过饱和铁芯二维磁场的数值计算

本文用有限元法和差分法分别采用拟牛顿迭代和低松弛系数迭代,计算了过饱和铁芯变压器的磁场,均取得稳定的收敛解。文章还对这两种方法作了比较。最后,给出过饱和铁芯托卡马克极向场系统二维磁场计算示例。     

基于Python的托卡马克磁场快速计算程序

本文编写了一个快速计算托卡马克磁体磁场的程序。该程序基于Python语言编写,使用可视化界面来输入磁体参数,建立模型;采用解析方法计算磁场;并采用图形界面展示磁场计算结果。通过与有限元软件磁场计算结果对比表明,该程序的计算速度可达到有限元软件的十倍左右,可快速进行托卡马克磁体系统的建模与磁场计算,有利于更快地开展托卡马克磁体系统的设计与分析。     

J-TEXT铁芯模型欧姆放电数值模拟

本文采用有限元软件分析了J-TEXT的完整铁芯模型、等离子体电流丝模型和简化中心螺线管模型的磁场特征,确定了简化中心螺线管的几何参数与电流,之后把有限长度中心通电螺线管参数加到托卡马克模拟程序TSC模型中,模拟J-TEXT的欧姆放电过程,获得了欧姆放电电流、电子温度、等离子体密度、等离子体电流,磁轴位置等参数。模拟结果与实验结果数据相符,为具有铁芯结构的托卡马克放电模拟提供了有效手段。     

托卡马克装置的击穿条件

在CT-6B托卡马克实验装置上研究了充气气压、环向磁场、杂散磁场、环电压等放电条件对击穿的影响。发现垂直方向和水平方向的杂散磁场对击穿影响不同。指出实验结果与汤生放电模型的偏离。用Monte-Carlo方法解出击穿阶段电子分布函数,对汤生模型公式作出修正。 关键词：     

HT-7铁芯超导托卡马克等离子体电流和水平位移多变量反馈控制

对有双层低温厚壁铜壳的铁芯超导托卡马克等离子体电流和位移反馈控制进行了分析,采用一种新颖的方法对铁芯饱和而引起的电磁参数非线性和时变性进行了处理,用等效正反串线圈模型代替厚壁铜壳,从而建立了HT-7超导托卡马克等离子体电流和水平位移反馈控制状态方程模型.并采用了检测中间状态变量进行补偿而达到解耦的目的,设计出了托卡马克等离子体位移和电流反馈控制系统,在实验中得到了很好的结果.该方法大大减少了反馈控制的计算工作量并提高了响应速度.使得铁芯、厚壁铜壳与线圈之间的强耦合给等离子体控制带来的困难迎刃而解. 关键词：     

铁芯变压器对极向场的影响

本文叙述了对HL-1装置铁芯变压器作无限长均匀磁化假定后,给出了极向场线圈(包括等离子体电流环)在空气区产生的磁场解析表达式,及数值计算,并在一比四模拟变压器上做了实验,计算结果与实验结果符合。     

HT－7托卡马克中等离子体平衡研究

本文解决了二维轴对称近似下带铁芯的托卡马克中等离子体平衡问题，计算了ＨＴ－７托卡马克中的等离子体平衡位形以及极向场系统的非线性电感和垂直场系数。最后应用Ｋｉｒｃｈｈｏｆｆ方程组和平衡垂直场公式得到了一组等离子体、加热场和垂直场线圈的电流波形的自洽曲线。     

高温超导磁浮电磁铁特性分析

构建了超导悬浮磁铁的三维模型,使用ansoft对电磁铁的三维模型进行电磁场仿真,分析了超导线圈电流、悬浮气隙、横向位移偏差、铁芯长度、铁芯高度等的变化对磁浮列车悬浮力和导向力的影响.结果 表明,超导线圈通入不同的电流,悬浮电磁铁的磁场饱和度出现明显的变化,随着超导线圈通入的电流和悬浮气隙、横侧偏移的变化,悬浮力和导向力出现不同的变化特征.同时铁芯高度的增加能有效缓解电流增大时电磁铁铁芯中部的磁场饱和度,进而能够增大悬浮力,提高悬浮性能.     

HT—7托卡马克中等离子体平衡研究

本文解决了二维轴对称近似下带铁芯的托卡马克中等离子体平衡问题，计算了ＨＴ－７托卡马克中的等离子体平衡位形以及极向场系统的非线性电感和垂直场系数。最后应用Ｋｉｒｃｈｈｏｆｆ方程组和平衡垂直场公式得到了一组等离子体，加热场和垂地直场线圈的电流波形的自洽曲线。     

永磁导轨磁场的三维有限元计算及纵向磁场不均匀性分析

在高温超导磁悬浮车永磁轨道中,由于轨道的连接处存在缝隙,将影响永磁轨道纵向磁场的分布。文中用CEDRAT公司的Flux3D电磁计算软件,建立了高温超导磁悬浮车导轨磁场的三维计算模型。该模型的计算结果与实验结果一致性较好。用该模型计算并分析了分段导轨连接处无缝隙和具有1mm、2mm和5mm缝隙时的导轨磁场;并分析了纵向磁场的不连续性。     

