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弹性波慢度表面的计算
引用本文:朱合,任伟,肖刘琴.弹性波慢度表面的计算[J].杭州电子科技大学学报,2008,28(2):5-8.
作者姓名:朱合  任伟  肖刘琴
作者单位:杭州电子科技大学电子信息学院,浙江,杭州,310018
摘    要:由声场本构方程导出速度场的波动方程,令本征矩阵的行列式为零,得到含参量的三次方程。弹性波慢度的计算涉及到张量运算、矩阵运算、公式化简等。对于一般的各向异性媒质,方程有三个互不相等的特征根:一个准纵波和两个准横波;对于各项同性媒质,方程有两个互不相等的特征根,其中一个为重根:一个纵波和一个横波。该文给出了弹性波慢度归一化后的空间分布图形。

关 键 词:弹性波慢度  色散方程  特征波数
文章编号:1001-9146(2008)02-0005-04
修稿时间:2007年9月4日

Computation of Acoustic Wave's Slowness Surface
ZHU He,REN Wei,XIAO Liu-qin.Computation of Acoustic Wave's Slowness Surface[J].Journal of Hangzhou Dianzi University,2008,28(2):5-8.
Authors:ZHU He  REN Wei  XIAO Liu-qin
Affiliation:( School of Electronics & lnfonnoZion, Hangzhou Dianzi University, Hang'zhou Zhejiang 310018, China)
Abstract:The problem of acoustic wave' s slowness surface is derived from the acoustic waves equation, parametric triple equation whose roots are characteristic slowness numbers is obtained after setting the determinant of eigen - matrix to zero. Acoustic wave' s slowness is involved with the calculations of the tensor computing, matrix opera- tions, formulaic simplification and so on. The general anisotropic media, there are three different characteristic roots in the equation: a prospective longitudinal wave and two prospective horizontal waves; to the isotropic media, there are two different characteristic roots, one of them is a same root: a longitudinal wave and a horizontal wave. In order to make the abstract concept more intuitive, give the acoustic wave' s slowness return of the spatial distribution of graphics.
Keywords:acoustic wave' s slowness  dispersion equation  characteristic waves
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