Fe78Si13B9/铁氧体复合材料磁粉芯制备及其软磁性能

用Mn-Zn铁氧体溶胶对非晶Fe78Si13B9粉体包覆,模压成型制备了复合磁粉芯,并研究了复合材料磁粉芯的软磁性能.实验结果表明,铁氧体粉体在500℃×2h的热处理条件下逐渐生成,并在非晶Fe78Si13B9颗粒表面较好包覆;铁氧体溶胶的加入,大大提高了非晶Fe78Si13B9磁粉芯的品质因数Q值.当铁氧体溶胶量为7%、30℃的测试温度时,Fe78Si13B9/铁氧体复合材料磁粉芯的磁导率在1MHz时达到最大值32,Q值高达23.     

粉末挤出成型法制备FeSiAl/FeCuNbSiB磁粉芯

采用粉末挤出成型法制备了FeSiAl/Fe-CuNbSiB纳米晶磁粉芯,并讨论了FeSiAl粉复合量、粉胶质量比对磁粉芯磁性能的影响。结果表明粘结剂配方为硬脂酸1%、聚丙烯20%、石蜡79%,挤出成型粉胶质量比10∶1的FeSiAl/FeCuNbSiB纳米晶磁粉芯,磁粉芯密度达到4.69g/cm3。200目FeSiAl粉与300目FeCuNbSiB纳米晶粉复合,当磁粉芯磁粉质量配比为"200目FeSiAl粉30%+300目FeCuNbSiB纳米晶粉70%"、粉胶质量比为10∶1、44℃×0.5h石油醚脱脂、热处理温度160℃×1h时,磁粉芯取得最佳的软磁性能,磁粉芯中心频率f为600kHz,有效磁导率μe达到16.48,品质因数Q值为57.5;频率及温度的变化对磁粉芯的有效磁导率的影响小。     

铁硅铝磁粉芯研究

采用模压成型制备了FeSiAl磁粉芯。研究了粘结剂和绝缘剂及其添加量等对其磁导率、磁损耗、品质因数Q值及压溃强度的影响规律。结果表明,当绝缘剂含量为1.0%,粘结剂含量为3.5%时,在50kHz,0.05T时的性能达到:磁粉芯磁导率达到125,磁粉芯的压溃强度可达到19.24MPa,损耗不高于80mW/cm,品质因数为41。3     

Fe73．5Cu1Nb3Si13．5B9纳米晶磁粉芯磁性能研究

用Fe73.5Cu1Nb3Si13.5B9纳米晶粉体,加入一定量的塑化剂,通过模压成型方法制备磁粉芯.实验结果表明,在一定粒度范围内,磁导率μ随粉体粒度增大而增大,品质因数Q,随着粒度的增大而减小,且在一定频率范围内,μ呈现良好的频率稳定性;塑化剂质量百分含量α越大,μ越小.当α=6.5%时,μ达到最大值31.8.0～300kHz范围内,α与Q成反比;300～1000kHz范围内,α与Q成正比例关系;磁导率μ随着成型压力的增加而提高,相反,压力越大,Q值越小;磁导率随着磁粉芯测试温度的提高逐渐减小,0≤f≤700kHz范围内,温度升高,Q降低,700kHz≤f≤1000kHz范围内时,温度升高,Q值升高;随退火温度的增加,μ和Q均呈现先增大后减小的趋势.     

纳米晶软磁复合磁粉芯在中高频段性能研究

介绍了利用球磨后的FeCuNbSiB合金粉末冷压制作纳米晶复合磁粉芯的工艺.探讨了粉末粒度为80～200目,绝缘剂量为1%～8%时纳米晶复合磁粉芯的频率特性,直流叠加特性及品质因数Q.制备出的平均粒度为80目的磁粉芯有效磁导率μe在1MHz范围内恒为85,在100kHz时其峰值Q为65,在f=50kHz,Bm=50mT测试条件下其损耗为102mW/cm3.其功率损耗比传统铁粉芯,Fe-Ni粉芯小.     