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For simplifying the calculation the magnetic distribution on tokamak, some two-dimensional analytic models including the effect of the iron core were established, such as the infinite long iron core model and the spool model. The assumptions of these two-dimensional analytic models lead to different results with the actual magnetic field due to the distinctive boundary condition. In order to accurately calculate the three-dimensional magnetic field distribution in the tokamak with iron core, a three-dimensional numerical finite element model was established based on J-TEXT tokamak. In two conditions, where the total toroidal current is nonzero or zero respectively, more comparison were carried out between the derived results of two-dimensional models and the results at different toroidal positions in three-dimensional models. Furthermore, the toroidal asymmetry of the magnetic field distribution of the three-dimensional model of tokamak with iron core was investigated. The results indicate that the three-dimensional construction of iron core causes the toroidal asymmetric poloidal magnetic field and the difference between the two- and three-dimensional models in the condition with total current of nonzero. However, in the condition with total current of zero, the intensity of toroidal asymmetric is reduced and the difference between the two- and three-dimensional models is smaller.     

Observation of a light-induced nonohmic current in a toroidal-moment-possessing nanostructure

We report on the first observation of light-induced nonohmic current in a semiconductor nanostructure. The effect is revealed in an unbiased asymmetric InAs quantum well under excitation by far-infrared laser radiation in the presence of a tilted magnetic field. It is interpreted in terms of a nonzero toroidal moment of a two-dimensional electron gas.     

Current clamp at zero level in JT-60U current hole plasmas

It is found that no current is driven in a central region of a tokamak plasma once the central current density becomes nearly zero ("current hole"), in spite of high electric conductivity, at the current drive by a toroidal electric field and a radio-frequency wave in experiments on the JT-60U tokamak. This is a new, stiff, self-organized structure of a magnetic field in an axisymmetric toroidal plasma.     

HL-2M装置周边磁场分布及NBI束线磁屏蔽分析

采用电磁场模拟软件CST Studio中的电磁工作室计算了HL-2M装置纵向和极向场线圈在装置周边的磁场时空分布。计算结果表明,在中性束注入器中性化室及离子源引出区域的磁场超过2-10^-3T,需要在注入器的中性化和离子源区域采用磁屏蔽结构。利用CST软件模拟计算了基于纯铁材料的NBI 注入器离子源及中性化区域的磁屏蔽罩内的磁场分布。     

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The time and space distribution of the toroidal and poloidal magnetic field surrounding the HL-2M tokamak was simulated with the electromagnetic field simulation software CST Studio from Germany. The results show that the magnetic field intensity surrounding the neutralizer tank and ion source of NBI device was more than2?10^-3T, so the magnetic shielding of NBI neutralizer tank and ion source was necessary. Then the magnetic field distribution surrounding NBI neutralizer tank and ion source after shielding with iron was simulated with CST Studio.     

Energy Selecting Action of Limiters on Particle Fluxes Penetrating into the SOL-Plasma

A simple model of the penetration of particle effluxes from the core plasma into the SOL-plasma of tokamaks is proposed. The assumptions made are free streaming of particles parallel to the magnetic field and anomalous particle transport perpendicular to the toroidal field with a constant radial velocity. The model has been proved for measured particle fluxes of Li which was injected into the core plasma of the tokamak T-10. The dependence of the Li-particle flux on the minor radius as well as toroidal asymmetries in the SOL-plasma can be explained by the results of the calculations.     

Plasma Response to Resonant Perturbations at Tokamak Edge

In certain circumstances, plasma response suppresses magnetic islands expected at perturbed resonant magnetic surfaces. We investigate the plasma response to the resonant magnetic perturbations in a large aspect ratio tokamak perturbed by external resonant helical windings, considering polar toroidal coordinates for which analytical toroidal equilibrium solutions and perturbing fields are available. We apply an empirical approach to mimic the plasma screening effects by introducing presumed plasma current sheets on the resonance surfaces to cancel the RMP effects. Numerical examples show the effect of plasma response reducing magnetic islands at the plasma edge and also regularizing field lines around the resonant surface. The distribution of connection lengths along the plasma cross section indicates that the plasma response increases the connection lengths since more toroidal turns are performed until a field line reaches the tokamak wall.     

基于垂直引线和调制电流的三线环形磁导引

提出了一种在单层原子芯片上实现闭合且导引中心无磁场零点的环形磁导引的新方案. 芯片表面刻蚀的导线结构由同心等距三环线构成, 三环线的电流引线垂直于芯片表面. 加载直流电流后, 这种构型即可在芯片表面附近产生闭合的环形磁导引. 交流调制三环线电流后, 环形磁导引的势能极小值附近不再存在磁场零点且其磁场起伏小. 这种方案可用于基于物质波干涉的原子芯片陀螺仪研究.     

清洗放电前MUT托卡马克中的电流分布

本文利用磁探针阵测量清洗放电前ＭＵＴ托卡马克中角向磁场的分布，从而计算得到了等离子体的电流分布。结果表明，在清洗放电初期，由于存在大量杂质，等离子体的横向扩散非常大，因而。真空室的绝缘段几乎不起绝缘作用，此时所测到的环向电流中绝大部分是流经厚壁真空室的电流。