Tb对Fe81Ga19快淬合金薄带组织和磁致伸缩性能的影响

利用快淬甩带方法制备了Fe81Ga19Tbx(x=0,0.2,0.4,0.6)合金薄带,研究了合金薄带的显微组织结构和磁致伸缩性能。实验结果表明,Fe-Ga-Tb合金薄带的显微组织及磁致伸缩性能与合金的成分密切相关,合金薄带基体为Fe(Ga)无序固溶相体。Fe81Ga19Tb0.2合金的磁致伸缩系数最大,达到-1320×10-6,且薄带厚度方向[100]择优取向,Tb在晶界处富集。     

Al/Tb_(0.30)Dy_(0.70)Fe_(1.95)复合材料的制备与性能研究

采用真空粉末烧结法,制备了Al/Tb0.30Dy0.70Fe1.95复合材料,研究了该复合材料的物相、组织结构以及磁致伸缩性能,并对Al的加入量对复合材料的结构与性能的影响规律进行了探索.研究结果表明:烧结制备的Al/Tb0.30Dy0.70Fe1.95复合材料为多相结构,主要存在ReFe2、Al7ReFe5、Al2Re、Al3Re等相,随着Al的体积分数的增加,复合体中非GMM相渐渐增多,而GMM相则相应地减少,复合体内已不存在Al相;随着Al的体积分数的增加,复合材料的磁致伸缩系数λ起初略有上升,后明显下降,与纯GMM合金相比,Al/Tb0.30Dy0.70-Fe1.95复合材料的磁致伸缩性能均较差,当Al的体积分数为20%时,Al/Tb0.30Dy0.70Fe1.95复合材料的磁致伸缩系数约为合金的一半,为512×10-6;在GMM合金中适当增加廉价的Al元素后,可保持一定的磁致伸缩性能,还可以减少稀土等昂贵金属的含量,降低了成本.     

Tb0.3Dy0.7(Fe1-xAlx)1.95合金显微组织及低磁场的磁致伸缩性能研究

研究了Al添加量变化对Tb0.3Dy0.7(Fe1-xAlx)1.95合金显微组织、磁致伸缩系数的影响。结果发现,随着Al添加量的增加,晶体显微组织中的析出物增加;在一定的磁场强度下,磁致伸缩系数随Al添加量而变化,当磁场强度低于40kA/m时,磁致伸缩系数随Al添加量的变化曲线出现一峰值,当磁场强度高于40kA/m时,磁致伸缩系数随Al添加量的增加而降低。     

Tb0.3Dy0.7(Fe1-xAlx)1.95合金显微组织及低磁场的磁致伸缩性能研究

研究了Al添加量变化对Tb0.3Dy0.7(Fe1-xAlx)1.95合金显微组织、磁致伸缩系数的影响.结果发现,随着Al添加量的增加,晶体显微组织中的析出物增加;在一定的磁场强度下,磁致伸缩系数随Al添加量而变化,当磁场强度低于40kA/m时,磁致伸缩系数随Al添加量的变化曲线出现一峰值,当磁场强度高于40kA/m时,磁致伸缩系数随Al添加量的增加而降低.     

Y对铸态Fe_(81)Ga_(19)合金组织结构及磁致伸缩性能的影响

采用非自耗电弧炉制备了铸态Fe_(81)Ga_(19-x)Y_x(x=0.1,0.2,0.3,0.4,0.5)合金,通过金相观察、X射线衍射分析和磁致伸缩应变测量,研究了Y掺杂对铸态Fe_(81)Ga_(19)合金显微组织结构和磁致伸缩性能的影响。结果显示,Y的掺杂细化了合金的晶粒;掺Y后Fe_(81)Ga_(19)合金的择优取向增强;除了基体相(无序A2相)外,在铸态Fe_(81)Ga_(19-x)Y_x合金中还检测到DO_3相;Fe_(81)Ga_(19)-xYx合金最大饱和磁致伸缩应变在2500 Oe磁场强度下为97×10~(-6),与Fe_(83)Ga_(17-x)Y_x相比饱和磁致伸缩应变显著降低,DO_3相的析出是导致Fe_(81)Ga_(19-x)Y_x饱和磁致伸缩应变降低的原因。     