粉末冶金法制备Fe-Si-Ni磁粉芯及其磁性能

采用熔炼-铸锭-球磨的方法制备了Fe-Si-Ni粉末,经过预退火热处理、绝缘包覆后将粉末压制成磁粉芯,并对成型后的磁粉芯进行去应力退火处理。对Fe-Si-Ni粉末及磁粉芯的性能系统地进行了检测分析。结果显示:经过预退火处理后的Fe-Si-Ni粉末具有较高的饱和磁化强度(Ms)。Fe-Si-Ni磁粉芯的有效磁导率(μe)在10~1000kHz的频率范围内变化很小,且随着Ni含量和退火温度的升高而增大。Fe-Si-Ni磁粉芯有着良好的直流叠加特性(dc-bias),当Ni≥5wt.%时,尽管磁导率百分比随着退火温度的升高逐渐减小,然而在外加直流磁场强度为50Oe时,磁粉芯的磁导率百分比均在70%以上。品质因数(Q)随着Ni含量和退火温度的升高逐渐增大,磁芯损耗随着Ni含量和退火温度的升高而减小。当Ni=8wt.%,退火温度为750℃时,磁粉芯在50kHz,50mT下的磁芯损耗有最小值312mW/cm3。     

Fe/FeSiB磁粉芯软磁性能研究

采用模压成型制备FeSiB非晶磁粉芯。并讨论了退火温度和时间、非晶粉体的粒径、不同粒径混合及Fe粉复合量等对磁粉芯磁性能的影响。结果表明,在200～500℃范围内退火,随着退火温度的升高,磁粉芯的μe先增大后减小,375℃时达到最佳,其最佳退火时间为2h。在100kHz～1MHz内,频率稳定性良好,其中心频率在500kHz附近;非晶粉体的粒径越大,磁粉芯的磁性能越好;粉体粒径为60～100目时,其μe达到最大;当粒径为60～100目与100～200目复合时,60～100目的FeSiB非晶粉体含量为60%时最佳。当复合Fe粉后,发现其软磁性能得到了明显改善,Fe粉量为30%时,μe达到32,Q值达到33。     

铁硅铝磁粉芯的磁特性研究

采用球磨制粉和模压成型方法制备了铁硅铝磁粉芯,并研究了其频率特性和直流叠加特性。结果表明,在测量的频率范围内（1～500kHz）,铁硅铝磁粉芯有效磁导率基本保持不变,而品质因数随频率的增加而增大,达到峰值后缓慢下降。在相同频率下,随着粉料粒度的减小,磁粉芯的有效磁导率降低,品质因数增加。铁硅铝磁粉芯具有良好的直流叠加特性,当直流偏磁场强度为1000e时,其有效磁导率变化率小于50％,且减小磁粉粒度可改善磁粉芯的直流叠加特性。     

Fe-6.5％Si/Fe73.5Cu1Nb3Si13.5B9纳米晶复合磁粉芯的制备及其软磁性能研究

采用Fe-6.5%Si粉末复合Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9纳米晶粉末制备了复合磁粉芯,并讨论了Fe-6.5%Si粉末复合量对复合磁粉芯磁性能的影响。结果表明,随着Fe-6.5%Si粉末的添加量从20%增加到80%,复合磁粉芯的密度几乎从5.46g/cm3线性增加到6.01g/cm3。复合磁粉芯的有效磁导率在20～500kHz的频率范围内具有良好的稳定性。随着Fe-6.5%Si粉末添加量从20%增加到80%,复合磁粉芯的有效磁导率几乎从33.7线性增加到38.3。复合磁粉芯的损耗随着Fe-6.5%Si粉末添加量的增加而增加。复合磁粉芯的直流偏置性能随着Fe-6.5%Si粉末添加量的增加而逐渐降低。当直流偏置场为7.96kA/m时,随着Fe-6.5%Si粉末添加量从0增加到80%,复合磁粉芯直流偏置性能从79.6%逐渐下降到62.2%。     

