基于Visua C＋＋的非线性电路实验模拟

在Visual C＋＋开发环境下,通过龙格库塔方法求解非线性电路微分方程组,得到数值解并模拟显示李萨茹图形。在相同线路参数下模拟结果与实验室实验中观察到的结果一致,同时模拟显示可以容易地得到稳定的X,Y方向上的输出波形。通过该模拟实验可以很好地观察研究非线性电路中的混沌现象。     

GEM电极的三维电场分布计算

基于有限元方法对GEM电极的电场分布进行模拟和计算,得到了完整的三维电场分布.研究不同几何构型的GEM场强分布对电荷收集效率的影响,给出了4种构型GEM电极的电场线透过率分别为:双倒锥型33.12%;圆柱型34.85%;单锥型40.70%;单倒锥型16.70%.计算得到的电场线透过率比二维电场分布的结果更加接近实验结果     

利用Matlab直观感受不等量异种电荷电场和电势

文章通过Matlab软件,模拟不等量异种电荷的电场线和等势面,使原本抽象难懂的电场线和等势面变得直观形象,有助于解答学生的疑问,拓展学生的思维.     

电场线的三维演示现象的机理研究

本文对电场线的三维演示新方法进行机理分析，为实验提供理论依据。     

利用运动模拟绘制点电荷的电场线和等势线

电场线和等势线是研究电学问题的重要工具,在高中水平上利用物体运动的模拟和计算机绘制点电荷的电场线和等势线,为进一步探究电场和电势的特点提供素材。     

静电场的复势函数与模拟法描绘电场线的原理

静电场描绘是理工科院校普遍开设的物理实验题目，通常用恒定电流场来模拟静电场的电势分布，再由描绘出的等势线族根据它们和电场线(电力线)正交的特点徒手画出相应的电场线分布来。这样画出的电场线误差较大，很难给出电场线及电极表面电荷密度分布的准确物理图象．为解决这一同题，     

电场线的应用

电磁学的高斯定理、环路定理是静电场的基础,电场线又与高斯定理、环路定理等价:静电场里许多不易定量计算或不用定量计算的问题都可以借助电场线的概念来解决．下面探讨电场线的应用．1电场线的概念     

电场线的三维演示新方法

本文采用多根细丝线附在带电导体上的方法，来演示电场线。其优点是所演示的电场线的空间性强，可以比较形象地演示出带电导体在空间中的电场线分布。     

静电场的复势函数与模拟法描绘电场线的原理

静电场的复势函数与模拟法描绘电场线的原理上海交通大学乔卫平，陈新雷静电场描绘是理工科院校普遍开设的物理实验题目，通常用恒定电流场来模拟静电场的电势分布，再由描绘出的等势线族根据它们和电场线（电力线）正交的特点徒手画出相应的电场线分布来”‘二这样画出的...     

基于MATLAB的点电荷系电场分布的用户图形界面设计

电场强度与电势是描述静电场性质的重要物理量,利用电场线与等势面可以形象地描述静电场的分布,对其进行数值计算和模拟显示,可以使教学内容更加直观,提高教学效率.本文利用MATLAB编程和MATLAB的GUIDE开发了点电荷系所形成的电场场强分布及电势分布的用户图形界面(GUI),实现了二维平面内任意点电荷系电场的电场线和等势面分布的可视化,并可以方便地调整电荷数目、电量及位置并实时显示,在教学中能起到很好的演示作用.     

利用Matlab模拟点电荷系的电场线和等势面

根据电场叠加原理,利用Matlab的绘图功能,绘出二维平面内点电荷系的等势面和电场线。以三个点电荷为例,模拟了它们的电场线和等势面,并通过改变电荷的位置和电荷量的大小对电场的分布情况进行分析比较,在教学中能起到很好的演示作用。     

一维电荷分布系统的电场线

推导一维电荷分布系统的电场线满足的方程,并使用数学软件MatLab将其电场线精确地作出来,其图像既具科学性而又优于传统的手绘图像.     

Equivalent representation of orthogonal-field electrodynamics by system of covariant lines of force

It is shown that the electrodynamics of orthogonal magnetic and electric fields can be represented as the dynamics of covariant lines of force. Such a representation is provided for the Lienard-Wichert field of an arbitrary moving charge and the field of a charge that moves uniformly about a circle. The four vector of the electric lines of force is written as the sum of the four vector of the charge and the radius four vector directed along the light cone to the observation point. This vector is a solution of an equation that formally coincides with the equation of motion of the magnetic moment in external fields for a zero intrinsic magnetic moment. The electromagnetic field is reconstructed according to a system of lines that correspond to the total equation of motion of the magnetic moment. Such a field for a uniformly circulating charge is examined.Erevan Physics Institute. Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Radiofizika, Vol. 35, Nos. 3, 4, pp. 313–323, March–April, 1992.     

