导体对磁场的屏蔽作用分析

分析了导体球壳对静磁场和对交变磁场的屏蔽作用,讨论了影响导体球壳对静磁场和对交变磁场的屏蔽作用的因素.     

不均匀磁场中的静磁波传播和导波光衍射理论

理论研究了不均匀静磁场对静磁体波传播和导波光布拉格衍射特性的影响。计算表明,在场强不均匀磁场中,静磁体波的振幅有所增加,从而可以明显提高导波光的布拉各衍射效率。此外,有望通过不均匀静磁场来控制衍射光的发散。     

电磁场作用下溶质元素在镁合金AZ61的分布

通过研究不同外场作用下镁合金AZ61的凝固组织，发现在静磁场单独作用时的晶界主要由镁基体和连续的网状化合物组成，在静磁场与交流电组合外场下的晶界主要由镁基体和网状及点状Mg-Al-Zn化合物组成，而在静磁场与直流电组合外场下晶界上的连续网状化合物彻底消失，化合物以不连续的薄片形态分布于镁基体上.相对于单一静磁场作用时，静磁场与电流共同作用时提高了镁合金晶内溶质含量，降低了晶界上的溶质含量. 关键词： 镁合金 静磁场 电流 晶内溶质含量     

一些复杂静电场与静磁场边界条件之论述

通过对几个具体的典型的复杂静电场、静磁场边界条件的求解,论述了求解复杂静电场、静磁场边界条件的一般方法.并就目前一些电动力学教科书上一些相关静电场、静磁场边界条件的结论进行了分析与讨论.     

用磁介质磁化理论的两种观点妙解静磁场——兼论与界线距离成反比分布的等量异种磁荷板的磁场

本文利用磁介质磁化理论的分子电流观点对一静磁场进行了求解,然后,根据静磁场的解利用磁介质磁化理论的磁荷观点求出了该场的极化磁荷分布,在此基础上,利用静磁场的叠加原理求出了一个磁荷分布——真空中与界线距离成反比分布的无限大等量异种磁荷板的磁场.     

轴对称的静磁场的两种简便解法

对于轴对称的静磁场,推导出了矢势的柱函数展开式,得出了用对称轴上的磁场表示轴外任意点磁场分布的级数展开式.最后,给出了用这两种方法求解轴对称静磁场的例子.     

静磁场对镁合金凝固组织的影响

镁合金是一种具有发展潜力的轻合金材料，但尚有待进一步的研究.通过实验研究静磁场作用下镁合金AZ61的凝固过程及其组织，发现在施加静磁场后镁合金的组织发生明显变化，晶界减薄，溶质元素含量在晶内显著增加，而在晶界处略有下降，因此静磁场改善了镁合金的组织，对提高镁合金的性能有重要意义. 关键词： 镁合金 静磁场 溶质元素     

铷-氙气室原子磁力仪系统磁场测量能力的标定

本文针对微弱磁场精密测量问题,在自主研制的铷-氙气室原子磁力仪系统上,探讨了两种磁场测量的方式,分别实现了对交流磁场与静磁场的测量,并对它们的磁场测量能力进行了实验标定.交流磁场测量原理是基于测量外磁场对~(87)Rb原子极化的影响,实验标定结果为在2100 Hz频率范围内磁场测量的灵敏度约为1.5 pT/Hz~(1/2),带宽约为2.8 kHz;静磁场测量原理是基于测量铷-氙气室内超极化~(129)Xe的拉莫进动频率,实验上首先测得超极化~(129)Xe的横向、纵向弛豫时间分别约为20.6和21.5 s,然后通过标定给出静磁场测量精度约为9.4 pT,测量范围超过50μT.相比无自旋交换弛豫原子磁力仪,该磁力仪在同一体系内实现了交流磁场与静磁场的测量,且交流磁场测量具有更大的带宽,静磁场测量可在地磁场下正常工作,将有望应用于地磁测量、基础物理等方面的研究.     

