带两个Carleman位移的奇异积分方程Noether可解的充分必要条件

带Carleman位移的奇异积分方程理论,近年来得到了很大发展。在[1]中建立了这种奇异积分方程的Noether理论,所用的基本方法是建立所谓的对应方程组(是不带位移的奇异积分方程组,它的理论是已知的,参看[2],[3])。在[4]中讨论了带两个Carleman位移的奇异积分方程Noether可解的充分条件,并给出了计算指数的公式。本文目的是在文章[4]的基础上,利用不同的方法解决带两个Carleman位移的奇异积分方程Noether可解的充分必要条件问题,并把所得结果对带两个Carleman位移及未知函数复共轭值的奇异积分方程进行推广。     

圆周上超奇异积分计算及其误差估计

许多科学和工程计算问题归化为积分方程。这些积分方程往往是奇异的,有些甚至是超奇异的。特别是自然边界归化无一例外都导致超奇异积分方程。由于通常的数值积分方法对计算超奇异积分都无效,故长期以来边界元研究中总是回避超奇异积分方程。但近年来     

复超球面上的奇异积分方程

<正> 一维的奇异积分方程的理论已经相当完整,并有着极为广泛和重要的应用(例如参阅(?)高维的奇异积分方程还未完整.(?)写了一本关于高维奇异积分与奇异积分方程的书,总结了近年来的发展及其影响,从中可以看出,高维奇异积分方程距离完整还有一定的距离.     

Hermite三次样条多小波自然边界元法

针对应用自然边界元方法解上半平面的Laplace方程的Neumann边值问题时存在奇异积分的困难,本文提出了Hermite三次样条多小波自然边界元法.Hermite三次样条多小波具有较短的紧支集、很好的稳定性和显式表达式,而且它们在不同层上的导数还是相互正交的.因此,本文将它与自然边界元法相结合,利用小波伽辽金法离散自然边界积分方程,使自然边界积分方程中的强奇异积分化为弱奇异积分,从而降低了问题的复杂性.文中给出的算例表明了该方法的可行性和有效性.     

带卷积的Riemann边值问题及其应用

本文考虑一类广泛的带卷积的 Riemann 边值问题,它包括了几类最基本的奇异积分方程或边值问题,即 Riemann 边值问题、Cauchy 奇异积分方程、卷积型方程、Winer-Hopf 方程及对偶积分方程等,并将它们统一起来处理,运用的局部性理论研究了此问题 Noether 性的必要充分条件,并确定其指标公式,作为应用特例,讨论了变系数的Cauchy 核与卷积核混合的奇异积分方程。     

Volterra积分方程的蒙特卡罗数值求解方法

本文讨论了第一类、第二类以及具有奇异核的Volterra积分方程的数值解问题.利用重要抽样蒙特卡罗随机模拟方法获得积分方程解的近似计算结果.通过对文献中算例的实现表明文中所提方法扩展了Volterra型积分方程的数值求解方法,     

奇异积分方程

一个积分方程里如果有未知函数出现在发散的积分号下,而积分意味着取Cauchy主值时,便称为奇异积分方程(以下简称奇异方程——译者)。以后这样的积分叫作奇异积分。分析学里出现奇异积分的,首先是关于Cauchy型积分的边界值以及单层场位的一阶导数的边界值,是用某些奇异积分表示的。与弗里得霍伦(Fredholm)型方程比较,奇异积分具有这样的本质特异性,即所出现的奇异积分乃是有界的算子,但在相应的函数空间中并不是个全连续算子。这点使得弗里得霍伦理论不能应用到奇异方程上去。奇异方程的另一特性乃是不同的独立变数个数不是一律类似的。必须分别考虑一个与m个(m≥2)独立变数的情形。一个独立的奇异方程的一些叙述可参阅Б.И.斯米尔诺夫(CMИpHOB)以及     

用正交函数求超奇异积分的近似值及其误差估计

基于 Hadamard有限部分积分定义, 当密度函数是多项式、正弦函数和余弦函数时, 本文推导出了计算超奇异积分准确值的公式, 进而利用这些公式给出了密度函数为一般连续函数的超奇异积分近似值的计算方法. 本文还对近似值进行了误差分析, 据此可以在事先给定的误差下来计算超奇异积分的近似值. 最后将前面的理论应用到超奇异积分方程求近似解的问题. 数值算例表明该方法的可行性和有效性.     

三维重调和方程的双方程边界积分方程法

以守恒积分为工具,推导了三维重调和方程的新的边界积分方程,所得出的新方程与传统的边界积分方程相比较,降低了奇异性,避免了传统边界元方法中的强奇异积分的计算.对不同边界都采用第二类积分方程,得到了三维重调和方程的双方程方法.     

复双球面上变系数奇异积分方程的正则化

利用复双球面上的立体角系数的方法和置换公式,讨论复双球垒域上变系数奇异积分方程的正则化问题,推广了复超球面上变系数奇异积分方程的结论．     

On the existence and uniqueness of solutions of the inverse boundary value problem for determining the permittivity of materials

The problem of determining the permittivity of material samples of arbitrary shape placed in a rectangular waveguide with perfectly conducting walls is investigated. The problem is reduced to solving a nonlinear volume singular integral equation. A theorem on the existence and uniqueness of solutions to the nonlinear volume singular integral equation and of the inverse boundary value problem for determining the permittivity of the material is proved.     

