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首页> 外文期刊>Bulletin of the Seismological Society of America >Estimates of regional and local strong motions during the great 1923 Kanto, Japan, earthquake (Ms 8.2). Part 2: Forward simulation of seismograms using variable-slip rupture models and estimation of near-fault long-period ground motions
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Estimates of regional and local strong motions during the great 1923 Kanto, Japan, earthquake (Ms 8.2). Part 2: Forward simulation of seismograms using variable-slip rupture models and estimation of near-fault long-period ground motions

机译:对1923年日本关东大地震期间地区和地方强烈运动的估计(Ms 8.2)。第2部分:使用可变滑移断裂模型和近似断层长周期地面运动的地震记录正演模拟

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摘要

This article addresses the forward simulation of regional and local strong motions from the 1923 Kanto, Japan, earthquake (Ms 8.2), using two variable-slip rupture models: the Wald and Somerville (1995) slip model (WS slip model) derived from geodetic and teleseismic data and a resampled version of the Takeo and Kanamori (1992) slip model (TK slip model) that was obtained from the forward simulation of the Ewing seismoscope record at Hongo (HNG, epicentral distance R = 60 km). Green's functions are calculated using Bat-layered velocity models for specific source-receiver paths, which were developed in our first article (Sate ct al., 1998). For regional stations Sendai (R = 350 kill) and Gifu (R = 220 In), the WS slip model provides a much better match to the waveform data than the TK slip model, For local station HNG, the first 40 sec of the N77 degrees E Imamura seismogram is successfully reproduced by both of the slip models, although the arrivals are delayed in the TK slip model. The large-amplitude long-duration, long-period (13 sec) later phases in the southwest-component Ewing seismogram are not reproduced by either of the slip models. Our results suggest that the WS slip model gives a better representation of the overall rupture process of the 1923 event than the TK slip model does. Near-fault long-period ground motions calculated at several stations using the WS slip model suggest that the motions at HNG were not the largest in the Tokyo metropolitan area during the 1923 event. in addition, we estimate that the ground motions near the southern margin of the fault plane were significantly larger than the recorded near-fault motions of recent magnitude 7 earthquakes, such as North-ridge and Kobe, for periods longer than several seconds. This suggests that design codes based on the experience of these recent events may not adequately describe the long-period response expected during a magnitude 8 earthquake. [References: 54]
机译:本文使用两个可变滑动破裂模型:Wald和Somerville(1995)滑动模型(WS滑动模型),从大地测量学出发,对1923年日本关东地震(Ms 8.2)的区域和局部强运动进行正演模拟。和远震数据,以及Takeo和Kanamori(1992)滑动模型(TK滑动模型)的重采样版本,该模型是通过对本乡Ewing地震仪记录的正向模拟获得的(HNG,震中距离R = 60 km)。 Green的功能是使用蝙蝠分层速度模型针对特定的源-接收器路径计算的,该模型是在我们的第一篇文章中开发的(Sate等,1998)。对于区域站仙台(R = 350杀)和岐阜(R = 220 In),WS滑移模型提供的波形数据匹配度比TK滑移模型好得多。对于本地站HNG,N77的前40秒两种滑动模型都成功地再现了E今村地震图,尽管TK滑动模型中的到达时间有所延迟。两种滑动模型均未再现西南分量尤因地震图中的大振幅,长时间,长周期(13秒)。我们的结果表明,WS滑移模型比TK滑移模型能更好地表示1923年事件的整体破裂过程。在几个站点上使用WS滑动模型计算的近断层长周期地面运动表明,在1923年事件期间,HNG的运动并不是东京都会区内最大的。此外,我们估计,断层平面南缘附近的地​​震动要长于几秒钟,远大于记录的最近7级地震(如北岭和神户)的近断层震动。这表明基于这些最近事件的经验的设计规范可能无法充分描述8级地震中预期的长期响应。 [参考:54]

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