首页 | 本学科首页   官方微博 | 高级检索  
     检索      

三维结线动力无穷元
引用本文:陈健云,林蓓.三维结线动力无穷元[J].计算力学学报,1999,16(4):453-459.
作者姓名:陈健云  林蓓
作者单位:1. 大连理工大学土木工程系,大连,116023
2. 大连市政设计院
摘    要:构造一 亲的半解析结线动力无穷元。这种单元摆脱了一般离散型无穷元的形式,将衰减函数分别定义在无穷向结线上,从而不仅可同时考虑多种波动(R波、P波、S波)形式,而且对于不同介质,不必通过改变节点坐标分布的形式实现介质间的过渡,而直接以结线上参数的改变来实现。因而可以更好地模拟无穷波动场,使用起来为更方便,更容易推广。

关 键 词:动力无穷元  波动场
修稿时间::1997-12-1

3-D half-analytical dynamic infinite element
Chen Jianyun,Lin Gao,Lin Pei.3-D half-analytical dynamic infinite element[J].Chinese Journal of Computational Mechanics,1999,16(4):453-459.
Authors:Chen Jianyun  Lin Gao  Lin Pei
Institution:Chen Jianyun, Lin Gao, Lin Pei;(Dept. of Civil Engineering, Dalian University of Technology, Dalian 116023,China)
Abstract:In this paper, a new 3\|D dynamic infinite element is presented. Since the wave displacement field of the present element is defined on the infinite edge instead of on the whole element as the conventional infinite element, it is very convenient to use this element to simulate the R\|wave, P\|wave, SH\|wave and SV\|wave simultaneously, and to satisfy the displacement continuity along the common boundary of neighbouring infinite elements in the case of dimulating multiple material layers. The transfer of different media is completed by the definition of parameters of the infinite edge, not by the modification of the node coordinate as the convertionalinfinite element. It is more economical to use this element to model the wave field of the unbounded domain.
Keywords:dynamic infinite element  wave field
本文献已被 CNKI 维普 万方数据 等数据库收录!
点击此处可从《计算力学学报》浏览原始摘要信息
点击此处可从《计算力学学报》下载免费的PDF全文
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号