Estimation of Coda Wave Attenuation in Northern Morocco

被引:0
作者
Abderrahim Boulanouar
Lahcen El Moudnib
Simanchal Padhy
Mimoun Harnafi
Antonio Villaseñor
Josep Gallart
Antonio Pazos
Abdelaali Rahmouni
Mohamed Boukalouch
Jamal Sebbani
机构
[1] Mohamed V University,Physics Department, Faculty of Science
[2] Mohamed V University,Earth Science Department, Scientific Institute
[3] National Geophysical Research Institute,Institute of Earth Science “JaumeAlmera”
[4] CSIC,Geophysical Department
[5] Royal Naval Observatory,undefined
来源
Pure and Applied Geophysics | 2018年 / 175卷
关键词
Attenuation; coda waves; northern morocco; the single scattering model;
D O I
暂无
中图分类号
学科分类号
摘要
We studied the attenuation of coda waves and its frequency and lapse-time dependence in northern Morocco. We analysed coda waves of 66 earthquakes recorded in this region during 2008 for four lapse time windows of length 30, 40, 50, and 60 s, and at five frequency bands with central frequency in the range of 0.75–12 Hz. We determined the frequency dependent Qc relation for the horizontal (NS and EW) and vertical (Z) component seismograms. We analyzed three-component broadband seismograms of 66 local earthquakes for determining coda-Q based on the single back-scattering model. The Qc values show strong frequency dependence in 1.5–12 Hz that is related to high degree of heterogeneity of the medium. The lapse time dependence of Qc shows that Q0 (Qc at 1 Hz) significantly increases with lapse time that is related to the depth dependence of attenuation and hence of the level of heterogeneity of the medium. The average frequency-dependent Qc(f) values are Qc=(143.75±1.09)f(0.864±0.006),\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q_{\text{c}} = (143.75 \pm 1.09)f^{(0.864 \pm 0.006)},$$\end{document}Qc=(149.12±1.08)f(0.85±0.005)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q_{\text{c}} = (149.12 \pm 1.08)f^{(0.85 \pm 0.005)}$$\end{document} and Qc=(140.42±1.81)f(0.902±0.004)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q_{\text{c}} = (140.42 \pm 1.81)f^{(0.902 \pm 0.004)}$$\end{document} for the vertical, north–south and east–west components of motion, respectively. The frequency-dependent Qc(f) relations are useful for evaluating source parameters (Singh et al. 2001), which are the key inputs for seismic hazard assessment of the region.
引用
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页码:883 / 897
页数:14
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