↗
21. 10.1016/j.ijplas.2016.10.00310.1016/j.ijplas.2016.10.003 ↗
22. 10.1038/s41598-017-11001-w10.1038/s41598-017-11001-w ↗
23. 10.1080/21663831.2016.115300410.1080/21663831.2016.1153004 ↗
24. 10.1080/21663831.2018.143911510.1080/21663831.2018.1439115 ↗
25. 10.1016/j.ijplas.2013.07.00210.1016/j.ijplas.2013.07.002 ↗
26. 10.1016/j.actamat.2023.11867310.1016/j.actamat.2023.118673 ↗
27. 10.1016/j.ijplas.2014.08.01310.1016/j.ijplas.2014.08.013 ↗
28. 10.1016/j.actamat.2016.06.02310.1016/j.actamat.2016.06.023 ↗
29. 10.1038/s41467-024-48435-610.1038/s41467-024-48435-6 ↗
30. 10.1016/j.surfcoat.2017.12.02110.1016/j.surfcoat.2017.12.021 ↗
31. 10.1103/PhysRevMaterials.5.08360110.1103/PhysRevMaterials.5.083601 ↗
32. 10.1016/j.jnucmat.2023.15469310.1016/j.jnucmat.2023.154693 ↗
33. 10.1016/j.proeng.2011.04.02110.1016/j.proeng.2011.04.021 ↗
34. 10.1016/j.scriptamat.2010.11.01110.1016/j.scriptamat.2010.11.011 ↗
35. 10.1016/j.actamat.2016.06.03210.1016/j.actamat.2016.06.032 ↗
36. 10.1016/j.jmst.2020.04.07310.1016/j.jmst.2020.04.073 ↗
37. 10.1557/s43577-021-00055-x10.1557/s43577-021-00055-x ↗
38. 10.1016/j.scriptamat.2021.11411710.1016/j.scriptamat.2021.114117 ↗
39. 10.1038/ncomms1060210.1038/ncomms10602 ↗
40. 10.1016/j.jmst.2022.03.02410.1016/j.jmst.2022.03.024 ↗
41. 10.1016/j.actamat.2017.07.02910.1016/j.actamat.2017.07.029 ↗
42. 10.3390/ma1105066210.3390/ma11050662 ↗
43. 10.1016/j.msea.2017.06.08610.1016/j.msea.2017.06.086 ↗
44. 10.1016/j.actamat.2017.02.03610.1016/j.actamat.2017.02.036 ↗
45. 10.1016/j.matdes.2022.11077410.1016/j.matdes.2022.110774 ↗
46. 10.1016/j.actamat.2017.04.03310.1016/j.actamat.2017.04.033 ↗
47. 10.1016/j.jmst.2021.01.06010.1016/j.jmst.2021.01.060 ↗
48. 10.1016/j.msea.2021.14154510.1016/j.msea.2021.141545 ↗
49. Yang M. · Appl. Phys. Sci. · 2018 · 115 · 7224
50. 10.1016/j.addma.2020.10120210.1016/j.addma.2020.101202 ↗
51. 10.1016/j.jmst.2021.07.04210.1016/j.jmst.2021.07.042 ↗
52. 10.1080/08957959.2011.61423810.1080/08957959.2011.614238 ↗
53. 10.1016/S1359-6462(02)00335-410.1016/S1359-6462(02)00335-4 ↗