材料科学与技术 ›› 2022, Vol. 120 ›› Issue (0): 8-14.DOI: 10.1016/j.jmst.2021.12.037
收稿日期:2021-09-23
修回日期:2021-12-07
接受日期:2021-12-14
出版日期:2022-09-01
发布日期:2022-03-06
Chao Wang1, Peng Shen1, Yikun Fang, Shuai Wang, Qiangfeng Li, Lei Wang, Wei Li(
), Minggang Zhu(
)
Received:2021-09-23
Revised:2021-12-07
Accepted:2021-12-14
Online:2022-09-01
Published:2022-03-06
Contact:
Wei Li,Minggang Zhu
About author:mgzhu@126.com (M. Zhu).1 These authors contributed equally to this work.
. [J]. 材料科学与技术, 2022, 120(0): 8-14.
Chao Wang, Peng Shen, Yikun Fang, Shuai Wang, Qiangfeng Li, Lei Wang, Wei Li, Minggang Zhu. Cellular microstructure modification and high temperature performance enhancement for Sm2Co17-based magnets with different Zr contents[J]. J. Mater. Sci. Technol., 2022, 120(0): 8-14.
Fig. 2. SEM images of Sm(CobalFe0.09Cu0.09Zrx)7.2 magnets; (a) and (a1), (b) and (b1), (c) and (c1), (d) and (d1) corresponding to x of 0.025, 0.030, 0.035, 0.040 at solid-solution and final states.
Fig. 3. (a) Demagnetization curves of Sm(CobalFe0.09Cu0.09Zrx)7.2 magnets (x = 0.025, 0.030, 0.035, 0.04) at 300 K, (b) Demagnetization curves and B-H curves of Sm(CobalFe0.09Cu0.09Zrx)7.2 magnets (x = 0.025, 0.030, 0.035, 0.04) at 773 K.
| x | Br/T | Empty Cell | Hcj / (kA m-1) | Empty Cell | β/(% K-1) | (BH)max / (kJ m-3) | |||
|---|---|---|---|---|---|---|---|---|---|
| 300 K | 773 K | Empty Cell | 300 K | 773 K | Empty Cell | 300 -773 K | 300 K | 773 K | |
| 0.025 | 0.959 | 0.729 | 2668.19 | 556.32 | -0.1673 | 177.83 | 93.93 | ||
| 0.030 | 0.931 | 0.700 | 2429.39 | 613.55 | -0.1580 | 167.96 | 87.24 | ||
| 0.035 | 0.926 | 0.671 | 2281.34 | 644.68 | -0.1516 | 164.45 | 79.15 | ||
| 0.040 | 0.902 | 0.639 | 1926.32 | 666.89 | -0.1382 | 154.42 | 71.10 | ||
Table 1. Magnetic properties of Sm(CobalFe0.09Cu0.09Zrx)7.2 magnets with different Zr contents at 300 K and 773 K.
| x | Br/T | Empty Cell | Hcj / (kA m-1) | Empty Cell | β/(% K-1) | (BH)max / (kJ m-3) | |||
|---|---|---|---|---|---|---|---|---|---|
| 300 K | 773 K | Empty Cell | 300 K | 773 K | Empty Cell | 300 -773 K | 300 K | 773 K | |
| 0.025 | 0.959 | 0.729 | 2668.19 | 556.32 | -0.1673 | 177.83 | 93.93 | ||
| 0.030 | 0.931 | 0.700 | 2429.39 | 613.55 | -0.1580 | 167.96 | 87.24 | ||
| 0.035 | 0.926 | 0.671 | 2281.34 | 644.68 | -0.1516 | 164.45 | 79.15 | ||
| 0.040 | 0.902 | 0.639 | 1926.32 | 666.89 | -0.1382 | 154.42 | 71.10 | ||
Fig. 4. TEM bright-field images with c-axis perpendicular (left) and parallel to the imaging plane (right) for the (a) Zr25, (b) Zr30, (c) Zr35 and (d) Zr40 magnets; and the SAED patterns corresponding to Zr25 (e), Zr30 (f), Zr35 (g) and Zr40 (h) magnets. The variation trends of average cell size and lamellar phase density for the magnets are shown in (i).
Fig. 5. STEM EDS-mapping of Sm(CobalFe0.09Cu0.09Zrx)7.2 magnets and the corresponding typical composition profiles of cells and cell boundaries marked in HAADF images by white lines: Zr25 (a) and (e), Zr30 (b) and (f), Zr35 (c) and (g), Zr40 (d) and (h).
Fig. 6. (a-d) Rietveld analysis for powder XRD patterns of Fig. 1(b); (e) the variation of Cu content at cell boundaries and cell boundary phase weight fraction with x value.
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