改进型Helmholtz线圈及其磁场均匀性的分析

提出将Helmholtz线圈改为3个同半径的串联线圈,以得到改进型的Helmholtz线圈,经计算得到了改进型Helmholtz线圈磁场的简单公式,对公式的分析表明：改进型Helmholtz线圈的均匀磁场区比一般Helmholtz线圈大得多。     

3个共轴圆线圈形成的匀强磁场

分析了3个共轴圆线圈形成磁场的均匀性，得到了3个共轴圆线圈形成匀强磁场的条件，并且通过数值计算，全面展示3个共轴圆线圈磁场的均匀性．只要合理配置3个共轴圆线圈的大小、线圈中的电流强度和线圈之间的距离，3个共轴圆线圈的磁场在强度和均匀性方面都优于亥姆霍兹线圈的磁场。     

四个平行共轴等大载流方线圈磁场的均匀性分析

匀强磁场广泛应用于科学研究和工程技术.以毕奥-萨伐尔定律和磁场叠加原理为基础,建立了4个平行共轴等大载流方线圈磁场磁感应强度的表达式;用泰勒级数展开方法,发现了线圈系统磁场均匀性最好的条件;借助于数值计算,讨论了3种具体情况下线圈系统磁场的均匀性.结果表明:在最佳状态下,线圈系统能够在较大空间区域产生相对偏差小于0.01%、方向偏差小于0.01度的均匀性极高的磁场,并且磁场的均匀性和空间范围都明显优于方形亥姆霍兹线圈的磁场.     

均匀磁化介质椭球的退磁因子及退磁场

在椭球坐标系中求解了均匀椭球磁介质在匀强磁场中的磁化问题,得到了空间磁标势、磁场、介质中退磁场和退磁因子的表达式,研究了椭球形状与退磁因子的关系,分析了介质磁化率对退磁场方向的影响.结论为:椭球磁介质内的退磁场是匀强磁场;退磁因子的大小与椭球形状有关,与椭球大小无关,沿椭球长轴方向的退磁因子较小;一般而言退磁场方向与外磁场方向既不相同也不相反.铁磁质椭球内的退磁场几乎与外磁场反向.     

亥姆霍兹线圈磁场的探究

定量计算了亥姆霍兹线圈空间磁场的分布,并用Mathmatic进行空间模拟,形象地描述了亥姆霍兹线圈的空间磁场分布,同时就其均匀性与三线圈和载荷旋转圆盘的磁场进行了对比讨论.     

通电圆线圈轴线上磁场分布分析

由毕奥一萨伐尔定律导出通电圆线圈轴线上磁场分布公式．由该公式出发推出一个更适用的表达式,并据此分析了单线圈的磁场和双线圈合成磁场．用标准偏差理论分析了两线圈间距取不同值时,两线圈间磁场的均匀程度．     

平行共轴线圈的磁场特征研究与实验设计

通过计算机及相关的传感器和数据采集接口辅助,研究了平行共轴双线圈间距分别为0.5R,R,1.5R时,轴线方向磁场强度的分布规律及特征.从平行共轴双线圈间距为R的亥姆霍兹线圈所形成的均匀磁场出发,结合理论推导,自己设计并组装了三线圈实验装置,实现了平行共轴三线圈均匀磁场区域扩大、强度增强的实验设计,在一定程度上弥补了传统亥姆霍兹线圈磁场测量的不足并有助于对其深入的理解和研究.     

电磁感应中不闭合回路电势高低的判断和计算

讨论了导体棒在匀强磁场中切割磁感线,导体棒处在变化的磁场中,不闭合线圈处在变化的磁场中三种情况线产生的感应电动势的计算和两点电势高低的判断.     

宽平顶低横向场分量螺线管线圈设计

介绍了非均匀绕线技术和匀场环技术在螺线管线圈设计中的应用。分析表明这两种技术的采用可以减小线圈间隙的磁场波动、屏蔽线圈磁场的横向分量,从而设计出宽平顶低横向场分量的螺线管线圈。针对中国工程物理研究院12 MeV直线感应加速器螺旋管线圈的设计结果表明,非均匀绕线技术可以使线圈间隙处的轴向磁场波动减小约70%,匀场环的采用则能使线圈磁场的横向分量减小96.5%。     

感生电动势成因的分析研究

在均匀增加的匀强磁场中，有两个闭合金属线框，一个为圆形，另一个为正方形，线框平面均与磁场方向垂直，如图1、图2所示。     

基于螺线盘聚焦径向电子束的理论分析与仿真研究

对径向电子束在浸没式聚焦条件下的传输特性进行了理论分析,得到了束流传输过程中轴向扩张幅值与外加引导磁场强度之间的解析表达式。阐述了螺线盘在空间中任意一点产生磁场的理论,给出了通以相反方向电流的螺线盘之间磁场的分布规律。设计了一种基于螺线盘聚焦径向电子束的引导磁场系统,并对电子束的传输特性进行了仿真研究,结果表明径向电子束能够在设计的引导磁场系统下实现束流的稳定传输。     

