导电地壳中非稳态电动力学效应的模拟

O. Majaeva, Y. Fujinawa, M. Zhitomirsky
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引用次数: 9

摘要

由于其精确可解性而选择的层状半空间中,计算了由电动效应产生的球形时变压力源的磁场。除了广泛讨论的稳态相外,电动力源的电磁信号还有一个瞬态相,这与它们通过导电地壳的传播相对应。瞬态阶段的持续时间取决于离压力梯度源的距离和地壳电导率。当特征电导率为0.1-10-3 S/m,距离为几公里时,瞬态相位持续10-100秒。虽然在层状模型中,瞬态和稳态外磁场都为零,但在一般情况下并非如此。因此,如果在充水断层中发生电动力效应,则瞬态磁场会以极低频脉冲的形式出现在地表。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Modeling of non-stationary electrokinetic effect in a conductive crust
The magnetic field, generated by the electrokinetic effect is calculated for a spherical, time-varying pressure source in a layered half-space chosen due to its exact solvability. In addition to a widely discussed steady-state phase, electromagnetic signals of electrokinetic origin have a transient phase which corresponds to their propagation through a conductive crust. The duration of the transient phase depends on a distance from there pressure gradient source and on the crustal conductivity. For characteristic conductivities of 0.1-10-3 S/m and distances of several kilometers the transient phase lasts for 10-100 sec. Although in the layered model both transient and steady state external magnetic fields are zero, this is not so in the general case. Therefore, if the electrokinetic effect occurs in a water filled fault, the transient magnetic field can appear at the surface as an ULF pulse.
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