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SPS烧结双主相Sm_(2)Co_(17)-Ce_(2)Co_(17)复合永磁体的微观组织
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作者 徐成福 傅森杨 +5 位作者 马冬冬 顾正飞 马垒 阳永泉 高新强 刘荣进 《材料热处理学报》 CAS CSCD 北大核心 2024年第5期40-47,共8页
研究了放电等离子烧结(SPS)工艺和退火温度对双主相Sm_(2)Co_(17)-Ce_(2)Co_(17)复合永磁体微观组织的影响。结果表明:制备双主相Sm_(2)Co_(17)-Ce_(2)Co_(17)复合永磁体的最佳SPS工艺为:烧结温度750℃、压强64 MPa、烧结时间10 min,这... 研究了放电等离子烧结(SPS)工艺和退火温度对双主相Sm_(2)Co_(17)-Ce_(2)Co_(17)复合永磁体微观组织的影响。结果表明:制备双主相Sm_(2)Co_(17)-Ce_(2)Co_(17)复合永磁体的最佳SPS工艺为:烧结温度750℃、压强64 MPa、烧结时间10 min,这样有利于减少稀土元素之间的扩散。退火可使烧结后磁体中存在的非晶相晶化。退火温度越高,双主相磁体中的稀土元素之间越容易相互扩散,Ce原子易扩散到Sm_(2)Co_(17)相中取代Sm原子,而Sm原子扩散到Ce_(2)Co_(17)相中取代Ce原子的机会就相对较少些,且在Sm_(2)Co_(17)相与Ce_(2)Co_(17)相的边界处形成一个过渡的富稀土区。 展开更多
关键词 双主相sm_(2)Co_(17)-Ce_(2)Co_(17)复合永磁体 放电等离子烧结(SPS) 退火温度 微观组织
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共沉淀还原扩散法制备Sm_2Fe_(17)N_x磁性材料 被引量:4
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作者 邓庚凤 孙光飞 姜坤 《过程工程学报》 CAS CSCD 北大核心 2008年第S1期251-255,共5页
采用共沉淀法制备钐-铁复合氧化物,先用氢预还原,再用Ca还原,得到成分均一的Sm_2Fe_(17)合金,渗氮后得到Sm_2Fe_(17)N_x磁性材料.着重研究了共沉淀法制备Sm_2Fe_(17)合金的前驱物—钐-铁复合氧化物的最佳沉淀工艺,探索共沉淀还原扩散法... 采用共沉淀法制备钐-铁复合氧化物,先用氢预还原,再用Ca还原,得到成分均一的Sm_2Fe_(17)合金,渗氮后得到Sm_2Fe_(17)N_x磁性材料.着重研究了共沉淀法制备Sm_2Fe_(17)合金的前驱物—钐-铁复合氧化物的最佳沉淀工艺,探索共沉淀还原扩散法合成Sm_2Fe_(17),合金的适宜温度及产物分离剂的选择.结果表明,以氨水为沉淀剂,反应温度为333K,pH=8,陈化时间为18h时共沉淀产物的Fe:Sm原子比最接近理论配比;以共沉淀法制备的复合氧化物为原料合成Sm_2Fe_(17)合金的温度为1273K.EDTA浓度为0.03 mol/L时,Sm_2Fe_(17)合金产物分离效果最好;渗氮后的Sm_2Fe_(17)N_x磁粉性能为B_r=0.83T,H_(cb)=288.4kA/m,H_(ci)=554.9kA/m,(BH)_(max)=58.4kJ/m^3. 展开更多
关键词 共沉淀法 还原扩散法 sm_2fe_(17) sm_2fe_(17)N_x
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Sm_2Fe_(17)和Sm_(10.5)Fe_(88.5)Zr_(1.0)的氮化行为 被引量:4
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作者 崔春翔 李杰民 +1 位作者 孙继兵 韩瑞平 《功能材料》 EI CAS CSCD 北大核心 2004年第1期31-33,共3页
 通过真空电弧炉制备了Sm2Fe17和Sm10.5Fe88.5Zr1.0母合金,铸态Sm2Fe17先经均匀化处理后再氮化,而Sm10.5Fe88.5Zr1.0则不经均匀化退火而直接在高纯氮气中氮化。运用扫描电子显微镜和X射线衍射技术对其氮化行为进行了研究。薄片扩散实...  通过真空电弧炉制备了Sm2Fe17和Sm10.5Fe88.5Zr1.0母合金,铸态Sm2Fe17先经均匀化处理后再氮化,而Sm10.5Fe88.5Zr1.0则不经均匀化退火而直接在高纯氮气中氮化。运用扫描电子显微镜和X射线衍射技术对其氮化行为进行了研究。薄片扩散实验表明氮在Sm2Fe17中的扩散要比在Sm10.5Fe88.5Zr1.0中的扩散快。运用Fick第二定律通过理论计算得出直径为20μm的Sm2Fe17合金和Sm10.5Fe88.5Zr1.0合金球形粉末粒子,实现充分氮化的时间为10h和16h。实际粉末实现完全氮化的时间要比理论计算的时间少。这和粒径分布、颗粒表面状态、氮化过程产生的微裂纹以及实际条件和理想条件的差异有关。对于直径为20μm的粉末,氮化时间为6h时氮化已基本完成,氮化时间过长,Sm2Fe17Nx会发生分解。 展开更多
关键词 sm2fe17 sm10.5fe88.5Zr1.0 氮化 扩散 永磁材料
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Sm_(2)Fe_(17)N_(x)永磁材料矫顽力机理探究及影响因素分析 被引量:1
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作者 李青华 刘冬 +5 位作者 胡国辉 贾立颖 王倩 李志宏 刘荣明 李炳山 《矿冶》 CAS 2022年第1期85-90,共6页
矫顽力是Sm_(2)Fe_(17)N_(x)(1≤x≤6)永磁材料的重要磁参量。矫顽力机理及其影响因素研究对于Sm_(2)Fe_(17)N_(x)永磁材料的开发具有重要意义。采用振动样品磁强计(VSM)测试Sm_(2)Fe_(17)N_(x)粉末在不同磁化场下的磁特性曲线,并对Sm_(... 矫顽力是Sm_(2)Fe_(17)N_(x)(1≤x≤6)永磁材料的重要磁参量。矫顽力机理及其影响因素研究对于Sm_(2)Fe_(17)N_(x)永磁材料的开发具有重要意义。采用振动样品磁强计(VSM)测试Sm_(2)Fe_(17)N_(x)粉末在不同磁化场下的磁特性曲线,并对Sm_(2)Fe_(17)N_(x)永磁材料的矫顽力机理进行探究。结果发现,随着磁化场H_(app)的增大,取向样品的矫顽力H_(cj)和磁化强度M均逐渐增加,当磁化场H_(app)≥19 kOe时,矫顽力H_(cj)和磁化强度M均不再增加。Sm_(2)Fe_(17)N_(x)永磁材料的矫顽力属于反磁化畴形核机理。此外,还对还原扩散法制备Sm_(2)Fe_(17)N_(x)永磁材料的矫顽力影响因素进行了分析总结。结果发现,通过控制合理的还原扩散温度、氮化的温度和时间、球磨时间、球磨条件和防氧化,可获得接近单畴尺寸的均匀粒子,有利于减少软磁相α-Fe、杂质相和降低颗粒表层损伤,从而提高Sm_(2)Fe_(17)N_(x)粉末的矫顽力。 展开更多
关键词 sm_(2)fe_(17)N_(x)永磁材料 矫顽力机理 矫顽力 还原扩散法
