数值积分求解均匀带电圆环平面上的电场分布

本文用数值积分的方法计算椭圆积分，求出在均匀带电圆环平面上的场强与电势．     

均匀带电圆环内点电荷的非线性振荡

本文用数值方法求解含有椭圆积分的二阶微分方程，讨论了均匀带电圆环内点电荷的非线性振荡及其运动特征．     

关于夫琅禾费椭圆孔衍射积分的精确解

对于椭圆孔的衍射积分问题，在众多的理论光学书籍和文献中，人们只作定性讨论，没有严格解。本文试图从衍射积分公式出发，选取合适的正交曲线坐标系，并巧妙地利用贝塞尔函数，从而得到夫琅禾费椭圆扎衍时积分的精确解。     

边界元素法中有关积分的计算方法(Ⅱ)柱状边界条件下对曲面积分及椭圆积分的计算

在柱状边界条件下将对柱侧面的曲面积分表示成一维积分,同时还给出了椭圆积分的计算方法,由对空间立体角积分的算例可知,其计算的速度有了显着的提高。     

椭圆包层光纤场的迭代近似解与漏模损耗计算

试图理论上处理椭圆包层各向异性光纤复杂的折射率分布。数学过程包括折射率分布的级数展开、δ－涵数的导数和积分以及用格林函数求解方程的迭代技术。给出了椭圆包层各向异性光纤漏模损耗的解析表达式。数值结果表明椭圆包层各向异性光纤的漏模损耗比领结型光纤小，比阶跃型各向异性光纤大；偏心率越大越有利于制造单模单偏光纤。     

Kerr时空赤道面上零测地线方程的严格求解

运用欧拉-拉格朗日方程给出了Kerr时空赤道面上的零测地线方程并求出两个首次积分,结合零测地线所满足的恒等式求得轨道微分方程.通过把被积函数化成部分分式,以及解出被积函数中的一个四次方程并对根进行排序,可把轨道微分方程的解表示成第一类椭圆积分和第三类椭圆积分.     

边界元素法中有关积分的计算方法(Ⅰ)柱状边界条件下对空间立体角积分的计算

利用任意闭合曲面对曲面外任一点所张立体角为零的特点将柱状边界条件下对柱侧面的积分转变为对柱底面的积分,并将其表示成椭圆积分的形式。     

光格中旋量玻色-爱因斯坦凝聚的高阶非线性孤子激发

研究了一维光格中旋量玻色-爱因斯坦凝聚体的高阶非线性作用下的孤子激发,得出了用椭圆积分表示的明孤子解和特定参数条件下的暗孤子解析解,并求得了能量表达式.     

边界元素法中有关积分的计算方法(Ⅱ)柱状边界条件下对曲面积分及椭圆积分的计算

在柱状边界条件下将对柱侧面的曲面积分表示成一维积分，同时还给出了椭圆积分的计算方法，由对空间立体角积分的算例可知，其计算的速度有了显著的提高．     

复摆的振动分析

研究复摆的非线性振动，从能量和摆角两个方面来分析它们对复摆运动的影响，用第一类完全椭圆积分求出了复摆振动的解和周期，对非线性特征进行了分析。     

椭圆环电流中心的磁感强度

运用毕奥-萨伐尔定律和椭圆参数方程，计算出椭圆环电流中心的磁感强度。     

亥姆霍兹线圈磁场均匀范围的研究

推导了双环电流磁感应强度在直角坐标系中的解析式,将公式无量纲化,通过第一类和第二类完全椭圆积分计算场强的两个分量,从而计算合场强,画出亥姆霍兹线圈内外磁感应强度合场强曲面和三维均匀区域,发现磁场的均匀区域是“八爪”形状,并与双环电流不同距离的场强和均匀范围进行了比较.     

