J. Mater. Sci. Technol. ›› 2020, Vol. 44: 201-208.DOI: 10.1016/j.jmst.2019.10.038
• Research Article • Previous Articles Next Articles
Xiaojun Sunab, Jie Heab*(), Bin Chenab, Lili Zhanga, Hongxiang Jianga, Jiuzhou Zhaoab, Hongri Haoa
Received:
2019-09-19
Revised:
2019-10-09
Accepted:
2019-10-12
Published:
2020-05-01
Online:
2020-05-21
Contact:
Jie He
Xiaojun Sun, Jie He, Bin Chen, Lili Zhang, Hongxiang Jiang, Jiuzhou Zhao, Hongri Hao. Microstructure formation and electrical resistivity behavior of rapidly solidified Cu-Fe-Zr immiscible alloys[J]. J. Mater. Sci. Technol., 2020, 44: 201-208.
Fig. 1. SEM images of the as-quenched (a) (Cu0.55Fe0.45)90Zr10, (b) (Cu0.5Fe0.5)90Zr10, and (c) (Cu0.4Fe0.6)90Zr10 alloys, (d) size distribution of the particles in the as-quenched (Cu0.4Fe0.6)90Zr10 alloy.
Fig. 3. (a) STEM image of the as-quenched (Cu0.5Fe0.5)40Zr60 alloy (the inset is the SAED pattern), (b) size distribution of the glassy nanoparticles in the as-quenched (Cu0.5Fe0.5)40Zr60 alloy, (c) and (d) HRTEM images of the typical nanoparticles in the as-quenched (Cu0.5Fe0.5)40Zr60 alloy, exhibiting different appearances.
Fig. 6. Gibbs free energies of the undercooled Cu-Fe melt at T = 1500 K: (a) Gibbs free energies GL and Gγ-Fe of the melt and γ-Fe, (b) Gibbs free energy difference for phase separation in liquid and solidification of γ-Fe.
Fig. 7. (a) Calculated metastable miscibility gap and DSC curves of the (Cu1-xFex)90Zr10 system, (b) and (c) SEM images of the (Cu0.4Fe0.6)90Zr10 and (Cu0.8Fe0.2)90Zr10 alloy samples after a cooling DSC circle.
Fig. 8. (a) Calculated metastable miscibility gap of the (Cu1-xFex)40Zr60 system, (b) schematic diagram of viscosity changing with temperature. TL and Ts present the liquidus temperature and onset temperature of LLPS, respectively.
Fig. 9. (a) Variation of nomalized resistivity with temperature and DSC heating curve of (Cu0.5Fe0.5)40Zr60 alloys, (b) Variation of nomalized resistivity with temperature of Zr60Cu40 and Zr75Fe25 alloys.
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