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Ground Motion and Liquefaction Simulation of the 1886 Charleston, South Carolina, Earthquake

机译:1886年南卡罗来纳州查尔斯顿地震的地震动和液化模拟

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As part of a comprehensive earthquake loss and vulnerability evaluation of the state of South Carolina, ground motions were simulated for a moment magnitude (M) 7.3 "1886 Charleston-like" earthquake using finite-fault and point-source stochastic numerical modeling. The probability for liquefaction was also predicted based on factors of safety computed from average cyclic stress and shear-wave-velocity-based cyclic resistance ratios, clay content, and saturation. Because there is considerable uncertainty regarding the 1886 source, the rupture plane of the 1886 event was modeled as both a 100-km-long, 20-km-wide fault (static stress drop of 27 bars) and a 50-km-long, 16-km-wide fault (107-bar stress drop). The source was assumed to be a north-northeast-striking, strike-slip fault coincident with the Woodstock fault. Based on comparing the computed and observed 1886 liquefaction areas and ground motions for both the low and high stress drop events, the two cases were weighted 0.8 and 0.2, respectively. To accommodate epistemic uncertainty in eastern U.S. earthquake source processes, three region-specific point-source attenuation models were also developed and used: a single-corner frequency model with both a constant stress drop and a magnitude-dependent stress drop, and the double-corner frequency model. The finite-fault and point-source models were weighted 0.8 and 0.2, respectively. To incorporate site effects into the ground-motion estimates, an extensive effort was made to characterize the thicknesses, shear-wave velocities (V_s), and dynamic material properties of unconsolidated sediments. Characteristic V_s profiles were developed using the available subsurface information, which incorporated a wide range of soil and rock conditions. Amplification factors were computed for four site response categories, each of which were a function of soil thickness, input hard-rock motion, and spectral frequency. From the five weighted stochastic ground-motion models (two finite fault and three point source) and amplification factors, rock and soil ground motions were computed to produce statewide ground-motion maps for the M 7.3 scenario event. Weighting of the Charleston source and ground-motion models was implemented so that the resulting liquefaction areas matched the 1886 areas of liquefaction. Peak horizontal ground acceleration (PGA) values as high as 0.6g-0.7g were estimated in the vicinity of the modeled rupture. PGAs in the range of 0.3g-0.4g were estimated for Charleston consistent with the observed building damage and liquefaction. Significant ground shaking (PGA > 0.2g) extends out to distances of 50-60 km. Strong long-period (≥1.0 sec) ground motions are predicted throughout the state. The probabilities for liquefaction were highest in the epicentral region (>50%), consistent with the observed occurrences of liquefaction in 1886.
机译:作为对南卡罗来纳州的全面地震损失和脆弱性评估的一部分,使用有限断层和点源随机数值模型对矩震级(M)7.3“ 1886年查尔斯顿样”地震的地面运动进行了模拟。还根据安全系数预测液化的可能性,该安全系数由平均循环应力和基于剪切波速度的循环阻力比,粘土含量和饱和度计算得出。由于1886年震源存在很大的不确定性,因此将1886年事件的破裂面建模为100公里长,20公里宽的断层(静应力下降27巴)和50公里长的断层, 16公里宽的断层(应力降为107巴)。该震源被认为是北向东北走向的走滑断层,与伍德斯托克断层一致。根据比较计算得出的和观察到的1886年低应力和高应力下降事件的液化面积和地面运动,两个案例的权重分别为0.8和0.2。为了适应美国东部地震震源过程中的认识不确定性,还开发并使用了三个区域特定的点震源衰减模型:具有恒定应力降和幅度相关应力降的单角频率模型,以及双应力模型。拐角频率模型。有限故障模型和点源模型的权重分别为0.8和0.2。为了将场地效应纳入地面运动估算中,已进行了广泛的工作来表征未固结沉积物的厚度,横波速度(V_s)和动态材料特性。使用可用的地下信息开发了特征性的V_s剖面图,其中包含了广泛的土壤和岩石条件。计算了四个站点响应类别的放大因子,每个类别都是土壤厚度,输入的坚硬岩石运动和频谱频率的函数。根据五个加权随机地震动模型(两个有限断层和三个点源)和放大因子,计算了岩石和土壤地震动,以生成M 7.3情景事件的全州地震动图。对查尔斯顿源和地面运动模型进行了加权,以使最终的液化区域与1886年的液化区域相匹配。在模拟破裂附近估计最高水平地面加速度(PGA)值高达0.6g-0.7g。估计查尔斯顿的PGA在0.3g-​​0.4g范围内,与观察到的建筑物损坏和液化一致。明显的地面震动(PGA> 0.2g)延伸到50-60 km。在整个州内,预计会有很长的地面运动(≥1.0秒)。液化的可能性在震中区域最高(> 50%),与1886年观察到的液化发生率一致。

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