磁屏蔽罩在梯度静磁场中的受力研究

在有梯度的静磁场中,对由软磁材料制作的磁屏蔽罩所受的静磁力的量级进行了评估。使用有限元分析和实验测试的方法研究了纯铁方形屏蔽罩在梯度静磁场中的受力情况,结果表明：把内腔尺寸100mm×100mm×150mm、罩体厚度为20mm的方形屏蔽罩放置在强度约为0.2T、梯度为0.03T?m?1的磁场中,其所受的静磁力约为184N,与其自身重力相当;静磁力随磁场强度的升高而增大;有限元分析与实验测试结果的偏差在0.2T背景磁场下约为21%。因此,在考虑一定余量的情况下,使用有限元计算评估屏蔽罩在静磁场中的受力情况是一种有效和比较可靠的方法。     

横向静磁场对电磁悬浮液滴稳定性的影响

在利用电磁悬浮技术实现液滴悬浮的过程中,液滴内部往往存在剧烈对流、外部伴随快速旋转和质心的水平位移等不稳定因素;因此,实现液滴的稳定悬浮是完善电磁悬浮技术的关键.本文采用实验观测的方法,通过U形静磁场组件对液滴所在空间施加横向静磁场,利用高速相机记录了不同磁场强度下纯铜熔融液滴的振荡变形过程;分析了横向静磁场对悬浮铜液滴振荡频率、振幅以及旋转的影响.实验发现:对于熔融前的固态铜颗粒,若静磁场强度超过0.3 T,铜颗粒几乎以静止状态悬浮.熔融后,当施加0.15 T的静磁场,与未加静磁场时相比,液滴俯视图轮廓线拟合出的椭圆分别与x轴和y轴的交点坐标之差R-、椭圆面积A和椭圆长轴长度Dmax的振幅分别减小了25%,76%和60%;随着磁场强度的继续增加,振幅和频率继续减小,但在静磁场强度为0.3 T时,相比静磁场强度为0.2 T,频率增加了1 Hz.横向静磁场还抑制了悬浮铜液滴的旋转,当磁场强度增加到0.53 T时,悬浮液滴只在10?的角度范围内摆动.这些结果表明,施加横向静磁场能够有效提高悬浮液滴的稳定性.     

悬线式力矩器磁路设计中的有限元分析应用

光学头力矩器的空间磁场分布直接决定了力矩器的动态性能,对磁场进行准确分析是力矩器设计的前提。分析了悬线式力矩器的空间磁场产生机理,并采用有限元分析法进行了理论推导。以一款动线圈式二维对称型只读悬线式力矩器为例,采用有限元仿真软件（ANSYS）分析并设计了其空间磁场分布,对影响力矩器空间磁场分布的相关因素进行了分析。将采用有限元法对悬线式力矩器空间磁场仿真计算得出的力矩器动态特性参数与实测力矩器动态特性参数相比,其结果均符合力矩器的设计要求,证明基于有限元分析法的悬线式力矩器空间磁场设计是可行的。     

Polarization and transmission of microwaves in the magnetic suspension in the applied magnetic field

The production method of magnetic suspension consisting of ferromagnetic particles dispersed in cedarwood oil is presented at the beginning of this article. Next, the set-up for microwaves generation using a klystron is described. The main part of this paper concerning microwave transmission and polarization during its passage in samples of the produced magnetic suspension placed in a magnetic field is based on the following parameters: induction of this field, filling factor of magnetic suspension by ferromagnetic particles, dimensions of particles, viscosity of liquid carrier, and ratio of the magnetic field changes. Conducted investigations show that microwaves are damped and polarized in these magnetic suspensions. Obtained results are discussed and observed effects are explained by ordering of ferromagnetic particles in magnetic suspension by applied magnetic field.     

Single-domain magnetic nanoparticles as force generators for the nanomechanical control of biochemical reactions by low-frequency magnetic fields

The dynamics of single-domain magnetic nanoparticles cross-linked into multiparticle aggregates by organic ligands is considered. Mechanical factors of the effect of low frequency magnetic field on macromolecules attached to magnetic nanoparticles/aggregates within a suspension or gel are analyzed. The optimum conditions ensuring the best control over biochemical reactions in suspension by an external magnetic field (i.e., the ranges of frequency and magnetic field intensities, and the size of magnetic nanoparticles and shells covering them) are determined.     

On the stability of a free surface of a magnetic fluid under microgravity

We have investigated the behavior of a free surface of a suspension of ferrimagnetic particles in heptane under strongly reduced gravity. It was found that the free surface is destabilized when a homogeneous magnetic field parallel to the surface is applied. The strength of the critical magnetic field parallel to the surface varies with the volume concentration of magnetic particles in the suspension. We show that the destabilization of the fluid layer is forced by the influence of the suspension on the homogeneity of the magnetic field producing a magnetic field component normal to the fluid surface. The dependence of the critical magnetic field on the volume concentration of magnetic particles can be explained by applying the theory of the normal-field instability to this field component under conditions of strongly reduced gravity. The experiments were carried out at the drop tower ‘Bremen’ of the Center of Applied Space Technology and Microgravity (ZARM) in Bremen.     

