微量镍元素添加对铁基非晶/纳米晶磁芯软磁性能的影响

用单辊法制备的宽20 mm,厚25μm的Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9和Fe_(73.5)Ni_(0.3)Cu_1Nb_3Si_(14.2)B_8合金带材,绕制成外径为40 mm,内径为25 mm的环型磁芯,然后将磁芯在不同的温度下进行退火处理,研究了微量Ni元素添加对合金带材的晶化行为以及对横向磁场退火后的非晶/纳米晶磁芯的软磁性能的影响。结果表明:与Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9合金带材相比,添加微量Ni元素的Fe_(73.5)Ni_(0.3)Cu_1Nb_3Si_(14.2)B_8合金带材的一级起始晶化温度Tx1和一级晶化峰温度Tp1降低,其二级起始晶化温度Tx2和二级晶化峰温度Tp2升高,两级起始晶化温度之间的差值ΔTx增大;与横向磁场退火后的Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9非晶/纳米晶磁芯相比,横向磁场退火后的Fe_(73.5)Ni_(0.3)Cu_1Nb_3Si_(14.2)B_8非晶/纳米晶磁芯的起始磁导率μi和饱和磁感应强度Bs减小,矫顽力Hc增大;当测试频率f和最大磁感应强度Bm不变时,有效幅值磁导率μa增大,比总损耗Ps和矫顽力Hc减小;当测试频率f不变时,电感Ls和品质因数Q增大;当励磁电流I不变时,感应电动势E大。     

非晶软磁损耗研究

本文对Fe_5Co_(70)Si_(15)B_(10),Fe_(40)Ni_(40)P_(14)B_6,(Fe_(0.1)Ni_(0.35)Co_(0.55))_(78)Si_8B_(14)非晶在不同状态下的损耗进行了测量。并作了损耗分离,与1J_(79)(坡莫)晶态合金的损耗数据进行对比。观察到Fe_5Co_(70)Si_(15)B_(10)与1J_(79)损耗相比,非晶的反常涡流损耗在总损耗中所占比例大几倍到十倍。Fe_5Co_(70)Si_(15)B_(10)和Fe_(40)Hi_(40)P_(14)B_6二种非晶磁场热处理对损耗影响效应相差很大(几倍到十倍)。在部分淬态非晶样品中,观察到每周损耗随频率变化在某一频段内出现反常下降现象。对上述几种实验现象进行了解释     

压力对非晶态合金电阻的影响

本文计算了金属玻璃电阻率压强系数α_p,给出了相应的表达式。在0—12×10~8Pa压强范围内测量了金属玻璃Fe_(78)B_(22)、Cu_(25)Zr_(75)、Ni_(60)Zr_(40)和(Fe_(4.3)Co_(93.7)V_2)_(74)Si_8B_(18)的室温电阻随压强的变化关系,并与计算结果进行了比较。同时结合金属玻璃电阻温度行为的理论和实验结果,对推广的Ziman液态金属理论做了进一步的讨论。     

Ni_(80)Fe_(20)镀层对Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9非晶条带磁阻抗效应的影响(英文)

采用磁控溅射镀膜工艺,在Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9非晶条带的光滑面上溅射了130~650 nm厚的Ni_(80)Fe_(20)薄膜,制备了一系列Ni_(80)Fe_(20)/Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9复合结构样品.研究了镀层厚度对材料的镀层形貌、巨磁阻抗效应(Giant Magneto-Impedance,GMI)和磁滞回线的影响.结果发现,镀层厚度为260 nm厚时,样品的表面形貌最平整致密,最大磁阻抗比提高到33.0%.在玻璃基片上溅射了相同厚度的系列Ni_(80)Fe_(20)薄膜,其磁滞回线结果发现薄膜的各向异性方向随着厚度的增加由平行表面转变成垂直于表面.正是Ni_(80)Fe_(20)镀层各向异性的方向改变,影响了镀层与条带间的相互作用,进而影响复合结构样品的磁阻抗效应.     