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Phase structure evolution and its effect on magnetic and mechanical properties of B-doped Sm_(2)Co_(17)-type magnets with high Fe content
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作者 Yao-Wen Li Zhuang Liu +8 位作者 Hai-Chen Wu Fang Wang Chao-Qun Zhu Dong-Liang Tan Yu Liu Yang Yang Ming-Xiao Zhang Ren-Jie Chen A-Ru Yan 《Chinese Physics B》 SCIE EI CAS CSCD 2024年第9期582-588,共7页
The unique cellular microstructure of Fe-rich Sm_(2)Co_(17)-type permanent magnets is closely associated with the structure of the solid solution precursor.We investigate the phase structure,magnetic properties,and me... The unique cellular microstructure of Fe-rich Sm_(2)Co_(17)-type permanent magnets is closely associated with the structure of the solid solution precursor.We investigate the phase structure,magnetic properties,and mechanical behavior of B-doped Sm_(2)Co_(17)-type magnets with high Fe content.The doped B atoms can diffuse into the interstitial vacancy,resulting in lattice expansion and promote the homogenization of the phase organizational structure during the solid solution treatment in theory.However,the resulting second phase plays a dominant role to result in more microtwin structures and highly ordered 2:17R phases in the solid solution stage,which inhibits the ordering transformation of 1:7H phase during aging and affects the generation of the cellular structure,and to result in a decrease in magnetic properties,yet the interface formed between it and the matrix phase hinders the movement of dislocations and enhances the mechanical properties.Hence,the precipitation of high flexural strain grain boundary phase induced by B element doping is also a new and effective way to improve the flexural strain of Sm_(2)Co_(17)-type magnets.Our study provides a new understanding of the phase structure evolution and its effect on the magnetic and mechanical properties of Sm_(2)Co_(17)-type magnets with high Fe content. 展开更多
关键词 sm_(2)Co_(17)-type magnets magnetic and mechanical properties
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高能球磨制备高矫顽力各向异性Sm_(2)Fe_(17)N_(3)磁粉 被引量:1
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作者 李伟 郭家瑞 +3 位作者 左思源 王亚娜 黄光伟 郑立允 《粉末冶金材料科学与工程》 2021年第6期554-559,共6页
为了获得高矫顽力的Sm_(2)Fe_(17)N_(3)磁粉,对平均粒径为2.5μm的商用Sm_(2)Fe_(17)N_(3)磁粉进行0~60 min高能球磨,研究球磨时间对Sm_(2)Fe_(17)N_(3)磁粉结构与磁性能的影响。结果表明,随球磨时间延长,Sm_(2)Fe_(17)N_(3)粉体的矫顽... 为了获得高矫顽力的Sm_(2)Fe_(17)N_(3)磁粉,对平均粒径为2.5μm的商用Sm_(2)Fe_(17)N_(3)磁粉进行0~60 min高能球磨,研究球磨时间对Sm_(2)Fe_(17)N_(3)磁粉结构与磁性能的影响。结果表明,随球磨时间延长,Sm_(2)Fe_(17)N_(3)粉体的矫顽力先增大后减小,球磨时间为12 min时,Sm_(2)Fe_(17)N_(3)相晶粒尺寸从原始粉末的40.8 nm减小至31.8 nm,粉体具有最高矫顽力,为875.6 kA/m,且磁粉仍保持磁各向异性。球磨时间为30 min时,虽然晶粒尺寸进一步减小,但Sm_(2)Fe_(17)N_(3)分解生成SmN和α-Fe等软磁相,导致磁粉的矫顽力降低,球磨时间为60 min的磁粉矫顽力仅为477.6 kA/m。本研究制备的Sm_(2)Fe_(17)N_(3)粉体可作为高性能Sm_(2)Fe_(17)N_(3)黏结磁体的优质原料粉末。 展开更多
关键词 sm_(2)fe_(17)N_(3)粉体 高能球磨 矫顽力 磁性能 各向异性
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Hydrogen Decrepitation of a Sm_2Fe_(17)Alloy
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作者 赵旭 李东华 +3 位作者 范存淦 李冬法 王安川 李依依 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 1992年第6期457-460,共4页
