基于晶化动力学对Co70Fe10Si9B7Cu1Nb3非晶合金软磁性能的调控

钴基非晶合金作为应用广泛的软磁材料具有高磁导率、低矫顽力等优点,但饱和磁感应强度普遍偏低。为此,采用单辊急冷法制备Co₇₀Fe₁₀Si₉B₇Cu₁Nb₃非晶合金薄带,通过晶化动力学的计算对其晶化行为进行分析,并合理制定退火温度,实现对Co₇₀Fe₁₀Si₉B₇Cu₁Nb₃非晶合金软磁性能的调控。结果表明：Co₇₀Fe₁₀Si₉B₇Cu₁Nb₃非晶合金晶化反应过程中起始晶化反应激活能E_x1大于峰值晶化反应激活能E_p1,即晶体的形核过程比晶体长大过程更困难,但起始晶化反应温度T_x要低于峰值晶化反应温度T_p,因此选择...     

添加P对Fe78Si9B13合金非晶形成能力及软磁性能的影响

在惰性气体保护下制备了Fe78Si(9-x)B13Px(x=0,1,3,5,7)合金的楔形试样和非晶条带,用多种分析手段考察了合金的非晶形成能力和磁性能。结果表明,P的加入可提高合金的非晶形成能力,P含量为3at%时非晶厚度达497μm。合金的综合软磁性能则在P含量为1at%时达到最佳,此时的饱和磁感应强度上升至1.81 T,矫顽力为32.02 Oe。     

Fe73.5Cu1Nb3Si13.5B9非晶合金薄膜压磁效应的特征及负压磁效应现象研究

本文以Fe_73.5Cu₁Nb₃Si_13.5B₉非晶合金薄膜作为研究对象,研究了其压磁效应的特征及其负压磁效应现象。研究结果表明,淬态下的Fe_73.5Cu₁Nb₃Si_13.5B₉非晶合金薄膜在0-0.6KPa压力带具有显著的正压磁效应,随着压应力增大,薄膜电感值下降。当压应力σ=0.6kPa时,压磁效应值Si%达到5.5%;环境温度对压磁效应灵敏度有影响,在20~30 ℃范围内,压磁效应和灵敏度稳定性最好,随着环境温度升高,薄膜灵敏度和压磁效应值均降低;薄膜经过退火处理后,薄膜内应力状态会发生变化,当退火温度≧350℃时,薄膜的压磁效应类型由“正压磁效应”转变为“负压磁效应”,且随着薄膜中内应力降低,|Si%|值下降,且薄膜的压磁效应受环境温度影响减小。当退火温度为555℃时,|Si%|值最小,σ=0.66kPa时,|Si%|值0.5%;当退火温度达到薄膜的晶化温度时,薄膜的压磁效应受环境温度影响最小。     

Fe78Si9B13非晶箔快速微细电阻焊接

使用微型逆变式直流焊机对厚度为30 μm的Fe78Si9B13非晶箔进行快速微细电阻焊接分析,探讨了焊接工艺参数对非晶接头的影响.在焊接时间为2 ms、焊接电压为0.2V、焊接力为56 N时,获得的接头焊接效果良好,无裂纹、缩孔等焊接缺陷.接头平均抗剪强度可达632 MPa,经XRD检测接头仍为非晶态结构,具有实际工程应用价值.通过形核动力学分析,接头冷却速度高达7.9×106K/s,远高于Fe78Si9B13非晶的临界冷却速率,有效防止接头区晶化.     

纵向磁场退火处理对Fe73.7Si15.3Cu1Nb3B7合金组织结构和性能的影响

研究了纵向磁场不同温度退火处理对组成为Fe_73.7Si_15.3Cu₁Nb₃B₇的1k107B纳米晶合金带材的组织结构和软磁性能的影响。结果表明：在纵向加磁电流为150 A、退火温度区间为525～595℃时,合金的矩形比均在0.97以上,晶粒尺寸(D)和矫顽力(H_c)小幅度增加,最大磁导率(μ_m)则与之相反,损耗(P_s)在575℃时取得最小值(99 W/kg@50 kHz, 0.4 T);有效磁导率(μ_e)随着退火温度的升高呈先增加后减小的趋势;通过磁光克尔显微镜观察到纵向磁场退火后合金内部形成规则的平行于磁场方向的条纹畴,且随着退火温度的升高磁畴壁厚度逐渐增大。     

脉冲磁场处理Fe52Co34Hf7B6Cu1非晶的低温真空退火效应

对Fe₅₂Co₃₄Hf₇B₆Cu₁非晶合金进行了低频磁脉冲处理,研究低温真空退火对磁脉冲处理Fe_52Co₃₄Hf₇B₆Cu₁非晶软磁性能的影响.结果表明,磁脉冲处理导致非晶合金发生纳米晶化,析出晶态相α-Fe（Co）,晶粒尺寸为5-10 nm,形成的纳米晶粒弥散分布于非晶基体的双相纳米合金中.对磁脉冲处理的试样进行低温真空退火,可以进一步优化纳米合金的软磁性能,在100℃退火可以得到最佳的软磁性能.     

