Fe-Ga-B合金室温塑性及轧制材料磁致伸缩性能

研究了0.5%(原子分数)B对Fe83 Ga17合金室温力学性能的影响及(Fe81 Ga19)99.5 B0.5轧制薄片磁致伸缩性能.结果表明,少量B添加提高了Fe-Ga合金的室温塑性,实现(Fe81 Ga19)99.5 B0.5合金的轧制成形.热处理对(Fe81 Ga19)99.5 B0.5合金薄片材料磁致伸缩性能有很大影响.在同一热处理制度条件下,磁致伸缩性能随变形量的增加而减小;对于变形量为93.5%的样品,同一热处理时间,样品磁致伸缩性能随热处理温度的升高而增加,同一热处理温度时,样品磁致伸缩性能都表现出先升高后降低的变化趋势,样品在1300℃保温2h后,磁致伸缩性能最好,达到1.65×10-4.热处理对(Fe81 Ga19)99.5 B0.5合金薄片材料磁致伸缩性能的影响归因于对样品织构的影响.具有{100}＜012＞织构样品的磁致伸缩性能最高,而{111}＜110＞和{111}＜112＞织构对应的磁致伸缩性能较低.     

快淬和退火对Fe_(83)Ga_(17)Ce_(0.8)合金结构和磁致伸缩性能的影响

采用电弧熔炼法制备了稀土Ce掺杂的Fe83Ga17Ce0.8铸态合金,然后对其进行快淬处理,获得Fe83Ga17Ce0.8快淬态合金,最后对Fe83Ga17Ce0.8快淬态合金在1 223K下进行退火热处理5h。用X射线衍射(XRD)、扫描电镜及能谱仪(SEM/EDS)和磁致伸缩测试方法研究了快淬和退火对合金结构和磁致伸缩性能的影响。结果表明,Fe83Ga17Ce0.8铸态合金由bcc结构的Fe(Ga)相和少量的CeFe2第二相组成。Fe83Ga17Ce0.8快淬态合金除了含有大量的Fe(Ga)相和少量的CeFe2相外,合金中还出现了非对称DO3结构的Fe3Ga相。Fe83Ga17Ce0.8快淬态合金经退火热处理后,合金中的CeFe2相转化为贫稀土Ce2Fe17相。在外磁场为557kA/m时,Fe83Ga17Ce0.8快淬态合金的磁致伸缩系数(3.82×10-4)明显大于铸态合金(3.56×10-4)和退火态合金(1.82×10-4)的磁致伸缩系数。     

Co元素添加对Fe83Ga17合金结构及磁性能的影响

制备目标成分为Fe83-xCoxGa17(x=0,0.5,1.5,2.5,3.5)系列的合金铸锭,研究了Co元素添加对该系列合金结构、磁致伸缩性能、磁性能及硬度的影响.实验结果表明,随着Fe-Ga合金中Co元素的增加,合金饱和磁致伸缩值先增加后降低,在x=1.5时,合金饱和磁致伸缩值最高,达到195·10-6,并且该成...     

热处理对快淬Fe83Ga17Ce0.8合金结构和磁致伸缩性能的影响

采用电弧熔炼法制备了稀土Ce掺杂的Fe83Ga17Ce0.8铸态合金,然后对其进行快淬处理,获得快淬态Fe83Ga17Ce0.8合金,最后对快淬态Fe83Ga17Ce0.8合金在不同温度(850℃、950℃和1050℃)下进行退火处理5h.用X射线衍射(XRD)、扫描电镜及能谱仪(SEM/EDS)和磁致伸缩测试方法研究了退火温度对合金结构和磁致伸缩性能的影响.结果表明,快淬态Fe83Ga17Ce0.88合金经退火处理后,合金中的CeFe2相转化为贫稀土Ce2Fe17相.随退火温度的升高,合金的磁致伸缩系数绝对值先减小后大幅度增大.退火温度为1050℃时,合金的磁致伸缩系数达最大(在外磁场为398 kA/m时,磁致伸缩系数为656×10-6).磁致伸缩系数的增大与该合金中形成较多的Ce2Fe17相以及合金中A2相沿[100]方向择优取向有关.     

Fe-Ga超磁致伸缩材料的性能和中子衍射分析

Fe-Ga合金具有较大的磁致伸缩应变λ,低的饱和磁化场.Fe83Ga17饱和磁致伸缩应变可以达到3.00×10-4.为了进一步验证不同相结构对合金磁致伸缩性能的影响,对样品进行中子衍射和差热分析,发现Fe83Ga17合金在700℃附近存在相结构变化,结构变化导致合金磁致伸缩系数的改变.     