高温下Fe_73Cu_1.5Nd_3Si_13.5B_9非晶合金结构演化的原位X射线研究

利用原位X射线衍射测量结构参数方法,研究了Fe_73Cu_1.5Nd_3-Si1_3.5B_9非晶合金热力学结构弛豫.通过Fourier变换得到不同温度的径向分布函数、近邻原子间距等原子构型的结构信息.研究结果表明,发生热力学结构弛豫时,大块金属玻璃的非晶结构保持稳定,但温度改变该非晶短程有序的次近邻局域原子构型.     

对X射线散射测定非晶合金原子分布函数的误差分析

在测定Pd_(77) Si_(16.5) Ag_(6.5)和Co_(42.9)Ni_(27.3)Fe_(7.8)Si_8B_(14)等几种过渡族金属—类金属非晶合金结构的基础上,本文对原始测量的计数强度误差和数据处理中引入的误差作了一般性的讨论。进而对数据处理中的一些主要参量人为地引入较大的误差,由付立叶变换具体地计算了它们分别对原子分布函数的影响,来说明在实际结构测量中各种误差对结果影响的大小。     

非晶态Fe_(79)B_(16)Si_5合金退火脆化与晶化

本文研究了非晶态Fe_(79)B_(16)Si_5合金的退火脆化行为,分析了此合金的脆化规律;通过脆化温度、晶化温度、脆化与晶化激活能的测定,探讨了Fe_(79)B_(16)Si_5非晶态合金退火脆化与晶化之间的联系。     

结构弛豫对铁基非晶合金退火脆化的影响

本文研究了铁基非晶合金 Fe_(78)B_(13)Si_9在退火过程中的延—脆转变行为,用等温加热的方法测定了 Fe_(78)B_(13)Si_9非晶合金的脆化时间、脆化温度和脆化激活能。用内耗法测定了 Fe_(78)B_(13)Si_9非晶合金结构弛豫温度范围及结构弛豫激活能。据脆化过程、晶化过程和结构弛豫过程温度范围和激活能的对比,认为 Fe_(78)B_(13)Si_9非晶合金的退火脆化与晶化无关。而与退火过程中的结构弛豫过程有关。     

Fe_(77.3)Cu_(0.7)Nb_(1.3)Si_(13.5)B_(7.2)合金磁性的研究

研究了非晶 Fe_(77.3)Cu_(0.7)Nb_(1.3)Si_(13.5)B_(7.2)合金在400～600℃的温度范围内退火后磁性的变化。磁性测量结果表明,获得高磁导率的最佳退火温度约540℃左右;经 X 射线衍射分析证实:在该温度下退火,非晶态合金已经晶化并形成体心立方结构的α—FeSi 固溶体,其晶粒直径约10～15nm。这种超细晶粒的纳米晶是高磁导率的根源。     

Structure and corrosion resistance of Al–Cu–Fe alloys

The microstructure and electrochemical properties of Al–Cu–Fe alloys with the atomic compositions of Al_(65)Cu_(20)Fe_(15),Al_(78)Cu_7Fe_(15)and Al_(80)Cu_5Fe_(14)Si_1have been studied.The alloys were produced by induction melting of pure elements with copper mold casting.The microstructure of the alloys was analyzed by X-ray diffraction and high-resolution transmission electron microscopy.The formation of quasicrystalline phases in the Al–Cu–Fe alloys was confirmed.The presence of intermetallic phases was observed in the alloys after crystallization in a form of ingots and plates.The electrochemical measurements were conducted in 3.5%NaCl solution.The electronic structure of the alloys was determined by X-ray photoelectron spectroscopy.The post corrosion surface of the samples was checked using a scanning electron microscope equipped with the energydispersive X-ray detector.It was observed that the Al_(65)Cu_(20)Fe_(15)alloy had the highest corrosion resistance.The improved corrosion resistance parameters were noted for the plate samples rather than those in the as-cast state.And the hardness of the Al_(65)Cu_(20)Fe_(15)alloy was significantly higher than the other alloy samples.     

