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Electroseismic Waves From Point Sources In Layered Media

机译:层状介质中点源的电震波

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摘要

The macroscopic governing equations controlling the coupled electromagnetics and acoustics of porous media are numerically solved for the case of a layered poro-elastic medium.It is shown that these coupled equations decouple into two equation sets describing two uncoupled wavefield pictures. That is, the PSVTM picture where the compressional and vertical polarized mechanical waves drive currents in the PSV particle motion plane that couples to the electromagnetic wavefield components of the TM mode. And the SHTE picture where the horizontal polarized rotational mechanical waves drive currents in the SH particle motion plane that couples to the electromagnetic wavefieldcomponents of the T E mode. The global matrix method is employed in computingelectroseismograms in layered poro-elastic media in the PSVTM picture.The principal features of the converted electromagnetic signals are the following:(1) contacts all antennas at approximately the same time; (2) arrives at the antennasat half of the seismic traveltime at normal incidence reflected P waves; and (3) changessign on opposite sides of the shot.The seismic pulse is shown to induce electric fields that travel with the compressionalwavespeed and magnetic fields that travel with the rotational wavefield. The frequencycontent of the converted electromagnetic field has the same frequency content of thedriving incident seismic pulse, as long as the propagation distances are much less thanthe electromagnetic skin depth.Snapshots in time and converted electromagnetic amplitudes versus seismic pointsource-antenna offset-are calculated for contrasts in mechanical and/or electrical mediumproperty. Conversion happens there where the seismic wavefront passes a contrast inmedium properties due to generated imbalances in current across the contrast. The TMcomponent amplitude radiation pattern away from the interface shows similarities with an effective electric dipole radiation pattern, or its dual, an effective magnetic currentloop radiation pattern centered right beneath the source at the contrast's depth. TheTM mode amplitudes decay rapidly with traveled distance and suggest the importanceof a Vertical Electroseismic Profiling geometry to enhance recording of the convertedelectromagnetic signal by positioning the antennas closer to the target (contrast) ofinterest.
机译:在层状孔隙弹性介质的情况下,数值求解了控制多孔介质耦合电磁和声学的宏观控制方程,结果表明这些耦合方程解耦为描述两个未耦合波场图像的两个方程组。也就是说,在PSVTM图片中,压缩和垂直极化机械波驱动PSV粒子运动平面中的电流,该电流耦合到TM模式的电磁波场分量。在SHTE图像中,水平极化旋转机械波驱动SH粒子运动平面中的电流,这些电流耦合到T E模式的电磁波场分量。整体矩阵法用于计算PSVTM图像中层状孔隙弹性介质中的地震图。转换后的电磁信号的主要特征如下:(1)几乎同时接触所有天线; (2)在法向入射反射的P波处到达地震传播时间一半的天线; (3)改变了镜头两侧的符号。地震脉冲被显示为感应以压缩波速传播的电场和以旋转波场传播的磁场。只要传播距离远小于电磁趋肤深度,转换后的电磁场的频率成分与驱动入射地震脉冲的频率成分相同。计算时间和转换快照与地震点源-天线偏移的对比机械和/或电气介质属性。转换发生在地震波前通过对比介质特性的地方,这是由于跨对比电流产生的不平衡。远离界面的TMcomponent振幅辐射图显示出与有效电偶极辐射图或它的双重,有效磁电流环辐射图相似的地方,即在对比深度处居于源正下方。 TM模式振幅随行进距离而迅速衰减,并表明垂直电地震剖面几何形状对于通过将天线放置在更靠近目标物体(对比度)的位置来增强转换电磁信号记录的重要性。

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