Electric Field in a Gravitational Field

The potential of a static electric charge located in a Schwarzschild gravitational field is given by Linet. The expressions for the field lines derived from this potential are calculated by numerical integration and drawn for different locations of the static charge in the gravitational field. The field lines calculated for a charge located very close to the central mass can be compared to those calculated by Hanni–Ruffini. Maxwell equations are used to analyze the dynamics of the falling electric field in a gravitational field.     

均匀带电平面折线在空间产生的电场及其可视化

推导了均匀带电线段在二维平面中产生的电势的简要公式,进而推导了在三维直角坐标系中的电势公式,形成了带电折线(包括任意多边形)的电势简要公式.根据电势与电场强度之间的关系,列出了场强的表达式.将公式无量纲化,利用MATLAB指令,绘制了各种形状的带电多边形和折线的等势面和三维电场线,并显示了电场在空间的分布规律.     

Deconfinement transition in three-dimensional compact U(1) gauge theories coupled to matter fields

It is shown that permanent confinement in three-dimensional compact U(1) gauge theory can be destroyed by matter fields in a deconfinement transition. This follows from a nontrivial infrared fixed point caused by matter, and an anomalous scaling dimension of the gauge field. This leads to a logarithmic interaction between the defects of the gauge fields, which form a gas of magnetic monopoles. For logarithmic interactions, the original electric charges are unconfined. The confined phase, which is permanent in the absence of matter fields, is reached at a critical electric charge, where the interaction between magnetic charges is screened by a pair-unbinding in a Kosterlitz-Thouless-like phase transition.     

Aspects of electrostatics in a weak gravitational field

Several features of electrostatics of point charged particles in a weak, homogeneous, gravitational field are discussed using the Rindler metric to model the gravitational field. Some previously known results are obtained by simpler and more transparent procedures and are interpreted in an intuitive manner. Specifically: (a) We discuss possible definitions of the electric field in curved spacetime (and noninertial frames), argue in favour of a specific definition for the electric field and discuss its properties. (b) We show that the electrostatic potential of a charge at rest in the Rindler frame (which is known and is usually expressed as a complicated function of the coordinates) is expressible as A ₀ = q/λ where λ is the affine parameter distance along the null geodesic from the charge to the field point. (c) This relates well with the result that the electric field lines of a charge coincide with the null geodesics; that is, both light and the electric field lines ‘bend’ in the same manner in a weak gravitational field. We provide a simple proof for this result as well as for the fact that the null geodesics (and field lines) are circles in space. (d) We obtain the sum of the electrostatic forces exerted by one charge on another in the Rindler frame and discuss its interpretation. In particular, we compare the results in the Rindler frame and in the inertial frame and discuss their consistency. (e) We show how a purely electrostatic term in the Rindler frame appears as a radiation term in the inertial frame. (In part, this arises because charges at rest in a weak gravitational field possess additional weight due to their electrostatic energy. This weight is proportional to the acceleration and falls inversely with distance—which are the usual characteristics of a radiation field.) (f) We also interpret the origin of the radiation reaction term by extending our approach to include a slowly varying acceleration. Many of these results might have possible extensions for the case of electrostatics in an arbitrary static geometry.     

Dynamics of induction charging for multiple particle agglomerations with a thin conducting surface layer

In electrostatic applications, particles are typically stacked in an arbitrary array. In this paper, multiple particle agglomerations with a finite volume conductivity, surface conductivity and permittivity have been simulated. Upon exposure to the electric field, electric shielding can occur due to the proximity of other particles, which greatly reduces the maximum accumulated charge and affects the charging time. All results have been obtained using the COMSOL commercial software. The simulation results show that shielding the electric field from a given particle reduces its saturation charge and the rate of charge accumulation was mainly affected by the volume and surface conductivities.     

由接地导体限定的无限深槽内线电荷的电场

利用复数坐标系z上的施瓦茨-克利斯多菲变换和镜像法,计算由接地导体限定的无限深槽内线电荷电场中的电势分布和场强分布,给出电场线与等势线方程,并利用数学软件Matlab绘制出其电势分布三维图、电场线和等势线(面)图.     

用计算机模拟点电荷在二维平面上的静电场

二维平面上的点电荷的静电场是静电场问题的基础，作者独立开发了软件用以模拟，此程序由用户决定点电荷的所有参数，快速地生成视阈内的等势线与电场线，使用户方便的获得电场直观印象，并可以得到任意点的电势与场强，该程序操作简单，对于学生、教师的学与教都能起到很好的辅助作用。