Соболев空间中函数的有限元逼近以及在近似求解微分方程中的应用

用插值节点的均匀性,在空间中函数具有嵌入性质的条件下,导出了最佳逼近的误差估计,本文仍利用插值节点均匀性假设,对空间中的一般函数,也导出了逼近的误差估计,不再要求函数的嵌入性质; Ciarlet在仿射等价和空间函数具有嵌入性质的条件下,对一个二阶椭圆边值问题论证数值积分并不影响有限元子空间近似解逼近变分问题真解的速度。本文借助於空间中的一般函数的有限元逼近理论,对这一特殊的二阶椭圆边值问题,在基函数满足均匀性条件下,不要嵌入性质同样得到上面结果。     

嵌在弹性半空间的刚性变直径圆轴的扭转*

本文用线载荷积分方程法(LLIEM)研究嵌在弹性半空间的刚性变直径圆轴的轴对称扭转.利用将“半空间的点环力偶”(PRCHS)这一虚的基本载荷沿对称轴的圆轴区间中分布就能使本问题归结为一个一维的非奇异的Ferdholm第一种积分方程,且很易用数值求解.文中给出刚性圆锥,圆柱,圆锥柱嵌在弹性半空间的扭转的数值计算的例并和他人的已知结果相比较.文中也给出了刚性半球嵌在弹性半空间的扭转的精确解.     

一化学反应扩散方程组解的渐近性态

本文研究地下水中一化学反应模型全局解的渐近性质．利用半群理论和Ｓｏｂｏｌｅｖ空间嵌入定理，得到了当时间ｔ＋∞时的模型解的极限，并给出了明确的收敛速度估计．     

半连续格和半代数格的映射性质

研究了半连续格及半代数格的一些映射性质,讨论了强连续格的函数空间,给出了强连续格到方体的嵌入定理.     

RN上一类半线性椭圆方程组的多重解

利用对称山路引理,L2(RN)上加权Sobolev空间紧嵌入定理和一个线性耦合特征值问题,本文证明了RN上一类半线性椭圆方程组的多重解的存在性.     

多项式增长群具有性质A的初等证明方法

在粗几何的研究中,顺从性可以推出性质A;具有性质A的离散度量空间可以粗嵌入到Hilbert空间;粗Baum-Connes猜想和Novikov猜想可以由粗嵌入性质推出.因此,顺从性和性质A在粗几何研究中占有重要地位.主要关注一种特殊的群,称为多项式增长群.仅从多项式增长群和性质A的基本定义出发,证明了多项式增长群具有顺从性和性质A.     

半线性椭圆问题Petrov-Galerkin逼近及亏量迭代

本文考虑了二阶半线性椭圆问题的Petrov-Galerkin逼近格式,用双二次多项式空间作为形函数空间,用双线性多项式空间作为试探函数空间,证明了此逼近格式与标准的二次有限元逼近格式有同样的收敛阶.并且根据插值算子的逼近性质,进一步证明了半线性有限元解的亏量迭代序列收敛到Petrov-Galerkin解.     

一类渐近线性双调和方程非平凡解的存在性

通过建立新空间H,证明了一个嵌入定理.进一步,利用该嵌入定理与山路引理得到了一类渐近线性双调和问题在空间H中非平凡解的存在性.     

一类热弹性板的空间衰减估计

研究了二维空间中半无限带形区域上一类含有双调和算子的热弹性系统板解的空间性质.首先构造一个能量表达式,然后利用微分不等式技术,推导出该能量表达式是可由它本身的一阶导数控制的微分不等式,最后得到解的空间衰减估计.该结果可看成是Saint-Venant原则在双曲抛物耦合双调和方程组上的应用.     

一类模糊不动点定理及其应用

在半序模糊距离空间中,讨论了一类单调模糊映射的性质,并且把其应用于研究RegularFNN和解模糊方程.     

嵌入弹性半空间的弹性迴转轴的扭转*

本文用线载荷积分方程法(LLIEM)研究嵌在弹性半空间的弹性迴转轴的扭转问题.将“点环力偶(PRC)”和“半空间点环力偶(PRCHS)”分别分布于迴转轴内和外的轴线上,就能将本问题归结为一维的Fredholm第一种积分方程组.直接用离散法求解时,会发现有时解是不稳定的,也就是病态情形.本文采用以带小参数的Fredholm第二种积分方程代替病态的Fredholm第一种积分方程的方法可以得到稳定的解,此法比Tikhonov正规化法简单,易于在计算机上运行.文中给出圆维、圆柱、圆锥-圆柱、抛物线轴等数值例子.     

