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Yin Liu Zhecheng Wang Li Zhao Jun Zhou Yueqin Wang 《Journal of the American Ceramic Society》2019,102(11):6680-6687
xSrFe12O19/(1−x)NiFe2O4 composites (0 ≤ x ≤ 1.0) were synthesized by using a conventional solid-state synthetic route. The results show that magnetic hysteresis loops of the xSrFe12O19/(1−x)NiFe2O4 composites are similar to those of individual component ferrites, except for the 0.1SrFe12O19/0.9NiFe2O4 and 0.3SrFe12O19/0.7NiFe2O4, suggesting that the hard/soft magnetic phases are well exchange-coupled. The saturation magnetization, coercivity, and remanent magnetization of the xSrFe12O19/(1−x)NiFe2O4 composites are increased with increasing content of SrFe12O19, with maximal values of 42.1 Am2 kg−1, 78.7 kA m−1, 17.2 Am2 kg−1, respectively, as the content x is about 0.5. They are higher than those of the individual components, implying that interface coupling is present in the magnetic composites. The coercivity and remanent magnetization of the composites are increased initially with increasing sintering temperature and then show a downward tendency. For the component SrFe12O19 and NiFe2O4, the minimum reflection losses are −12.5 dB and −18.3 dB at match thicknesses of 2.5 mm and 2 mm, respectively. Compared with those of the component SrFe12O19 and NiFe2O4, the microwave absorption performances of the xSrFe12O19/(1−x)NiFe2O4 composites are improved remarkably, especially for the samples of x = 0.3 and x = 0.9. The minimum reflection losses values of the 0.3SrFe12O19/0.7NiFe2O4 composite are −31.6 dB (12.7 GHz) and −20.2 dB (13 GHz), while those of the 0.9SrFe12O19/0.1NiFe2O4 composites are −23.7 dB (16.3 GHz) and −33.5 dB (15.8 GHz), as the matching thicknesses are 2.5 mm and 2 mm, respectively. Therefore, the xSrFe12O19/(1−x)NiFe2O4 composites could be used as potential microwave absorption materials. 相似文献
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以Nd9.5Fe76Zr3Co5B6.5合金为研究对象,研究了不同快淬速度(8~65 m/s)对合金的磁性能、交换耦合作用和微观结构的影响。结果表明,快淬速度对合金退火后的微观结构和磁性能具有显著地影响,适当的快淬速度将使合金退火后的晶粒细化、分布均匀,提高软、硬磁性相间的交换耦合作用,进而提高合金的磁性能。当淬速为15 m/s时,合金退火后具有最佳的综合磁性能:Br=0.976 T,Hcj=711.57 kA/m,(BH)max=150.61 kJ/m3。 相似文献
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Dependence of Effective Anisotropy on Grain Size in Nanocrystalline Nd2 Fe14 B Hard Magnetic Material 总被引:2,自引:2,他引:0
Anisotropy of material is the key factor determin ing coercivity and anisotropy of nano grain is dramati cally influenced by grain size[1~2]. So the coercivityof nano magnetic material with different grain sizeswould have obvious difference.… 相似文献
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以软磁性相α-Fe和硬磁性相Nd2Fe14B为例,研究了软、硬磁性晶粒间的交换耦合作用和有效各向异性常数〈Ksh〉随晶粒尺寸的变化关系。由于晶粒间的交换耦合作用,晶粒可分为晶粒内部无界面交换耦合作用影响和晶粒表面有界面交换耦合作用影响两部分,其各向异性常数为两部分的统计平均值。计算结果表明:对固定的软磁性晶粒尺寸Ds,〈Ksh〉随硬磁性晶粒尺寸Dh一致增加;对固定的Db,〈Ksj〉随Ds一致减小。为使软、硬磁性晶粒间的有效各向异性常数墨。保持较高的值,应控制硬磁性晶粒大于35nm,软磁性晶粒在10nm左右。 相似文献
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《材料科学技术学报》2019,35(8):1655-1661
Fe83.2-xCoxP10C6Cu0.8 (x = 0, 4, 6, 8 and 10) alloys with a high amorphous-forming ability and good soft-magnetic properties were successfully synthesized. Saturation magnetic flux density (Bs) is effectively enhanced from 1.53 T to 1.61 T for as-quenched alloy by minor Co addition, which is consistent well with the result of the linear relationship between average magnetic moment and magnetic valence. For Co-contained alloys, the value of corecivity (Hc) is mainly determined by magneto-crystalline anisotropy, while effective permeability (μe) is dominated by grain size and average saturation polarization. After proper heat treatment, the Fe79.2Co4P10C6Cu0.8 nanocrystalline alloy exhibited excellent soft-magnetic properties including a high Bs of 1.8 T, a low Hc of 6.6 A/m and a high μe of 15,510, which is closely related to the high volume fraction of α-(Fe, Co) grains and refined uniform nanocrystalline microstructure. 相似文献
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