A 1D finite element method in time domain is developed in this paper and applied to calculate in-plane wave motions of free field exited by SV or P wave oblique incidence in an elastic layered half-space. First, the l...A 1D finite element method in time domain is developed in this paper and applied to calculate in-plane wave motions of free field exited by SV or P wave oblique incidence in an elastic layered half-space. First, the layered half-space is discretized on the basis of the propagation characteristic of elastic wave according to the Snell law. Then, the finite element method with lumped mass and the central difference method are incorporated to establish 2D wave motion equations, which can be transformed into 1D equations by discretization principle and explicit finite element method. By solving the 1D equations, the displacements of nodes in any vertical line can be obtained, and the wave motions in layered half-space are finally determined based on the characteristic of traveling wave. Both the theoretical analysis and the numerical results demonstrate that the proposed method has high accuracy and good stability.展开更多
为研究不同轨道结构形式对地铁车内噪声的影响,测试了列车通过普通整体道床、减振扣件道床、梯形轨枕道床、中档钢弹簧浮置板道床、高档钢弹簧浮置板道床等5种轨道结构形式时的车内噪声。采用A计权声压级对车内噪声时域与频域特性进行分...为研究不同轨道结构形式对地铁车内噪声的影响,测试了列车通过普通整体道床、减振扣件道床、梯形轨枕道床、中档钢弹簧浮置板道床、高档钢弹簧浮置板道床等5种轨道结构形式时的车内噪声。采用A计权声压级对车内噪声时域与频域特性进行分析,探究列车通过5种不同轨道结构时车内噪声分布规律。结果表明:普通整体道床车内噪声瞬时A计权声压级均值为76. 6 d B,减振扣件为82. 3 d B,梯形轨枕道床为77. 2 d B,中档钢弹簧浮置板道床为76. 8 d B,高档钢弹簧浮置板道床为81. 6 d B; 5种轨道结构形式车内噪声A计权声压级频谱差异明显;车内噪声总A计权声压级在空间分布上,同一水平车厢两侧近门窗处比车厢中部约高1. 5 d B,在垂向上声压级随高度的增加逐渐减小,坐高处比站高处噪声总A计权声压级高0. 5 d B。展开更多
基金the National Natural Science Foundation of China(50478014)the National 973 Program(2007CB714200)the Beijing Natural Science Foundation(8061003).
文摘A 1D finite element method in time domain is developed in this paper and applied to calculate in-plane wave motions of free field exited by SV or P wave oblique incidence in an elastic layered half-space. First, the layered half-space is discretized on the basis of the propagation characteristic of elastic wave according to the Snell law. Then, the finite element method with lumped mass and the central difference method are incorporated to establish 2D wave motion equations, which can be transformed into 1D equations by discretization principle and explicit finite element method. By solving the 1D equations, the displacements of nodes in any vertical line can be obtained, and the wave motions in layered half-space are finally determined based on the characteristic of traveling wave. Both the theoretical analysis and the numerical results demonstrate that the proposed method has high accuracy and good stability.
文摘为研究不同轨道结构形式对地铁车内噪声的影响,测试了列车通过普通整体道床、减振扣件道床、梯形轨枕道床、中档钢弹簧浮置板道床、高档钢弹簧浮置板道床等5种轨道结构形式时的车内噪声。采用A计权声压级对车内噪声时域与频域特性进行分析,探究列车通过5种不同轨道结构时车内噪声分布规律。结果表明:普通整体道床车内噪声瞬时A计权声压级均值为76. 6 d B,减振扣件为82. 3 d B,梯形轨枕道床为77. 2 d B,中档钢弹簧浮置板道床为76. 8 d B,高档钢弹簧浮置板道床为81. 6 d B; 5种轨道结构形式车内噪声A计权声压级频谱差异明显;车内噪声总A计权声压级在空间分布上,同一水平车厢两侧近门窗处比车厢中部约高1. 5 d B,在垂向上声压级随高度的增加逐渐减小,坐高处比站高处噪声总A计权声压级高0. 5 d B。
