不同直径玻璃包覆非晶微丝的制备及其磁性能

采用熔融拉丝法制备了直径范围分别在6.1～28.0μm和14.0～35.2μm之间的玻璃包覆非晶Fe基和Co基合金微丝, 测试了不同合金直径和不同玻璃包覆层厚度的玻璃包覆合金微丝样品的静磁性能. 结果表明: 轴向矫顽力和轴向剩磁比随着微丝直径的增大而降低, 随着玻璃包覆层的增大而升高; 径向剩磁比的变化趋势则相反. 微丝合金直径和玻璃包覆层厚度改变, 静磁性能变化的主要原因是作用在合金芯上的内应力的变化, 导致了具有不同磁畴结构的合金内芯区和合金外壳区体积比的改变.     

玻璃包覆Fe79-xCox Si8 B13非晶合金微丝的磁性能

实验以熔融纺丝法制备的玻璃包覆Fe79-xCoxSi8B13非晶合金微丝为对象,分析了微丝成分、尺寸以及玻璃包覆层去除对微丝静磁性能的影响。研究结果表明,玻璃包覆Fe79-xCoxSi8B13非晶合金微丝存在明显的磁各向异性,微丝轴向为易磁化方向;随着Co含量的增加,微丝的饱和磁化强度先增大后减小,Co含量为10%的Fe69Co10Si8B13非晶合金微丝饱和磁化强度最高,为1323emu·cm-3;对于玻璃包覆Fe69Co10Si8B13非晶合金微丝,当芯丝半径与玻璃包覆层厚度比值k约小于0.5时,其轴向磁滞回线为近矩形,表现出大巴克豪森效应;微丝的轴向剩磁比随k值的增大而减小,而微丝径向剩磁比保持很小,仅0.03左右;微丝的轴向和径向矫顽力均随比值k的增大而减小;当芯丝半径为10.9μm、玻璃包覆层厚度为9.7μm(k为1.12)时,去除包覆层后微丝的轴向矫顽力降低30%、径向矫顽力降低11%;而轴向剩磁比降低33%、径向剩磁比降低67%。     

玻璃包覆磁性合金微丝的介电性能分析与模拟

玻璃包覆磁性合金微丝的介电性能与非磁导电微丝的不同。分别从理论上分析了平行和随机分布的玻璃包覆磁性合金微丝/电介质复合材料的介电常数公式,并模拟了典型的玻璃包覆磁性合金微丝/橡胶复合材料的介电常数,探讨了不同频率及磁畴分布的玻璃包覆磁性合金微丝/电介质复合材料的介电性能的变化规律。结果表明:玻璃包覆磁性合金微丝的介电性能在中高频及微波频率范围内通过阻抗受其磁性能的影响,可以通过控制磁性能对其高频介电性能进行调控。     

含核壳异质结构6.5% Si高硅钢铁芯的制备与磁性能

以构建高磁感、低铁损、免轧制高硅电工钢铁芯为出发点,提出采用单辊甩带制备非晶铁硅合金薄带、微氧化法在铁硅合金粉末表面包覆高电阻率铁硅氧化物薄膜制备核壳异质结构高硅电工钢纳米粉末、放电等离子烧结快速成形制备颗粒间绝缘的高硅电工钢铁芯。研究了不同氧化包覆时间对SPS烧结试样密度、物相组成、微观结构和静磁性能的影响。研究表明,在氧化包覆5h烧结温度800℃工艺条件下,制备的6.5%Si高硅电工钢铁芯的静磁性能最佳,饱和磁化强度为128.84A.m2/kg、矫顽力为2.25kA/m、剩磁为3.47A.m2/kg。其饱和磁化强度与粉末压延法制备的高硅钢相当,但矫顽力降低了1/3。     

玻璃包覆磁性合金微丝复合媒质的微波介电性能

利用熔融拉微丝法制备了玻璃包覆非晶态磁性合金微丝，采用微波矢量网络分析仪及同轴线法测试了不同含量和排布的玻璃包覆磁性合金微丝-石蜡复合媒质的微波复介电常数，并和铁镍合金微丝-石蜡复合媒质的介电性能进行了比较。结果表明玻璃包覆磁性合金微丝复合媒质具有比相同含量的铁镍合金微丝复合媒质具有更低的复介电常数。圆周排列的玻璃包覆磁性合金微丝复合媒质在所测试的微波频率范围内具有电偶极子共振特征，一定含量的短玻璃包覆磁性合金微丝复合媒质具有电禁带结构。讨论了含量和排列方式影响玻璃包覆非晶磁性合金微丝复合媒质微波介电性能的原因。     

