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Measurement of the seismoelectric response from a shallow boundary

机译:浅边界地震电响应的测量

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摘要

Field experiments carried out at a site near Vancouver, Canada have shown that a shallow lithologic boundary can be mapped on the basis of its seismoelectric response. As seismic waves cross the boundary between organic-rich fill and impermeable glacial till, they induce electric fields that can be measured at the surface with grounded dipole receivers. Sledgehammer and blasting cap seismic sources, positioned up to 7 m away from the interface, have produced clear seismoelectric conversions. Two types of seismoelectric signals are observed. The primary response is distinguished by near simultaneous arrivals at widely separated receivers. Its arrival time is equal to the time required for a seismic P-wave to travel from the shotpoint to the fill/till boundary. On the surface, its maximum amplitude (about 1 mV/m) is measured by dipoles located within a few meters of the shotpoint. At greater distances, the amplitude of the primary arrival decays rapidly with offset, and secondary seismoelectric arrivals become dominant. They differ from the primary response in that their arrival times increase with dipole offset, and they appear to be generated in the immediate vicinity of each dipole Sensor. Our studies show that the responses cannot be attributed to piezoelectricity or to resistivity modulation in the presence of a uniform telluric current. We infer that seismically induced electrokinetic effects or streaming potentials are responsible for the seismoelectric conversion, and a simple electrostatic model is proposed to account for the two types of arrivals. Although our experiments were small in scale, the results are significant in that they suggest that the seismoelectric method may be used to map the boundaries of permeable formations.
机译:在加拿大温哥华附近的一个地点进行的现场试验表明,可以根据地震电响应来绘制浅岩性边界。地震波越过富含有机物的填充物和不可渗透的冰川土之间的边界时,它们会感应出可以用接地偶极子接收器在地表测量的电场。距离界面最远7 m的大锤和爆破帽地震源已经产生了清晰的地震电转换。观察到两种类型的地震电信号。主要响应的特点是几乎同时到达相距较远的接收器。它的到达时间等于地震P波从发射点传播到填充/耕作边界所需的时间。在表面上,其最大振幅(大约1 mV / m)由位于发射点几米内的偶极子测量。在更大的距离处,一次到达的振幅随偏移而迅速衰减,而二次地震电波则占主导地位。它们与主要响应的不同之处在于,它们的到达时间随偶极子偏移的增加而增加,并且似乎是在每个偶极子传感器的紧邻区域中生成的。我们的研究表明,在存在均匀碲电流的情况下,响应不能归因于压电性或电阻率调制。我们推断,地震感应的动电效应或流动电位是造成地震电转换的原因,并且提出了一种简单的静电模型来解释两种到达形式。尽管我们的实验规模很小,但结果是有意义的,因为它们表明地震电法可用于绘制渗透性地层的边界。

著录项

  • 来源
    《Geophysics》 |1996年第6期|p.1769-1778|共10页
  • 作者单位

    Department of Geophysics and Astronomy, The University of British Columbia, 2219 Main Mall, Vancouver BC, V6T 1Z4, Canada;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 地球物理学;
  • 关键词

  • 入库时间 2022-08-18 00:20:13

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