Effect of proportion change of aluminum and silicon on magnetic entropy change and magnetic properties in La0.8Ce0.2Fe11.5Al1.5-xSix compounds
来源期刊:JOURNAL OF RARE EARTHS2017年第7期
论文作者:傅斌 韩洁 王超伦
文章页码:673 - 676
摘 要:The microstructure, magnetic entropy changes, hysteresis and magnetic properties of La0.8Ce0.2Fe11.5Al1.5–xSix(x=0.4, 0.5, 0.6, 0.7) compounds were studied by X-ray diffraction(XRD) and a superconducting quantum interference device magnetometer(SQUID). The results showed that all the compounds presented cubic Na Zn13-type structure. Their Curie temperatures changed complicatedly with decreasing Al content due to changes of antiferromagnetic and ferromagnetic interaction. Under a field change from 0 to 2 T, the maximum magnetic entropy change for La0.8Ce0.2Fe11.5Al1.1Si0.4, La0.8Ce0.2Fe11.5Al1.0Si0.5, La0.8Ce0.2Fe11.5Al0.9Si0.6 and La0.8Ce0.2Fe11.5Al0.8Si0.7 were found to be –9.6, –4.8, –5.8 and –11.7 J/(kg·K), respectively. Moreover, their hysteresis losses were 1.13 J/(kg·K) or less. The large magnetic entropy changed and small hysteresis losses made them potential candidates for practical magnetic refrigeration application.
傅斌1,韩洁2,王超伦3
1. School of Materials Science and Engineering, Tianjin University of Technology2. College of Science, Tianjin University of Technology3. Department of Electrical Engineering, East China Normal University
摘 要:The microstructure, magnetic entropy changes, hysteresis and magnetic properties of La0.8Ce0.2Fe11.5Al1.5–xSix(x=0.4, 0.5, 0.6, 0.7) compounds were studied by X-ray diffraction(XRD) and a superconducting quantum interference device magnetometer(SQUID). The results showed that all the compounds presented cubic Na Zn13-type structure. Their Curie temperatures changed complicatedly with decreasing Al content due to changes of antiferromagnetic and ferromagnetic interaction. Under a field change from 0 to 2 T, the maximum magnetic entropy change for La0.8Ce0.2Fe11.5Al1.1Si0.4, La0.8Ce0.2Fe11.5Al1.0Si0.5, La0.8Ce0.2Fe11.5Al0.9Si0.6 and La0.8Ce0.2Fe11.5Al0.8Si0.7 were found to be –9.6, –4.8, –5.8 and –11.7 J/(kg·K), respectively. Moreover, their hysteresis losses were 1.13 J/(kg·K) or less. The large magnetic entropy changed and small hysteresis losses made them potential candidates for practical magnetic refrigeration application.
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