粉末挤出成型法制备FeCuNbSiB纳米晶磁粉芯

采用粉末挤出成型法制备了FeCuNbSiB纳米晶磁粉芯,并讨论了纳米晶粉体粒度对磁粉芯磁性能的影响。结果表明,粘结剂配方为硬脂酸1%、聚丙烯40%、石蜡59%采用粉末挤出成型法可以制备粉体与粘结剂比例为5∶1的FeCuNbSiB纳米晶磁粉芯;粉级搭配可提高磁粉芯密度,300、200与100目质量比为6∶3∶2的磁粉芯密度相对于300目FeCuNbSiB纳米晶磁粉芯提高了5%,达到了3.76g/cm2;200目FeCuNbSiB纳米晶粉为33%,180℃、1h热处理,磁粉芯有效磁导率μe为10.44、中心频率为600kHz、中心频率品质因数Q值为44。     

On the interaction of magnetic fields and magnetic shields

Some general mathematical expressions have been derived for the induced self and mutual inductances of the wires inside a cylindrical ferromagnetic shell. An application of these results is given. It is shown that the effect of the ferromagnetic shell on the inductances of the multiconducting wires is strongly geometry dependent; the closer the wires to the magnetic shell, the stronger the effect. For wires in the center of the cylinder, no significant result will be caused by the presence of the magnetic shell.     

Structural and magnetic behaviour of soft magnetic Finemet-type ribbons

Different kinds of magnetic anisotropies have been induced during the nanocrystallization process of Co- and Ni-rich amorphous ferromagnetic (Finemet) ribbons by the application of a constant stress or an axial magnetic field during the annealing process. Magnetization measurements have evidenced the presence od macroscopic anisotropy in the treated samples. The main goal of this work has been, after a careful DSC study, the structural analysis of the treated ribbons using X-ray Diffraction and Atomic Force Microscopy (AFM), detecting substantial differences in the crystallization state and grain size of the samples depending on the thermal treatment that was carried out. Moreover, AFM measurements revealed in all the treated samples a strong nanocrystallisation of the surface without evidences of amorphous matrix, which contrast with XRD measurements that have shown a high content of amorphous phase in the bulk of the ribbons. Magneto-optical Kerr effect measurements have been performed with the aim to elucidate the complex magnetic behaviour that is expected for the surface of the ribbons, measuring surface hysteresis loops that showed much higher coercive field values than that obtained in the bulk material.     

Capillary magnetic field flow fractionation and analysis of magnetic nanoparticles

This paper reports the purification and analysis of magnetic nanoparticles using capillary magnetic field flow fractionation, which utilizes an applied magnetic field oriented orthogonal to the capillary flow. To validate this approach as a separation method for nanometer-scale particles, samples of magnetic nanoparticles composed of either gamma-Fe2O3 (maghemite) or CoFe2O4 with average diameters ranging from 4 to 13 nm were prepared and characterized by transmission electron microscopy and SQUID magnetometry. Retention of the samples on the capillary was investigated as a function of solvent flow rate and the nanoparticle size and composition; the elution times of the nanoparticles are strongly dependent on their magnetic moments. We demonstrate the use of this method to separate a mixture of nanoparticles into size-monodisperse fractions. The magnetic moments of the particles are calculated based on analysis of the retention parameters and correlate with values obtained in separate SQUID magnetometry measurements.     

Fe-Si磁性颗粒/环氧树脂复合材料的冲击和磁学性能

采用双酚A型WSR-615和缩水甘油胺型AG-80环氧树脂为基体,以Fe-Si磁性颗粒为填料,通过热压成型方法制备了高含量磁性Fe-Si颗粒/环氧树脂复合材料。研究了环氧树脂基体的玻璃化温度和冲击强度及Fe-Si磁性颗粒含量对Fe-Si/环氧树脂复合材料的冲击强度和磁化强度的影响及温度敏感性。研究结果表明：随着磁性颗粒含量的增加,Fe-Si/环氧树脂复合材料的冲击强度和磁性能增加。当磁性颗粒体积分数由54 vol%增加到66 vol% 时,Fe-Si/环氧树脂的冲击强度和饱和磁化强度分别由4.03 kJ/m²和162.07 emu/g增加到7.16 kJ/m²和175.04 emu/g。Fe-Si/环氧复合材料在-60 ℃~140 ℃ 范围内的温度敏感性低,符合实际应用对复合材料稳定性的要求。     