玻璃包覆铁基合金微丝的微结构与吸波性能

采用熔融纺丝工艺制备了玻璃包覆Fe基非晶合金微丝,通过X射线衍射分析研究了工艺条件对其微结构的影响,采用扫描电子显微镜分析了拉丝速度对微丝直径、玻璃包覆层厚度等结构参数和形貌的影响,利用微波矢量分析仪测量了2～18GHz的复磁导率和复介电常数,计算模拟了1mm厚度单层吸波材料的吸波性能.结果表明,通过冷却水急冷淬火可以获得非晶态结构,氩气保护可以防止合金氧化;拉丝速度提高有利于减小微丝直径,但玻璃包覆层的体积含量也随之增加;由该玻璃包覆Fe基非晶合金微丝设计的薄层吸波材料,在3～18GHz的宽频段内可以获得＜-2.5dB的微波吸收性能.     

玻璃包覆磁性微丝的制备及微波电磁性能

采用Taylor-Ulitovsky方法制备了Fe基和Co基非晶态玻璃包覆微丝,测试并分析了玻璃包覆微丝的微结构、微观形貌、静磁性能及其微波复磁导率和复介电常数.研究结果表明,通过改变拉丝速度,可以制备出直径6.3～23.5μm的非晶态玻璃包覆微丝;制备时通过水冷或气氛保护可以控制样品的物相组成.典型样品的各项异性等效场高达7.96×103A/m.Fe基样品磁导率在6.3GHz具有自然共振峰,Co基样品在所测频率范围没有共振峰,此测量结果和根据理论计算的自然铁磁共振频率基本一致.典型样品的相对微波复介电常数均低于25且随频率升高而降低.     

Fe-Si-B-P-Mo系高饱和磁感应强度非晶软磁合金

通过在Fe-Si-B-P合金体系中微合金化添加Mo元素,并提高铁含量,成功制备了具有较强非晶形成能力和优异软磁性能的非晶软磁合金。研究发现,Mo元素微合金化能有效提高合金的非晶形成能力,1%的Mo可以将该非晶合金体系的Fe含量极限提高到84%以上,从而得到了饱和磁感应强度(Bs)高达1.63 T的非晶合金。其中Fe80Si4.75B9.5P4.75Mo1非晶合金可以铸造形成非晶块体样品,临界直径达到1mm,饱和磁感应强度达到1.54 T,矫顽力为1.9 A/m。在整个成分范围内,该合金体系都具有1.9~5.1 A/m的低矫顽力和高于传统Fe-Si-B合金的饱和磁感应强度(Bs),具有较好的应用前景。     

退火对玻璃包覆Fe_(69)Co_(10)Si_8B_(13)非晶微丝磁性能及力学性能的影响

研究了退火对玻璃包覆Fe69Co10Si8B13非晶合金微丝磁性能和力学性能的影响。结果表明,退火温度为450℃时,矫顽力和剩磁比最小,轴向和径向矫顽力分别为1.8Oe和8.5Oe,比退火前降低了31%和36%,轴向和径向剩磁比分别为0.031和0.012,比退火前降低了74%和63%。当退火温度低于450℃时,芯丝抗拉强度基本保持不变,平均抗拉强度约2500MPa;当退火温度高于450℃时,芯丝抗拉强度迅速降低。未退火及退火温度低于450℃退火时,合金芯丝断口存在少量的脉状花样,且脉状花样及花样交叉的数量越多,所对应的芯丝抗拉强度越高;经500℃以上退火后,放射状撕裂区占芯丝断口大部分面积,芯丝表现出更大的脆性。在450℃20min条件下退火,微丝具有较低的矫顽力和较高的强度,综合性能优良。     

高温退火对高饱和磁感应强度Fe-Co合金磁性能的影响

对具有高饱和磁感应强度的1J22型Fe-Co软磁合金进行高温退火实验,并研究了其质量、磁性能随退火温度及时间的变化.结果表明,合金在500℃以下退火时,质量无明显增加且磁体磁性能并无降低;而当合金在500℃以上退火后,合金增重速率增加,且磁性能明显下降.当合金在600℃退火后,合金饱和磁感应强度Bs降至2178mT,矫顽力Hc增至76.1A/m.微观结构研究表明,高温退火后合金晶粒尺寸及形貌无明显变化,而合金表面完全生成Fe3O4.合金磁性能的降低是由氧化物的增多及杂质的引入造成的.     

