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Three methods for the description of the temporal response to a SH plane impulsive seismic wave in a soft elastic layer overlying a hard elastic substratum

机译:描述覆盖硬硬弹性层的软弹性层中SH面脉冲地震波时间响应的三种方法

摘要

We treat the case of a flat stress-free surface (i.e., the ground in seismological applications) separating air from a homogeneous, isotropic, solid substratum overlain by a homogeneous, isotropic, solid layer (in contact with the ground) solicited by a SH plane body wave incident in the substratum. The analysis is first carried out in the frequency domain and subsequently in the time domain. The frequency domain response is {it normal} in that no resonances are excited (a resonance is here understood to be a situation in which the response is infinite in the absence of dissipation). The translation of this in the time domain is that the scattered pulse is of relatively-short duration. The duration of the pulse is shown to be largely governed by radiation damping which shows up in the imaginary parts of the complex eigenfrequencies of the configuration. Three methods are elaborated for the computation of the time history and give rise to the same numerical solutions for a large variety of configurations of interest in the geophysical setting under the hypothesis of non-dissipative, dispersionless media. The method appealing to the complex eigenfrequency representation is shown to be the simplest and most physically-explicit way of obtaining the time history (under the same hypothesis). Moreover, it is particularly suited for the case in which modes can be excited as occurs when the incident wave is not plane or the boundary condition is not of the stress-free variety for all transverse coordinates on the ground plane.
机译:我们处理的是平坦无应力的表面(即地震应用中的地面),该表面通过SH求出的均质,各向同性,固态层(与地面接触)将空气与均质,各向同性,固态底层覆盖平面波入射在基底中。首先在频域中进行分析,然后在时域中进行分析。频域响应是{正常的},因为没有谐振被激发(此处的谐振被理解为在没有耗散的情况下响应是无限的情况)。这在时域上的转换是散射脉冲的持续时间相对较短。脉冲的持续时间在很大程度上受辐射衰减的控制,辐射衰减出现在配置的复杂特征频率的虚部。详细阐述了三种计算时间历程的方法,并在非耗散,无分散介质的假设下,针对地球物理环境中感兴趣的多种配置,给出了相同的数值解。事实证明,吸引复杂本征频率表示的方法是获得时间历程(在相同假设下)的最简单,最明确的方法。此外,它特别适用于这样的情况,即当入射波不是平面的或者边界条件对于地平面上的所有横向坐标不是无应力变化时,可以激发模式。

著录项

  • 作者

    Wirgin Armand;

  • 作者单位
  • 年度 2006
  • 总页数
  • 原文格式 PDF
  • 正文语种 en
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