Crystallization Behavior and Magnetic Properties of （Fe0.6Co0.4）86Hf7B6Cu1 Alloy

(Fe0.6Co0.4)86HfTB6Cu1 nanocrystalline alloy obtained in isothermal annealing process from amorphous precursor was investigated as candidate of soft magnetic materials for high temperature applications. Co substitution for Fe can enhance the curie temperature of amorphous alloy (Tc = 630℃) and improve the magnetization of nanocrystalline alloy at high temperature ( ≈ 1.56T at 550℃). After annealing amorphous precursor at 550℃ for 1 hour, the optimum nanocrystalline alloy can be obtained which shows the local minimum coercivity ( ≈ 16 A/m). The coercivity increases with the increase of annealing temperature corresponding to the formation of ferromagnetic phase in the secondary crystallization. Furthermore, additions of Hf and B elements reduce the melting temperature of the alloy studied comparing with the Fe-Co binary alloy.     

金属间化物Nd(Fe_(1-x)Co_x)_(10)V_2的磁性能机制

通过X射线衍射.磁测量和M(?)ssbauer谱测定了Nd（Fe1-Cox）10V2的结构和磁性.结果表明,Nd（Fe1-xCox）10V2（x=0,0.05,0.10,0.15,0.20）化合物的晶体结构均为ThMn12型结构;随着 Co含量x的增大,晶格常数将单调减少.Co原子的替代将导致化合物各个Fe晶位上的磁超精细场值Bhf逐渐增加.Co部分取代Nd（Fe1-xCox）10V2中的Fe原子时.将择优占据8i铁晶位.取向样品NdFe10V2的热磁曲线和变温M(?)ssbauer谱研究结果表明.该化合物在T=120K条件下存在自旋重取向现象.     

Nd(Fe_(1-x)Co_x)_(10)V_2的Mssbauer谱

通过X射线衍射、磁测量和M ssbauer谱等测试方法研究了Nd(Fe1-xCox) 10 V2 的结构和磁性。结果表明 :Nd(Fe1-xCox) 10 V2 (x =0 ,0 .0 5 ,0 .1,0 .15 ,0 .2 )化合物的晶体结构均为ThMn12 型结构 ;随着Co含量增大 ,晶格常数将单调减少 ,居里温度Tc 呈单调增大 ,饱和磁化强度Ms 逐渐增加。Co部分取代Nd(Fe1-xCox) 10 V2 中的Fe原子 ,将择优占据 8i铁晶位。     

预退火对纳米晶Fe86Zr7B6Cu1合金显微组织和软磁性能的影响

研究在常规退火前的高温短时间预退火对非晶Fe86Zr7B6Cu1合金晶化过程的影响,通过分析温度对形核速率和晶粒长大速率的影响规律,讨论预退火对非晶Fe86Zr7B6Cu1合金晶化过程的影响机制。结果表明,合适的预退火引起纳米晶Fe86Zr7B6Cu1合金中结晶α-Fe相的晶粒尺寸的减小和体积分数的增加。非晶Fe86Zr7B6Cu1合金经600℃退火1 h后的结晶α-Fe相的晶粒尺寸和体积分数分别为13.2 nm和65.2%,而在750℃保温2 min再在600℃退火1 h后的结晶α-Fe相的晶粒尺寸和体积分数分别为9.5 nm和72.4%。在750℃保温2 min再在600℃退火1 h后的试样比常规退火得到的试样具有更为优良的软磁性能。     

Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9非晶合金的晶化动力学

用差热分析(DTA)结合X射线衍射(XRD),研究了Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9非晶合金的晶化动力学。结果表明:温度在0～700℃范围内,该合金的晶化相为α-Fe和Fe_2B;α-Fe相晶化表观激活能为452.39kJ/mol,Fe_2B相的晶化表观激活能395.23kJ/mol;两相在晶化初期激活能最小,随晶化量X_c的增加而迅速增大,在α-Fe的体积分数为30％～80％,Fe_2B的体积分数为40％～80％时,呈现极大值。     

Crystallization Behavior and Magnetic Properties of (Fe_(o.6)Co_(0.4))_(86)Hf_7B_6Cu_1 Alloy

MORE RECENTLY,it was found that Co substitutionfor Fe in Fe-M-B-Cu(M=Nb,Hf or Zr)alloys canimprove the magnetic properties at high temperature byincreasing the Curie temperature of amorphous phase.Attributed to the exchange coupling ofnanocrystal-amorphous-nanocrystal,the magneticanisotropy can be averaged over many grains andorientations when the grain size is smaller than theexchange coherence length,resulting in a greatlyreduced coercivity.But when the temperature is higherthan the …     

Zr含量对Al3(ZrxEr1-x)相价电子结构与合金性能的影响

用固体与分子经验电子理论(EET)计算研究了微量元素Er,Zr添加到铝合金中产生的Al3Er和Al(ZrIxEr1-x)相的价电子结构,探讨了不同Zr含量对Al3(ZrxFr1-x)相各电子结构参数的影响.计算结果表明:随着Zr原子含量的增加,表征强度性能的最强键上的共价电子对数na和相结构形成因子S会减小,这说明合金...     

