首页> 外文期刊>International Journal of Solids and Structures >TWO-DIMENSIONAL TIME DOMAIN BEM FOR SCATTERING OF ELASTIC WAVES IN SOLIDS OF GENERAL ANISOTROPY
【24h】

TWO-DIMENSIONAL TIME DOMAIN BEM FOR SCATTERING OF ELASTIC WAVES IN SOLIDS OF GENERAL ANISOTROPY

机译:一般各向异性的弹性波散射的二维时域边界元

获取原文
获取原文并翻译 | 示例
       

摘要

An efficient two-dimensional time-domain application of the Boundary Element Method is presented to solve elastodynamic boundary/initial-value problems in solids of general anisotropy. The method is based on the use of integral expressions for the Green's functions derived by Wang and Achenbach (1994) [Elastodynamic fundamental solutions for anisotropic solids. Geophys. J. int. 118, 384-392], and on the partition of these Green's functions into singular static and regular dynamic parts. The singular static parts are the elastostatic Green's functions, which have relatively simple explicit expressions in closed form. The regular dynamic parts are given in terms of line integrals over a unit circle, whose integrands have a simple structure which physically corresponds to a superposition of plane waves. The partition of the Green's functions leads to the decomposition of the singular elastodynamic boundary integral equation into terms corresponding to a singular elastostatic integral equation plus regular dynamic terms. The calculation effort is reduced by analytically evaluating both the integration over each boundary element and the time-convolution over each time-step. As a result only regular line integrals over the unit circle have to be computed numerically. Applications are discussed for scattering of elastic waves by cavities. The method has been checked by comparing numerical results against existing analytical solutions for an isotropic solid. Numerical results for scattering of elastic waves in a transversely isotropic material by a circular cylindrical cavity have also been obtained. Copyright (C) 1996 Elsevier Science Ltd. [References: 21]
机译:提出了一种边界元方法的有效二维时域应用,以解决一般各向异性固体中的弹性动力学边界/初值问题。该方法基于对Wang和Achenbach(1994)[各向异性固体的弹性力学基本解]推导的格林函数的积分表达式的使用。地理学。 J.int 118,384-392],然后将这些格林函数划分为单个静态和规则动态部分。奇异的静态部分是弹性静态格林函数,具有封闭形式的相对简单的显式表达式。规则的动态部分是根据单位圆上的线积分给出的,其积分数具有简单的结构,其物理上对应于平面波的叠加。格林函数的划分导致奇异弹性力学边界积分方程分解为与奇异弹性静力学积分方程加规则动力学项相对应的项。通过分析评估每个边界元素的积分和每个时间步长的时间卷积,可以减少计算工作量。结果,仅需数值计算单位圆上的规则线积分。讨论了通过腔体散射弹性波的应用。通过将数值结果与各向同性固体的现有分析解决方案进行比较,对方法进行了检验。还获得了通过圆柱形空腔在横向各向同性材料中散射弹性波的数值结果。版权所有(C)1996 Elsevier Science Ltd. [引用:21]

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号