Magnetic Properties and MCE in Heusler-Type Glass-Coated Microwires

We prepared Heusler-type Ni–Mn–Ga glass-coated microwires with total diameters, D, from 16 until 65 μm consisted of a metallic nucleus with diameters, d, between 10 and 31 μm and surrounded by the glass coating by the Taylor–Ulitovsky technique and measured the magnetocaloric effect, MCE, by the recently introduced precise method allowing the detection of a change in the temperature, ΔT, with an accuracy of below 10^?3 K. As-prepared microwires did not show ferromagnetic ordering at least near room temperature. Annealing above 773 K even for few minutes results in drastic change of magnetic properties: annealed sample show magnetization versus temperature dependence typical for ferromagnetic behavior with the Curie temperature about 315 K. Analysis of the X-ray diffraction allows us to identify presence of cubic phase in as-prepared state with the space group Fm3m and some amount of the tetragonal phase with space group I4/mmm. We measured directly the MCE, ΔT, in annealed samples. Before glass removal, we observed ΔT≈0.06 K for sample 1 and 0.08 K for sample 2. After glass removal of sample 1, ΔT increased until 0.22 K. Observed MCE is associated with magnetic (paramagnetic–ferromagnetic) and probably structural (austenite–martensite) phase transitions. Temperatures of the peak values of MCE were found to be of ～318 K and ～309 K, respectively Use of the glass-coating fabrication technique allows fabrication of composite thin wires from the brittle Ni–Mn–Ga alloy that cannot be cold-drawn to create fibers by conventional methods.     

Magnetic properties of sputtered Co-Ni-Fe-Pd films for thin-filmheads

Magnetic properties of Co-Ni-Fe-M (M=Rh, Ir, Pd, Pt) films prepared by sputtering are investigated. It is found that addition of Pd decreases the magnetostriction constant of the films from 1×10^-5 to around zero. On the other hand, addition of other elements, such as Rh, Ir, and Pt, increases it. However, coercive forces of Co-Ni-Fe-Pd films become more than 10 Oe when the magnetostriction is less than 2×10^-6. Multilayered films are investigated to obtain films with low coercive force. 43Co-27Ni-15Fe-15Pd films of 0.17 μm and Al₂O₃ films of 0.01 μm in thickness are layered time-sequentially. This multilayered film has saturation induction of 1.4 T, ≈0 magnetostriction, and a low coercive force of 1.5 Oe. Furthermore, Co-Ni-Fe-Pd films are ascertained to be as resistant to corrosion as Permalloy films. Recording heads with multilayered Co-Ni-Fe-Pd films with Al₂O₃ interlayers as magnetic cores have been fabricated. Recording characteristics were evaluated. These laminated Co-Ni-Fe-Pd/Al₂O₃ heads exhibit about 6 dB better overwrite than Permalloy heads     

高能球磨技术制备Fe_(78-x)MxSi_(13)B_9磁性材料

采用高能球磨技术制备Fe78-xMxSi13B9软磁非晶合金粉体,利用X射线衍射仪、差示扫描量热分析仪、扫描电镜和振动样品磁强计分析过渡金属元素M(Zr、Nb、Mo)的添加对合金粉体微观组织结构、热稳定性及软磁性能的影响。结果表明,Zr、Nb的添加有利于Fe-Si-B系合金的非晶转变,其最大过冷液相区ΔTx为70.62 K,玻璃转变温度Tg和开始晶化温度Tx分别为785.05、855.67 K;饱和磁化强度Ms为111 emu/g,矫顽力Hc约为2 028.443 A/m。     

