Fe80-xCoxZr8Ge2B10 (x=0,8, 16)合金的热性能、结构和磁性能

用单辊快淬法制备Fe80-xCoxZr8Ge2B10(x=0,8,16)非晶合金,再对3种合金进行不同温度下退火处理.利用差热分析仪(DTA)、X射线衍射仪(XRD)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,Fe80-xCox Zr8 Ge2 B10(x=0,8,16)合金在快淬态时均形成非晶.Fe80 Zr8 Ge2B10和Fe72 Co8 Zr8 Ge2 B10的晶化过程类似,比较复杂;Fe64 Co16 Zr8 Ge2 B10合金的晶化过程不同于其他两种合金,相对简单.3种合金的比饱和磁化强度整体上随着Co含量的增加而增大.     

Fe(Co,Ni)ZrB非晶/纳米晶的制备及晶化过程研究

采用机械合金化法制备了Fe70Zr10B20、Fe63Co7Zr10B20和Fe63Ni7Zr10B20合金.利用X射线衍射仪(XRD)研究了3种合金的机械合金化过程及晶化过程.Fe70Zr10 B20球磨50h后的合金由大量非晶相和少量晶态相组成,Co的添加对FeZrB非晶合金的形成起到了抑制作用;Ni的添加对FeZrB非晶合金的形成起到了促进作用.Fe70-Zr10B20、Fe63Co7Zr10B20合金的晶化过程容易进行,而Fe63 Ni7Zr10 B20合金的晶化比较困难.     

Ni-Fe-(Nb)-Si-B非晶合金的等温晶化与结构转变

采用旋铸急冷工艺在大气环境中制备出(Ni0.75Fe0.25)78-xNbxSi10B12(x=0,5)非晶合金带材.X射线衍射(XRD)分析表明样品为完全非晶态.用差热分析仪(DTA)在高纯氩气保护下测量了非晶薄带的Tg、Tx、Tm,并分析了其热稳定性.根据DTA结果分析表明,(Ni0.75Fe0.25)78Si10B12非晶合金退火温度为695,715,745和765K,在715和745K退火时,非晶基体上析出了单一的γ-(Fe, Ni)固溶体,平均晶粒尺寸分别约为10.3和18.5nm;765K退火后的结晶相为γ-(Fe, Ni)固溶体,Fe2Si,Ni2Si和Fe3B.(Ni0.75Fe0.25)73Nb5Si10B12非晶合金的退火温度为720,750和800K,退火后不能在非晶基体上析出单一的晶化相,晶化析出相为γ-(Fe, Ni)固溶体,(Fe, Ni)23B6,Ni31Si12和Nb2NiB0.16.     

添加Ni对FeZrNbB合金的非晶形成能力与软磁性能的影响

利用单铜辊甩带法制备Fe(86-x)Zr2Nb2B10Nix(x=0、1、3和5)非晶合金带材。采用X射线衍射仪、差示扫描量热仪、振动样品磁强计以及精密磁性器件分析仪研究Ni元素对FeZrNbB合金带材的非晶形成能力和软磁性能影响。结果表明Ni元素能明显提高该体系合金的非晶形成能力,并使淬火态非晶合金带材的一级起始晶化温度提高;通过合金的退火处理,在Fe(86-x)Zr2Nb2B10Nix合金体系中含Ni元素的合金带材可以析出最小粒径为12(12.15)nm的α-Fe(a)纳米晶,获得较低的矫顽力为8.1A/m;其中Fe85Zr2Nb2B10Ni1非晶合金带材经过510℃保温20min热处理后可以获得较高的饱和磁感应强度为1.61T,有效磁导率提升到48.4k,矫顽力下降到8.3A/m。     

Fe-Nd-B-Zr块体非晶合金的形成能力和磁性能

以Fe-Nd-B系块体非晶合金为前驱体制备永磁材料。在Fe70Nd10B20三元合金及其邻近成分点中微量添加Zr元素,采用熔体旋淬法和铜模喷注法制备样品,通过XRD和DSC表征非晶形成能力。对Fe70Nd9B20Zr1块体非晶合金进行退火晶化处理,采用XRD分析晶化产物,通过VSM表征不同晶化阶段的磁性能。结果表明,合金体系的非晶形成能力得到提高,在Zr原子分数为1%时获得临界尺寸为2mm的块体非晶合金;Fe70Nd9B20Zr1块体非晶合金在946K,600s退火时得到最佳硬磁性能,剩磁(Br)、内禀矫顽力(iHc)和最大磁能积(BH)max分别为0.54T,348kA/m和24.1kJ/m3。该合金体系可应用于直接通过铸造和热处理工艺制备块体纳米复合永磁材料。     