La_(0.6)Pr_(0.4)Fe_(11.4)Si_(1.6)B_(0.2)合金及其氢化物磁热性能研究

采用工业纯原料感应熔炼制备出公斤级La_(0.6)Pr_(0.4)Fe_(11.4)Si_(1.6)B_(0.2)合金,经退火后通过吸氢处理提高其居里温度到室温附近。研究了在1373~1473 K温度下经不同时间和温度退火对合金微观组织结构的影响。实验发现在1473 K经30 h退火样品的居里温度为202 K,在0~1.5 T变化磁场下的最大磁熵变达8.1~8.6 J/kg·K。在0.13 MPa氢气压力下,经553 K吸氢5 h氢化处理合金的居里温度为320 K,最大磁熵变达7.7~8.0 J/kg·K。     

(Fe_(1-x)Co_x)_(80)Zr_(10)B_(10)(x=0,0.1,0.2,0.3)合金的热性能、结构和磁性能研究

采用单辊快淬法制备(Fe1-x Cox)80Zr10B10(x=0,0.1,0.2,0.3)非晶合金,并对4种合金在不同温度下进行等温热处理。利用差热分析仪(DTA),X射线衍射仪(XRD),透射电镜(TEM)和振动样品磁强计(VSM)等测试手段对样品的热性能、微观结构及磁性能进行研究。结果表明,未添加Co元素的Fe80Zr10B10合金的热稳定性明显高于添加Co元素的合金,而(Fe1-x Cox)80Zr10B10(x=0.1,0.2,0.3)合金的热稳定性相差不大。Fe80Zr10B10和Fe72Co8Zr10B10合金的晶化过程相似;Fe64Co16Zr10B10和Fe56Co24Zr10B10合金的晶化过程相似。4种合金的矫顽力(Hc)呈现先上升后下降的趋势,在873 K达到最大值。     

Tb_xDy_(1-x)(Fe_(0.6)Co_(0.4))_2合金的磁性和磁致伸缩性能

利用电弧熔炼法制备Tb_xDy_(1-x)(Fe_(0.6)Co_(0.4))_2合金(0.27≤x≤0.40),对合金的磁性和磁致伸缩性能进行研究。利用XRD、交流初始磁化率测试仪、超导量子干涉仪和标准应变测试仪,对样品的物相组成、居里温度、磁化曲线和磁致伸缩性能进行表征。结果表明:当x≤0.27时合金的易磁化方向为á100?方向,当x≥0.30时合金的易磁化方向变为〈 111〉方向;合金的居里温度随x的增加而增加;x=0.32附近时合金的磁晶各向异性常数K_1有极小值,室温时合金在x=0.32附近时达到各向异性补偿;当x=0.32时饱和磁致伸缩系数达到9.57×10~(-4);随Co含量的增加,合金的各向异性补偿点向Tb含量高的方向移动。Tb_(0.32)Dy_(0.68)(Fe_(0.6)Co(0.4))_2合金具有高磁致伸缩系数和低各向异性,是一种实用的磁致伸缩候选材料。     

磁致Fe78Si9B13非晶合金纳米晶化磁矩的理论计算

用低频脉冲磁场处理非晶Fe78Si9B13合金,在低温下发生了纳米晶化,利用M?ssbauer谱和LDJ9600震动样品磁强计进行了微结构和磁性分析.借助于固体与分子经验电子理论中的BLD方法,计算了非晶Fe78Si9B13合金磁致低温纳米晶化前后的价电子结构,并算出了磁矩,其理论计算值与实验测定值的误差小于7%,满足一级近似要求,说明从价电子层次上计算非晶合金的磁矩是可以实现的.     

Influence of low-temperature nitridation on low-frequency magnetization of Fe82Nb7B10Cu1 nanocrystalline alloy ribbons

The nanocrystaUine Fe82Nb7B10Cu1 soft magnetic ribbons were treated with the mixture gas flow of ammonia and hydrogen at 673 K. The influence of the nitridation treatment was studied by the low-frequency permeability spectra. The result shows that this kind ofnitridation treatment can improve the soft magnetic properties under some application conditions. The reason for the improvement of the soft magnetic properties by slight nitridation was discussed on the basis of domain wall bulging model. Therefore for the Fe-based nanocrystalline soft magnetic alloy ribbons, the nitridation treatment can be used as an effective and easy method to control the magnetic properties.     

