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首页> 外文期刊>Journal of Seismology >Peak surface motion due to scattering of plane harmonic P, SV, or Rayleigh waves by a rough cavity embedded in an elastic half-space
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Peak surface motion due to scattering of plane harmonic P, SV, or Rayleigh waves by a rough cavity embedded in an elastic half-space

机译:由于嵌入在弹性半空间中的粗糙空腔散射平面谐波P,SV或瑞利波而导致的峰值表面运动

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Scattering of plane harmonic P, SV, or Rayleigh waves by a two-dimensional rough cavity completely embedded in an isotropic elastic half-space is investigated by using a direct boundary integral equation method. The cavity’s roughness is assumed to be in the form of periodic or random perturbations of arbitrary amplitude superimposed to a smooth elliptical shape. For the randomly corrugated cavities the normal or the uniform probability distribution functions are assumed. Based on multiple random cavity results, the corresponding average surface response is computed. These are compared with the corresponding periodically corrugated and smooth cavity responses. The surface response is evaluated for different cavity shapes and incident waves and for a range of frequencies. The surface motion results are used to determine the peak surface motion frequencies. They depend strongly upon the basic inclusion shape (the principal axes) and the nature of the incident wave. Strong similarity in the peak surface motion frequencies can be observed for the rough and smooth cavity models for both circular and elliptical shapes. In order to quantify the importance of the cavity corrugation upon the surface motion, a roughness influence factor is defined in terms of the rough and smooth cavity surface responses. This factor strongly depends upon the type of the incident wave, the nature of the cavity corrugation, the basic cavity shape, and the frequency. The factor clearly shows the effect of the cavity roughness upon the surface motion.
机译:利用直接边界积分方程方法研究了完全嵌入各向同性弹性半空间中的二维粗糙空腔对平面谐波P,SV或瑞利波的散射。假定空腔的粗糙度为任意振幅的周期性或随机扰动的形式,叠加到光滑的椭圆形上。对于随机波纹腔,假定正态或均匀概率分布函数。基于多个随机腔结果,计算相应的平均表面响应。将这些与相应的周期性波纹和平滑型腔响应进行比较。针对不同的腔体形状和入射波以及一系列频率评估了表面响应。表面运动结果用于确定峰值表面运动频率。它们在很大程度上取决于基本的夹杂物形状(主轴)和入射波的性质。对于圆形和椭圆形的粗糙和光滑腔模型,可以观察到峰值表面运动频率的强烈相似性。为了量化腔波纹对表面运动的重要性,根据粗糙和光滑的腔表面响应来定义粗糙度影响因子。这个因素在很大程度上取决于入射波的类型,空腔波纹的性质,基本的空腔形状和频率。该因子清楚地显示了腔体粗糙度对表面运动的影响。

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