水雾化制备Fe74Al4Sn2P10C2B4Si4非晶合金粉末及其磁粉芯性能研究

采用水雾化方法制备Fe7Al4Sn2P10C2B4Si4合金粉末,研究发现该合金具有强的非晶形成能力和高热稳定性,在粉末粒度小于400目时可以形成非晶态合金.采用该非晶粉末制备的磁粉芯在高频下品质因数显著高于MPP粉芯,说明该磁粉芯高频损耗较低.分析表明,非晶合金磁粉芯高频下损耗低的主要原因是电阻率较高.     

粉末状态对激光立体成形Zr55Cu30Al10Ni5块体非晶合金晶化行为的影响

基于金属熔体结构的遗传性, 激光熔池的快速熔凝导致粉末的晶化状态可能会对最终成形件的晶化产生重要影响, 理清其影响规律对于制备大块非晶合金具有重要意义. 本文选取等离子旋转电极法所制粉末和1000 K退火态粉末为沉积材料, 采用激光立体成形技术沉积Zr₅₅Cu₃₀Al₁₀Ni₅块体非晶合金, 考察了粉末中已有晶化相对熔池及热影响区晶化行为的影响. 结果发现, 原始粉末组织由非晶相及粗大的Al₅Ni₃Zr₂相组成; 当激光线能量较低时, 相应熔覆层的熔池和热影响区皆含有Al₅Ni₃Zr₂相; 随着线能量的提高, 熔池中Al₅Ni₃Zr₂相消失, 保持了非晶态, 但热影响区晶化加重, 并有大量Al₅Ni₃Zr₂相析出; 当采用退火态粉末时, 即使线能量较小, 相应熔覆层仍主要由非晶构成, 几乎无Al₅Ni₃Zr₂相析出. 这是由于原始粉末在退火时其微观结构发生重排, 与Al₅Ni₃Zr₂相关的原子短程/中程有序结构减少, 导致已沉积层非晶区的热稳定性提高, 不利于Al₅Ni₃Zr₂相析出. 可见, 提高线能量将会加剧非晶沉积体的晶化, 而粉末中的Al₅Ni₃Zr₂团簇相状态对Zr₅₅Cu₃₀Al₁₀Ni₅合金沉积层的晶化有重要影响.     

FeNiMo/SiO2复合粉芯的制备与软磁性能调控

目前金属软磁粉芯材料在高频电感等电子元件的应用前景广阔,然而其主要的构成元素属于过渡金属,表面易形成致密的氧化层,影响其软磁性能的调控.为了解决这些问题,本文引入H₂/Ar混合气体高温预处理工艺对FeNiMo原粉进行还原,证实了还原性气氛高温处理可以有效地去除材料表面的金属氧化物,增加金属单质的含量,进而显著提升FeNiMo原粉的有效磁导率.对预处理后的FeNiMo粉末进行SiO₂绝缘包覆,所获得的FeNiMo/SiO₂软磁复合材料表面包覆均匀;与未处理FeNiMo原粉包覆SiO₂所形成的软磁复合粉芯相比, H₂/Ar混合气体高温预处理后的FeNiMo/SiO₂具有更高的有效磁导率、更低的损耗.与同类其他软磁复合粉芯相比,通过H₂/Ar混合气体高温预处理工艺和绝缘包覆工艺的协同效应,所制备的FeNiMo/SiO₂复合粉芯具有优异的软磁性能.因此经过还原性气氛高温预处理工艺后的绝缘包覆可以更大程度地提升软磁粉芯复合...     

Kr2+辐照导致的Ca8LnNa(PO4)6F2(Ln=La,Nd和Sm)磷灰石结构陶瓷材料的非晶转变

采用传统固相烧结法成功制备出磷灰石结构材料Ca₈LnNa（PO₄）₆F₂（Ln=La，Nd和Sm），并通过常规X射线衍射（X-ray diffraction，XRD）进行表征确定三种样品都为单一相。在室温条件下用800 keVKr2+对三种样品进行辐照实验，辐照后的样品利用掠入射X射线衍射（grazing incidence X-ray diffraction，GIXRD）进行表征获取其表面辐照损伤层的结构信息。发现在实验辐照剂量范围内（1.0×1014~7.0×1014cm-2）三种样品都发生了从晶体结构到非晶结构的转变，不过三种样品的抗辐照非晶性能却有差异，抗辐照非晶能力大小关系是Ca₈LaNa（PO₄）₆F₂ > Ca₈NdNa（PO₄）₆F₂ > Ca₈SmNa（PO₄）₆F₂。这是由于在Ca₈LnNa（PO₄）₆F₂中，当镧系核素半径越小时，将有更大概率占据Ca（2）位置与F形成比Ca-F更弱的离子键。因此，镧系核素半径越小，辐照下将有更多的点缺陷保留下来，更容易发生非晶相变。     

