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MnFe(P,Si)一级相变热磁发电材料的制备与磁性研究 被引量:3

Investigation on the synthesize and magnetic properties of first-order phase transition thermomagnetic power generation compound MnFe(P,Si)
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摘要 通过机械合金化和固相烧结方法,制备一系列MnFe(P,Si)一级相变化合物,并测定其结构、磁热性能及部分热力学性能。研究结果表明:MnFe(P,Si)系列化合物呈Fe_2P型六角结构,空间群为P-62 m,其中部分化合物存在少量Fe_3Si或Fe_5Si_3第二相。MnFe_(0.9)P_(0.5)Si_(0.5)呈单相Fe_2P型六角结构,由铁磁态到顺磁态(升温)和顺磁态到铁磁态(降温)的转变分别出现在Ttw=330K,Ttc=318K,其热滞ΔThys=12K。升降温相变较快,均在10K以内完成,说明相变是一级相变。在0~1.5T的外磁场中最大等温磁熵变-ΔS_(max)=18.6J/(kg·K);其比热容最高为(升温)C_p=1 571J/(kg·K),(降温)C_p=1 447J/(kg·K)。由此推断,MnFe_(0.9)P_(0.5)Si_(0.5)化合物符合热磁发电工作需求,是一种具有良好磁热性能的热磁发电候选材料。 The first-order phase transition compounds MnFe (P, Si) have been prepared by mechanical alloying and solid-state reaction method, and investigated the structure,magnetocaloric properties and thermodynamic properties. The results show that the obtained MnFe(P, Si) compounds are composed of a main phase of Fe2 P-type hexagonal structure with space group P-62m, and a secondary phases of Fe3 Si or Fe5 Si3, which appeared in some of them. Mn- Fe0.9 P0. 5 Si0. 5 crystallizes in single phase with Fe2 P-type hexagonal structure, the transitions from ferromagnetic state to paramagnetic state (heating process) and paramagnetic state to ferromagnetic state (cooling process) are appeared at Ttw = 330 K and Ttc = 318 K, respectively. Its thermal hysteresis is AThys = 12 K and the transition in heating and cooling process are completed in 10 K, which means these transitions are of first-order phase transition. The maximum value of magnetic entropy change is-ΔS_(max)= 18.6 J/(kg · K) in a magnetic field change of 0-1.5 T. The maximum heat capacity is Cp=1571 J/(kg · K) (heating process) and Cp=1447 J/(kg · K) (cooling process). Therefore, it can be inferred that MnFe0. 9 P0.5 Si0. 5 compound is an excellent candidate material for thermomagnetic power generation.
出处 《金属功能材料》 CAS 2016年第3期11-16,共6页 Metallic Functional Materials
基金 国家自然科学基金资助(51161017 11404176) 内蒙古自治区自然科学基金资助(2014BS0108)
关键词 一级相变化合物 巨磁热效应 居里温度 热磁发电 first-order phase transition giant magnetocaloric effect Curie temperature thermomagnetic power generation
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