地震地震动相谱的可微性与群延迟时间数值计算的改进

Atsushi Nozu
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引用次数: 1

摘要

讨论了地震动相谱的可微性问题,提出了计算地震动群延迟时间的一种新的数值格式。除了“解包裹”过程造成的不连续外,当地震地面运动的傅里叶变换位于复平面的原点时,相位谱理论上是不可微的。这意味着群延迟时间不能被定义为频率的傅里叶振幅谱为零。从这一观点出发,回顾了群延迟时间与地震地震动时间特征之间的传统理论联系。证实了不可微性不影响连杆。即使傅里叶变换不精确地定位在复平面的原点处,当傅里叶变换足够靠近原点时,相位增量和群延迟时间的数值计算也会不稳定。为了减轻这一困难,提出了一种新的计算地震地震动群延迟时间的数值格式。新方法使用了“修正”群延迟时间,它被定义为传统群延迟时间与傅里叶振幅谱的平方相乘。即使对于傅立叶振幅谱为零的频率,也可以定义“修正”群延迟时间。此外,“修正”的群延迟时间在数值上是稳定的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
DIFFERENTIABILITY OF PHASE SPECTRUM OF EARTHQUAKE GROUND MOTION AND IMPROVEMENT OF NUMERICAL CALCULATION OF GROUP DELAY TIME: A SUPPLEMENTARY WORK
The differentiability of the phase spectrum of earthquake ground motion is discussed and a new numerical scheme is proposed for the calculation of the group delay time of earthquake ground motion. In addition to the discontinuity due to the “unwrapping” procedure, the phase spectrum can theoretical-ly be non-differentiable when the Fourier transform of the earthquake ground motion is located at the origin of the complex plane. This implies that the group delay time cannot be defined for frequencies for which the Fourier amplitude spectrum is zero. From such a point of view, the conventional theoretical link between the group delay time and the temporal characteristics of earthquake ground motion is re-viewed. It is confirmed that the non-differentiability does not affect the link. Even when the Fourier transform is not located precisely at the origin of the complex plane, the numerical calculation of the phase increment and the group delay time can be unstable when the Fourier transform is located close enough to the origin. To mitigate the difficulty, a new numerical scheme is proposed for the calculation of the group delay time of earthquake ground motion. The new method uses the ‘modified’ group delay time, which is defined as the multiplication of the conventional group delay time with the squared Fourier amplitude spectrum. The ‘modified’ group delay time can be defined even for frequencies for which the Fourier amplitude spectrum is zero. In addition, the ‘modified’ group delay time is numerically stable.
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