Fe66Ni1Al5Ga2P9.65B7.6Si3C5.75非晶合金循环预处理的热力学分析

采用XRD、DSC方法研究了循环预处理对Fe₆₆Ni₁Al₅Ga₂P_9.65B_7.6Si₃C_5.75非晶合金热力学参数的影响和晶化过程中析出相自由能的变化。结果表明:与淬火态相比,经循环预处理后晶化样品的Tg、Tx、Tp均有所降低,过冷液相区扩大,整个非晶的晶化阶段均有所提前;晶化析出相种类增加,晶化体积大幅增加,其中经冷热循环处理样品的晶化体积最大为60.197%;晶化相Fe₃P、AlNi₃C_0.5、Fe₂P的ΔGT与温度的变化成正比例函数。     

热处理条件对Fe78Si9B13非晶合金磁性能的影响

部分晶化法是一种具有实用前景的Fe78Si9B13非晶合金热处理方法。研究了不同热处理温度、热处理时间、保护气氛及冷却速度对Fe78Si9B13非晶合金磁性能的影响,探讨了获得具有一定恒导磁性能Fe78Si9B13非晶合金磁芯的方法。随热处理温度的上升,Fe78Si9B13非晶磁芯0A下的电感量单调下降,1A下的电感量先上升后下降。在一定保温温度和保护气氛下,随热处理时间的延长,Fe78Si9B13非晶磁芯0A下电感量单调减小,1A下电感量单调增加。较低的保温温度有利于在较宽保护气氛下获得所需磁性能的磁芯,过高真空度不利于获得所需的磁芯性能。不同冷却速度对Fe78Si9B13非晶磁芯电感量没有明显影响。     

Fe69Co8Nb7-xVxB15Cu1非晶条带热稳定性与软磁性能研究

基于Slater-Pauling曲线,运用"元素替代"成分设计法则,通过单辊旋淬工艺成功制备出Fe69Co8Nb7-xVxB15Cu1(x=0,2,5,7)非晶合金条带。利用XRD、TEM和DSC对合金系的非晶形成能力、热稳定性进行研究,并通过PPMS和B-H磁滞回线仪研究合金系的软磁性能。结果表明:随着V含量的增加,合金系的非晶形成能力、热稳定性和矫顽力逐渐降低,而饱和磁感应强度、居里温度逐渐增高;当x=2时非晶合金具有最宽两次晶化温度区间,热处理温区宽达225.9℃;当x=7时非晶合金具有最佳高温软磁性能,其饱和磁感应强度为0.96 T,矫顽力仅为8.95 A/m,而居里温度高达TC=349.42℃。     

Fe85Zr10B5三元非晶合金的非晶形成能力及磁热性能

采用单辊甩带法成功制备了Fe₈₅Zr₁₀B₅非晶合金,并对其非晶形成能力、磁性能和磁热效应进行了研究。结果表明：Fe₈₅Zr₁₀B₅非晶合金具有较大的过冷液相区宽度、γ参数和临界截面厚度,表明其优异的抗晶化热稳定性和非晶形成能力。Fe₈₅Zr₁₀B₅非晶合金在325 K的居里温度(T_c)下表现出3.26 J/(kg·K)的磁熵变峰值(-ΔS_m^peak),高于其他T_c相近的Fe基非晶合金。Arrott曲线和-ΔS_m^peak∝H^0.74的线性关系表明了Fe₈₅Zr₁₀B₅非晶合金典型的二级磁相变行为,这使该合金具有超宽的工作温度区间和较大的磁制冷能力(约546.4 J/kg)。F...     

