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Estimation of temporal variations in the magnetic field arising from the motional induction that accompanies seismic waves at a large distance from the epicentre

机译:估计距震中很远的地震波伴随运动感应而产生的磁场的时间变化

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摘要

Temporal variations in the electromagnetic field that accompany earthquakes are generated by various mechanisms, of which this study focuses on variations in the magnetic field arising from motionally induced electric currents that accompany seismic waves at large distances (several hundred kilometres) from the epicentre. A simple situation is considered in which seismic waves are approximated by plane waves and the electrical conductivity of the Earth's crust has a stratified structure. Solutions of Maxwell's equations corresponding to this situation have analytical expressions. Analysis of the solutions verifies that SH waves do not generate variations in the EM field above the ground surface, thereby implying that Rayleigh waves are dominant at a significant distance from earthquake epicentres. Numerical examples demonstrate that the amplitudes of the variations in the magnetic field monotonically increase with increasing conductivity, although attenuation because of the skin effect cannot be ignored. The amplitudes of the generated magnetic field can be sensitive to the conductivity of both the shallow and deep crust. Nevertheless, calculations assuming a simplified conductivity structure provide an upper limit to the possible amplitudes of variations in the magnetic field because of seismic waves. For example, the amplitudes of variations in the magnetic field arising from a Rayleigh wave with displacement amplitude of 10 cm and a period of 30 s are as large as 0.1 nT, close to the limit of detection under typical observation conditions. It is also suggested that phase differences between seismic ground motions and variations in the magnetic field are insignificantly influenced by details of conductivity structures, and they occur within a rather narrow range of values determined by the direction orientation of the ambient geomagnetic field. In the future, if a detection limit of 0.01 nT becomes available, phase difference may be used to distinguish variations arising from the motional induction, from variations arising from other mechanisms.
机译:伴随地震发生的电磁场的时间变化是由多种机制产生的,其中,本研究的重点是由运动感应电流产生的磁场变化,该感应电流伴随着与震中相距较大距离(几百公里)的地震波。考虑一种简单的情况,其中地震波由平面波近似并且地壳的电导率具有分层结构。对应于这种情况的麦克斯韦方程组的解具有解析表达式。对解决方案的分析证明,SH波不会在地表上方的EM场中产生变化,从而表明瑞利波在距地震震中很远的距离内占主导地位。数值示例表明,磁场的变化幅度随电导率的增加而单调增加,尽管由于集肤效应而引起的衰减不能忽略。产生的磁场的幅度可能对浅层和深层地壳的电导率都敏感。然而,假设简化的电导率结构的计算为由于地震波而引起的磁场变化的可能幅度提供了上限。例如,位移振幅为10 cm,周期为30 s的瑞利波引起的磁场变化幅度高达0.1 nT,接近典型观察条件下的检测极限。还建议地震传导和磁场变化之间的相位差受电导率结构细节的影响很小,并且它们出现在由环境地磁场的方向确定的相当窄的值范围内。将来,如果有0.01 nT的检测极限可用,则可以使用相位差来将运动感应引起的变化与其他机制引起的变化区分开。

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  • 作者

    Yamazaki Ken’ichi;

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  • 年度 2012
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  • 原文格式 PDF
  • 正文语种 en
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