1.IntroductionThe rhombohedral compoundSmFeN(x=1~3)is currently attractinginterest due to its promise as a new perma-nent magnet material.Its magnetic proper-ties have been investigated in details.TheSm-Fe-N material... 1.IntroductionThe rhombohedral compoundSmFeN(x=1~3)is currently attractinginterest due to its promise as a new perma-nent magnet material.Its magnetic proper-ties have been investigated in details.TheSm-Fe-N materials with quite good mag- 展开更多
关键词 HYDROGEN decrepitation sm_2fe_(17)
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Tb_2Fe_(17)和Tb_2(Fe,Si)_(17)磁性单晶的生长和相图
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作者 陈京兰 孟丽琴 +2 位作者 王文洪 余晨辉 吴光恒 《人工晶体学报》 EI CAS CSCD 北大核心 2000年第S1期26-,共1页
R2 Fe17(R为稀土 )是一大类稀土金属间化合物 ,具有硬磁特性。本工作生长了Tb2 Fe17和以Si部分替代Fe的Tb2 Fe17-xSix(x =1 ,2 ,3)的单晶 ,并研究了单晶的磁性和该化合物的相图。实验发现 ,该材料单晶生长的择优方向为其基本结构 ,六方T... R2 Fe17(R为稀土 )是一大类稀土金属间化合物 ,具有硬磁特性。本工作生长了Tb2 Fe17和以Si部分替代Fe的Tb2 Fe17-xSix(x =1 ,2 ,3)的单晶 ,并研究了单晶的磁性和该化合物的相图。实验发现 ,该材料单晶生长的择优方向为其基本结构 ,六方Th2 Ni17的c轴方向 ,有Si替代和无Si替代均能同成分生长。这一结果与最新版本所载的Tb Fe二元相图中Tb2 Fe17为强烈的包晶反应是不一致的。为此做了Tb2 Fe17成分附近各种成分的差热分析。证明了这一化合物的同成分熔化性质 ,确定了其熔点和附近的一个共晶点 ,修正了以往的相图。物性研究发现 ,当Si替代Fe达到x =3时 ,化合物结构出现基本的Th2 Ni17和另一种三角结构Th2 Zn17的混合。化合物的居里温度随Si含量增加而上升。Si的替代产生了低温下c轴方向的矫顽力 ,认为是Si取代Fe位引起的能垒变化对磁畴的钉扎所致。在无Si替代的单晶样品中 ,难磁化的c轴样品出现一级磁化过程 (FOMP) ,其起始磁场为 2 .5T ,比以往报道的 3.5T降低很多 ,表明较高的完整性和较低的缺陷密度降低了磁畴的钉扎势垒。 展开更多
关键词 磁性晶体 Tb_2fe_(17)晶体 Tb_2(fe Si)_(17)晶体 相图
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富铁低锆Sm_(2)Co_(17)型烧结永磁材料磁性能提升机理研究
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作者 王帅 雍辉 +2 位作者 韩婷 朱亚武 胡季帆 《功能材料》 CAS CSCD 北大核心 2023年第1期1202-1207,共6页
高磁能积Sm_(2)Co_(17)型烧结永磁体的磁性能和其合金成分及微观结构密切相关。通过调整Fe、Zr含量,优化微观结构,使磁体最大磁能积(BH)_(max)和内禀矫顽力H_(cj)得到了同步提升。采用PFM、EPMA、TEM等先进的分析测试方法,研究了微观结... 高磁能积Sm_(2)Co_(17)型烧结永磁体的磁性能和其合金成分及微观结构密切相关。通过调整Fe、Zr含量,优化微观结构,使磁体最大磁能积(BH)_(max)和内禀矫顽力H_(cj)得到了同步提升。采用PFM、EPMA、TEM等先进的分析测试方法,研究了微观结构对磁体磁性能的影响。研究表明,随着Fe含量由15%增加到19%,Zr含量由3%降低到2.6%(质量分数),磁体剩磁B r由1.07 T增加到1.13 T,(BH)_(max)也由217.15 kJ/m^(3)增加到241.19 kJ/m^(3),同时,磁体H_(cj)也得到一定提高,由2641.13 kA/m增加到2774.86 kA/m。通过提高Fe含量,降低Zr含量,可以使磁体内避免生成块状富Zr相,提高磁体B r和(BH)_(max)。当Fe含量为19%(质量分数),Zr含量为2.6%(质量分数)时,磁体获得了较大尺寸的胞组织,胞壁处有较高的峰值Cu浓度(26.9%(质量分数)),这是磁体H_(cj)同时提高的主要原因。 展开更多
关键词 sm_(2)Co_(17)型永磁材料 微观结构 fe含量 内禀矫顽力 磁性能
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高性能Sm_(2)Co_(17)型烧结永磁体的制备及微结构研究
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作者 王帅 雍辉 +3 位作者 侯卫宵 马江微 崔燕 王志成 《太原科技大学学报》 2023年第3期258-262,共5页
高性能2∶17型SmCo永磁体的磁性能和其微结构密切相关。通过优化Cu含量以及微结构制备出最大磁能积((BH)_(max))为32.88MGOe的高性能SmCo永磁体,并且磁体具有较高内禀矫顽力(H_(cj)).研究了磁体内禀矫顽力和微结构的关联。研究表明,随... 高性能2∶17型SmCo永磁体的磁性能和其微结构密切相关。通过优化Cu含量以及微结构制备出最大磁能积((BH)_(max))为32.88MGOe的高性能SmCo永磁体,并且磁体具有较高内禀矫顽力(H_(cj)).研究了磁体内禀矫顽力和微结构的关联。研究表明,随着Cu含量增加,磁体剩磁B r逐渐减小,H cj逐渐增大。Cu含量对Sm(Co_(bal)Cu_(x)Fe_(0.285)Zr_(0.023))7.6(x=0.051、0.062、0.073)磁体胞尺寸和片状相密度几乎没有影响,但随着Cu含量由0.051增加到0.073,胞壁处峰值Cu浓度明显增大,这是磁体内禀矫顽力增强的主要原因。 展开更多
关键词 sm_(2)Co_(17)型烧结永磁体 CU含量 微观结构 磁性能
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Microwave absorption properties regulation and bandwidth formula of oriented Y_(2)Fe_(17)N_(3-δ)@SiO_(2)/PU composite synthesized by reduction-diffusion method 被引量:1
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作者 Hao Wang Liang Qiao +4 位作者 Zu-Ying Zheng Hong-Bo Hao Tao Wang Zheng Yang Fa-Shen Li 《Chinese Physics B》 SCIE EI CAS CSCD 2022年第11期341-351,共11页
