Phase stability and magnetic properties of SrFe18O27 W-type hexagonal ferrite

W-type ferrite is a member of the hexagonal ferrite family and a potential permanent magnet material. However, its synthesis conditions are not fully understood yet. Samples were sintered either at 1400°C in air and quenched, or at 1300°C at reduced oxygen partial pressure. The precise stability conditions of this W-type ferrite were investigated in the temperature range of 1200°C-1400°C using thermogravimetry, XRD, and electron microscopy. At 1300°C, the ferrite is stable at oxygen partial pressures of . At more oxidizing conditions, the ferrite decomposes into M-type ferrite and hematite, while at more reducing atmospheres Sr₄Fe₆O₁₃ and magnetite are formed. The nonstoichiometry δ of SrFe_18−δO₂₇ was derived from thermal analysis data at 1300°C as function of oxygen partial pressure and was found to be mainly due to cation vacancies. Magnetization measurements show that this W-type ferrite exhibits M_s = 103 emu/g at T = 4 K, which agrees well with a ferrimagnetic spin arrangement according to Gorter's model. As alternative, Zn-substituted W-ferrite was found to be stable in air at 1200°C with a large M_s = 123 emu/g at 4 K.     

径向充磁表贴式正弦磁极电机转矩密度最大化研究

本文提出一种利用三次谐波削极,增加径向充磁表贴式正弦磁极永磁同步电机输出转矩而不增加转矩脉动的方法。根据永磁磁极形状可以将表贴式永磁电机分为弧形永磁磁极和面包形永磁磁极。对于所有极槽配合的径向充磁弧形永磁磁极永磁电机,注入最优三次谐波幅值为基波的1/6;但对于径向充磁面包形永磁磁极永磁电机,最优三次谐波幅值随极对数（P）、永磁体厚度和转子半径而变化,因此现有推导的最优三次谐波解析模型是不准确的,对于面包形永磁磁极永磁电机,此模型是无效的。本文推导了径向充磁面包形表贴式正弦磁极注入最优三次谐波幅值解析模型,可以在不提高转矩脉动的情况下最大程度的提高转矩。最后用有限元验证了模型的准确性。     

浸液复合磁化探伤装置产生的磁场分析

分析了浸液复合磁化探伤装置产生的合成磁场。结果表明,该合成磁场是个平面旋转磁场,故与受检工件侧面圆柱面同心的弧状裂纹无法用穿棒法检出,而工件的退磁因子与复合磁化法中所用的磁化方式无关。     

Co-W-C系合金的磁性及其应用

研究了Co粉、Co－W－C固溶体合金及WC－Co硬质合金的饱和磁化强度和矫顽磁力，提出了比娇顽磁力（Hsc）物理量。结果表明，用比饱和磁化强度4πσ和比娇顽磁力Hsc分别取代饱和磁化强度Ms和矫顽磁力Hc表征该系合金的磁性更为合理；该系合金的磁性受多种因素制约，其磁性与合金碳含量间不存在“单一性”对应关系，Ms值与抗弯强度σbb间也无“良好的”对应关系；用Ms鉴定硬质合金的碳含量和综合评估合金材质，例如鉴定人造金刚石生产专用硬质合金顶锤的材质是有条件和有限度的。     

稳恒磁场在金属相变过程中的应用

稳恒磁场在材料科学中的应用越来越受到关注。本文从稳恒磁场作用下生成的磁化力和洛伦兹力两个角度归纳了稳恒磁场对金属材料的固态相变和液态相变的影响。其中磁化力可以影响固态相变过程，形成取向．引起磁对流，进行磁性分离。而洛伦兹力可以抑制熔体的流动和波动，提高溶质离子在基体中的固溶度，另外，利用洛伦兹力还可以在电磁离心铸造中获得均匀的凝固组织。     

Fishtail magnetization in single crystal Tl2Ba2CuO6

We report extensive magnetization measurements on single crystals of Tl₂Ba₂CuO₆ superconductors. The fishtail magnetization is found to disappear above a characteristic temperature (60 K), which corresponds to a crossover temperature in the temperature dependence of the irreversibility line. Since the low temperature irreversibility field can be modeled by a Josephson coupled layered system, we propose that the fishtail magnetization in the Tl₂Ba₂CuO₆ system is due to dimensional crossover.     

Heat conduction in Ba1?xKxBiO3

We have investigated heat conduction of single crystal Ba_1–xK_xBiO₃ in the temperature range of 2–300 K and in a magnetic field of up to 6 Tesla. Temperature dependence of thermal conductivity(T) reveals the participation of both electrons and phonons with their relative contributions that depend critically on the potassium doping concentration. Crystals underdoped with potassium (samples with higherT _c) exhibit a strong suppression of and a glass-like temperature dependence. In contrast, those with a higher potassium content (lowerT _c) show an increase as temperature decreases with a peak near 23 K. Field dependence of(H) is also very sensitive to the level of potassium doping. Crystals exhibiting a large phonon contribution show an initial drop in(H) at low fields followed by a minimum and then a slow rise to saturation as the field increases. The initial drop is due to the additional phonon scattering by magnetic vortices as the sample enters a mixed state. The high field behavior of(H), arising from a continuous break-up of Cooper pairs, exhibits scaling which suggests the presence of an unconventional superconducting gap structure in this material.     

Flux pinning in high-Tc superconductive films

Magnetization measurements have been performed onc-axis oriented Y- and Gd-based superconductive films in a wide range of the temperaturesT (4.2–85 K) and magnetic fieldsH (0–8 T) withH c-axis. The influence of flux creep on both the temperature dependence of critical current densityJ _cm and the scaling behavior of flux pinning forceF _p has been discussed in detail. The experimental results show that Y and Gd films have different pinning mechanism. Flux pinning-force peaks in high fields are observed in Gd film at high temperatures and can be considered as evidence for collective pinning.     

Co47.6Fe20.4B21.9Si5.1Nb5-xZrx(x=0~5)合金的非晶形成能力和磁性能

采用铜模吸铸法制备了直径d为2~5mm的Co_(47.6)Fe_(20.4)B_(21.9)Si_(5.1)Nb_(5-x)Zr_x(x=0~5)合金。利用X射线衍射(XRD)、差示扫描量热仪(DSC)、振动样品磁强计(VSM)和显微硬度计分析合金的非晶形成能力(GFA)、磁性能及显微硬度。结果表明:该合金体系具有较好的GFA,随着Zr含量的增加,其GFA呈逐渐降低的趋势。Zr含量为0~2%(原子分数)时,能制得d为3mm的非晶合金;Zr含量为0~3%(原子分数)时,可制得d为2mm的非晶合金。直径2mm的棒状非晶合金(Zr含量为0~3%(原子分数))表现为明显的软磁性,饱和磁化强度Ms趋于一定值。该体系非晶合金均具有很高的显微硬度,Zr含量为3%(原子分数)时达到1420HV。