稀土物理冶金的新进展

叙述了Nd_2Fe_(14)B磁体和terfenol磁致伸缩合金用Nd、Tb和Dy的制备,terfenol磁致伸缩合金的加工以及高纯金属方面取得的进展。讨论的其他问题包括:1) 立方LaNi_2 Laves相是否存在;2) 25℃下稀土的亚稳定bcc相;3) 多层稀土材料;4) 稀土用于抑制腐蚀;5) 一种可能的新永磁体的发现;6) 在定域/离域交叉点上半重费米子化合物Ce Si_x(x≈1.85)电阻率巨大异常。     

( Tb,Dy) Fe2合金表面离子注入渗氮改性及抗腐蚀性能研究

采用离子注入技术在(Tb,Dy)Fe2稀土超磁致伸缩材料表面引入氮离子进行改性处理,研究了加速电压对材料表面相结构、微观形貌、表面硬度、抗酸碱腐蚀性能及磁致伸缩性能的影响.结果表明:离子注入渗氮后,(Tb,Dy)Fe2合金表面的REFb相分解,生成了REN,α-Fe和Fe8N新相,材料表面微观形貌发生了明显变化,表面硬度明显提高.通过测试极化曲线研究了渗氮前后(Tb,Dy)Fe2合金在不同PH值NaCl溶液中的抗酸碱腐蚀性能,发现pH值相同条件下渗氮处理后(Tb,Dy) Fe2合金的自腐蚀电位Ecorr较渗氮前明显正移且有钝化现象发生.在加速电压140 kV,离子注入剂量5.0×1017 ion.cm -2条件下渗氮处理的(Tb,Dy)F合金,处于20℃,3.5％ NaCl溶液环境中,pH=4时,△Ecorr=0.23413 V; pH =7时,△Ecorr =0.18992 V; pH=10时,△Ecorr =0.01268 V,渗氮处理后(Tb,Dy)Fe2合金的抗酸腐蚀性能明显增强,抗碱腐蚀性能变化不明显.随着pH值的增大,渗氮与未渗氮(Tb,Dy) Fe2合金的抗腐蚀性能均变差.由于离子注入表面渗氮的渗氮层很薄,渗氮温度很低,渗氮处理没有破坏材料的内部基体结构,因此渗氮后材料渗氮处理没有破坏材料的内部基体结构,其磁致伸缩性能几乎未受影响.研究表明离子注入渗氮是(Tb,Dy)Fe2磁致伸缩材料表面改性的一种有效方法.     

速凝成晶-烧结法制备磁致伸缩材料的研究

用速凝成晶方法制造Tb0.30Dy0.70We1.80合金薄片，合金薄片经过制粉、磁场取向压制成型和烧结制造磁致伸缩材料。结果表明：制造的速凝成晶Tb0.30Dy0.70We1.80合金薄片的显微组织以柱状晶为主。对速凝成晶Tb0.30Dy0.70We1.80合金粉末磁场取向后，烧结样品〈111〉晶向的取向程度提高；对速凝成晶Tb0.30Dy0.70We1.80合金薄片热处理后，烧结样品的磁致伸缩性能明显好于未热处理速凝成晶Tb0.30Dy0.70We1.80合金粉末的烧结样品。     

不同Tb/Dy比例对稀土磁致伸缩材料性能的影响

研究了不同Th/Dy比例对(TbxDy1-x)Fe1.95(x=0.30,0.32,0.34和0.35)合金的矫顽力、自旋再取向温度以及变温和加压磁致伸缩性能等的影响.结果表明,随着x值的增大,合金的矫顽力增大,自旋再取向温度降低.x为0.34时,合金的磁致伸缩温度系数较小,更适用于低温且工作温度变化大的环境.随着x值的增大,当施加压应力时,合金的磁致伸缩系数λ有明显的"跳跃效应",低场下尤为突出.     