As concepts closely related to microwave absorption properties,impedance matching and phase matching were rarely combined with material parameters to regulate properties and explore related mechanisms.In this work,red... As concepts closely related to microwave absorption properties,impedance matching and phase matching were rarely combined with material parameters to regulate properties and explore related mechanisms.In this work,reduction–diffusion method was innovatively applied to synthesize rare earth alloy Y_(2)Fe_(17).In order to regulate the electromagnetic parameters of absorbers,the Y_(2)Fe_(17)N_(3-δ)particles were coated with silica(Y_(2)Fe_(17)N_(3-δ)@SiO_(2))and absorbers with different volume fractions were prepared.The relationship between impedance matching,matching thickness,and the strongest reflection loss peak(RLmin)was presented obviously.Compared to the microwave absorption properties of Y_(2)Fe_(17)N_(3-δ)/PU absorber,Y_(2)Fe_(17)N_(3-δ)@SiO_(2)/PU absorbers are more conducive to the realization of microwave absorption material standards which are thin thickness,light weight,strong absorbing intensity,and broad bandwidth.Based on microwave frequency bands,the microwave absorption properties of the absorbers were analyzed and the related parameters were listed.As an important parameter related to perfect matching,reflection factor(√ε_(r)/μ_(r))was discussed combined with microwave amplitude attenuation.According to the origin and mathematical model of bandwidth,the formula of EAB(RL<-10 dB)was derived and simplified.The calculated bandwidths agreed well with experimental results. 展开更多
关键词 microwave absorption rare earth alloy reduction-diffusion method Y_(2)fe_(17)N_(3-δ)@SiO_(2) reflection factor impedance and phase matching bandwidth formula
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Effect of spin-reorientation transition of cell boundary phases on the temperature dependence of magnetization and coercivity in Sm_(2)Co_(17) magnets
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作者 涂思思 刘雷 +6 位作者 周波 董创辉 叶力铭 孙颖莉 丁勇 闫阿儒 毛信表 《Chinese Physics B》 SCIE EI CAS CSCD 2023年第12期541-546,共6页
Four Sm_(2)Co_(17)magnets with spin-reorientation transition(SRT)of cell boundary phases(CBPs)are prepared by liquid-phase sintering.The temperature of the SRT of CBPs(T_(SR)^(1:5))is regulated from 125 K to 195 K by ... Four Sm_(2)Co_(17)magnets with spin-reorientation transition(SRT)of cell boundary phases(CBPs)are prepared by liquid-phase sintering.The temperature of the SRT of CBPs(T_(SR)^(1:5))is regulated from 125 K to 195 K by adding 0 wt.%,3 wt.%,6 wt.%and 9 wt.%Dy_(88)Cu_(12)alloy powder.The effect of SRT of Sm_(2)Co_(17)magnet CBPs on the temperature dependence of the magnetization(M-T)and coercivity(H-T)is systematically investigated.The temperature dependence of the magnetization is influenced by the SRT of CBPs.The M-T curves measured during the heating process are larger than those measured during the cooling process when T<T_(SR)^(1:5).When T=T_(SR)^(1:5)there is a bifurcation point.When T>T_(SR)^(1:5)the M-T curves overlap and the M-T derivation curve shows that the magnetization of