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Results from a 1500 m deep, three-level downhole seismometer array: Site response, low Q values, and f_(max)

机译:1500 m深的三层井下地震仪阵列的结果:场地响应,低Q值和f_(max)

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摘要

A three-level downhole array is being operated in a 1500-m-deep borehole within the seismically active Newport-Inglewood fault zone, Los Angeles basin. The array consists of three three-component 4.5 Hz seismometers deployed at the surface, and at 420 and 1500 m depth. An M = 2.8 earthquake that occurred 0.9 km away from the array at a depth of 5.3 km on 31 July 1986 generated rays traveling almost vertically up the downhole array. The P- and S-wave pulse shapes show increasing pulse rise time with decreasing depth, and the initial pulse slope is less steep at the surface than at 1500 m. The average value of t_s/t_p between 1500 and 420 m depth is 1.7 and between 420 and 0 m is 3.4. A near-surface site response results in amplification on the P wave by a factor of four and S waves by a factor of nine. These data indicate a near-surface Q_α of 44 ± 13 for rays traveling almost vertically. In the case of S waves, most of the high frequency content of the waveform beyond ∼ 10 Hz observed at 1500 m depth is lost through attenuation before the waveform reaches 420 m depth. The average Q_β is 25 ± 10 between 1500 and 420 m depth and 108 ± 36 between 420 and 0 m depth. The spectra of the S waves observed at 420 and 0 m of the downward reflected S phases may overestimate Q_β, because they are limited to a narrow band between 5 and 10 Hz and affected by the near-surface amplification. A Q_c of 160 ± 30 at 6 Hz was determined from the decay rate of the coda waves at all three depths. The corner frequency as determined from displacement spectra may be higher (f_c ∼ 10 Hz) at 1500 m depth than at (f_c ∼ 7 Hz) 420 and 0 m depth. Similarly, f_(max) significantly decreases as the waveforms travel toward the earth's surface, indicating that f_(max) is affected by near-surface attenuation. Beyond f_c, the average slopes of the spectra falloff of P-wave spectra is ∼f^(−2) at 1500 m depth and ∼ f^(−3) at the surface.
机译:一个三层井下阵列正在洛杉矶盆地纽波特-英格伍德断层地震活跃的1500米深的井眼中运行。该阵列由部署在地面,深度为420和1500 m的三个三分量4.5 Hz地震仪组成。 1986年7月31日,M = 2.8地震发生在距阵列0.9公里处,深度为5.3 km,产生的射线几乎垂直向上传播至井下阵列。 P波和S波脉冲形状显示出随深度减小而增加的脉冲上升时间,并且在地表的初始脉冲斜率不如1500 m陡。 1500至420 m深度之间的t_s / t_p平均值为1.7,而420至0 m之间的平均值为3.4。近地表位置响应导致P波放大4倍,S波放大9倍。这些数据表明,几乎垂直传播的光线的近表面Q_α为44±13。在S波的情况下,在1500 m深度处观察到的约10 Hz以上的波形的大部分高频成分在波形达到420 m深度之前通过衰减而丢失。在1500至420 m深度之间的平均Q_β为25±10,在420至0 m深度之间的平均Q_β为108±36。在向下反射的S相的420和0 m处观察到的S波的光谱可能会高估Q_β,因为它们仅限于5至10 Hz之间的窄带并受近表面放大的影响。根据在所有三个深度处尾波的衰减率确定在6 Hz时的Q_c为160±30。由位移谱确定的转折频率在1500 m深度处可能比(f_c〜7 Hz)420和0 m处的频率更高(f_c〜10 Hz)。类似地,f_(max)随波形向地球表面传播而显着降低,表明f_(max)受近地表衰减的影响。除f_c以外,P波谱的谱衰减的平均斜率在1500 m深度处为〜f ^(-2),在表面处为〜f ^(-3)。

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