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Structure of an ambient vibration wavefield in the frequency range of engineering interest ([0.5, 20] Hz): Insights from numerical modelling

机译:工程感兴趣的频率范围([0.5,20] Hz)中的环境振动波场的结构:数值建模的见解

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The expected structure of an ambient vibration wavefield at the top of a shallow soft layer overlying a rigid bedrock is explored by applying a full wavefield physical model, under the hypothesis that ambient vibrations are the effect of a uniform distribution of random independent point-like harmonic sources at the surface of a flat, weakly dissipative Earth. The comparison of the results provided by this model with those deduced on the assumption that surface waves dominate the wave-field allows evaluation of the respective roles of body and surface waves (Love and Rayleigh) in their fundamental and higher modes. This analysis reveals that the structure of the ambient vibration wavefield strongly depends on the subsoil structure (P- and S-wave velocity profiles and thickness of the uppermost soft sedimentary layer) and on the distribution of ambient vibration sources around the receiver. This dependence also changes along with the frequency range of interest. In this regard, three frequency domains are identified, each showing a different sensitivity to the relevant parameters: below the fundamental resonance frequency for S-waves f_s, above the frequency f_u ≡ min {2f_s, f_p}, where fp is the resonance frequency for P-waves and in-between. A consequence that emerges is that a number of possible combinations of body and surface waves are possible, which could account for the heterogeneous results obtained from experimental studies. These findings also indicate constraints on the use of simplified models based on the assumption that surface waves dominate the ambient vibration wavefield, as is currently the case in most engineering applications.
机译:在假设环境振动是随机独立的点状谐波均匀分布的影响的假设下,通过应用完整的波场物理模型,探索了覆盖刚性基岩的浅软层顶部的环境振动波场的预期结构。源位于平坦的弱耗散地球表面。通过将该模型提供的结果与假设表面波主导波场的假设进行比较,可以评估体波和表面波(Love和Rayleigh)在其基本模式和更高模式下的各自作用。该分析表明,环境振动波场的结构很大程度上取决于地下土壤结构(P波和S波速度剖面和最上部软沉积层的厚度)以及接收器周围的环境振动源分布。这种依赖性也随感兴趣的频率范围而变化。在这方面,确定了三个频域,每个频域对相关参数表现出不同的敏感性:在S波的基本谐振频率f_s之下,在频率f_u≡min {2f_s,f_p}之上,其中fp是P波及其之间。由此产生的结果是,体波和表面波的许多可能组合是可能的,这可以解释从实验研究中获得的异质结果。这些发现还表明,基于表面波在环境振动波场中占主导地位的假设(如当前大多数工程应用中的情况),简化模型的使用受到了限制。

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