A wavelets method for plane elasticity problem

A Neumann boundary value problem of plane elasticity problem in the exterior circular domain is reduced into an equivalent natural boundary integral equation and a Poisson integral formula with the DtN method. Using the trigonometric wavelets and Galerkin method, we obtain a fast numerical method for the natural boundary integral equation which has an unique solution in the quotient space. We decompose the stiffness matrix in our numerical method into four circulant and symmetrical or antisymmetrical submatrices, and hence the solution of the associated linear algebraic system can be solved with the fast Fourier transform (FFT) and the inverse fast Fourier transform (IFFT) instead of the inverse matrix. Examples are given for demonstrating our method has good accuracy of our method even though the exact solution is almost singular.     

Numerical Solution for the Helmholtz Equation with Mixed Boundary Condition

We consider the numerical solution for the Helmholtz equation in R~2 with mixed boundary conditions.The solvability of this mixed boundary value problem is estab- lished by the boundary integral equation method.Based on the Green formula,we express the solution in terms of the boundary data.The key to the numerical real- ization of this method is the computation of weakly singular integrals.Numerical performances show the validity and feasibility of our method.The numerical schemes proposed in this paper have been applied in the realization of probe method for inverse scattering problems.     

Inverse problems for the Sturm-Liouville equation with the discontinuous coefficient

In this study we derive the Gelfand-Levitan-Marchenko type main integral equation of the inverse problem for the boundary value problem $L$ and prove the uniquely solvability of the main integral equation. Further, we give the solution of the inverse problem by the spectral data and by two spectrum.     

The Behaviour of Elastic Fields and Boundary Integral Mellin Techniques Near Conical Points

For the computation of the local singular behaviour of an homogeneous anisotropic clastic field near the three-dimensional vertex subjected to displacement boundary conditions, one can use a boundary integral equation of the first kind whose unkown is the boundary stress. Mellin transformation yields a one - dimensional integral equation on the intersection curve 7 of the cone with the unit sphere. The Mellin transformed operator defines the singular exponents and Jordan chains, which provide via inverse Mellin transformation a local expansion of the solution near the vertex. Based on Kondratiev's technique which yields a holomorphic operator pencil of elliptic boundary value problems on the cross - sectional interior and exterior intersection of the unit sphere with the conical interior and exterior original cones, respectively, and using results by Maz'ya and Kozlov, it can be shown how the Jordan chains of the one-dimensional boundary integral equation are related to the corresponding Jordan chains of the operator pencil and their jumps across γ. This allows a new and detailed analysis of the asymptotic behaviour of the boundary integral equation solutions near the vertex of the cone. In particular, the integral equation method developed by Schmitz, Volk and Wendland for the special case of the elastic Dirichlet problem in isotropic homogeneous materials could be completed and generalized to the anisotropic case.     

On the convergence of a numerical method for a hypersingular integral equation on a closed surface

We consider a linear integral equation with a hypersingular integral treated in the sense of the Hadamard finite value. This equation arises in the solution of the Neumann boundary value problem for the Laplace equation with a representation of a solution in the form of a double-layer potential. We consider the case in which the interior or exterior boundary value problem is solved in a domain; whose boundary is a smooth closed surface, and an integral equation is written out on that surface. For the integral operator in that equation, we suggest quadrature formulas like the method of vortical frames with a regularization, which provides its approximation on the entire surface for the use of a nonstructured partition. We construct a numerical scheme for the integral equation on the basis of suggested quadrature formulas, prove an estimate for the norm of the inverse matrix of the related system of linear equations and the uniform convergence of numerical solutions to the exact solution of the hypersingular integral equation on the grid.     

Recovery of the unknown coefficients in a two-dimensional hyperbolic equation

In this paper, an inverse boundary value problem for a two-dimensional hyperbolic equation with overdetermination conditions is studied. To investigate the solvability of the original problem, we first consider an auxiliary inverse boundary value problem and prove its equivalence to the original problem in a certain sense. We then use the Fourier method to reduce such an equivalent problem to a system of integral equations. Furthermore, we prove the existence and uniqueness theorem for the auxiliary problem by the contraction mappings principle. Based on the equivalency of these problems, the existence and uniqueness theorem for the classical solution of the original inverse problem is proved. Some discussions on the numerical solutions for this inverse problem are presented including some numerical examples.     

一类复合材料焊接的界面裂纹问题

利用复变方法和解析函数边值问题的基本理论，研究一类复合材料焊接线上出现裂纹的平面弹性基本问题，笔者通过适当的函数分解和积分变换，将寻找复应力函数的问题转化为求解一正而型奇异积分方程，并借助积分方程理论给出了方程的求解方法。     

Helmholtz equation outside an open arc in a plane with a mixed boundary condition

A boundary value problem for the Helmholtz equation outside an open arc in a plane is studied with mixed boundary conditions. In doing so, the Dirichlet condition is specified on one side of the open arc and the boundary condition of the third kind is specified on the other side of the open arc. We consider non-propagative Helmholtz equation, real-valued solutions of which satisfy maximum principle. By using the potential theory the boundary value problem is reduced to a system of singular integral equations with additional conditions. By regularization and subsequent transformations, this system is reduced to a vector Fredholm equation of the second kind and index zero. It is proved that the obtained vector Fredholm equation is uniquely solvable. Therefore the integral representation for a solution of the original boundary value problem is obtained. (© 2008 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)