具有抛物线边界的各向异性体的二维变形问题

文章通过Lekhnitskii方法及映射函数法系统地研究了具有抛物线边界的各向异性体的二维变形问题,并利用所获得的结果研究了一种特殊的结构--半无限裂纹问题,求得了裂纹尖端的应力奇异场及应力强度因子。     

具有双曲线边界的各向异性介质的二维问题

文章研究了在纯弯矩M₀作用下,具双曲线边界的各向异性介质的二维变形问题,求得了介质内部的应力应变场的具体形式,在此基础上,以单晶铝板(立方晶系介质)为例,我们求得了沿双曲线边界的环向应力及x₂=0面上的应力分布,当双曲线退化成一双边裂纹时,文章也求得了相应的应力强度因子(k₁,k₂,k₃),并且也发现,k₁与材料的弹性性质无关。     

含椭圆夹杂二维各向异性电磁弹性介质的耦合问题

研究了无限大二维各向异性电磁弹性固体的椭圆夹杂问题.基于广义Stroh方法、保角变换和扰动概念,得到了基体和夹杂内电场、磁场和弹性场的封闭解.本文结果可用于研究电磁弹性复合材料的有效性能.     

半平面压电体的Green函数及其应用

本文研究半平面压电体在线力、电荷和位错作用下的弹性场和电场，即Green函数．基于各向异性弹性力学中的Stroh方法和解析延拓理论，推导了Green函数的封闭形式的解．作为解的应用，分析了含半无限裂纹的无限大压电介质的机电耦合场，给出了应力和电位移强度因子的解析表达式．     

沿抛物线分布的各向异性曲线裂纹问题

文章利用Ｓｔｒｏｈ法及映射法研究了沿抛物线Ω分布的各向异性曲线裂纹问题，获得了有关的应力及位移场，这种解不仅适用于平面问题，而且也适用于反平面变形或两者偶合的情形，对于单位边裂纹和双曲边裂纹问题，文章还获得了它们的应力和位移场的封闭解，并求得了相应斥强主因子及裂纹面上的张开位移。     

直位错和线性力作用下点群10十次对称二维准晶的弹性场研究

本文研究了直位错和线性力作用下点群10十次对称二维准晶的弹性场.首先将Stroh公式推广到点群10十次对称二维准晶研究中,在此基础上,采用推广的Stroh公式给出了应力和位移的通解,结合边界条件,获得了应力的解析表达式,为实际应用奠定了理论基础.     

横观各向同性电磁弹性介质中裂纹对SH波的散射

研究横观各向同性电磁弹性介质中裂纹和反平面剪切波之间的相互作用．根据电磁弹性介质的平衡运动微分方程、电位移和磁感应强度微分方程,得到SH波传播的控制场方程．引入线性变换,将控制场方程简化为Helmholtz方程和两个Laplace方程A·D2通过Fourier变换,并采用非电磁渗透型裂面边界条件,得到了柯西奇异积分方程组．利用Chebyshev多项式求解积分方程,得到应力场、电场和磁场以及动应力强度因子的表达,并给出了数值算例．     

具有自由边界的二维渗流问题

渗流的自由边界问题是工程上很受关注的问题．现有的数值分析方法需事先估计边界形态，逐次逼近．本文采用“变分不等式”的模式，结合有限元方法研究有自由边界的渗流问题，在整个结构区域内作有限元剖分，避免了传统的有限元分析中估计自由边界、反复修正计算区域的迭代过程．本文方法为简单而快速地分析渗流自由边界问题提供了一条有效的途径．     

十次对称二维准晶中的楔形裂纹问题

研究了集中力作用下十次对称二维准晶中的楔形裂纹问题.采用推广的Stroh公式给出了应力和位移的一般解,在此基础上,讨论了声子场环向应力和相位子场环向应力的变化规律.作为特例,给出了十次对称二维准晶半无限裂纹问题应力和位移的解析表达式.     

任意形状孔口单边裂纹问题的边界配位解法

本文提出了一组复应力函数,采用边界配位方法对不同形状孔口(包括圆、椭圆、矩形及菱形孔口)的单边裂纹平板的应力强度因子进行了计算.计算结果表明,对长度和宽度远大于孔口和裂纹几何尺寸的试件,配位法与用其他方法所得的无限大板含圆或椭圆孔边裂纹问题的解符合得很好.同时,对其他孔口问题,特别是有限大板情形,本文给出了一系列计算结果.本文所提出的函数及计算过程可以应用于任意形状孔口单边裂纹平板的计算.     

Univalent Functions in Two-Dimensional Free Boundary Problems

The main goal of the paper is to bring together methods of the classical theory of univalent functions and some problems of fluid mechanics. Our interest centers on free boundary problems. We study the time evolution of the free boundary of a viscous fluid in the zero- and nonzero-surface-tension models for planar flows in Hele-Shaw cells either with an extending to infinity free boundary or with a bounded free boundary. We consider special classes of univalent functions that admit an explicit geometric interpretation to characterize the shape of the free interface. Another model is two-dimensional solidification/melting of a nucleus in a forced flow.     

Implicit Solution of a Two-Dimensional Parabolic Inverse Problem with Temperature Overspecification

Three different implicit finite difference schemes for solving the two-dimensional parabolic inverse problem with temperature overspecification are considered. These schemes are developed for indentifying the control parameter which produces, at any given time, a desired temperature distribution at a given point in the spatial domain. The numerical methods discussed, are based on the second-order (5,1) Backward Time Centered Space (BTCS) implicit formula, and the second-order (5,5) Crank-Nicolson implicit finite difference formula and the fourth-order (9,9) implicit scheme. These finite difference schemes are unconditionally stable. The (9,9) implicit formula takes a huge amount of CPU time, but its fourth-order accuracy is significant. The results of a numerical experiment are presented, and the accuracy and central processor (CPU) times needed for each of the methods are discussed and compared. The implicit finite difference schemes use more central processor times than the explicit finite difference techniques, but they are stable for every diffusion number.     

Optimal Control of a Parabolic Equation with Dynamic Boundary Condition

We investigate a control problem for the heat equation. The goal is to find an optimal heat transfer coefficient in the dynamic boundary condition such that a desired temperature distribution at the boundary is adhered. To this end we consider a function space setting in which the heat flux across the boundary is forced to be an L ^p function with respect to the surface measure, which in turn implies higher regularity for the time derivative of temperature. We show that the corresponding elliptic operator generates a strongly continuous semigroup of contractions and apply the concept of maximal parabolic regularity. This allows to show the existence of an optimal control and the derivation of necessary and sufficient optimality conditions.