Fe61Co10Zr5W4B20块体非晶合金的形成及其力学性能

采用铜模吸铸法获得直径为2 mm的Fe61Co10Zr5W4B20块体非晶合金.采用X射线衍射、扫描电镜、示差扫描量热仪、微显硬度及压缩实验等研究了非晶合金的结构、热稳定性、显微硬度与压缩性能.结果表明:Mo的引入不利于非晶合金的形成;Fe61Co10Zr5W4B20块体非晶合金表现为二级晶化,玻璃转变温度为561.1℃,晶化起始温度为619.0℃,第一晶化峰值温度为632.6℃,第二晶化峰值温度为747.0℃,过冷液相区为57.9℃;该非晶合金的显微硬度为1207HV0.2,抗压强度σbc为1707.6 MPa.     

高Fe含量FeCuNbSiB系非晶/纳米晶合金制备及其磁性研究

研究了过渡金属元素(Zr,Nb,Mo)和Cu元素对Fe78Si9B13合金系非晶形成能力、热稳定性和磁性的影响;在Fe74Cu1Nb3Si13B9合金的基础上,通过逐步提高Fe含量,利用单辊甩带法制备Fe(76+x)Cu1Nb3Si(11-x)B9(x=0,2,4)和Fe(79+x)Cu1Nb2Si(6-x)B12(x=0,2,4)非晶/纳米晶合金薄带;利用XRD、DSC、TEM和VSM研究了高Fe含量Fe-Cu-Nb-Si-B系非晶/纳米晶合金的微观结构和磁性,并通过添加Nb元素优化了高Fe含量合金的磁性。研究结果表明:Zr和Nb元素的添加能明显提高Fe78Si9B13合金的非晶形成能力和热稳定性;高Fe含量的Fe-Cu-Nb-Si-B系纳米晶合金为典型的非晶/纳米晶双相结构,合金的饱和磁化强度Ms180 emu/g,且合金的矫顽力Hc在2Oe-9Oe之间,具有良好的软磁性能;Nb元素能显著细化Fe-Cu-Nb-Si-B系合金晶粒尺寸,从而能显著降低合金的矫顽力,改善合金的软磁性能;当Fe含量在80%-83%(原子百分比,下同)之间时,合金具有良好的软磁性能,但当Fe含量达到85%时,会有Fe2B、Fe3B相析出,从而显著恶化其软磁性能。     

Fe60Co8Zr10Mo5W2B15块体非晶合金的形成及热处理对性能的影响研究

用铜模吸铸法获得直径为2mm的Fe60Co8Zr10Mo5W2B15和Fe60Co8Zr10Mo5W2B15块体非晶合金。采用X射线衍射（XRD）、示差扫描量热分析（DSC）、显微硬度及压缩实验等研究了非晶合金的结构、热稳定性及热处理前后的显微硬度与压缩性能。结果表明Nb的引入不利于非晶合金的形成；Fe60Co8Zr10Mo5W2B15非晶合金的显微硬度为1343HV0．2，抗压强度σbe为972．6MPa；在低于晶化起始温度的热处理，硬度稍有下降；但在高于晶化峰值温度的热处理，硬度值随时间变化先升高，后下降；在热处理时间相同的条件下，随着热处理温度的升高，合金的硬度升高，但压缩强度会明显下降。     

Co对Nd-Fe-Al大块非晶合金的晶化行为和磁性能的影响

采用示差扫描量热法(DSC)，X射线衍射(XRD)和振动样品磁强计(VSM)研究了Co对Nd—Fe-Al大块非晶合金的非晶形成能力，晶化行为和磁性能的影响。结果表明：加入Co元素后可以显著提高Nd—Fe-Al大块非晶合金的非晶形成能力以及提高合金的居里温度。Nd60Fe30-xAl10Cox(z=0、5、10)大块非晶合金在室温有较高的内禀矫顽力，具有硬磁性。内禀矫顽力随着Co含量的增加变化不大．但是饱和磁化强度和剩磁则随着Co含量的增加有所下降。Nd60Fe3-xAl10Cox(x=0、5、10)大块非晶合金具有的硬磁性能来自于非晶相。合金少量晶化后，磁性能变化不大。完全晶化后合金的硬磁性迅速消失。     

Fe70Zr10B20非晶合金的制备及其热稳定性和磁性能研究

采用机械合金化技术制备了Fe70Zr10B2。磁性非晶合金粉末。分析Fe70Zr10B20非晶合金的形成机制、晶化机制：研究Fe70Cr10B20非晶合金不同热处理温度下的磁性及球磨过程中样品的磁性。结果表明：Fe70Cr10B20非晶相的形成是由原子的扩散和晶格崩渍共同作用的结果；Fe70Cr10B20非晶合金的热致晶化模式为一次晶化；球磨过程厦非晶熟处理后样品的磁性与其结构、晶粒尺寸、应力和缺陷等因素有关。     

