Acta Metallurgica Sinica (English Letters) ›› 2022, Vol. 35 ›› Issue (4): 662-678.DOI: 10.1007/s40195-021-01346-7
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H. R. Rezaei Ashtiani1(
), A. A. Shayanpoor1
Received:2021-06-27
Revised:2021-08-23
Accepted:2021-09-17
Online:2022-04-10
Published:2022-04-10
Contact:
H. R. Rezaei Ashtiani
About author:H. R. Rezaei Ashtiani, hr_rezaei@arakut.ac.ir; hrr.Ashtiani@gmail.comH. R. Rezaei Ashtiani, A. A. Shayanpoor. Effect of Initial Grain Size on the Hot Deformation Behavior and Microstructural Evolution of Pure Copper[J]. Acta Metallurgica Sinica (English Letters), 2022, 35(4): 662-678.
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| Si | Sn | Ag | Al | Fe | Zn | Cu |
|---|---|---|---|---|---|---|
| 0.001 | 0.0147 | 0.0022 | 0.0173 | 0.0183 | 0.001 | 99.92 |
Table 1 Chemical composition (wt.%) of investigated pure copper
| Si | Sn | Ag | Al | Fe | Zn | Cu |
|---|---|---|---|---|---|---|
| 0.001 | 0.0147 | 0.0022 | 0.0173 | 0.0183 | 0.001 | 99.92 |
Fig. 1 Schematic of annealing heat treatment used for generation of two different grain sizes of specimens and thermo-mechanical conditions of hot compression test after annealing
Fig. 2 Microstructures of annealed copper with different cooling methods of a air-cooled (with an average grain size of 50 μm), b furnace cooled (with an average grain size of 20 μm) copper
Fig. 3 True stress-strain curves of pure copper at various strain rates, IGS, and deformation temperatures of a 673 K, b 773 K, c 873 K, d 973 K, e 1073 K
Fig. 4 Influences of IGS and Zener-Hollman (Z) parameter (strain rate and temperature) on the dominant deformation mechanism and flow stress behavior of pure copper
Fig. 14 Microstructures of the central part of the deformed sample at 673 K and 0.001 ${\text{s}}^{ - 1}$ and the strain of 0.6 with IGS a 20 μm and b 50 μm
Fig. 15 Microstructures of the hot deformed samples with IGS of a 20 μm, b 50 μm at 1073 K and 0.001 ${\text{s}}^{ - 1}$ and samples with IGS of c 20 μm and d 50 μm at 773 K and 0.001 ${\text{s}}^{ - 1}$
Fig. 17 Microstructures of the deformed samples with IGS of a 20 μm, b 50 μm at 973 K and 0.1 ${\text{s}}^{ - 1}$ and samples with IGS of c 20 μm and d 50 μm at 973 K and 0.001 ${\text{s}}^{ - 1}$
Fig. 19 Relationship between $\ln \left\{ {\ln \left[ {1/\left( {1 - X_{{{\text{DRX}}}} } \right)} \right]} \right\}$ and $\ln \left[ {\left( {\varepsilon - \varepsilon_{{\text{c}}} } \right)/\varepsilon_{{\text{p}}} } \right]$ at different strain rates and temperatures for determination slope n and intercept k for IGS of a 20, b 50 μm
Fig. 20 Volume fraction of DRX as a function of strain at different strain rates and deformation temperatures of a 673 K, b 773 K, c 873 K, d 973 K, e 1073 K
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