The origin of magnetic birefringence and dichroism in magnetic fluids

The optical birefringence and dichroism observed in magnetic fluids when subjected to a magnetic field are generally ascribed to orientation of the particles, to anisotropic spatial ordering, or to string formation. Magnitude, concentration- and time dependence of the anisotropies predicted by these mechanisms are compared with the available experimental data. This leads to the conclusion that orientation of small aggregates and secondary aggregation of large aggregates into strings are the most likely cause of the large anisotropies. Orientation of single particles can be responsible for small anisotropies only. Field-induced spatial ordering has, at least optically, not (yet) been observed.     

Correlation between magnetic and electroacoustic parameters of audio magnetic tapes

Coercivity, squareness, remanent coercivity, coercivity factor, rotational hysteresis loss and its integral were measured on two sets of tapes (γ-Fe2O3and crO2) and related to their electroacoustic performances. The static magnetic measurements explain some of the properties of the particulate media: it was found that while CrO2rotates either coherently or incoherently depending on the direction of the applied field, γ-Fe2O3rotates incoherently, and the departure from the model of "fanning chain of spheres" can be related to the imperfections of the particles which are sources of demagnetizing fields. Good agreement with audio performance is found not only for parameters like coercivity and squareness, whose role is well known, but also with the other static parameters which were previously disregarded as ruling analogue recording.     

分散的Sm-Co永磁纳米颗粒的机械化学合成及磁性能

通过机械化学合成方法制备了矫顽力分别为2.95×106、2.83×106和8.60×105 A/m的分散的单晶纳米Sm2Co7、SmCo5和Sm2Co17硬磁颗粒。研究了球磨时间、原料配比和退火工艺等对所制备的纳米永磁颗粒的微观组织、结构和磁性能的影响。结果表明,机械化学球磨时间至少是4h或更长时间才能获得Sm-Co硬磁合金粉末。原料经过高能球磨后、未退火时,由于大部分颗粒为非晶结构,矫顽力较低,随着退火温度的上升,矫顽力增大,当退火温度为600℃时,达到最大值为2.83×106 A/m,然后,随着退火温度的进一步升高,矫顽力减小。Sm-Co纳米颗粒的粒径随着退火温度的降低而明显减小。     

Characterization of magnetic dispersions: Rheological, mechanical and magnetic properties

The rheological properties of magnetic oxide dispersions have been studied, varying dispersing agent, magnetic oxide, milling time and oxide loading level. Magnetic properties of handcoats as well as mechanical and magnetic properties of free films prepared from these dispersions have also been studied. The results show a good correlation between rheological, magnetic and physical properties. As a result, rheological measurements can be a convenient and powerful tool for evaluating the dispersibility of a magnetic oxide and the efficiencies of formulation components such as dispersing agents. Rheological measurements can also determine optimum oxide loading, optimum dispersant level, and optimum milling time. Results show that for a given oxide, there exists an oxide-binder ratio where mechanical, rheological and magnetic properties are optimized. This optimum suggests the existence of a well-defined oxide-binder structure. Results at oxide loadings lower and higher than the optimum can be explained, respectively, on the basis of individual particles with no long range structure formation and on the basis of possible clustering of particles.     

FeCo基纳米晶合金的结构及高频特性

研究了(Fe0.5Co0.5)73.5Nb2V1Si13.5B9Cu1合金经不同温度退火后的结构及磁谱曲线.XRD分析表明,随着退火温度的升高,晶化相体积增加;同时晶格常数减少说明更多的Co溶入到晶化相α-FeCo(Si)中.用阻抗分析仪测量了合金在1kHz-10MHz范围的磁谱曲线.结果表明,合金的截止使用频率可达103～106Hz,且随退火温度的升高,合金的截止使用频率逐渐提高,但初始磁导率μi和截止使用频率f0的乘积保持为常数,用畴壁运动方程及畴壁钉扎理论对此进行了解释.并讨论了进一步提高合金高频性能的途径.