弹性力学问题的局部边界积分方程方法

提出了弹性力学平面问题的局部边界积分方程方法。这种方法是一种无网格方法,它采用移动最小二乘近似试函数,且只包含中心在所考虑节点的局部边界上的边界积分。它易于施加本质边界条件。所得系统矩阵是一个带状稀疏矩阵。它组合了伽辽金有限元法、整体边界元法和无单元伽辽金法的优点。该方法可以容易推广到求解非线性问题以及非均匀介质的力学问题。计算了两个弹性力学平面问题的例子,给出了位移和能量的索波列夫模,所得计算结果证明：该方法是一种具有收敛快、精度高、简便有效的通用方法。     

用无网格局部Petrov-Galerkin法分析非线性地基梁

利用无网格局部Petroy-Galerkin法求解了非线性地基梁.在Petroy-Galerkin方法中,采用移动最小二乘(MLS)近似函数作为场变量挠度的试函数并取移动最小二乘近似函数中的权函数作为近似场函数的加权函数,采用罚因子法施加本质边界条件.文末给出了两个计算实例,算例的结果表明,Petrov-Galerkin法不仅能成功地分析线性地基梁,而且也适用于求解非线性地基梁,在分析非线性地基梁时具有收敛快,稳定性好的优点.     

用局部Petrov-Galerkin法分析薄板自由振动

利用薄板振型方程的等效积分弱形式和对振型函数采用移动最小二乘近似函数进行插值,本文进一步研究了无网格局部Petrov-Galerkin方法在薄板自由振动问题中的应用.它不需要任何形式的网格划分,所有的积分都在规则形状的子域及其边界上进行.在插值近似时,采用虚拟-实际节点值变换方法直接引入本质边界条件.通过数值算例和与其他方法的结果进行比较,表明无网格局部Petrov-Galerkin法求解弹性薄板自由振动问题具有收敛性好、精度高等一系列优点.     

壳结构的无网格局部Petrov-Galerkin方法

无网格近似函数具有高度光滑性,能够很好的逼近曲壳表面及其位移场。无网格局部Petrov-Galerkin方法不论插值还是离散都不需要单元,是一种真正的无网格方法。本文基于无网格局部Petrov-Galerkin方法的基本原理,采用移动最小二乘插值,利用控制微分方程弱形式,建立了Mindlin壳结构的无网格局部Petrov-Galerkin分析方法,用屋顶壳、受夹圆柱壳、几何非线性圆柱壳作为计算实例分析了求解精度、收敛性和稳定性,并与精确解和有限元计算结果进行了对比,表明该方法计算精度高及收敛性好。     

无网格局部Petrov-Galerkin方法的并行计算研究

研究了无网格局部Petrov-Galerkin方法MLPG(Meshless Local Petrov-Galerkin Method)的并行算法与并行实现过程。将MLPG方法推广到弹性动力学问题,研究了MLPG方法中节点搜索、积分点搜索、数值积分及方程组求解等过程的并行算法,并给出了MLPG方法并行计算的具体实现过程。两个数值算例验证了MLPG并行算法的有效性;计算结果表明,MLPG方法的并行计算具有很好的并行性能和可扩展性。     

基于局部Petrov-Galerkin离散方案的无网格法

基于局部Petrov-Galerkin离散方案,选用自然邻近插值构造试函数,用Shepard函数作为权函数,提出了一种无网格方法(MNNPG),这种方法充分发挥了局部Petrov-Galerkin法的优势,并且结合了自然邻近插值的特点,方便引入边界条件,由于以Shepard函数的圆形支集作为积分子域,用分片中点插值来完成区域积分,无需额外背景网格,是一种真正的无网格法。本文将该无网格方法用于求解二维弹性力学边值问题,算例结果很好地吻合了精确解,表明该方法具有良好的数值精度和稳定性。     

基于Voronoi结构的无网格局部 Petrov-Galerkin方法

基于自然邻结点近似位移函数提出了一种用于求解弹性力学平面问题的无网格局部 Petrov-Galerkin方法. 这种方法在结构的求解域${itOmega}$ 内任意布置离散的结点,并且利用需求结点的自然邻结点和Voronoi结构来构造整体求解的近似位移函数. 对于构造好的近似位移函数,在局部的Delaunay三角形子域上采用局部Petrov-Galerkin方法建立整体求解的平衡控制方程,这样平衡方程的积分可在背景三角形积分网格的形心上解析计算得到,而采用标准Galerkin方法的自然单元法需要三个数值积分点. 该方法能够准确地施加边界条件,得到的系统矩阵是带状稀疏矩阵,对软件用户来说,它还是一种完全的、真正的无网格方法. 所得计算结果表明,该方法的计算精度与有限元法四边形单元相当,但计算和形成系统平衡方程的时间比有限元法四边形单元提高了将近一倍,是一种理想的数值求解方法.     

A MESHLESS LOCAL PETROV-GALERKIN METHOD FOR GEOMETRICALLY NONLINEAR PROBLEMS

Nonlinear formulations of the meshless local Petrov-Galerkin （MLPG） method are presented for geometrically nonlinear problems. The method requires no mesh in computation and therefore avoids mesh distortion difficulties in the large deformation analysis. The essential boundary conditions in the present formulation axe imposed by a penalty method. An incremental and iterative solution procedure is used to solve geometrically nonlinear problems. Several examples are presented to demonstrate the effectiveness of the method in geometrically nonlinear problems analysis. Numerical results show that the MLPG method is an effective one and that the values of the unknown variable are quite accurate.     

