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首页> 外文期刊>Bulletin of the Seismological Society of America >The 2015 Gorkha, Nepal, Earthquake Sequence: II. Broadband Simulation of Ground Motion in Kathmandu
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The 2015 Gorkha, Nepal, Earthquake Sequence: II. Broadband Simulation of Ground Motion in Kathmandu

机译:2015年Gorkha,尼泊尔,地震序列:II。 加德满都地面运动的宽带仿真

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摘要

The relatively low damage in the Kathmandu Valley caused by the 2015 M-w 7.8 Gorkha earthquake has attracted much attention. To gain a deeper understanding of this phenomenon, we conduct broadband ground-motion simulations for both the mainshock and the M-w 7.2 Dolakha aftershock through a hybrid method that combines deterministic 3D synthetics at relatively low frequencies (< 0.3 Hz) and semi-stochastic synthetics at higher frequencies (> 0.3 Hz). Because they are summarized in a companion paper (Wei et al., 2018), the 3D deterministic synthetics were generated by embedding a finite-fault rupture model in a 3D velocity model that is characterized by a simplified basin structure for the Kathmandu Valley. We tested different weighting schemes using a finite slip model and backprojection results to weight the high-frequency sources. Our simulations were guided by fitting the observations from five strong-motion stations in Kathmandu Valley and the intensity and mortality distributions. Site effects were handled by amplitude spectra ratio derived from the vertical component of a hard-rock station (KTP). Our broadband ground-motion simulations show that (1) the stress parameter (3.8 MPa) of the mainshock was much lower in comparison to the M-w 7.2 aftershock (23 MPa) that suggests the rupture process of the mainshock was relatively deficient in radiating high-frequency energy and different fault friction property between the mainshock and the aftershock; (2) the soft deposits in the Kathmandu Valley experienced a pervasive nonlinear site response during the mainshock and the M-w 7.2 aftershock, which also contributed to the reduction of high-frequency motions; and (3) the high-frequency ground motions during the mainshock were primarily radiated from the down-dip rupture. Hence, we suggest considering the difference in the distribution of high-frequency radiation and fault slip in the broadband ground-motion simulations for scenario and historical earthquakes.
机译:由2015 M-W 7.8 Gorkha地震引起的加德满都谷造成相对较低的伤害引起了很多关注。为了深入了解这种现象,我们通过混合方法对主轴和MW 7.2 Dolakha余震进行宽带地面运动模拟,该混合方法将确定性3D合成物在相对低的频率(<0.3Hz)和半随机合成中结合在一起更高的频率(> 0.3 Hz)。因为它们总结在伴侣论文中(Wei等,2018),所以通过在3D速度模型中嵌入有限速度破裂模型来产生3D确定性合成,其特征在于加入万古谷的简化盆地结构。我们使用有限的滑动模型和背部注入结果测试了不同的加权方案,以重量高频源。我们的模拟是通过拟合加德满都谷的五个强运动站和强度和死亡率分布的观察来指导。通过从硬岩站(KTP)的垂直分量衍生的幅度谱比处理现场效应。我们的宽带地运动模拟显示(1)与MW 7.2余震(23MPa)相比,主轴的应力参数(3.8MPa)大得多,表明主震动的破裂过程相对缺乏辐射高 - 主轴和余震之间的频率和不同故障摩擦物质; (2)加德满都谷的软矿床在主屏蔽期间经历了普遍的非线性部位响应,M-W 7.2余震,也有助于降低高频运动; (3)主轴期间的高频接地运动主要从下降浸渍破裂辐射。因此,我们建议考虑在情景和历史地震中宽带地面运动模拟中的高频辐射和故障滑动分布的差异。

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