真空磁场热处理对Fe-Ga-Al合金磁致伸缩的影响

采用电弧炉熔炼方法得到Fe82Ga18-xAlx(x=3,9,12)合金的多晶样品。利用X射线衍射(XRD)和金相观察对合金的相组成进行分析,并对其磁致伸缩系数进行测量。经过真空磁场热处理后,对Fe-Ga-Al合金的结构和磁致伸缩性能进行研究。结果表明,真空磁场热处理后Fe-Ga-Al合金磁致伸缩系数均有提高,其中Fe82Ga9Al9合金经磁场热处理后,磁致伸缩达到114×10-6;Fe82Ga15Al3合金经磁场热处理后,其磁致伸缩增幅最大,比处理前增加165%。     

元素Zr添加对铸态Tb0.3Dy0.7Fe1.95合金组织与磁致伸缩性能的影响

采用高真空电弧炉制备了Tb0.3Dy0.7Fe1.95-xZrx（x=0、0.03、0.06、0.09）合金,研究了不同Zr含量Tb0.3Dy0.7Fe1.95-xZrx（x=0、0.03、0.06、0.09）合金的晶体结构、微观组织及磁致伸缩性能。结果表明添加Zr后的Tb0.3Dy0.7Fe1.95-xZrx（x=0.03、0.06、0.09）合金基体相仍保持为MgCu2（C15型）立方Laves相结构,Zr添加后取代了Tb0.3Dy0.7Fe1.95合金中的稀土原子Tb、Dy而使晶格常数减小。添加Zr后,初生相ZrFe2的形成使得凝固液体富稀土从而抑制了RFe3有害相的生成,Zr在基体相RFe2中有限固溶而在富稀土相Re中不溶。初生相ZrFe2（C15型）可溶于与自身结构相同的RFe2（C15型）相中形成（Re、Zr）Fe2相。当Zr含量x=0.09时,Zr的溶解过饱和,从而在（Re、Zr）Fe2基体相上析出了富Zr相。Zr的添加量x对磁致伸缩的影响很大,少量Zr的添加对磁致伸缩的提高有利,但当含量x=0.09时,由于富Zr相,富Re相的析出对磁致伸缩的提高不利,但相对于Tb0.3Dy0.7Fe1.95母合金有少量提高。     

〈110〉轴向取向Fe83Ga17合金中原子间作用与磁致伸缩的关系

采用定向凝固的方法制备出棒状〈110〉轴向取向多晶Fe83Ga17样品,Fe83Ga17合金样品经过淬火处理后,饱和磁致伸缩应变λs可以达到2.42×10-4。实验发现样品的磁致伸缩应变与合金中的短程序密切相关。淬火处理后样品的磁性Fe原子周围的原子占位发生了改变,合金部分有序。文中采用"原子对模型"(pairmodel),从能量最小原理出发,分析讨论了Fe Ga合金中原子对间的相互作用与磁致伸缩应变的关系。     

Fe及Fe83Ga17和Fe83Ga17Pr0.3合金的微结构与磁致伸缩性能

本研究对比研究了Fe、Fe_(83)Ga_(17)及Fe_(83)Ga_(17)Pr_(0.3)磁致伸缩材料的微结构与磁致伸缩性能。采用真空非自耗电弧炉在氩气保护下熔炼制备了合金样品。采用X射线衍射仪(XRD)和光学显微镜(OM)分析观察了合金样品的晶体结构和显微组织。采用扫描电镜配合能谱仪(SEM/EDS)测定了稀土Pr元素在Fe_(83)Ga_(17)Pr_(0.3)合金中的分布。通过电阻应变法测量了合金的磁致伸缩性能。结果表明:Fe和Fe_(83)Ga_(17)合金均由单一的bcc结构A2相组成,而Fe_(83)Ga_(17)Pr_(0.3)合金由A2主相和少量的富稀土Pr相组成。稀土Pr掺杂使合金中的A2相沿〈100〉晶向择优取向。Fe及Fe_(83)Ga_(17)和Fe_(83)Ga_(17)Pr_(0.3)合金的微观组织分别呈现细长的条状晶、晶粒粗大的等轴晶和晶粒细小的柱状晶。Fe的磁致伸缩系数为负值,而Fe_(83)Ga_(17)和Fe_(83)Ga_(17)Pr_(0.3)合金的磁致伸缩系数均为正值,三种材料的磁致伸缩系数绝对值的排序为FeFe_(83)Ga_(17)Fe_(83)Ga_(17)Pr_(0.3)。     