the magnet has low temperature dependence of magnetization above T_(SR)^(1:5).With increasing T_(SR)^(1:5),the initial temperature of the low temperature dependence of magnetization shifts towards a higher temperature.The coercivity temperature coefficient becomes positive as the SRT effect increases,and the temperature range of the positive coercivity temperature coefficient moves towards higher temperatures as T_(SR)^(1:5)increases.This reveals that SRT of CBPs has little effect on the temperature dependence of magnetization above T_(SR)^(1:5),while the temperature dependence of coercivity is optimized.The temperature range of magnetization and coercivity with low temperature dependence tends towards higher temperatures,which is conducive to the preparation of magnets with a low temperature coefficient at higher temperatures. 展开更多
关键词 spin-reorientation transformation low-temperature coefficient sm_(2)Co_(17)magnets
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Study on the Easy Direction of Magnetization of Sm_(0.88)Dy_(0.12)Fe_2 Alloy
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作者 朱明源 张慧友 +3 位作者 诸于良 金红明 金慧娟 许桂琴 《Journal of Rare Earths》 SCIE EI CAS CSCD 1996年第3期185-188,共4页
By Mossbauer-effect, the changes of easy direction of magnetization for Sm0.88Dy0.12.Fe2 alloy have been studied in this paper. It was found that as temperature increases, the easy direction of magnetization changes... By Mossbauer-effect, the changes of easy direction of magnetization for Sm0.88Dy0.12.Fe2 alloy have been studied in this paper. It was found that as temperature increases, the easy direction of magnetization changes gradually from [110] to [111] axis in the temperature range of 153 to 213 K. Two easy directions of magnetization [110] and [111] coexist and do not change suddenly from [110] to [111] at the same temperature. 展开更多
关键词 sm_(0. 88)Dy_(0. 12)fe_2 alloy Easy direction of magnetization Magnetostriction M sshauer-effect
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Synthesis of size-controlled and dispersible Sm_(2)Fe_(17)N_(3) magnetic particles by reduction diffusion process using molten salt
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作者 Junhua Xi Zhi Yang +8 位作者 Muhammad Haseeb Yuanyuan Chen Xiaofeng Nie Liying Cong Qiong Wu Enfeng Fu Hongguo Zhang Weiqiang Liu Ming Yue 《Journal of Rare Earths》 SCIE EI CAS CSCD 2024年第11期2105-2111,I0004,共8页
The synthesis of size-controlled Sm_(2)Fe_(17) magnetic particles is a prerequisite for the fabrication of highperformance Sm_(2)Fe_(17)N_(3) permanent magnetic materials.Here,Sm_(2)Fe_(17) was synthesized using a cos... The synthesis of size-controlled Sm_(2)Fe_(17) magnetic particles is a prerequisite for the fabrication of highperformance Sm_(2)Fe_(17)N_(3) permanent magnetic materials.Here,Sm_(2)Fe_(17) was synthesized using a costeffective reduction-diffusion method.The calcium chloride molten salt was introduced to control the particle size and achieve a single phase of Sm_(2)Fe_(17).The effects of reduction-diffusion reaction temperature and the amount of added calcium chloride on the phase constitution and microstructure of the final product of reduction-diffusion were systematically investigated.Adding