非晶质磁性材料

迄今所用的非晶质磁性材料多是由磁性金属原子(M)与类金属原子(X)相组合的MaXb合金,例如,Fe_(80)B_(20)、(Co_(0～94)Fe_(0～6))Si_(10)B_(11)等。由于组成合金的金属原子与类金属原子的体积和重量相差悬殊,因此,当合金熔液急速冷却时,较易形成非晶质材料。也正因为这种悬殊差异使材料的磁性经时变化十分显著。例如,以Co为主体的CoFe-SiB系高导磁率非晶质材料,     

稀土Y对Fe_(71.4)Si_(13)B_(9.6)Mo_2Cr_1Cu_1P_2合金晶化行为及磁性能的影响

采用单辊甩带法,在大气环境下制备Fe_(71.4-y)Si_(13)B_(9.6)Mo_2Cr_1Cu_1P_2Y_y(y=0、0.0050、0.0077)合金条带,并将其绕制成环状铁芯,利用差热分析法、HT35铁芯测量仪和软磁性能测量仪等手段,分析添加微量稀土元素Y对Fe_(71.4_Si_(13)B_(9.6)Mo_2Cr_1Cu_1P_2合金晶化行为及磁性能的影响。结果表明,随着稀土元素Y含量的增加,合金条带的初始晶化温度逐渐降低,与没有添加稀土元素Y的试样相比,其最佳退火温度降低5~10℃;添加稀土元素Y可提高合金的磁导率和磁感应强度,其中,当y=0.0077时,所制合金的最大磁导率为5.5×10~5Gs/Oe,饱和磁感应强度达到1.192T;所制合金的矫顽力和损耗随稀土元素Y含量的增加均有所增大。     

Interfacial behavior of Fe76Si9B10P5/Zn0.5Ni0.5Fe2O4 amorphous soft magnetic composite during spark plasma sintering process

Fe_(76)Si_9B_(10)P_5/Zn_(0.5)Ni_(0.5)Fe_2O_4 amorphous composite with micro-cellular structure and high electrical resistivity was prepared by spark plasma sintering(SPS) at 487 °C. XRD and SEM results showed that the Fe_(76)Si_9B_(10)P_5 alloy powders remained the amorphous state and the composite was dense. A fusion zone at interface of Fe_(76)Si_9B_(10)P_5 cell body and Zn_(0.5)Ni_(0.5)Fe_2O_4 cell wall was observed by TEM, which also indicates the formation of local high temperature. The interface bonding based on the formation of local high temperature in SPS process was observed. It is believed that the tip effect of Zn_(0.5)Ni_(0.5)Fe_2O_4 nanoparticles promotes the local discharging and plasmas creation in the gaps, and the discharging energy forms an instantaneous local high temperature to complete the local sintering and the densification of Zn_(0.5)Ni_(0.5)Fe_2O_4 particles at a low nominal sinter temperature. Simultaneously, the local high temperature stimulates the adjacent gaps discharging, thus facilitate the continuous formation of new discharging path. Finally, sintering and densification of the amorphous composite is complete.     

Fe-B-Si非晶合金晶化过程分析

采用DSC法测定了铁基非晶合金Fe_(78)B_(13)Si_9在连续加热条件下的晶化温度。并用透射电镜、X射线衍射仅、俄歇电子谱仪对Fe_(78)B_(13)Si_9非晶合金的淬态组织及晶化过程进行了较深入的研究。在淬态非晶合金中发现了极少量的晶化相FeAl_3。晶化过程中会出现二种形式的亚稳晶化相FeB和Fe_3B。最终得到的稳定晶化相为α-Fe(si)+Fe_2B+FeSi_2。     

金属玻璃Fe_(75)Mo_3Si_5B_(17)的微蠕变和内耗研究

研究了金属玻璃Fe_(75)Mo_3Si_5B_(17)由室温至500℃范围内的微蠕变和内耗.发现在结构弛豫过程中在较低温度的微蠕变回复能达到零,反映滞弹性性质;在较高温度则不能达到零,反映粘弹性性质.微蠕变的平均激活能为1.73eV.整个内耗曲线随频率增加向高温移动,具有弛豫型特征,激活能有一较宽分布.讨论了微蠕变和内耗的微观机制.     