SH波对界面含有半圆形脱胶的圆柱形弹性夹杂的散射的近似分析

采用Green函数法、复变函数法研究了SH波对界面附近含有半圆形脱胶的圆柱形弹性夹杂的散射,并给出了动应力集中系数的数值结果．首先,界面将整个空间分成上下两部分．在下半空间,给出在含有半圆形凸起的圆柱形弹性夹杂的弹性半空间中,水平表面上任意一点承受时间谐和的出平面线源荷载作用时的位移函数．其次,取该位移函数作为Green函数．上下空间连接时在界面处满足连续性条件,构造出半圆形脱胶裂纹,进而求出应力和位移的表达式．最后作为算例,给出了动应力集中系数的数值结果,分析了介质参数和入射波参数对动应力集中的影响情况．     

椭圆孔边裂纹对SH波的散射及其动应力强度因子

采用复变函数和Green函数方法求解具有任意有限长度的椭圆孔边上的径向裂纹对SH波的散射和裂纹尖端处的动应力强度因子．取含有半椭圆缺口的弹性半空间水平表面上任意一点承受时间谐和的出平面线源荷载作用时的位移解作为Green函数,采用裂纹“切割”方法,并根据连续条件建立起问题的定解积分方程,得到动应力强度因子的封闭解答．讨论了孔洞的存在对动应力强度因子的影响．     

线载荷积分方程法分析桩顶受任意荷载的弹性斜桩

嵌在各向同性均匀弹性半空间的弹性斜桩顶部,受任意荷载的位移和应力,可分解为在倾斜平面xOz及其法平面yOz内进行分析.将Mindlin力作为基本虚载荷,令集度为未知函数X(t)、Y(t)、Z(t),分别平行于x、y、z轴,的基本载荷沿桩轴t的[0,L]内分布,并在桩顶作用集中力Q_x,Q_y、Z,力偶矩M_y、M_x,根据弹性桩的边界条件,将问题归结为一组Fredholm-Volera型的积分方程.文中给出数值解.计算结果的精度可用功的互等定理来检查.     

Effect of a Concentrated Normal Force on the Surface of an Orthotropic Half Space

An analytic solution is given for the stressed-deformed state of an orthotropic half space acted on by a normal concentrated force applied to its boundary. It is shown that the traditional choice of a general representation of the displacements in a gradient form, where the potential functions are in the form of double Fourier integrals with unknown densities, reduces the problem to solving two systems of linear algebraic equations – homogeneous and inhomogeneous. A solution obtained by taking a limiting transition is given for the case of an isotropic half space.     

用复变函数法求解弹性力学空间轴对称问题的方法及解例

本文证明了空间轴对称问题的Love应力函数可用两个适当选择的复变量广义解析函数[1]表示,并导出了应力分量、位移分量及边界条件的复变函数表达式.为了表明文中所述方法的可行性以及检验所得公式的正确性,本文用幂级数法求解了含有球形空腔的圆柱体在周围受压及两端受拉时的解答,与用其他方法得到的该问题的解答完全一致.最后本文还求解了一个锥体在侧面受均匀剪力时的解答,同时通过把常体力化为表面力以后还求解了锥体在重力作用下的解答.     

Vertical oscillations of multimass system on elastic half space with a cylindrical cavity

A problem on oscillations of a multimass system (MS) is considered on an elastic half space with a cylindrical cavity. Equations of motions of an MS are given, which are modeled by masses that are connected by springs and dampers. A motion of the half space with a cavity is characterized by a transmitting function,which is known from a solution of a contact problem with vertical oscillations of a die on the half space given. The conditions of interrelation of the MS with the base close the system of algebraic linear equations for determining amplitudes of oscillations of each element of the MS. Translated from Dinamicheskie Sistemy, No. 7, pp. 13–18, 1988.     

About embedded eigenvalues for a spectral problem arising in the study of elastic surface waves in a topographical waveguide

In this paper, we are interested with the spectral study of an operator given by an elastic topographical waveguide, a deformed half‐space, of which the cross‐section is a local perturbation of a homogeneous half‐plane. We look for guided waves propagating more rapidly than Rayleigh waves (which mathematically would correspond to embedded eigenvalues) and prove that there are no guided waves propagating more rapidly than S‐waves. Thanks to the boundary of the deformed half‐plane and some reduced equations, these eventual eigenmodes must locally vanish. Adapting to our case a unique continuation principle for the elasticity system, we conclude that these eigenmodes vanish everywhere. Copyright © 2002 John Wiley & Sons, Ltd.     

Dynamic strength around a coated nanowire with surfaces/interfaces in a half solid

In this paper, the multiple scattering of anti-plane shear waves around a coated nanowire with surfaces/interfaces embedded in a half solid is studied, and the dynamic stress at the two surfaces/interfaces is presented. The boundary condition at the edge of the half solid is satisfied by the image method. The analytical solutions of displacements in the two half solids, in the coating layers, and inside the nanowire are expressed by wave function expansion method. The expanded mode coefficients are determined by satisfying the boundary conditions at the two surfaces/interfaces of the coated nanowire and the straight edge of the structure. The addition theorem for cylindrical wave function is employed to accomplish the superposition of displacement fields in the two half solids. Analyses show that the properties of the outer and inner interfaces show different effect on the dynamic stress around the nanowire. The dynamic stress distribution around the nanowire is also significantly related to the interfacial properties at the edge and the position of the nanowire.