Eu,Dy共掺杂SrAl2O4长余辉材料制备新工艺

活化Al-Sr合金粉末水解制备SrAl₂O₄长余辉材料的前驱体,并采用高温固相反应法制备出Eu,Dy共掺杂的SrAl₂O₄长余辉材料,对其微观结构和发光特性进行了研究。实验结果表明:前驱体中Al、Sr元素在微观状态下分布均匀,所制成的长余辉发光材料的发射主峰位于520nm附近,为典型的Eu²⁺离子4f5d-4f的特征发射,初始亮度达到18cd/m²,余辉时间长达46h。     

纳米La2(MoO4)3∶Eu/Fe3O4磁性荧光粉末的制备及用于指纹显现的研究

采用水热法和共沉淀法分别合成了纳米La₂(MoO₄)₃∶Eu荧光材料和纳米Fe₃O₄磁性材料，并利用透射电子显微镜、X射线衍射仪、荧光光谱仪表征纳米材料的形貌尺寸、晶体结构、荧光性能。经表征，纳米La₂(MoO₄)₃∶Eu荧光材料的微观形貌为片状结构，晶体结构为四方晶型，其发射光谱中出现了Eu3+的特征发射峰；纳米Fe₃O₄磁性材料的微观形貌为球形颗粒，晶体结构为立方晶型，并具有超顺磁性。然后，将以上两种纳米材料以一定比例混合均匀，制备了具有超顺磁性的La₂(MoO₄)₃∶Eu/Fe₃O₄纳米荧光粉末。经表征，该磁性纳米荧光粉末的微观形貌为片状结构与球形颗粒的混合，其发射峰位置未发生变化，而发光强度有所降低，但仍能够满足指纹显现的需要。最后，将制备的纳米磁性荧光粉末用于显现不同类型客体表面的潜在指纹。显现效果表明，对于光滑客体表面的指纹，使用磁性纳米荧光粉末与纳米荧光粉末的显现效果无明显差异；对于粗糙客体表面的指纹，使用磁性纳米荧光粉末能够清晰显现出指纹的细节特征，其显现效果明显优于普通纳米荧光粉末，并能够有效避免粉末扬尘现象。本研究制备的纳米磁性荧光粉末是一种理想的指纹显现材料，其指纹显现具有背景干扰低、显现效果好、适用范围广、无粉末扬尘等优点，在刑事案件现场具有广阔的应用前景。     

高压Ni77P23非晶合金自由体积变化的同步辐射研究

利用同步辐射高能X光散射的方法，研究了室温下非晶合金Ni₇₇P₂₃的自由体积的变化所引起的压缩行为的变化规律，通过傅里叶变换得到不同压力下的径向分布函数，并由此获得了不同压力下，该非晶合金的配位数、近邻原子间距等原子构型的结构信息. 研究表明，至直30.5GPa压力，Ni₇₇P₂₃合金仍保持稳定的非晶结构,根据Bridgman方程通过拟合数据，得到状态方程为-ΔV/V₀=0.08606P-3.2×10^-4P²+5.7×10^-6P³. 关键词： 非晶合金 自由体积 同步辐射     

非晶锂离子导体P2O5-0.7Li2O-0.4LiCl-0.1Al2O3的离子导电性与结构研究

本文研究了非晶锂离子导体P₂O₅-0.7Li₂O-0.4LiCl-0.1Al₂O₃的60目、120目、200目粉末、粉末压片和整片非晶在60至380℃的离子电导率和激活能。发现颗粒度减小能使离子电导率提高四倍以上,但不影响激活能,它归因于同一非晶相的界面效应。各样品在380℃等温热处理76h内的离子电导率和X射线衍射研究表明:颗粒度越小,晶化就越容易。整片非晶比粉末压片不仅电导率提高两个数量级,激 关键词：     

压力对Zr46.75Ti8.25Cu7.5Ni10Be27.5大块非晶合金玻璃转变和晶化动力学的影响

利用X射线衍射和差示扫描量热分析研究了高温高压下Zr_46.75Ti_8.25Cu_7.5Ni₁₀Be_27.5大块非晶合金的玻璃转变和晶化行为，结果发现压力降低了该大块非晶合金中的自由体积、热焓和晶化激活能. 关键词： 大块非晶合金 高压 差示扫描量热分析 玻璃转变     

退火处理Fe43Co43Hf7B6Cu1非晶合金的正电子湮没研究

对熔体急冷法制备的Fe₄₃Co₄₃Hf₇B₆Cu₁非晶合金进行了200,300,400和500 ℃保温30 min的退火处理,用正电子湮没寿命谱、X射线衍射、穆斯堡尔谱等方法研究了退火后试样的结构及结构缺陷变化.结果表明,在非晶合金的制备态,正电子主要在非晶基体相空位尺寸的自由体积中湮没,湮没寿命τ₁为158.4 ps,强度I₁关键词： 43Co₄₃Hf₇B₆Cu₁非晶')" href="#">Fe₄₃Co₄₃Hf₇B₆Cu₁非晶 退火处理 正电子湮没寿命 结构与结构缺陷     