Effects of Nb Alloying on Nano-Crystallization Kinetics of Fe55-x Cr18Mo7B16C4Nbx(x=0, 3) Bulk Amorphous Alloys

Crystallization kinetics of Fe55-xCr18Mo7B16C4Nbx(x= 0, 3) bulk amorphous alloys were analyzed using X-ray diffraction and differential scanning calorimetric (DSC) tests. In practice, crystallization and growth mechanism were evaluated using DSC tests at four different heating rates (10, 20, 30, and 40 K/min) and kinetic models. Two-step crystallization behavior was observed when Fe55Cr18Mo7B16C4 and Fe52Cr18Mo7B16C4Nb3 bulk amorphous alloys were annealed, where Fe36Cr12Mo10 phase was crystallized in the first step of crystallization. Results show that Fe36Cr12Mo10 and Fe3C phases were crystallized in the structures of the alloys after further annealing process. Activation energy for the crystallization of Fe36Cr12Mo10 phase was measured to be 543 kJ/mol in Fe52Cr18Mo7B16C4Nb3 alloy and 375 kJ/mol for Fe55Cr18Mo7B16C4 alloy according to Kissinger-Starink model. Moreover, a two-dimensional diffusion controlled growth mechanism with decreasing nucleation rate was found in Fe52Cr18Mo7B16C4Nb3 alloy whereas a three-dimensional diffusion controlled growth mechanism with decreasing nucleation rate was found in crystallization of Fe36Cr12Mo10 phase dur- ing annealing of Fe55Cr18Mo7B16C4 alloy. TEM (transmission electron microscopy) observations reveal that crystalline Fe36Cr12Mo10 phase nucleated in the structures of the alloys in an average size of 10 nm with completely mottled morphology.     

机械合金化制备Fe-Zr-B非晶合金及其晶化动力学行为研究

在高纯氩气保护下使用机械合金化法对原子组成为Fe60Zr40-xBx(x=10、20、30)的混合粉体进行实验,成功地制取了非晶合金粉。结合X射线衍射与DSC的分析,认为:Fe60Zr20B20和Fe60Zr10B30体系因B原子含量较高,使得其非晶化效率及热稳定性都要高于B原子含量较少的Fe60Zr30B10体系。计算得出Fe60Zr20B20和Fe60Zr10B30两个体系的非晶晶化激活能数据分别为(201.7±58.5)kJ·mol-1和(220.3±18.1)kJ·mol-1。     

Crystallization of (Fe, Co)78Si9B13 alloys: influence of relaxation processes

Crystallization of Fe78-xCoxSi9B13 amorphous alloys has been studied by differential scanning calorimetry (DSC), thermomagnetic gravimetry and X-ray diffraction techniques. Thermal stability of the amorphous alloy monotonically decreases with increasing cobalt content. The devitrification process as detected by DSC occurs in two main stages partially overlapping in temperature, but magnetic characterization reveals a third stage for cobalt-rich alloys. Primary precipitation of -(Fe, Co) is followed by a polymorphic reaction to give (Fe, Co)2B phase. Fe3B-type phase is also detected at the end of the first crystallization stage for iron-rich alloys and -Co(Si) and Co2B phases are found in fully crystallized samples for x=60. The influence of relaxation processes on the crystallization was investigated, but no significant effects of pre-annealing on the crystallization parameters resulted. © 1998 Chapman & Hall     

Formation of nanocrystalline structure during electron irradiation induced crystallization in amorphous Fe-Zr-B alloys

Effect of electron irradiation on the crystallization and phase stability of Fe₈₈Zr₉B₃ and Fe₇₁Zr₉B₂₀ amorphous alloys was examined. Electron irradiation at an accelerated voltage of 2000 kV was performed at room temperature. The Fe₇₁Zr₉B₂₀ alloy showed a wide supercooled liquid region and the ΔT_x value was 71 K, while no glass transition was observed in Fe₈₈Zr₉B₃ alloy. The amorphous phase in Fe–Zr–B alloys was not stable under irradiation and crystallization from the amorphous phase was accelerated by the irradiation. Nanocrystalline structure composed of α-Fe and cubic-Fe₂Zr was formed in Fe₈₈Zr₉B₃ alloy by irradiation induced crystallization, while no nanoscale precipitates of intermetallic compounds were formed during annealing. In Fe₇₁Zr₉B₂₀ alloy, the formation of nanocrystalline precipitates was also confirmed by irradiation induced crystallization, although the formation of nanocrystalline structure had not been realized in high B concentration Fe–Zr–B alloys by annealing. These new results show that electron irradiation is effective in producing a new nanocrystalline structure.     