Poloidal–toroidal decomposition in a finite cylinder. I: Influence matrices for the magnetohydrodynamic equations

The Navier–Stokes equations and magnetohydrodynamics equations are written in terms of poloidal and toroidal potentials in a finite cylinder. This formulation insures that the velocity and magnetic fields are divergence-free by construction, but leads to systems of partial differential equations of higher order, whose boundary conditions are coupled. The influence matrix technique is used to transform these systems into decoupled parabolic and elliptic problems. The magnetic field in the induction equation is matched to that in an exterior vacuum by means of the Dirichlet-to-Neumann mapping, thus eliminating the need to discretize the exterior. The influence matrix is scaled in order to attain an acceptable condition number.     

Demagnetization factors for cylindrical shells and related shapes

Magnetostatic self and interaction energies can be computed via demagnetization factors whenever the magnetic state is close to a uniform state, e.g. in the presence of a strong applied field, or when the dimensions involved are within the single-domain limit. We derive analytical expressions for the demagnetization factors of cylindrical shells and rings with rectangular and square cross-sections. The factors are given either as a combination of elliptic integrals or as a series expansion in powers of the dimensionless ratio between inner and outer radii. Limiting cases are analysed for particular ranges of the shape parameters. We also investigate the ring with a square cross-section, and the elliptic ring, where analytical expressions are provided only for small eccentricity. Finally, we introduce the dipolar coupling integral encoding magnetostatic interactions between a magnetized cylinder and a thin coating on its lateral surface.     

载流有限长密绕螺线管的磁场分布

对于通以恒定电流的有限长螺线管,首先用柱函数展开法推导出矢势的表达式,再利用磁感应强度与矢势的关系式,得出积分形式的磁场表达式.然后用直接积分的方法计算出磁场分布的级数表达式.最后讨论了某些特殊位置处的磁场.     

Poloidal–toroidal decomposition in a finite cylinder. I: Influence matrices for the magnetohydrodynamic equations

The Navier–Stokes equations and magnetohydrodynamics equations are written in terms of poloidal and toroidal potentials in a finite cylinder. This formulation insures that the velocity and magnetic fields are divergence-free by construction, but leads to systems of partial differential equations of higher order, whose boundary conditions are coupled. The influence matrix technique is used to transform these systems into decoupled parabolic and elliptic problems. The magnetic field in the induction equation is matched to that in an exterior vacuum by means of the Dirichlet-to-Neumann mapping, thus eliminating the need to discretize the exterior. The influence matrix is scaled in order to attain an acceptable condition number.     

有限长厚壁载流螺线管的磁场分布

对于通以恒定电流的有限长厚壁螺线管,用柱函数展开法推导出矢势的表达式,再根据磁感应强度与矢势的关系式得出磁场的积分形式表达式．用直接积分的方法,计算出厚壁螺线管内部和外部的磁场分布的级数表达式．另外还用本文得出的公式求得中轴线上的磁场．     

Magnetic field penetration into half-space for type-II superconductors of the second kind

Equations that simulate the magnetic induction and current density distributions in half-space in view of the power I-V characteristic are derived. The magnetization front velocity is determined for a given mean rate of external magnetic field variation at the boundary of the sample. An integral condition for the electrical resistance (nonlinearly depending on the magnetic field) under which the magnetic flux penetrates into the sample with a finite rate is found. An analytical solution that simulates the power variation of the magnetic field at the boundary is given. The Bean generalized model describing the current density distribution near the critical current is considered. It is shown that solutions like shock waves may arise beyond the applicability domain of the Bean model.     

Unitarity of the Knizhnik-Zamolodchikov-Bernard connection and the Bethe Ansatz for the elliptic Hitchin systems

We work out finite-dimensional integral formulae for the scalar product of genus one states of the groupG Chern-Simons theory with insertions of Wilson lines. Assuming convergence of the integrals, we show that unitarity of the elliptic Knizhnik-Zamolodchikov-Bernard connection with respect to the scalar product of CS states is closely related to the Bethe Ansatz for the commuting Hamiltonians building up the connection and quantizing the quadratic Hamiltonians of the elliptic Hitchin system.