Fe100-x（Ga0.75Al0.25x（21．2≤x≤26．8）合金的结构与磁性

采用X射线衍射仪（XRD）对Fe100-x（Ga0.75Al0.25x（21．2≤x≤26．8）合金的相组成和晶格常数进行分析，表明晶格常数随Ga、Al替代量的增加而变化，反映了合金中A2相的减少和B2、D03有序相的增加。在差热分析仪（DTA）上测得Fe100-x（Ga0.75Al0.25x（x=25．2）合金样品的DTA曲线。研究发现Fe100-x（Ga0.75Al0.25x（21．2≤X≤26．8）合金经650℃均匀化退火处理后，当X≤22．8时为无序的体心立方结构A2相。当x=25．2时，合金为B2单相结构。当x=26．8时，合金的组织基本为DO3单相。采用振动样品磁强计（VSM）对此系列合金的磁性进行研究。研究发现其饱和磁化强度表现出先减小后增大的变化规律，这是该系列合金中有序相的存在引起的。分析认为晶格常数与饱和磁化强度的变化与合金磁致伸缩改变存在必然联系。     

Effect of Minor Alloying on Crystallization Behavior and Thermal Properties of Zr_(64.5)Ni_(15.5)Al_(11.5)Cu_(8.5) Bulk Amorphous Alloy

Minor alloying plays an important role in the synthesis and improvement of thermal stability of bulk metallic glasses(BMGs).The present study was conducted to investigate the effect of minor additions of Y,Ti and Nb on the crystallization behavior and the thermal properties of Zr64.5Ni15.5Al11.5Cu8.5 alloy.Thermal parameters and the activation energies for crystallization were calculated for four(Zr0.645Ni0.155Al0.115-Cu0.085)100-xMx(M=Y,Ti and Nb,while x=0,2 at.) alloys.The present alloys have wide supercooled liquid region of ≥87 K.Maximum activation energy was found to be greater than 300 kJ/mol for the base alloy.Four crystalline phases were identified in the samples annealed at 823 K for 20 min.Reduced glass transition temperature(Trg) and other thermal parameters such as γ,δ and β were improved by Y and Ti addition.Nb addition resists crystallization below annealing temperature 713 K,however,its effect on thermal properties is not very promising.     

Magnetic anisotropy in Sm2Fe17-xMx (M = Al, Ga) and (Sm1-xTmx)(2)Fe14Al3

1. IntroductionMany illtermetajlic compounds of R-Fe and R-Co(R: rare earths) have some ideal properties as highquality permanent magnet materials where a largemagnetic anisotropy of 4f electrons is coupled withstrong exchange interaction of 3d electrons via the4f-3d illteraction.In 1967 the SmCos magnet was discovered as thefirst rare earth permanent magnet, and in 1973 moreimproved magnet in the form of SmZCo17 was developed, These two compounds were found to have excellellt permanellt m…     

金属间化合物YFe12-xMx（M=V,Cr）的结构和磁性研究

采用线性缀加平面波展式结合改进的局域轨道方法(APW+lo),基于密度泛函理论(DFT),优化、计算和分析了Y、Fe、V、Cr和YFe12-xMx(M=V、Cr;x=0～5)体系的结构和能量。系统的总磁矩和原子磁矩的计算表明,YFe12-xMx的磁矩主要来源于Fe,但是随着M浓度的增加而减小,这是因为M的加入不仅会降低体系中Fe的浓度,而且还将影响Fe之间相互作用导致Fe磁矩下降。利用计算获得的系统总的电子态密度和Fe的电子态密度对计算结果进行了分析。     

Magnetic Anisotropy in Sm2Fe17-xMx (M＝A1, Ga)and (Sm1-xTmx)2Fe14Al3

In Sm2Fe17-xMx(M＝Al, Ga), there was observed a kind of spin-reorientation with temperature, and in (Sm1-xTmx)2Fe14Al3, the anisotropy field HA increases as high as 20% from 5.4 up to 6.5 kOe with Tm.     

