岩土工程研究

P波斜入射陡坎地形对地面运动的影响

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  • 1. 苏州科技大学 江苏省结构工程重点实验室,江苏 苏州 215011;2. 中国地震局工程力学研究所,黑龙江 哈尔滨 150080
丁海平,男,1966年生,博士,教授,主要从事地震工程和防灾减灾工程。

收稿日期: 2015-10-16

  网络出版日期: 2018-06-05

基金资助

国家自然科学基金项目(No.51278323);国家自然科学基金重大研究计划集成项目(No.91215301)。

Effects of scarp topography on seismic ground motion under inclined P waves

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  • 1. Key Laboratory of Structure Engineering of Jiangsu Province, Suzhou University of Science and Technology, Suzhou, Jiangsu 215011, China; 2. Institute of Engineering Mechanics, China Earthquake Administration, Harbin, Heilongjiang 150080, China

Received date: 2015-10-16

  Online published: 2018-06-05

Supported by

This work was supported by the National Natural Science Foundation of China (51278323) and the Major Research Plan Program of National Natural Science Foundation of China (91215301).

摘要

针对陡坎地形,采用数值模拟方法,探讨了陡坎地形在P波斜入射时,入射角度 、坡角 和入射方向变化等参数对地震波传播的影响。结果表明:(1)从陡坎底部到陡坎顶部,放大系数逐渐增大,而入射角度、坡角和入射方向没有影响。(2)入射角度 一定时,无论地震波顺着陡坎方向(左)入射还是逆着陡坎方向(右)入射,陡坎上侧的放大系数大于陡坎下侧的放大系数。同时,放大系数随着坡角 的增大而增大。(3)坡角 不变,地震波顺着陡坎方向(左)入射时,x 分量的放大系数随着入射角的增大而增大,z分量的放大系数则随着入射角的增大而减小。(4)地震波逆着陡坎方向(右)入射时,放大系数最大值基本在陡坎上侧边缘。地震波顺着陡坎方向(左)入射时,放大系数最大值并没出现在陡坎上侧边缘,坡角越大,偏离越大。(5)地震波顺着陡坎方向(左)入射时, x分量的放大系数比地震波逆着陡坎方向(右)入射时的大,z分量变化不大。

本文引用格式

丁海平,于彦彦,郑志法, . P波斜入射陡坎地形对地面运动的影响[J]. 岩土力学, 2017 , 38(6) : 1716 -1724 . DOI: 10.16285/j.rsm.2017.06.021

Abstract

In this study, the seismic ground motion of the scarp topography under inclined P waves was analyzed using numerical simulation method. The effects of the incident degree, the slope angle, and the incident direction of seismic ground motion were discussed as well. It is found that from the bottom of scarp to the top, the amplification factor increased gradually, whereas it had no influence on the incident degree, the slope angle and the incident direction. When the incident degree was constant, the amplification factor of the scarp upside region was greater than that of the scarp downside region, regardless of the incident directions. At the same time, the amplification factor at the crest of the slope increased with the increase of the slope angle. When the slope angle was constant and the waves travelled away from the slope, the amplification factor of x component increased, while the amplification factor of z component decreased with the increase of incident angle. The results show that for waves travelling into the slope, the maximum amplification factor is generally found around the crest of the slope. For waves travelling away from the slope, the maximum amplification factor shifted from the slope crest. Moreover, the larger the slope angle, the farther the departure. The amplification factor of x component was larger for waves travelling away from the slope as compared to waves travelling into the slope, but the amplification factor of z component had no obvious change with the incident direction.
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