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北京市自然科学基金(1112005)

作品数:4 被引量:4H指数:1
相关作者:刘丹敏张红国岳明张东涛徐明锋更多>>
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发文基金:北京市自然科学基金国家自然科学基金新金属材料国家重点实验室开放基金更多>>
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MnFePSiGe合金的结构及磁热性能研究
近年来,室温磁制冷技术因其节能、环保、易于小型化和运行稳定等诸多优点得到科学界和产业界的广泛关注,十分有望在室温区取代传统的气体压缩制冷。作为开发这项技术的关键,具有室温区巨磁热效应的新型磁致冷材料逐渐成为国际磁性材料领...
徐明锋徐航岳明张东涛刘卫强张久兴
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间隙原子H,B,C对LaFe_(11.5)Al_(1.5)化合物磁性和磁热效应的影响
2018年
研究了金属化合物LaFe_(11.5)Al_(1.5)H_x(x=0,0.12,0.6,1.3),LaFe_(11.5)Al_(1.5)B_y(y=0.1,0.2,0.3)和LaFe_(11.5)Al_(1.5)C_z(z=0.1,0.2,0.3,0.4,0.5)的磁性、结构和磁热效应.金属化合物样品均形成了良好的NaZn_(13)型单相结构.基于固相-气相反应或者固相-固相反应引入间隙H,B,C原子后,磁性基态从反铁磁态变为铁磁态,饱和磁化强度(M_s)和居里温度(T_c)均呈升高趋势.值得注意的是:随着B和C含量的增加,化合物的相变性质由弱一级相变过渡至二级相变;而随着H含量的增加,相变性质却从二级相变过渡至弱一级相变.同时,化合物LaFe_(11.5)Al_(1.5)H_x,LaFe_(11.5)Al_(1.5)B_y和LaFe_(11.5)Al_(1.5)C_z均呈现出相当大的磁熵变.在0—5 T的外磁场作用下,LaFe_(11.5)Al_(1.5)H_(1.3),LaFe_(11.5)Al_(1.5)B_(0.1)和LaFe_(11.5)Al_(1.5)C_(0.2)的最大磁熵变分别达到12.3,9.6和10.8 J/kg·K.此外,在0—5 T的外磁场作用下,LaFe_(11.5)Al_(1.5)H_(0.6)的制冷能力达到259.2 J/kg,LaFe_(11.5)Al_(1.5)B_(0.1)的制冷能力达到116.4 J/kg,而LaFe_(11.5)Al_(1.5)C_(0.1)的制冷能力达到230.4 J/kg.
杨静洁赵金良许磊张红国岳明刘丹敏蒋毅坚
关键词:磁相变磁热效应
Fe_2P型磁致冷材料研究进展被引量:3
2013年
MnFe(P,As,Ge,Si)合金是一类原料丰富、价格低廉、磁热性能优异的磁致冷材料.介绍了MnFe(P,As,Ge,Si)磁致冷材料的晶体结构、磁结构、磁相变、制备工艺及磁热性能优化方法等方面的研究进展.MnFe(P,As,Ge,Si)合金具有六方Fe2P型晶体结构;合金的居里温度在室温区附近随其成分变化连续可调;合金在磁相变过程中呈现巨磁热效应,磁热效应的物理本质是一级磁弹性相变;合金的制备工艺和成分对其综合磁热性能具有较大影响,经成分和工艺优化的MnFe(P,As,Ge,Si)合金是一种极具实用化潜能的新型室温区磁致冷材料.
岳明徐明锋张红国张东涛刘丹敏张久兴
关键词:磁致冷材料磁相变磁热效应
Effects of Pr substitution on the hydrogenating process and magnetocaloric properties of La1-xPrxFe11.4Si1.6Hy hydrides
2017年
In this paper, we study the effects of Pr substitution on the hydrogenating process and magnetocaloric properties of La_(1-x)Pr_xFe_(11.4)Si_(1.6)H_y hydrides. The powder x-ray diffraction patterns of the La_(1-x)Pr_xFe_(11.4)Si_(1.6) and its hydrides show that each of the alloys is crystallized into the single phase of cubic Na Zn_(13)-type structure. There are hydrogen-absorbing plateaus under 0.4938 MPa and 0.4882 MPa in the absorbing curves for the La_(0.8)Pr_(0.2)Fe_(11.4)Si_(1.6) and La_(0.6)Pr_(0.4)Fe_(11.4)Si_(1.6) compounds. The releasing processes lag behind the absorbing process, which is obviously different from the coincidence between absorbing and releasing curves of the La Fe_(11.4)Si_(1.6) compound. The remnant hydrogen content for La_(0.6)Pr_(0.4)Fe_(11.4)Si_(1.6) is significantly more than that for La_(0.8)Pr_(0.2)Fe_(11.4)Si_(1.6) after hydrogen desorption, indicating that more substitutions of Pr for La are beneficial to retaining more hydrogen atoms in the alloys. The values of maximum magnetic entropy change are 14.91 J/kg·K and 17.995 J/kg·K for La_(0.8)Pr_(0.2)Fe_(11.4)Si_(1.6)H_(0.13) and La_(0.6)Pr_(0.4)Fe_(11.4)Si_(1.6)H_(0.87),respectively.
许磊赵金良杨静洁张红国刘丹敏岳明蒋毅坚
Structure and magnetic properties of Mn_(1.2)Fe_(0.8)P_(0.76)Ge_(0.24) annealed alloy被引量:1
2012年
Bulk Mn_(1.2)Fe_(0.8)P_(0.76)Ge_(0.24) alloy was prepared by mechanical milling and subsequent spark plasma sintering technique.Effect of annealing on the structure and magneto-caloric properties of the alloy was investigated.XRD results show that both sintered and annealed samples possess a hexagonal Fe_2P-type crystal structure.After annealing,ferromagnetic impurity Fe_3Mn_4Ge_6,which exists in the sintered sample,was eliminated from the alloy.Furthermore,the lattice constants a and c change noticeably,leading to a decrease in c/a ratio,while the cell volume almost remains invariable.As a result,the Curie temperature of the alloy increases from 253 K to 298 K,but the maximum magnetic entropy change decreases from 37.5 to 11.7 J·kg·K^(-1) for 2 T magnetic field change.On the other hand,the thermal hysteresis of M-T curves around T_C upon heating and cooling is 14 and 8 K for the as-sintered and the annealed sample,respectively,showing evident change.
Xu, Hang Yue, Ming Zhao, Chuan Zhang, Dongtao Zhang, Jiuxing
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