Computer-assisted design of surface coils used in magnetic resonance imaging. I. The calculation of the magnetic field

For a number of reasons, it is desirable to fabricate coils which, for a known current, shall produce predetermined values of the magnetic field intensity at a number of points within a nuclear magnetic resonance imager. The calculation of the magnetic field intensity at a set of points involves the integration of the Biot-Savart equation for all components of the segments of conductor which make up the coil. This process in itself is a rather formidable task. When this process is parameterized in terms of coil diameter, coil spacing, etc. the problem is to determine the values of these parameters to match values of magnetic field intensities which are desired. The problem thereby increases in complexity to the point where, by ordinary methods, the problem becomes intractable. This note describes an algorithm and offers a computer subroutine to calculate magnetic fields for coils of arbitrary shape and complexity for fixed currents.     

用等均匀性曲面研究共轴三线圈磁场的均匀性

定义有均匀中心的矢量场的均匀度,通过解析和数值计算,得到了不同参数下的共轴三线圈的等均匀度曲面,找到了以前文献中未曾发现的均匀度最佳的参数值.     

球形线圈磁场均匀性的研究

研究非密绕球形线圈内部的磁场均匀性质.从圆形电流线圈轴线上的磁场出发,利用叠加原理和Mathematica软件的计算和符号推导功能,得到一个关于线圈内部磁场均匀性与其匝数的定量关系式,在此基础上通过实例说明设计球形线圈磁场均匀区的方法.     

目标场法在悬浮超导球体的球形线圈设计中的应用

文中把目标场法引入到悬浮超导球体的球形线圈设计中,根据目标场法产生均匀磁场的原理,通过离散化绕组来近似处理球形线圈在超导球体和球形线圈的间隙内产生均匀磁场的电流密度分布规律。利用有限元分析和验证,在超导球体与球形线圈之间的间隙内产生了具有很好均匀性的悬浮磁场,这会明显提高超导球体悬浮的刚度和稳定性。     

The Analysis of the Spurious Field about HL-2A Tokamak

To better the shielding of outer magnetic field when making the experiment on neutral particle measurement and neutral beam injection outside of HL-2A, it would be necessary to determine the distribution of outer magnetic field, which the excitation coils inducet. This experiment is done to measure and analyze the spurious field.     

Eddy current simulation in thick cylinders of finite length induced by coils of arbitrary geometry

Eddy currents are inevitably induced when time-varying magnetic field gradients interact with the metallic structures of a magnetic resonance imaging (MRI) scanner. The secondary magnetic field produced by this induced current degrades the spatial and temporal performance of the primary field generated by the gradient coils. Although this undesired effect can be minimized by using actively and/or passively shielded gradient coils and current pre-emphasis techniques, a residual eddy current still remains in the MRI scanner structure. Accurate simulation of these eddy currents is important in the successful design of gradient coils and magnet cryostat vessels. Efficient methods for simulating eddy currents are currently restricted to cylindrical-symmetry. The approach presented in this paper divides thick conducting cylinders into thin layers (thinner than the skin depth) and expresses the current density on each as a Fourier series. The coupling between each mode of the Fourier series with every other is modeled with an inductive network method. In this way, the eddy currents induced in realistic cryostat surfaces by coils of arbitrary geometry can be simulated. The new method was validated by simulating a canonical problem and comparing the results against a commercially available software package. An accurate skin depth of 2.76 mm was calculated in 6 min with the new method. The currents induced by an actively shielded x-gradient coil were simulated assuming a finite length cylindrical cryostat consisting of three different conducting materials. Details of the temporal-spatial induced current diffusion process were simulated through all cryostat layers, which could not be efficiently simulated with any other method. With this data, all quantities that depend on the current density, such as the secondary magnetic field, are simply evaluated.     

MFCG 2维磁流体力学程序中磁场计算的改进

 定子线圈中的电流在空间中产生的磁场是金属导体（套筒）膨胀压缩的主要对象,该磁场直接影响爆磁压缩发生器输出电流脉冲的大小。给出了面电流分布下2维磁场的计算公式,较点电流分布下的磁场公式更能细致准确地反映出磁场的变化。数值结果表明:面电流分布下的磁场公式不仅能准确地描述磁场的变化,而且计算效率大大提高,节约了计算时间。     

用于超导实验的背场磁体研制

在进行超导材料特性、交流损耗测量等超导实验时,需要为实验提供大小可变、均匀性好的背景磁场。文中对自行研制的背场磁体进行了测试研究,发现选择性对组合铜线圈供电能够提供合适的磁场,满足实验的要求。