New Fe-based amorphous compound powder cores with superior DC-bias properties and low loss characteristics

The Fe–Si–B–P–C metallic glassy alloys exhibit relatively high glass forming ability (GFA) as well as good soft magnetic properties such as ultra-low core loss. In this paper, the metallic glassy alloy (Fe_0.76Si_0.09B_0.10P_0.05)₉₈C₂ has been newly developed. A new Fe-based amorphous compound powder was prepared from FeSiB amorphous powder by crushing the amorphous ribbons as the first magnetic component and FeSiBPC metallic glassy powder by water atomization as the second magnetic component. Subsequently by adding organic and inorganic binders to the compound powder and cold pressing, the new Fe-based amorphous compound powder cores were fabricated. These new Fe-based amorphous compound powder cores combine the superior DC-bias properties and the excellently low core loss. The core loss of 453 kW/m³ at B_m=0.1 T and f=100 kHz was obtained when the mass ratio of FeSiB/FeSiBPC equals 3:2, and meanwhile the DC-bias properties of the new Fe-based amorphous compound powder cores just increased by 10% at H=100 Oe for μ=60 compared to those of the FeSiBPC powder cores. In addition, with the increase in the content of the FeSiPC metallic glassy powder, the core loss tends to decrease.     

High-frequency magnetic properties of soft magnetic cores based on nanocrystalline alloy powder prepared by thermal oxidation

FeSiBNbCu nanocrystalline alloy powder was thermally oxidized in an air atmosphere to enhance an oxide layer formation on the surface of the powder and subsequently toroidal shape FeSiBNbCu nanocrystalline alloy powder cores were prepared by compaction at room temperature. The phase change on the surface of FeSiBNbCu nanocrystalline alloy powder by thermal oxidation was analyzed and its effect on the high frequency magnetic properties of the compacted cores was investigated. By thermal oxidation, the formation of the oxide layer consisting of Fe₂O₃, CuO, and SiO₂ on the surface of FeSiBNbCu nanocrystalline alloy powder was enhanced and the thickness of oxide layer could be controlled by changing the thermal oxidation time. FeSiBNbCu nanocrystalline alloy powder core prepared from the powder treated by thermal oxidation exhibits a stable permeability up to high frequency range over 10 MHz. The core loss could be reduced remarkably and the dc-bias property could be improved significantly, which were due to the formation of oxide layer consisting of Fe₂O₃, CuO, and SiO₂ on the FeSiBNbCu nanocrystalline alloy powder. The improvement in high-frequency magnetic properties of the FeSiBNbCu nanocrystalline alloy powder cores could be attributed to the effective electrical insulation by oxide layer between the FeSiBNbCu nanocrystalline alloy powders.     

Comparative study on the high frequency performances of the easy-plane FeNi@SiO2 powder soft magnetic composite

In this work, an easy-plane FeNi@SiO₂ powder soft magnetic composite (SMC) was imitated and fabricated and its high frequency magnetic properties were comparatively investigated with a non-easy-plane composite. Due to the planar distribution of easy magnetization axes, the easy-plane composite exhibits a constant permeability of 38 up to 100 MHz. Moreover, the easy-plane SMC exhibits a lower core loss at higher frequencies. Loss separated results show that the hysteresis loss plays a dominant loss component in the composite, rather than dominant excess loss in the non-easy-plane powder composite. These results indicate that, compared with non-easy-plane powder composite, the easy-plane powder composites exhibit comprehensive advantages of higher permeability, wider effective operating frequencies and lower loss, which suggest that the use of easy-plane ferromagnetic powder is a promising and efficient measure to develop a new generation of soft magnetic composites for higher frequency application.     

Li2SO4—Li2B2O4,Li2SO4—(NH4)2SO4赝二元系相图及离子导电性研究

本文用差热分析和X射线衍射方法对Li₂SO₄-Li₂B₂O₄和Li₂SO₄-[NH₄]₂SO₄两个赝二元系相图进行了研究。Li₂SO₄-Li₂B₂O₄是共晶体系,共晶温度为720℃ 关键词：     