Fe_(83)Ga_(17)La_x合金的磁致伸缩性能及组织研究

用真空电弧熔炼法制备Fe_(83)Ga_(17)La_x(x=0,0.2,0.4,0.6,0.8)铸态合金,采用震动样品磁强计、透射电镜、能量分散光谱仪、光学显微镜和自制磁致伸缩测量设备研究不同La含量对Fe_(83)Ga_(17)合金磁性能以及组织结构的影响。结果表明,添加La明显增加了合金的磁致伸缩性能,其中Fe_(83)Ga_(17)La_(0.2)的磁致伸缩系数最高可达210×10~(-6)。La易在晶界处富集,随着La含量增加,合金晶粒尺寸逐渐减小。La有助于合金沿100取向的晶粒增多。     

Effect of Ho-doping on microstructure and magnetostriction of TbDyFe alloys

Tb0.3Dy0.7HoxFe1.95 (x=0.00, 0.05, 0.10, 0.15, 0.20, 0.35, 0.50, 0.65) quaternary alloys were prepared by arc-melting and followed by annealing. The phases present and structure of the alloys were determined using a D8-Advance X-ray diffractometer. The magnetostriction of the alloys was studied by standard strain gauge technique. The dependence of Ho content on the structure, magnetostriction and density of the alloys was investigated in detail. The research results showed that Ho-doping did not change MgCu2-type cubic Laves structure in Tb0.3Dy0.7Fe1.95. When Ho content x≤0.2, rich rare earth phase presented in the alloys increased and magnetostriction of the alloys reduced evidently with increasing x, but for alloys with x>0.2, the content of rich rare earth phase started to reduce and the magnetostriction increased quickly, especially at low magnetic field in the alloy with x=0.65 due to separation of rich rare earth phases on the surface of the alloy.     

超磁致伸缩材料的研究新进展

近年来,稀土超磁致伸缩TbDyFe材料的研究进展迅速,既有新的研究方向如材料力学性能、合金的凝固过程、磁畴取向的分布、组分处于准同型相界的合金的性能等,也有传统的如热处理时施加高磁场及应力处理、新热处理方法等方面。此外,科研人员不断开发出新的稀土超磁致伸缩材料合金体系,即不同元素对TbDyFe体系的部分取代与添加,主要有Pr、Nd、Sm、Gd、Ho和Er等稀土元素及第八族的Co元素。     

X-ray diffraction analysis by Rietveld refinement of FeAl alloys doped with terbium and its correlation with magnetostriction

Fe₈₁Al₁₉ polycrystalline alloys doped with Tb(0-0.25 at%) were obtained by arc melting.The introduction of Tb favors the formation of columnar grains in the micro structure of the alloys,which develops a texture in the [100]crystal direction.Microstructural examination shows that the alloys are composed in great proportion by the disordered body-centered cubic(bcc),A2 phase and by a small proportion of the ordered bcc,B2 phase.As a consequence of doping with Tb,the lattice ...     

Relationship between crystal growth mode, preferred orientation and magnetostriction of (Tb0.3Dy0.7)Fe1.95 alloys

The relationship between crystal growth mode, preferred orientation and magnetostrictive properties of (Tb0.3Dy0.7)Fe1.95 alloys was investigated at different directional solidification rates. The results showed that preferred orientation had a strong influence on the characteristics of (Tb0.3Dy0.7)Fe1.95 alloys. At lower solidification rates, the sample with <110> preferred orientation showed larger low-field magnetostriction and apparent compressive stress effect. The excessive solidification rate resulted in failure of preferred orientation and a poor magnetostrictive performance. With an increase in solidification rates, the crystal growth modes changed gradually from cellular and primary dendrite morphology to developed dendritic morphology. In addition, domain configurations were observed using magnetic force microscopy, and the change of magnetostrictive properties was interpreted in terms of revealing the domain configurations.     

Effect of Rare Earth on Microstructure of γ-TiAl Intermetallics

The rare earth (RE) elements (Ce, La) were added to binary Ti-47% Al alloys (atomic fraction) by Induction Skull Melting. The element Ce of 1.0 atomic percent was added individually, and La of 0.2 atomic percent was added individually. This article studied the influences of rare earth metal (Ce, La) on microstructure of as-cast TiA1 based alloy by XRD, SEM, EMPA and TEM measurement methodology. The results show that most of rare earth-rich phases (AlCe, Al-La) are uniformly distributed in grain boundary in the shape of discontinuous network, and some particles of rare earthrich phases within the grains are mainly ellipsoids. In addition, rare earth element can obviously refine the grain size and the lamellar thickness of as-cast TiAl based alloy samples. The grain size of Ti-47Al-1.0Ce-0.2La alloy reaches about 30～80μm, and the lameUar thickness of its γ phase and α2 phase are less than 200 and 20nm, respectively.     