退火温度对Fe_(73.5)Co_(0.3)Cu_1Nb_3Si_(14.2)B_8合金带材磁性能的影响

用单辊法制备的宽为20 mm,厚为25μm的Fe_(73.5)Co_(0.3)Cu_1Nb_3Si_(14.2)B_8合金带材,绕制成外径为40 mm,内径为25 mm的环型磁芯,再将磁芯进行退火处理。分析了合金带材的晶化行为,研究了退火温度对合金磁芯磁性能的影响。结果表明,淬火态Fe_(73.5)Co_(0.3)Cu_1Nb_3Si_(14.2)B_8合金带材为非晶态,一级起始晶化温度T_(x1)为512.8℃,二级起始晶化温度T_(x2)为671.9℃,当退火温度升高到550℃,在非晶基体中析出Fe(Si)软磁相,形成了非晶和纳米晶双相共存结构。当退火温度低于550℃时,随着退火温度的升高,合金磁芯的初始磁导率μ_i和饱和磁感应强度Bs增大,矫顽力Hc减小;当测试频率f和最大磁感应强度Bm不变时,合金磁芯的有效幅值磁导率μ_a增大,比总损耗Ps和交流矫顽力Hc减小;当测试频率f不变时,合金磁芯的电感Ls和品质因数Q增大。     

The improvement of surface quality and thickness stability of Fe_(78)Si_9B_(13) melt-spun ribbons by melt overheating

The influence of melt overheating on the viscosity of the melt and surface quality of the Fe_(78)Si_9B_(13) melt-spun ribbons have been studied by using oscillating vessel viscometry, X-ray diffraction, transmission electron microscopy, and field emission scanning electron microscopy. A critical temperature Tc(about 1350℃) of the melt transformation was determined via viscosity measurements during overheating and subsequent cooling processes. The Fe_(78)Si_9B_(13) amorphous ribbons were produced through planar flow melt spinning in the temperature range of 1300–1550℃. A detailed analysis of overheating effects on the melt viscosity and surface features of the as-spun ribbons were performed to rationalize the correlation between the melt state and surface quality of the ribbons. It was found that the enhanced homogeneity of the melt can be achieved by the overheating treatment higher than the critical temperature, which in turn improves the surface quality and thickness stability of the Fe_(78)Si_9B_(13) melt-spun ribbons.     

In及In-1%Cu熔体团簇的"热收缩"现象

利用液态金属X射线衍射仪对纯In熔体及In 1 %Cu熔体分别在 2 80℃、390℃、5 5 0℃、65 0℃、75 0℃进行了实验研究 ,获得了二者的衍射强度、结构因子、双体分布函数、径向分布函数以及平均最近邻原子间距、原子配位数 .结果表明 ,随温度由 2 80℃升高到 75 0℃ ,两种熔体的平均最近邻原子间距r1 和原子配位数Ns都呈现出减小的趋势 ,原子团簇都出现“热收缩”现象 ,加 1 %Cu后的熔体团簇热收缩程度较之纯In熔体大 .在整个测试温度区间内两种熔体的热收缩都不是均匀的 ,而是在某个温度区间发生突变 ,收缩明显 ,纯In熔体的突变区间为390℃～ 5 5 0℃ ,In 1 %Cu熔体的突变区间为 2 80℃～ 390℃ ,加 1 %Cu后突变区间向低温转移     

TiO_2封装对铁基纳米晶磁芯软磁性能的影响

以钛酸四丁酯为前驱体,二乙醇胺为抑制剂,采用溶胶-凝胶法制备TiO_2溶胶,再用浸渍提拉法在Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9纳米晶磁芯表面制备TiO_2涂层,研究了TiO_2封装对纳米晶磁芯软磁性能的影响。结果表明,与TiO_2封装前相比,TiO_2封装后纳米晶磁芯的初始磁导率μ_i、最大磁导率μ_m、饱和磁感应强度B_s、电感L_s、品质因数Q和感应电动势E减小;剩磁B_r、磁滞损耗P_u和矫顽力H_c增大。     

TiO_2封装对铁基纳米晶磁芯软磁性能的影响

以钛酸四丁酯为前驱体,二乙醇胺为抑制剂,采用溶胶-凝胶法制备TiO_2溶胶,再用浸渍提拉法在Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9纳米晶磁芯表面制备TiO_2涂层,研究了TiO_2封装对纳米晶磁芯软磁性能的影响。结果表明,与TiO_2封装前相比,TiO_2封装后纳米晶磁芯的初始磁导率μ_i、最大磁导率μ_m、饱和磁感应强度B_s、电感L_s、品质因数Q和感应电动势E减小;剩磁B_r、磁滞损耗P_u和矫顽力H_c增大。