快速凝固（Sm1—xBx）Fe2合金的结构和磁性

采用真空单辊快淬法（铜辊,线速度达２０～２３ｍ／ｓ）将成分为（Ｓｍ１－ｘＢｘ）Ｆｅ２（ｘ＝０,０．０１５,０．０３,０．０４５,０．０６）合金锭,制成快速凝固的鳞片状合金,再经粉碎在３０ＭＰａ压力下,模压成φ１０ｍｍ圆片,然后进行ＸＲＤ分析,比磁化强度和磁致伸缩（λ″－λ┴）的测量。实验结果表明各样品只有少量非晶相,主要是ＳｍＦｅ２及少量的ＳｍＦｅ５和ＳｍＦｅ７化合物。样品（Ｓｍ０．９８５Ｂ０．０１５）Ｆｅ２和（Ｓｍ０．９４Ｂ０．０６）Ｆｅ２,在７２０ｋＡ／ｍ磁场下,比磁化强度分别为：５９．５,５２．３Ａｍ２ｋｇ－１,在８８５ｋＡ／ｍ磁场下（λ″－λ┴）分别为：－５１０×１０－６和－３１０×１０－６。     

Nd7．5Fe85．9Nb0.25Dy0．75B5．5Cu0．1非晶合金中Nd2Fe14B相的晶化动力学

利用差示扫描热分析法（DSC）研究了非晶Nd7．5Fe85．9Nb0.25Dy0．75B5．5Cu0．1合金中Nd2Fe14B相的晶化动力学。结果表明：当非晶合金以10℃／min升温时,Nd2Fe14B的晶化峰值温度为697.93℃,晶化初期Nd2Fe14B相的晶化激活能为372．17kJ／mol,随其晶化体积分数的增加,晶化激活能逐渐减小。     

(Fe1-xCox)84Zr3.5Nb3.5B8Cu1非晶合金的高温和低温磁性

用磁天平（MB）及提拉样品磁强计（ESM）研究了（Fe1-xCox）84Zr3.5Nb3.5B8Cu1（x＝0－0．8）非晶合金高温与低温磁性的变化，结果表明，该非晶态合金加热到800－900℃后，除x＝0．8的合金外，，合金的室温饱和磁化强度均比淬态有所提高；X射线衍射的结果表明，x＝0，0．2，0．4，0．6的合金中析出单一的a-Fe（Co）相，x＝0．8的合金中析出Co3B，FeB相，当x＝1．0时合金中析出单一的fccCo相。该非晶合金在1．5K时的饱和磁化强度σs随Co含量的增加先增大，当x＝0．2时达到最大值，然后随着x的增大，合金的σs逐渐下降。     

Fe- and co-based nanocrystalline soft magnetic alloys modified with Hf, Mo, and Zr: Magnetic properties, thermal stability, and structure. Alloys (Fe0.6Co0.4)86Hf7B6Cu1 and (Fe0.7Co0.3)88Hf7B4Cu1

Nanocrystalline alloys (Fe_0.6Co_0.4)₈₆Hf₇B₆Cu₁ and (Fe_0.7Co_0.3)₈₈Hf₇B₄Cu₁ have been investigated to obtain materials with improved thermal stability and new features. In order to make the alloys produced by melt quenching on a rotating wheel nanocrystalline, they have been subjected to heat (HT) and thermomechanical (TMechT) treatments. The effect of HT and TMechT conditions on the magnetic properties, thermal stability, and structure of the alloys has been studied. The optimal HT conditions for obtaining the minimum values of the coercive force (H _c) in the alloys have been determined. It is shown that TMechT of the alloys leads to the induced longitudinal magnetic anisotropy with the axis of easy magnetization along the long side of the ribbon in the studied temperature range of 520–620°C. It has been established that the alloys (Fe_0.6Co_0.4)₈₆Hf₇B₆Cu₁ and (Fe_0.7Co_0.3)₈₈Hf₇B₄Cu₁ are thermally unstable at temperatures above 500°C.     

Crystallization process and soft magnetic properties of nanocrystalline (Fe0.5 Co0.5 ) 86 Hf7 B6 Cu1 alloy used in elevated temperature applications

Nanocrystalline (Fe0.5 Co0.5 )86 Hf7 B6 Cu1 HITPERM alloy was investigated as the candidate of soft magnetic material for high temperature applications, compared with Fe86 Hf7B6 Cu1 NANOPERM alloy. Amorphous alloy ribbons were prepared by single-roller melt-spinning technology. Crystallization process of as-quenched ribbon was investigated using differential scanning calorimeter at different heating rates. The coercivity was determined from quasi-static hysteresis loop measured at room temperature using a computerized hysteresis loop tracer. X-ray diffraction with Cu Kα radiation was used to determine the structure. The vibrating sample magnetometer was usedto measure the magnetization as a function of temperature of the nanocrystllized alloys. That Co substitution for Fein alloy enhances the Curie temperature of amorphous alloy and the magnetization of nanocrystalline alloy at hightemperature. After annealing amorphous precursor, the optimum nanocrystalline alloy obtained shows the local minimum coercivity. The coercivity increases with the increasing annealing temperature corresponding to the formation of ferromagnetic phase in the secondary crystallization.