New fracture morphology of amorphous Fe78Si9B13 alloy

The tensile fracture morphology of a brittle amorphous Fe-based ribbon was investigated by scanning electron microscopy（SEM）. The fracture surface consists of mirror, mist and river-pattern zones with crack propagating. The formation of nanoscale damage cavity structure is a main characteristic morphology on the fracture surface. Approaching the fracture source in the mirror, these damage cavities assemble and form the nanoscale periodic striation patterns, which are neither Wallner lines nor crack front waves. At shear deformation stage, the apparent surface energy yf of amorphous Fe78Si9B13 ribbon is much smaller than that of less-brittle amorphous alloys, which indirectly indicates amorphous Fe7sSi9Bl3 ribbon is perfectly brittle. The crack branching appears at the moment of final fracture due to the high crack propagating velocity.     

The corrosion behavior of amorphous and nanocrystalline Fe73.5Cu1Nb3Si15.5B7 alloy

The potentiodynamic polarization curves in 0.5 M NaCl solution before and after crystallization of Fe_73.5Cu₁Nb₃Si_15.5B₇ alloy have been studied in relation to the microstructure and alloy composition. It was shown that the corrosion resistance of the alloy strongly depending on these two factors. The observed decrease in corrosion resistance of the alloy after the heat treatment up to 480 °C in comparison to the corrosion resistance of the alloy in the as prepared state is attributed to the increased inhomogeneity of the alloy that coincides with the first appearance of Fe₃Si phase. Further heating (up to 600 °C) resulted in an increase in the number of Fe₃Si nanocrystallites and the appearance of a FeCu₄ phase. After annealing at 600 °C the lowest corrosion rate, 0.004 mm a⁻¹, was observed. Annealing of the samples at higher temperatures (>600 °C) induced formation of six crystalline phases which proved detrimental to the corrosion resistance of the Fe_73.5Cu₁Nb₃Si_15.5B₇ alloy. Solid corrosion products were identified on the surface of the samples after anodic polarization.     

Magnetic, electrical and plastic properties of Fe76Nb2Si13B9, Fe75Ag1Nb2Si13B9 and Fe75Cu1Nb2Si13B9 amorphous alloys

Influence of 1 h annealing in vacuum on magnetic, electrical and plastic properties of Fe₇₆Nb₂Si₁₃B₉, Fe₇₅Ag₁Nb₂Si₁₃B₉ and Fe₇₅Cu₁Nb₂Si₁₃B₉ melt spun ribbons were carefully investigated. It was shown that in all cases soft magnetic properties can be significantly enhanced by applying 1-h annealing at characteristic temperatures T_op. This optimization annealing causes that permeability increases more than 15-times and magnetic losses (tangent of loss angle) achieves a minimum in relation to the as quenched state. Using structural examinations (X-ray and HRTEM) it was shown that for the Fe₇₅Cu₁Nb₂Si₁₃B₉ alloy the optimized microstructure corresponds to a nanocrystalline αFe(Si) phase whereas in other alloys to a relaxed amorphous phase free of iron nanograins. As a consequence of this fact the Fe₇₆Nb₂Si₁₃B₉ and Fe₇₅Ag₁Nb₂Si₁₃B₉ alloys show higher plasticity in comparison to the nanocrystalline Fe₇₅Cu₁Nb₂Si₁₃B₉ alloy. Temperatures of the first stage of crystallization, and related diffusion parameters were determined using measurements of resistivity versus temperature with different heating rates.     

交流磁场处理对Fe78Si9B13非晶合金结构和性能影响的研究

利用X射线衍射仪(XRD)、振动样品磁强计(VSM)和差示扫描量热仪(DSC)对交流磁场处理前后Fe78Si9B13非晶合金条带的结构和性能进行了分析研究。XRD和VSM结果显示,随着交流电流的增大,合金的近邻原子间距离(d)和矫顽力(Hc)先减小后增大,但饱和磁感应强度则随交变电流的增大而变化幅度不大。d和Hc的变化是由合金中不均匀特征结构在结构磁驰豫过程中的相互作用所导致。由DSC曲线计算获得的表观激活能、局域激活能和局域Avrami指数显示,交流磁场处理提高了合金的初始晶化激活能和晶化反应的Avrami指数,降低了晶化反应的表观生长激活能。合金晶化行为的改变与磁后效导致的团簇原子对有序以及溶质原子与自由体积的扩散有关。     

Fe73.5Cu1Nb3Si13.5B9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Ｆｅ７３．５Ｃｕ１Ｎｂ３Ｓｉ１３．５Ｂ９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Ｆｅ２Ｂ;α－Ｆｅ相晶化表观激活能为４５２．３９ＫＪ／ｍｏｌ,Ｆｅ２Ｂ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Ｘｃ的增加而迅速境大,在α－Ｆｅ的体积分类为３０％～８０％,Ｆｅ２Ｂ的体积分