an appropriate amount of calcium chloride can effectively inhibit the overgrowth and sintering of the reduced particles.By employing the strategy of adding 20 wt% of calcium chlorides into the green compacts,we were able to successfully synthesize uniform Sm_(2)Fe_(17) particles that are well-dispersed,with an average size of 2.2 μm.Furthermore,by combining the optimal reduction-diffusion conditions and the nitriding process,the hard magnetic Sm_(2)Fe_(17)N_(3) material was successfully obtained.This study could be useful for the development of high-performance Sm_(2)Fe_(17)N_(3) magnetic materials utilizing reduction-diffusion technology. 展开更多
关键词 sm_(2)fe_(17)N_(3) Reduction-diffusion Rare earths Permanent magnets Molten salt
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Significant effect of ordered micro-domain on cell boundary phase distribution and demagnetization curve squareness of Sm_(2)Co_(17)-type magnet
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作者 Zhuang Liu Hai-Chen Wu +5 位作者 Chao-Yue Zhang Chao-Qun Zhu Guo-Xin Chen Huan-Ming Lu Ren-Jie Chen Aru Yan 《Rare Metals》 SCIE EI CAS CSCD 2024年第4期1724-1735,共12页
Cu-rich cell boundary phase is difficult to precipitate evenly,resulting in a generally poor demagnetization curve squareness for Fe-rich Sm_(2)Co_(17)-type magnet,which is a key factor limiting the further improvemen... Cu-rich cell boundary phase is difficult to precipitate evenly,resulting in a generally poor demagnetization curve squareness for Fe-rich Sm_(2)Co_(17)-type magnet,which is a key factor limiting the further improvement of magnetic energy product.In this study,we report that nanoscale strip-like ordered micro-domains distributed in1:7H disordered matrix phase of the solid solution precursor is a new factor significantly affecting the precipitation and distribution of the cell boundary phase.Long strip-like and continuous micro-twin structure with twin boundaries neatly perpendicular to the C-axis is observed after sintering treatment.After solution treatment,sequential and long strip-like micro-twins gradually transform into disordered state along the basal plane,forming narrow disordered 1:7H(TbCu_(7)-type structure)phase between the separated strip-like ordered micro-domains.This disordering transformation takes place via broken down of the long strip-like ordered micro-domains,which is accomplished by narrowing along the width direction followed by reduction of the length.Furthermore,a new model revealing the effect of the ordered micro-domains on the formation of the cell boundary phase is proposed.Antiphase boundaries enriched in Cu have already existed in the precursor with long strip-like ordered micro-domains.Therefore,the Cu-rich cell boundary phase acting as strong pinning centers cannot be precipitated homogeneously and distributed continuously after aging,resulting in a poor demagnetization curve squareness of Sm_(2)Co_(17)-type magnet.Our results indicate that significant broken down of the nanoscale ordered micro-domains in solution precursor is the key factor improving the distribution of cell boundary phase in Sm_(2)Co_(17)-type magnets. 展开更多
