导体球壳上感应电荷及空间电场的分布(1)

本文利用镜象法讨论了在接地导体球壳附近有点电荷时，空间的电场分布和球壳表面上感应电荷的分布。     

导体与点电荷之间的相互作用能的一点讨论

不带电荷的导体移到点电荷的静电场中时,导体表面会产生感应电荷.我们证明对任意形状的导体,导体和点电荷之间的相互作用能是点电荷与其镜象电荷之间库仑作用能的1/2,并且对此结果给出一个非常简单的解释.     

导体球壳上感应电荷及空间电场的分布(2)

本文利用镜象法讨论了在不接地导体球壳附近有点电荷时，空间的电场分布和球壳表面上感应电荷的分布。     

电磁学与电动力学中的磁单极—Ⅳ

本文为作者磁单极系列文章的第4篇,该系列文章在电磁学和电动力学框架内用尽量科普的方式分别介绍磁单极的若干奇特性质.在本篇文章中作者讨论用拓扑参量θ描写磁电介质,发现在这种介质上出现了电荷与磁单极作为双荷子共生的现象.如果进一步考虑到磁荷与电荷的量子化,则得到此介质的拓扑参量θ必须是π的分数或整数倍.     

电磁学与电动力学中的磁单极-I

本文及后继三篇文章在电磁学和电动力学框架内分别介绍磁单极的若干奇特性质.针对由一个磁单极和一个点电荷构成的体系,首先证明这个体系的电磁场角动量具有极简洁的表达式并讨论可能的电荷量子化,然后显式地演示体系角动量的转化与守恒.     

确定接地导体球内像电荷的一种原始思路

针对许多参考书中讨论电像法的基于相似三角形的切入思路,但此法思路并不自然,这里给出一种从极其自然的原始思路出发（只用点电荷的电势公式）,确定接地导体球内的像电荷的方法（包括电荷量的大小和位置）,并将接地无限大导体板问题作为本问题的特例处理．     

点电荷至接地导体球面的曳引时间的解析解及其渐近行为

在不计重力、空气阻力以及相对论效应的条件下,通过求解运动微分方程,计算出点电荷在其附近接地导体上的感应电荷作用下,被曳引到导体表面所需的时间.结果为用第一、二类完全椭圆积分的线性组合表示的解析解,并考察当球面变为平面时解析解的渐近行为,得出与已有文献一致的结果.     

求接地导体感应电荷的一种简便方法

由一道证明题引申出一个命题,对该命题给出了证明;通过几个实例说明应用该命题可以简便地求解某些接地导体的感应电荷.     

用电像法讨论点电荷与导体球间的相互作用

用电像法讨论点电荷与接地导体球、绝缘导体球、一个和电源连接的导体球之间的相互作用.     

点电荷与导体球系统的电场线

用电像法将点电荷与中性导体球系统的电场化为一维点电荷分布系统的电场,导出电场线满足的方程,利用Mathematica软件画出了电场线簇图形,并对点电荷与接地导体球、点电荷与带电导体球两系统的电场线进行了描绘。     

极化电荷与自由电荷之间区别的演示实验

通过将导体放入静电场发生的静电感应现象和将绝缘体（电介质）放入静电场发生的极化现象,演示一组实验,生动地显示了电介质被极化出的正、负电荷,既不能离开电介质,也不能在电介质中自由移动,就是将带有极化电荷的电介质与导体接触,极化电荷也不会与导体上的自由电荷中和,即极化电荷牢固地束缚在介质上．说明极化电荷与自由电荷之间的本质区别,加深学生对这些概念的理解和运用．     

Branch Processes of Regular Magnetic Monopole

In this paper, by making use of Duan＇s topological current theory, the branch process of regular magnetic monopoles is discussed in detail. Regular magnetic monopoles are found generating or annihilating at the limit point and encountering, splitting, or merging at the bifurcation point and the degenerate point systematically of the vector order parameter field φ（x）. Furthermore, it is also shown that when regular magnetic monopoles split or merge at the degenerate point of field function φ, the total topological charges of the regular magnetic monopoles are stilI unchanged.     

有磁单极子存在下的Aharnov-Bohm效应

有磁单极子存在下的Aharnov-Bohm效应 关键词： A-B效应 电磁对偶 几何相位     

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.     

Cloaking magnetic field and generating electric field with topological insulator and high permeability material

Topological insulator is a new state of quantum matter. When applied magnetic field is applied on a topological insulator, not only the magnetic field is induced, but also the electric field is induced, vice versa. We designed bi-layer magnetic cloak with topological insulator and high permeability material (HPM), derived the electric field and magnetic field inside and outside the bi-layer topological insulator and HPM. Calculation and simulation results show that the applied magnetic field is cloaked by the bi-layer topological insulator and HPM, and the uniform electric field is induced in the cloaked region.     

Magnetic charge and hyperfine splitting in hydrogen

The large spatial size of magnetic charges (or dyons) and parity considerations are used to show that in models of the proton based on dyons the hyperfine splitting must be due to the magnetic moment produced by the electric charge. The contributions of the magnetic monopoles cancel, otherwise the proton would have a large electric dipole moment.     

Magnetic symmetry and dyons

A self-consistent theory of dyons in Abelian and non-Abelian limits has been formulated in terms of an extra magnetic symmetry and topological magnetic charge. It has been shown that the restricted gauge potential describes the fields of dyons in terms of two regular (time-like) potentials only when recourse is made to the duality of topological (magnetic) and isocolour (electric) charges. Choosing a suitable Lagrangian density for the system of dyons in non-Abelian gauge theory, the field equations, energy-momentum tensor, Hamiltonian and momentum densities have also been derived and the conservation of the four-linear momentum and the total angular momentum has been demonstrated.     

Topological electric charge

By treating magnetic charge as a gauge symmetry through the introduction of a magnetic pseudo four-vector potential, we show that it is possible to construct a topological electric charge from a theory which originally contains gauge magnetic charge. This is an explicit realization of the Montonen-Olive conjecture that there should exist a dual theory to the usual 't Hooft-Polyakov monopole theory in which the roles of the gauge and topological charges are reversed. The physical distinction between 't Hooft-Polyakov monopoles and the dual theory with electric charge is that the strong and weak coupling regimes are reversed. Physically this leads to the mass of the electrically charged soliton being on the order of (1/137)M _W as opposed to the much larger mass (on the order of 137M _W) of the magnetically charged soliton. Thus even forM _W in the TeV range such an electrically charged particle could be observed at some future accelerator.