非晶态离子导体Li2B2O4晶化前期的离子导电性

本文研究了非晶态离子导体Li₂B₂O₄的离子电导率与温度的关系,特别着重于晶化前期的离子迁移特性。当温度低于T_K(≈310℃)时,离子电导率遵从Arrhenius关系。当高于晶化温度(≈411℃)时,以晶态中的离子迁移为主。在T_kc时,电导率偏离热激活机制呈反常增高。我们把这一过程称为晶化前期过程。可以用自由体积模型进行描述。晶化前期又可分为两部分:当温度低于、T_p(≈380℃)时,由于自由体积的重新分布,导致了电导率的增高;当T>T_p时,出现了少量微晶,但晶化量小于5%,由于非晶母体与微晶之间的界面效应使得离子导电性显著增强。可以通过室温淬火,把晶化前期非晶态的状态保持到室温,从而有可能制备出离子电导率高于纯非晶态的材料。 关键词：     

First-principles investigation of Mg2Ni phase and high/low temperature Mg2NiH4 complex hydrides

Using a density functional approach calculation, the structural, energetic and electronic properties of Mg₂Ni phase as well as its high/low temperature (HT/LT)-Mg₂NiH₄ complex hydrides are systematically investigated. The optimized structural parameters including lattice constants and atomic positions are very close to the experimental data determined from X-ray and neutron powder diffraction. A detailed study of the electronic structures including the energy band, density of states (DOS) and charge density distribution reveals the orbital hybridization and characteristics of bonding orbits within Mg₂Ni and its hydrides. Based on the calculated results of the reaction heat of hydrogenation, enthalpy of formation and energy cost to remove H atoms, it is found that the formation ability of LT-Mg₂NiH₄ is higher than that of the HT phase during the hydrogenation of Mg₂Ni alloy; moreover, LT-Mg₂NiH₄ has a relatively higher structural stability than HT phase, which is also well explained through the DOS and the charge distributions of HT/LT-Mg₂NiH₄ phases.     

高Br纳米晶Fe73.5Cu1Nb3Si13.5B9合金的损耗行为

在f=10—20000Hz和B_m=0.1—1.0T范围内,测量了高B_r纳米晶Fe_73.5Cu₁Nb₃Si_13.5B₉合金的损耗.把总损耗分离为磁滞损耗、经典涡流损耗和过剩损耗.测量结果表明,每周损耗随频率的变化表现出明显的非线性行为.用Bertotti的损耗统计理论描述了这种非线性行为.大致在两个频率范围内,有两种不同的描述方式. 关键词：     

Microstructure and magnetic properties of Fe72.5Cu1M2V2Si13.5B9 (M=Nb, Mo, (NbMo), (MoW)) nanocrystalline alloys

The microstructure and magnetic properties of Finemet-type Fe_72.5Cu₁M₂V₂Si_13.5B₉ (M=Nb, Mo, (NbMo), (MoW)) alloys have been systematically studied. Results show that the nanocrystalline alloy with M=NbMo has the smallest grain size of about 8 nm. The order of the effect of Nb, Mo and W additions in decreasing the α-Fe grain size in nanocrystalline alloys is Nb>Mo>W. The best DC soft magnetic properties are obtained in the alloy with M=Nb. In the case of AC soft magnetic properties, the Nb alloy also exhibits a very low core loss comparing with typical Finemet alloy. Therefore, the Nb alloy is suitable for use as a transformer core material. In addition, it is shown that a narrow grain size distribution and a uniform dispersion of α-Fe grains in the amorphous matrix are very crucial for the development of new Finemet-type nanocrystalline alloys with good soft magnetic properties.     

Microstructure and magnetic properties of bulk amorphous and nanocrystalline Fe61Co10Zr2.5Hf2.5Nb2W2B20 alloy

The microstructure and magnetic properties, i.e. the initial magnetic susceptibility, its disaccommodation, core losses and approach to ferromagnetic saturation of the bulk amorphous and partially crystallized Fe₆₁Co₁₀Zr_2.5Hf_2.5Nb₂W₂B₂₀ alloy are studied. From X-ray, Mössbauer spectroscopy and electron microscopy studies we have stated that all samples in the as-quenched state are fully amorphous. However, after annealing the samples at 850 K for 30 min the crystalline α-FeCo grains embedded in the amorphous matrix are found. Moreover, from Mössbauer spectra analysis we have stated that the crystalline phase in those samples exhibits the long-range order. The alloy in the as-quenched state shows good thermal stability of the initial magnetic susceptibility. Furthermore, the intensity of the magnetic susceptibility disaccommodation in the rod is lower than in the ribbon. It is due to low quenching rate during the rod preparation which involves the reduction of free volumes. From the analysis of the isochronal disaccommodation curves, assuming the Gaussian distribution of relaxation times, we have found that activation energies of the elementary processes responsible for this phenomenon range from 1.2 to 1.4 eV. After the annealing of the samples the initial susceptibility slightly enhances and disaccommodation drastically decreases. From high-field magnetization studies we have learned that the size of structural defects depends on the quenching rate (the shape of the samples) and changes after annealing.