Dynamic effects in the characterization of the magnetocaloric effect of LaFeSi-type alloys

C. Romero-Torralva, C. Mayer, V. Franco, A. Conde
{"title":"Dynamic effects in the characterization of the magnetocaloric effect of LaFeSi-type alloys","authors":"C. Romero-Torralva, C. Mayer, V. Franco, A. Conde","doi":"10.1109/INTMAG.2015.7157648","DOIUrl":null,"url":null,"abstract":"In this work, the influence of the rate of change of the applied field to three magnetocaloric samples is studied: a bulk Gd sample used as a reference material, and fully hydrogenated La0.7Ce0.3Fe11.7Si1.3H1.8 and La0.7Ce0.3(Fe0.882Mn0.018Si0.1)13H1.8 alloys, denoted as ERASTEEL-NX and ERASTEEL-11688, respectively . Bulk samples ERASTEEL-NX and ERASTEEL-1688 were prepared from powder batches obtained by gas atomization process as described in [4] . The powder was then sintered at 1150°C for 5 hours in Ar (it has to be noticed that this is not the optimal temperature for maximizing the proportion of NaZn13 type phase), and the obtained blocs were treated at 400°C for 1 hour in hydrogen . The final proportions of NaZn13 type phase is respectively 80 .5% (instead of 92% for optimized heat treatment) and 85% (instead of 92% also for optimized heat treatment) in ERASTEEL-NX and ERASTEEL-1688 . ERASTEEL-NX, with 30% of Ce substituted to La and no substitution on the Fe site shows a very strong 1st order transition, with a wide hysteresis . ERASTEEL-1688 contains some Mn atoms in substitution to Fe . This induces a softening of the 1st order character of the magnetic transition in this sample . The adiabatic temperature change of the samples has been measured using a commercial setup consisting of a set of Halbach cylinders as a variable field source up to 1.78 T, and a thermocouple placed between two pieces of sample, with dimensions of 8 x 4 x 0 .75 mm, which registers the temperature difference between the sample and the sampleholder . The sample is kept in vacuum inside a bath cryostat . The temperature of the sampleholder is stabilized before performing each of the adiabatic measurements . The rate of change of the field ranged from 0 .25 T s-1 to 3 T s-1, which is equivalent to frequencies of a magnetic refrigerator operating between 0 and 1 .78 T ranging from 0 .07 Hz to 0 .84 Hz .","PeriodicalId":381832,"journal":{"name":"2015 IEEE Magnetics Conference (INTERMAG)","volume":"36 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2015-05-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2015 IEEE Magnetics Conference (INTERMAG)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/INTMAG.2015.7157648","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1

Abstract

In this work, the influence of the rate of change of the applied field to three magnetocaloric samples is studied: a bulk Gd sample used as a reference material, and fully hydrogenated La0.7Ce0.3Fe11.7Si1.3H1.8 and La0.7Ce0.3(Fe0.882Mn0.018Si0.1)13H1.8 alloys, denoted as ERASTEEL-NX and ERASTEEL-11688, respectively . Bulk samples ERASTEEL-NX and ERASTEEL-1688 were prepared from powder batches obtained by gas atomization process as described in [4] . The powder was then sintered at 1150°C for 5 hours in Ar (it has to be noticed that this is not the optimal temperature for maximizing the proportion of NaZn13 type phase), and the obtained blocs were treated at 400°C for 1 hour in hydrogen . The final proportions of NaZn13 type phase is respectively 80 .5% (instead of 92% for optimized heat treatment) and 85% (instead of 92% also for optimized heat treatment) in ERASTEEL-NX and ERASTEEL-1688 . ERASTEEL-NX, with 30% of Ce substituted to La and no substitution on the Fe site shows a very strong 1st order transition, with a wide hysteresis . ERASTEEL-1688 contains some Mn atoms in substitution to Fe . This induces a softening of the 1st order character of the magnetic transition in this sample . The adiabatic temperature change of the samples has been measured using a commercial setup consisting of a set of Halbach cylinders as a variable field source up to 1.78 T, and a thermocouple placed between two pieces of sample, with dimensions of 8 x 4 x 0 .75 mm, which registers the temperature difference between the sample and the sampleholder . The sample is kept in vacuum inside a bath cryostat . The temperature of the sampleholder is stabilized before performing each of the adiabatic measurements . The rate of change of the field ranged from 0 .25 T s-1 to 3 T s-1, which is equivalent to frequencies of a magnetic refrigerator operating between 0 and 1 .78 T ranging from 0 .07 Hz to 0 .84 Hz .
动态效应在lafesi型合金磁热效应表征中的应用
本文研究了外加磁场变化率对三种磁热样品的影响:以体积Gd样品为基准材料,充分氢化的La0.7Ce0.3 fe11.7 si1.3 h1.8和La0.7Ce0.3(fe0.888 mn0.018 si0.1)13H1.8合金,分别记为ERASTEEL-NX和ERASTEEL-11688。用[4]中所述的气雾化工艺获得的粉末批次制备了散装样品ERASTEEL-NX和ERASTEEL-1688。然后将粉末在1150℃的氩气中烧结5小时(需要注意的是,这不是使NaZn13型相比例最大化的最佳温度),得到的块状物在400℃的氢气中处理1小时。在ERASTEEL-NX和ERASTEEL-1688中,NaZn13型相的最终比例分别为80.5%(优化热处理为92%)和85%(优化热处理为92%)。ERASTEEL-NX中,30%的Ce被La取代,而Fe位点没有被取代,表现出很强的一阶跃迁,具有较宽的滞后。ERASTEEL-1688含有一些取代铁的Mn原子。这引起了该样品中磁跃迁的一阶特性的软化。样品的绝热温度变化使用商业装置进行测量,该装置由一组哈尔巴赫圆柱体作为高达1.78 T的可变场源,以及放置在两块样品之间的热电偶组成,尺寸为8 x 4 x 0.75 mm,其记录了样品和样品支架之间的温差。样品在低温恒温器中真空保存。在进行每次绝热测量之前,样品架的温度是稳定的。磁场的变化率在0.25 T -1到3t -1之间,这相当于一台运行在0到1.78 T之间、0.07 Hz到0.84 Hz的磁制冷机的频率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信