改进广义移动最小二乘近似的无网格法

无网格法是求解微分方程定解问题的一种新数值方法.移动最小二乘近似只要求近似函数在各节点处的误差的平方和最小,对近似函数导数的误差没有任何约束.而广义移动最小二乘近似要求近似函数及其导数在所有节点处的误差的平方和最小.为了降低计算工作量,本文构造了要求近似函数在全部节点处和任意阶导数在部分节点处误差的平方和最小的改进广义移动最小二乘近似.数值计算显示本文提供的方法关于函数值和各阶导数值都具有很高的精度.     

大变形问题分析的局部Petrov-Galerkin法

在微机电系统(MEMS)的建模和模拟研究中,大变形或大移动要充分予以考虑.用有限元法分析这类问题,由于难以避免的网格畸变,使模拟效率精度降低甚至失效,无网格方法(Meshless Method)则能在分析这类问题时显示出明显的优势,无网格局部Petrov-Galerkin(MLPG)法被誉为是一种有发展前景的真正无网格法.本文进一步发展了MLPG法,通过对任意的离散分布节点采用局部径向基函数构造插值形函数和Heaviside权函数,分析方程采用局部加权弱形式离散,建立了变量仅依赖于初始构型的完全Lagrange分析格式,最后用Newton-Raphson法迭代求解.文中分析了悬臂梁典型算例和微机电开关非线性大变形问题,通过与有限元结果的比较,表明本文提出的大变形问题无网格局部Petrov-Galerkin法具有稳定性好及收敛性快等优点.     

Local Petrov-Galerkin method for a thin plate

The meshless local Petrov-Galerkin (MLPG) method for solving the bendingproblem of the thin plate were presented and discussed. The method used the moving least-squares approximation to interpolate the solution variables, and employed a local symmetricweak form. The present method was a truly meshless one as it did not need a finite elementor boundary element mesh, either for purpose of interpolation of the solution, or for theintegration of the energy. All integrals could be easily evaluated over regularly shapeddomains ( in general, spheres in three-dimensional problems ) and their boundaries. Theessential boundary conditions were enforced by the penalty method. Several numericalexamples were presented to illustrate the implementation and performance of the presentmethod. The numerical examples presented show that high accuracy can be achieved forarbitrary grid geometries for clamped and simply-supported edge conditions. No postprocessing procedure is required to computer the strain and stress, since the originalsolution from the present method, using the moving least squares approximation, is already smooth enough.     

A meshless method of a thin plate

A meshless approach to analysis of arbitrary Kirchhoff plates by the local boundary integral equation(LBIE) method is presented. The method combines the advantageous features of, all the three methods: the Galerkin finite element method (GFEM), the boundary element method (BEM) and the element-free Galerkin method (EFGM). It is a truly meshless method, which means that the discretization is independent of geometric subdivision into elements or cells, but is only based on a set of nodes (ordered or scattered) over a domain in question. It involves only boundary integration, however, over a local boundary centered at the node in question; It poses no difficulties in satisfying the essential boundary conditions while leading to banded and sparse system matrices using the moving least square (MLS) approximations. It is shown that high accuracy can be achieved for arbitrary geometries for clamped and simply-supported edge conditions. The method is found to be simple, efficient, and attractive. Project supported by the National Science Foundation of China (No. 19972019).     

Improved non-singular local boundary integral equation method

When the source nodes are on the global boundary in the implementation of local boundary integral equation method (LBIEM),singularities in the local boundary integrals need to be treated specially. In the current paper,local integral equations are adopted for the nodes inside the domain trod moving least square approximation (MLSA) for the nodes on the global boundary,thus singularities will not occur in the new al- gorithm.At the same time,approximation errors of boundary integrals are reduced significantly.As applications and numerical tests,Laplace equation and Helmholtz equa- tion problems are considered and excellent numerical results are obtained.Furthermore, when solving the Hehnholtz problems,the modified basis functions with wave solutions are adapted to replace the usually-used monomial basis functions.Numerical results show that this treatment is simple and effective and its application is promising in solutions for the wave propagation problem with high wave number.     

A STUDY ON THE WEIGHT FUNCTION OF THE MOVING LEAST SQUARE APPROXIMATION IN THE LOCAL BOUNDARY INTEGRAL EQUATION METHOD

The meshless method is a new numerical technique presented in recent years .It uses the moving least square (MLS) approximation as a shape function . The smoothness of the MLS approximation is determined by that of the basic function and of the weight function, and is mainly determined by that of the weight function. Therefore, the weight function greatly affects the accuracy of results obtained. Different kinds of weight functions, such as the spline function, the Gauss function and so on, are proposed recently by many researchers. In the present work, the features of various weight functions are illustrated through solving elasto-static problems using the local boundary integral equation method. The effect of various weight functions on the accuracy, convergence and stability of results obtained is also discussed. Examples show that the weight function proposed by Zhou Weiyuan and Gauss and the quartic spline weight function are better than the others if parameters c and a in Gauss and exponential weight functions are in the range of reasonable values, respectively, and the higher the smoothness of the weight function, the better the features of the solutions.