Co47.6Fe20.4B21.9Si5.1Nb5-xZrx(x=0~5)合金的非晶形成能力和磁性能

采用铜模吸铸法制备了直径d为2~5mm的Co_(47.6)Fe_(20.4)B_(21.9)Si_(5.1)Nb_(5-x)Zr_x(x=0~5)合金。利用X射线衍射(XRD)、差示扫描量热仪(DSC)、振动样品磁强计(VSM)和显微硬度计分析合金的非晶形成能力(GFA)、磁性能及显微硬度。结果表明:该合金体系具有较好的GFA,随着Zr含量的增加,其GFA呈逐渐降低的趋势。Zr含量为0~2%(原子分数)时,能制得d为3mm的非晶合金;Zr含量为0~3%(原子分数)时,可制得d为2mm的非晶合金。直径2mm的棒状非晶合金(Zr含量为0~3%(原子分数))表现为明显的软磁性,饱和磁化强度Ms趋于一定值。该体系非晶合金均具有很高的显微硬度,Zr含量为3%(原子分数)时达到1420HV。     

快速凝固Al_(88)Ce_2Ni_(10-x)Fe_x(x=0,1,3,5)非晶铝合金的形成和热稳定性分析

液淬Al(88)Ce2Ni(10-x)Fex(x＝0,1,3,5)非晶铝合金的形成倾向和热稳定随组元Fe含量的增加，表现出较大的差别：前者趋于降低，后者趋于增大。非晶铝合金的形成和热稳定性是由不同微观机理所决定的，其中3d过渡金属Fe与主量元素Al相异原子之间的强烈相互作用是导致热稳定性提高的主要原因。     

FeCoZrNbB合金的晶化过程及磁性能

采用单辊快淬法制备Fe_81-xCo_xZr₇Nb₂B₁₀(x = 2, 4, 6) 系非晶合金,并对该系非晶合金进行热处理。利用X射线衍射和振动样品磁强计研究FeCoZrNbB 合金系的晶化过程和磁性能。结果表明,Fe_81-xCo_xZr₇Nb₂B₁₀(x = 2, 4, 6) 系合金在快淬速率为30 m/s时完全形成非晶。Fe₇₉Co₂Zr₇Nb₂B₁₀合金的晶化过程为非晶→非晶+α-Fe→α-Fe + Fe₃Zr + Fe₂Nb_0.4Zr_0.6;Fe₇₇Co₄Zr₇Nb₂B₁₀与Fe₇₅Co₆Zr₇Nb₂B₁₀合金的晶化过程相同为非晶→非晶+α-Fe→ α-Fe + Fe₃Zr →α-Fe + Fe₃Zr + Fe₂Nb_0.4Zr_0.6。Co 含量的增加抑制了退火后α-Fe晶相的形核,并促使Fe 3Zr化合物更易析出。Fe_81-xCo_xZr₇Nb₂B₁₀(x = 2, 4, 6) 合金的比饱和磁化强度( M_s) 和矫顽力 ( H_c) 随退火温度的变化趋势相同。530℃ 之前退火,随退火温度的升高M s增加并不明显 ; 530℃之后退火,M_s迅速上升。530℃ 退火,H_c达到最小值;高于530℃ 退火,H_c随退火温度的升高而增加。      

Giant Magneto-Impedance Effect in Fe96-xZrxB4 (x＝7 or 10)Nanocrystalline Ribbons

The total ribbon voltage of as-quenched and annealed Fe96-xZrxB4 (x=7 or 10) ribbons has been measured as a function of applied de field and drive current frequency. The experimental results show that both samples exist the optimum annealing temperature and optimum frequency at which the relative change in ribbon voltage is strongest, and the sensitivity of the magnetic response of the annealed Fe89Zr7B4 ribbon is two order of magnitude larger than that of the annealed Fe86Zr10B4 ribbon. The effect of magnetic properties and structural characteristics on giant magneto-impedance was discussed.     

Fe基非晶和纳米晶合金的热膨胀

将非晶Ｆｅ７３．５Ｃｕ１Ｎｂ３Ｓｉ１３．５Ｂ９和Ｆｅ９１Ｚｒ７Ｂ２合金经退火制成纳米晶合金，测量了淬火态和退火态样品的热膨胀曲线，研究了退火温度对热膨胀的影响，结果表明，纳米晶粒的形成导致居里温度Ｔｃ以下的热膨胀系数急剧增加，而Ｔｃ以上的热膨胀系数几乎不随退火温度变化。