优越磁性能的SrFe12O19微管的模板法制备

脱脂棉作模板, 采用溶胶-凝胶法制备并在不同温度下煅烧后制得了SrFe₁₂O₁₉微管, 并用原溶胶-凝胶法制得了六角型纳米SrFe₁₂O₁₉. 利用X射线衍射技术(XRD)﹑扫描电子显微镜(SEM)﹑透射显微镜(TEM)对样品的物相﹑形貌和粒径进行表征, 并利用振动样品磁强计(VSM)对样品进行磁性能研究. 结果表明：借助脱脂棉模板, 采用溶胶凝胶法制备了外径在8~13μm之间, 壁厚在1~2μm之间的SrFe₁₂O₁₉微管, 与原溶胶凝胶法制备的六角型SrFe₁₂O₁₉相比, SrFe₁₂O₁₉微管的矫顽力提高了30％左右, 比饱和磁化强度和剩余磁化强度提高了20％左右, 最终制得了矫顽力、比饱和磁化强度和剩余磁化强度分别为47.2kA/m、70.1A·m²/kg和42.4A·m²/kg的纯六方磁铅石型SrFe₁₂O₁₉微管, 并对微管的形成以及磁性能提高的原因做了解释.     

Magnetic properties and longitudinal recording performance of corrosion-resistant alloy films

This paper describes the magnetic properties, recording performance and corrosion resistance of sputtered CoCr alloy films and CoCrTa alloy films. The saturation magnetization of CoCr was 525 emu/cc and not affected by substitution of a small amount of Ta. CoCrTa films exhibit greater coercive force values than CoCr films. The maximum coercive force of CoCrTa was 1400 Oe at a thickness of 400A, whereas at a similar thickness the coercive force of CoCr was 900 Oe. The coercive force decreases linearly with temperature (25°C. to 125°C.) at a rate of 3.16 Oe/°C. for CoCrTa and 1.87 Oe/°C. for CoCr. Longitudinal recording performance at -3 dB signal level was 8386 flux reversals/cm (21,300 fci) and 11,063 flux reversals/cm (28,100 fci) for CoCr and CoCrTa respectively. The alloys exhibited corrosion resistance at 80% relative humidity and 65° C. for a two-week period equivalent to at least six years under ambient disc drive conditions.     

Structure and properties of melt-spun iron-silicon alloy filaments having single crystalline structure

Melt-spun iron-silicon (Fe-Si) alloy filaments were obtained by a rapid solidification method using an in-rotating-water spinning apparatus. The silicon content in the alloy composition was selected to be about 6.5% by weight, which is expected to have no magnetostriction and to show the lowest coercive force in the magnetic field. Heat-treated filaments were also investigated in terms of the structure and the mechanical and magnetic properties. It was found that the cross-sectional areas and structures of as-spun filaments were affected by processing conditions, such as spinneret diameter, throughput, etc. In the case of the filaments with diameters less than about 90 m, well-grown structures having primary dendrite arms oriented towards the direction of the filament length, can be observed in place of the polycrystalline structure. By means of high-temperature heat treatment, the filaments with the above structure were found to show single-crystalline structure without any clear boundary. The single-crystalline filaments were found to have good ductility to bending through 180 ° and excellent magnetic properties such as an almost perfect rectangular loop, low coercive force, and high saturation magnetic flux density in the d.c. magnetization curve.     

Microstructure and Magnetic Properties of Soft Magnetic Composites with Silicate Glass Insulation Layers

In this study, a new soft magnetic composite (SMC) material design scheme was put forward. According to this design scheme, SMC with silicate glass insulation layers was prepared by powder metallurgy with nanometer glass powder and micron iron powder. It can be annealed at high temperature for reducing residual stress. The magnetic properties were good. The maximum permeability, saturation magnetic induction, residual magnetic flux density and coercivity were 467, 1.47 T, 1.25 T and 394 A/m, respectively. The core loss versus alternating magnetic field frequency showed linear growth. The core loss was 4.4 W/kg at an induction level of 1 T, 50 Hz.     

Surface and Bulk Magnetic Hysteresis Loops of Co-Rich Glass Covered Microwires

The magnetization reversal process in the surface and volume areas of Co-rich glass covered microwires has been investigated. The value of the helical anisotropy has been determined in two wires with different thickness of glass covering. The dependence of the coercive field on the frequency of the external axial magnetic field was studied in the surface and volume of the microwires