关键词 sm_(2)Co_(17) magnets Solution precursor Ordered micro-domains Disordering transformation Cellular structure
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Optimizing temperature coefficient of Sm_(2)Co_(17)-type magnets through adjusting the isothermal aging process
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作者 Chao Wang Die Hu +8 位作者 Qiangfeng Li Yikun Fang Meng Zheng Lei Wang Hongsheng Chen Lei Zhao Haizhou Wang Minggang Zhu Wei Li 《Journal of Rare Earths》 SCIE EI CAS CSCD 2024年第11期2097-2104,I0004,共9页
The high-temperature magnetic perfo rmance and micro structure of Sm_(1-x)Gd_(x)(Co_(bal)Fe_(0.09)Cu_(0.09)Zr_(0.025))_(7.2)(x=0.3,0.5) magnets were investigated.With the isothermal aging time decreasing from 11 to 3 ... The high-temperature magnetic perfo rmance and micro structure of Sm_(1-x)Gd_(x)(Co_(bal)Fe_(0.09)Cu_(0.09)Zr_(0.025))_(7.2)(x=0.3,0.5) magnets were investigated.With the isothermal aging time decreasing from 11 to 3 h,the temperature coefficient of intrinsic coercivity in the temperature range of 25-500℃,β_(25-500℃),was optimized from -0,167%/℃ to-0.112%/℃ for x=0.3 magnets.The noticeable enhancement(~33%) of temperature stability is correlated with the increased content of 1:5H cell boundary phase and its relatively high Curie temperature as well.However,for the x=0.5 magnet,it is found that the presence of Sm_(5)Co_(19) phases and wider nanotwin variants hinder the formation of 1:5H cell boundary phase.The insufficient 1:5H is not beneficial to the proper redistribution of Cu in cell boundary,making the x=0.5 magnet difficult to achieve higher temperature stability.Consequently,the approach of adjusting the isothermal aging process can offer guidance for attaining superior magnetic performance in the temperature range from 25 to 500℃ for Gd-substituted Sm_(2)Co_(17)-type magnets. 展开更多
关键词 Rare earths sm_(2)Co_(17)-type magnets Isothermal aging process Temperature coefficient of intrinsic coercivity
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高性能Sm_(2)Fe_(17)N_(x)粉体制备的研究进展
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作者 何颖 李超群 +6 位作者 陈小立 龙芝梅 赖嘉琪 邵斌 马毅龙 陈登明 董季玲 《材料研究学报》 EI CAS CSCD 北大核心 2022年第5期321-331,共11页
新能源汽车的高速发展,需要能稳定工作在120℃~200℃温度区间的永磁材料。居里温度为476℃、各向异性场为14.7 T的Sm_(2)Fe_(17)N_(3),具有优良的本征磁性能,可应用在这个温度区间。为了提高Sm_(2)Fe_(17)N_(3)粉体的磁性能,必须将颗粒... 新能源汽车的高速发展,需要能稳定工作在120℃~200℃温度区间的永磁材料。居里温度为476℃、各向异性场为14.7 T的Sm_(2)Fe_(17)N_(3),具有优良的本征磁性能,可应用在这个温度区间。为了提高Sm_(2)Fe_(17)N_(3)粉体的磁性能,必须将颗粒的粒径减小到临界单畴尺寸以实现高各向异性场;同时,还要避免颗粒尺寸减小产生的表面氧化,以保证高剩磁和最大磁能积。粉体破碎、机械合金化、甩带、薄带连铸、还原扩散以及表面镀覆等多种制备工艺,可用于制备高性能Sm_(2)Fe_(17)N_(3)。目前,实验室制备的Sm_(2)Fe_(17)N_(3)粉体的矫顽力和最大磁能积已经达到28.1 kOe和43.6 MGOe。本文评述近年来Sm_(2)Fe_(17)N_(3)粉体制备的研究成果,包括对制备机理的系统总结并提出仍待解决的关键问题:Sm_(2)Fe_(17)N_(3)粉体的矫顽力、剩磁等与其颗粒尺寸的量化规律以及与颗粒磁畴结构的关联机制;对NH_(3)/H_(2)混合气体中H_(2)对提高氮化效率的作用机制仍需探索;进一步开发在低氧环境下的颗粒粒径均匀化、控制形貌的二次破碎技术;对于还原扩散法,开发适合规模化应用的新前驱体及其制备方法以及快速去除钙副产物的水洗技术等。 展开更多
关键词 评述 金属材料 sm_(2)fe_(17)N_(x) 永磁 制备方法
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Preparation of Sm_2Fe_(17) alloy by reduction-diffusion process 被引量:2
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作者 Hai-Bo Chen Jing-Wu Zheng +3 位作者 Liang Qiao Yao Ying Li-Qiang Jiang Sheng-Lei Che 《Rare Metals》 SCIE EI CAS CSCD 2018年第11期989-994,共6页