Reentrant phases in compensated ferrocholesterics

Influence of magnetic field on orientation and magnetic properties of a compensated ferrocholesteric, a suspension of needle-like ferromagnetic particles in a cholesteric liquid crystal, was studied theoretically. A phase transition from a ferrocholesteric to a ferronematic state in a magnetic field oriented normally to the axis of the helical structure was considered. The dependences of the transition field to the ferronematic phase on the material parameters of the suspension and of the helical structure pitch and magnetization on the field strength were investigated. A possibility of existence of a reentrant ferrocholesteric phase was shown.

     

Lattice Boltzmann simulation of the two-dimensional flow of a magnetic suspension between two parallel walls under a non-uniform magnetic field

We have developed a lattice Boltzmann method based on fluctuation hydrodynamics that is applicable to the flow problem of a particle suspension. In this method, we have introduced the viscosity-modifying method, rather than the velocity-scaling method, in which a modified viscosity is used for generating random forces in lattice Boltzmann simulations. The viscosity-modifying method is found to be applicable to the simulation of a magnetic particle suspension. We have applied this method to the two-dimensional Poiseuille flow of a magnetic suspension between two parallel walls in order to investigate the behavior of magnetic particles in a non-uniform applied magnetic field. From the results of the snapshots, the pair correlation function between the magnetic pole and the magnetic particles and the averaged local particle velocity and magnetization distributions, it was observed that the behavior of the magnetic particles changes significantly depending upon which factor dominates the phenomenon in the balance between the magnetic particle–particle interaction, the non-uniform applied magnetic field and the translational and rotational Brownian motion.     

New aspects of energy transfer from an alternating magnetic field to a pendulum with ferromagnetic suspension

New data are presented about energy transfer from an alternating magnetic field to a pendulum with ferromagnetic suspension. For each frequency of the alternating magnetic field there is a certain field intensity for which energy transfer is maximum.     

Modulation of polarized optical radiation passing through magnetic liquid with nanotubes in the presence of magnetic field with variable direction

Technical Physics - Intensity modulation of polarized optical radiation passing through magnetic liquid and a suspension of magnetic liquid with nanotubes in the presence of magnetic field with...     

Two-dimensional Monte Carlo simulations of a suspension comprised of magnetic and nonmagnetic particles in gradient magnetic fields

Distributions of particles in a suspension comprised of magnetic particles (MPs) and nonmagnetic particles (NPs) under gradient magnetic fields are vitally important for the preparation of magnetic-nonmagnetic functionally graded materials (FGMs). In the present study, the effects of magnetic field gradient, magnetic interaction between MPs and concentration of NPs on the distributions of particles in the suspension are investigated using a two-dimensional Monte Carlo simulation. The results show that a gradient distribution of MPs is formed under gradient magnetic fields and increases with increasing the field gradient. However, as the interaction between MPs increases, the distribution gradient decreases, accompanied by the formation of chain-like MP clusters. Moreover, NPs are found to hinder the translation of MPs along the field direction. As the NP concentration increases, the translation of MPs becomes difficult.     

Quasi-2D Monte Carlo simulations of phase transitions and internal aggregate structures in a highly dense suspension composed of magnetic plate-like particles

The phase transitions and the internal aggregate structures of a highly dense suspension composed of magnetic plate-like particles with a magnetic moment normal to the particle axis have been investigated by means of the Monte Carlo method. The present study considered a quasi-2D system in order to clarify the influences of the volumetric fraction of particles and the magnetic field strength on particle aggregations and phase transitions. The internal structures of particle aggregates have been discussed quantitatively in terms of pair correlation functions, orientational pair correlation functions, nematic and polar order parameters. The main results obtained here are summarized as follows. When the influence of the magnetic interaction between particles is of the same order of that of the perpendicular magnetic field strength, the particles form column-like clusters, and the internal structure of the suspension shows solid-like structures. For the case of a strong applied magnetic field, the internal structure is transformed from solid-like structures into isotropic ones. However, as the volumetric fraction increases, the particles form brick wall-like structures under the situation of a strong applied magnetic field, and the internal structure exhibits solid-like ones. The brick wall-like structures also appear for a relatively weak magnetic field applied along the in-plane direction despite a slightly smaller volumetric fraction compared with the case of the perpendicular applied magnetic field.