地面探地雷达数据一维全波形反演理论

E. Slob
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引用次数: 1

摘要

在一维条件下,全波形反演是一个线性问题。我表明,如果磁导率可以假设为常数,电导率为零,测量表面或空气中的磁场就足以作为输入数据。我提出的理论用积分方程,描述电场在介质内的对比度源。通过求解马尔琴科方程,可以从测量到的磁场计算出介质内部的电场。一旦这个场是已知的,只有对比函数是未知的,可以通过矩阵反演找到。如果还测量了电场,则逆问题可以递归求解。在一维中,深度本质上是未知的,我使用记录时间作为替代坐标。在已知介电常数是介质内部从表面到深度的单向旅行时间的函数之后,可以通过积分来求深度。这产生了电介电常数作为深度的函数,并且完成了全波形反演。一个简单的数值算例说明了该方法。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Theory for 1D full waveform inversion of surface GPR data
In one dimension, full waveform inversion is shown to be a linear problem under several conditions. I show that if the magnetic permeability can be assumed constant and electric conductivity to be zero, measuring the magnetic field at the surface or in the air suffices as input data. I present the theory using integral equations that describe the electric field inside the medium in terms of contrast sources. The electric field inside the medium can be computed from the measured magnetic field by solving a Marchenko equation. Once this field is known only the contrast function is unknown and can be found by matrix inversion. If the electric field is also measured the inverse problem can be solved recursively. In one dimension depth is intrinsically unknown and I use recording time as a replacing coordinate. After the electric permittivity is known as a function of one-way travel time from surface to a depth level inside the medium, the depth level can be found by an integral. This produces electric permittivity as a function of depth and full waveform inversion is complete. A simple numerical example demonstrates the method.
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