Quenchability and Magnetic Properties of Nd_4Fe_(82)B_(14)

The glass forming ability (GFA), crystallization behaviour and magnetic properties of Nd4Fe82B14 produced by melt spinning were investigated. The experimental results show that the GFA is rather Strong; the crystals precipitation sequence is as follows: Am(amorphous)→Am'+bcc-Fe →Nd2Fe23B3+Fe23B6+bcc-Fe→Fe23B6+Fe3B+Nd2Fe14B+bcc-Fe→Fe3B+Nd2Fe14B+bcc-Fe. The magnetic properties after crystallization are not affected by the cooling rate and the best magnetic properties are Br=0.8436 T, Hcj=266.4 kA/m, (BH)max=48.08 kJ/m3.     

Ti-Cr-Mn-M(M=V、Fe、Ni、Cu)合金的储氢性能

为改善Ti(Cr-Mn)2 AB2型合金的储氢性能,采用A侧过化学计量和过渡金属部分替代Mn进行多元合金化,系统研究了Tix(Cr-Mn-M)2(x=1.0,1.1;M=V、Fe、Ni、Cu)合金的储氢性能.研究结果表明,V、Fe、Ni、Cu部分替代Mn进行多元合金化后,合金主相仍保持C14(MgZn2)型Laves相,合金晶胞体积增大.合金化元素部分替代Mn后合金的活化性能得到明显改善,合金吸放氢量增大,吸放氢压力滞后减小.除Fe使合金放氢平台压力有所升高外,其余合金化元素均使合金的吸放氢平衡压力有不同程度的降低,这是由于合金的晶胞体积增大所致.在所形成的合金中,以Ti1.1Cr1.2Mn0.5CuO0.3的综合性能最好,其室温下吸放氢量分别达到1.95%和1.72 9,6(质量分数).采用该合金与自制的轻质高压储氢容器(工作压力为40MPa)复合组成金属氢化物复合式高压储氢器,对其储氢密度的计算结果表明,当储氢合金的填充量(体积分数)达到0.20时,该复合式储氢器总的体积储氢密度将提高57%.     

Poly(methyl methacrylate) coating of soft magnetic amorphous and crystalline Fe,Co-B nanoparticles by chemical reduction

The structural and magnetic properties of a collection of nanoparticles coated by Poly(methyl methacrylate) through a wet chemical synthesis have been investigated. The particles display either an amorphous (M = Fe, Co) M-B arrangement or a mixed structure bcc-Fe and fcc-Co + amorphous M-B. Both show the presence of a metal oxi-hydroxide formed in aqueous reduction. The organic coating facilitates technological handling. The cost-effective synthesis involves a reduction in a Poly(methyl methacrylate) aqueous solution of iron(II) or cobalt(II) sulphates (< 0.5 M) by sodium borohydride (< 0.5 M). The particles present an oxidized component, as deduced from X-ray diffraction, M?ssbauer and Fe- and Co K-edge X-ray absorption spectroscopy and electron microscopy. For the ferrous alloys, this Fe-oxide is alpha-goethite, favoured by the aqueous solution. The Poly(methyl methacrylate) coating is confirmed by Fourier transform infrared spectroscopy. In pure amorphous core alloys there is a drastic change of the coercivity from bulk to around 30 Oe in the nanoparticles. The mixed structured alloys also lie in the soft magnetic regime. Magnetisation values at room temperature range around 100 emu/g. The coercivity stems from multidomain particles and their agglomeration, triggering the dipolar interactions.     

Fe_(88-x)Zr_xB_(12)合金的结构及晶化研究

采用机械合金化法制备Fe88-xZrxB12(X=5、10、15、20)系合金,利用X射线衍射仪(XRD)、差热分析仪(DTA)等测试手段对样品的结构及晶化进行研究.XRD结果表明,球磨60h,Fe88-xZrxB12(x=5、10、15)已形成α-Fe固溶体,Fe68Zr20B12完全形成非晶合金,表明Zr含量的增加使合金的非晶形成能力增强.Fe88-xZrxB12(x=5、10、15、20)合金的DTA图中均出现2个晶化放热峰.Fe68Zr20B12非晶合金的晶化模式为一次晶化.     

Influence of surface oxidation on transmission electron microscopy characterization of Fe–Ga alloys

Fe–Ga alloys are rapidly oxidized when exposed in air, forming both amorphous and crystalline surface oxides. These oxides hinder the observation of the ordered phases of B2 and D0₃ in Fe–Ga alloys by dark-field imaging and high-resolution imaging of transmission electron microscopy (TEM) techniques. Proper imaging techniques and reduction of surface oxides are necessary to obtain representative microstructural features to the bulk alloys by TEM.