SmFealloy is the intermediate material for the preparation of SmFeNx(x ≈ 3); thus, the synthesis of pure SmFemother alloy is the key to obtaining highperformance SmFeNx. Reduction-diffusion(R-D) is a cost-effective m... SmFealloy is the intermediate material for the preparation of SmFeNx(x ≈ 3); thus, the synthesis of pure SmFemother alloy is the key to obtaining highperformance SmFeNx. Reduction-diffusion(R-D) is a cost-effective method. In this study, the R-D process of synthesizing SmFewas analyzed by scanning electron microscopy(SEM), energy-dispersive X-ray spectroscopy(EDX), X-ray diffraction(XRD), and X-ray fluorescence(XRF). Furthermore, the influences of the tightness of compacted reactants, the compensation amount of SmO,and the particle size of Fe on the formation of SmFewere discussed from the aspects of the three raw materials.The results show that Sm reduced from SmOreacts with Fe particles to form intermetallic compound SmFedirectly in the R-D reaction process of preparing SmFe;the generation of Sm and its migration to the surface of Fe particles control the reaction rate; a proper tightness of compacted reactants is necessary for ensuring the purity of SmFeproduct; pure SmFecan be obtained when the compensation of SmOis 33 % of the stoichiometry; and the sufficiency of the reaction improves with the decrease in the size of Fe powders under the same reaction condition. 展开更多
关键词 sm_2fe_(17) Reduction-diffusion Rare earth Permanent magnet
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熔盐电解法制备单一Sm_(2)Fe_(17)合金相的机制研究
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作者 任梦 刘玥池 闫奇操 《稀有金属材料与工程》 SCIE EI CAS CSCD 北大核心 2023年第6期2220-2226,共7页
选择在LiF-CaF_(2)-SmF3熔盐体系中,采用熔盐电解法在1160℃下通过恒电流在Fe阴极表面获得了不同厚度(17.22~40.34μm)的Sm_(2)Fe_(17)合金层,同时通过循环伏安法与方波伏安法研究了Sm^(3+)在W与Fe阴极上的电化学行为。结果表明,Sm^(3+... 选择在LiF-CaF_(2)-SmF3熔盐体系中,采用熔盐电解法在1160℃下通过恒电流在Fe阴极表面获得了不同厚度(17.22~40.34μm)的Sm_(2)Fe_(17)合金层,同时通过循环伏安法与方波伏安法研究了Sm^(3+)在W与Fe阴极上的电化学行为。结果表明,Sm^(3+)无法单独沉积于W电极上,Sm^(3+)在铁阴极上的还原为Sm^(0)分为2步,首先在-0.33V(vs.Cr/Cr_(2)O_(3))发生Sm^(3+)还原为Sm^(2+)的可溶-可溶型反应,然后当电极电势超过-0.78V(vs.Cr/Cr_(2)O_(3))时Sm^(2+)开始在阴极界面处上发生欠电势还原,在Fe电极表面生成Sm_(2)Fe_(17)合金,这是由于在Sm_(2)Fe_(17)合金中降低了Sm元素的活度,使钐元素在Sm-Fe合金中更加稳定。 展开更多
关键词 熔盐电解法 sm_(2)fe_(17) LiF-CaF_(2) 计时电势法 预电解
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钙热还原制备Sm_(2)Co_(17)合金及磁性能研究
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作者 刘东辉 张小林 +1 位作者 牛飞 杨幼明 《稀土》 CAS CSCD 北大核心 2023年第4期202-213,I0007,共13页
钙作为还原剂无法直接还原SmF_(3)制备金属钐。本文以无水SmF_(3)为原料,对钴诱导SmF_(3)钙热还原制备Sm_(2)Co_(17)合金进行了热力学计算与实验研究。通过电感耦合等离子体光谱仪、X射线衍射仪、扫描电子显微镜及能谱仪和X射线光电子... 钙作为还原剂无法直接还原SmF_(3)制备金属钐。本文以无水SmF_(3)为原料,对钴诱导SmF_(3)钙热还原制备Sm_(2)Co_(17)合金进行了热力学计算与实验研究。通过电感耦合等离子体光谱仪、X射线衍射仪、扫描电子显微镜及能谱仪和X射线光电子能谱仪等测试方法对合金产物的化学组成、结构、形貌、元素分布和化学价态等进行了分析与表征。结果表明:钴诱导SmF_(3)钙热还原制备Sm_(2)Co_(17)合金在热力学上是可行的,还原产物为Sm_(2)Co_(17)合金与CaF_(2)。当SmF_(3)与Ca用量分别为摩尔比1.1与1.2,保温时间30 s时,获得合金产物中钐质量分数为22.98%,与Sm_(2)Co_(17)合金的理论成分几乎相同。铸态合金产物主要由Th_(2)Zn_(17)结构的2∶17相及CaCu_(5)结构的1∶5相组成。结合电负性原理与XPS分析结果研究了制备Sm_(2)Co_(17)合金的钴诱导机理。Sm_(2)Co_(17)合金快淬带的剩余磁化强度为0.47 T,内禀矫顽力为0.45 kA·m^(-1),最大磁能积为5.23 kJ·m^(-3)。与传统混熔工艺相比,此工艺在每生产一吨Sm_(2)Co_(17)合金中,金属钐制备成本节省约40%。该方法制备的钐钴合金可作为烧结稀土钐钴永磁材料的原料。 展开更多
关键词 氟化钐 sm_(2)Co_(17) 钙热还原 诱导机理 磁性能
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