LOVE表面波和电阻率用于描述近地表地球物理结构的理论思考

Ö. Çakır, N. Coşkun
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引用次数: 0

摘要

我们反演了Love表面波和电阻率,以共同研究深度范围小于50米的物理性质。分析这一深度范围对地震减灾工作至关重要。横波速度(VS30)对于描述浅层地球的动态特性尤为重要。洛夫表面波是根据相速度和群速度处理的。相位速度采用倾斜叠加法,群速度采用多重滤波法。假设一个典型的短集来模拟表面波数据的现场采集。相速度曲线表示检波器分布下的平均结构。群速度曲线表示从震源到检波器的平均结构。在单站方式下,每个检波器位置得到一组速度曲线。建立了一个线性系统,将这些单站群速度曲线转换为网格点处的局部群速度曲线。后一组速度被反转得到横波速度截面。采用类似的方法研究地下电阻率结构。利用理论模型对现场应用进行了模拟。电阻率数据的现场采集采用多电极极-极阵列。视(测量)电阻率值被反转,以获得以截面表示的真实电阻率结构。倒置结构是一维反射深度相关的横波速度和电阻率在研究区域。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
LOVE SURFACE WAVES AND ELECTRICAL RESISTIVITY USED TO DELINEATE THE NEAR SURFACE GEOPHYSICAL STRUCTURE: THEORETICAL CONSIDERATIONS
We invert Love surface waves and electrical resistivities to cooperatively examine the physical properties of the depth range shallower than 50-m. To analyze this depth range is essential for earthquake mitigation efforts. The shear-wave velocity (VS30) is particularly important to describe the dynamic characteristics of shallow Earth. The Love surface waves are treated in terms of both phase and group velocities. The phase velocities are obtained from the slant stacking while for the group velocities the multiple filter technique is utilized. A typical shot-gather is assumed to simulate the field collection of the surface wave data. The phase velocity curve represents the average structure beneath the geophone spread. The group velocity curve represents the average structure from the source to the geophone. In a single-station fashion, for each geophone location one group velocity curve is obtained. A linear system is set up to convert these single-station group velocity curves into local group velocity curves at grid points. The latter group velocities are inverted to attain the shear-wave velocity cross section. A similar approach is adopted to study the electrical resistivity structure of the underground. We simulate the field application using a theoretical model. Multiple electrode Pole-Pole array is assumed for the field collection of the resistivity data. The apparent (measured) resistivity values are inverted to attain the true resistivity structure in terms of a cross section. The inverted structures are one-dimensional reflecting depth dependent shear-wave velocities and electrical resistivities underneath the studied region.
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