Influence of Rare Earth Elements on Luminescent Properties of Y2SiO5:Tb

Photoluminescent(PL) and cathodoluminescent(CL) properties of rare earths (Sc3 , La3 , Gd3 and Lu3 ) doped (Y0.97Tb0.03)2SiO5 were studied. Rare earth doping clearly influences PL and CL properties of Y2SiO5:Tb. For La3 doped system, PL intensity increases nearly 10% at x=0.05 whereas for Lu3 doped system, the intensity increases about 20% at x=0.20. Gd3 doping and Sc3 doping reduce the intensity; at x=0.3, it is reduced about 30% for Gd3 doped system and about 15% for Sc3 doped system, respectively. Quenching concentration of activator became higher in rare earth doped samples, which may be understood by that the rare earth dopants might dilute the concentration of the activator. Additionally, doping also influences the color saturation of Y2SiO5:Tb. Sc3 , La3 , and Gd3 doping improve the color saturation, whereas Lu3 doping decreases the color saturation. CL measurements show that CL intensity increases for all rare earths doped systems. The energy transfer from Gd3 to Tb3 was discussed.     

Fe-Ga磁致伸缩合金力学性能强化研究进展

Fe-Ga磁致伸缩合金作为重要的磁驱动智能材料之一,不仅在低磁场条件下具有较高磁致伸缩应变的功能材料特性,同时还具有较高力学强度的结构材料特性,结构功能一体化特征明显,存在广泛的研究价值和应用前景.国内外学者围绕该材料的磁致伸缩性能、力学性能优化开展了大量研究工作.其中,通过在Fe Ga合金中添加元素来调控力学性能和磁...     

Effect of copper on magnetostriction and mechanical properties of TbDyFe alloys

The intrinsic brittleness of the TbDyFe alloy significantly decreases its mach inability and applications.This paper aims to improve the toughness of TbDyFe alloy by adding Cu. Various alloys of the type(Tb_(0.3)Dy_(0.7))_(0.37)Fe_(0.63-χ)Cu_χ(χ=0, 0,01.0.03, 0.05, 0.08, 0.1) were fabricated by an arc melting furnace under a high purity argon atmosphere. The microstructure, magnetostrictive properties and mechanical performance were studied systematically. The results show that the (Tb,Dy)Cu phase forms in these alloys upon the addition of Cu. Correspondingly, their toughness improves, attributed to the formation of a (Tb,Dy)Cu phase. Compared to the Cu-free alloy, the fracture toughness (Kic) increases 2-3 times with increasing Cu content. However, the magnetostriction performance of these alloys declines with Cu addition, due to the low-magnetic performance of the (Tb,Dy)Cu phase at room temperature. Compared with other alloys, the alloy with the addition of 1at%Cu shows the best compromise between the saturation magnetostriction and fracture toughness.     

高容量稀土基贮氢合金的研究

以金属RE、La、Ni、Co、Mn、Al作为稀土基贮氢合金的原料,制备了一系列不同成分的贮氢合金,进行了相应的组织结构分析及电化学性能的测试,研究了不同La、Co添加量对合金相结构与电化学性能的影响,选择确定了合适的合金配方,为生产高容量Ni-MH电池的负极材料提供了依据.     

Effect of rare-earth doping on adsorption of carbon atom on ferrum surface and in ferrum subsurface: A first-principles study

The adsorption of carbon atom on Fe surface and in Fe subsurface with and without rare earth (La and Ce) substitution in the surface layer and subsurface layer was studied by first-principles calculations. The carbon atom is predicted to adsorb at hollow and long bridge site on Fe(100) and Fe(110), respectively. However, the carbon atom shifts to occupy preferentially hollow site on both Fe(100) and Fe(110) with rare earth atom doping at surface layer. The lower adsorption energies involved with stronger adsorption abilities were obtained for carbon atoms on Fe surface with rare earth doping at surface layer, which was determined by the electronic structure of the surface atoms. The La atom was pulled out the surface after carbon adsorption due to strong interaction of La–C, which is consistent with the more charge transfer. In the subsurface region, the carbon atom prefers to occupy at octahedral site with rare earth doping at surface layer in Fe slab. These strong adsorption energies of the carbon atoms on Fe surface and in Fe subsurface with rare earth pose relevant insights into the interaction between carbon and rare earth, which helps to understanding the influence mechanism of rare earth in carburizing.