首页> 外文期刊>Pure and Applied Geophysics >A Fourth Order Accurate SH-Wave Staggered Grid Finite-difference Algorithm with Variable Grid Size and VGR-Stress Imaging Technique
【24h】

A Fourth Order Accurate SH-Wave Staggered Grid Finite-difference Algorithm with Variable Grid Size and VGR-Stress Imaging Technique

机译:具有可变网格尺寸和VGR应力成像技术的四阶精确SH波交错网格有限差分算法

获取原文
获取原文并翻译 | 示例
           

摘要

This article presents a new approach for the implementation of a planar-free surface boundary condition. It is based on a vertical grid-size reduction above the free surface during the explicit computation of a free surface boundary condition. This technique is very much similar to the well-known stress imaging technique. VGR-stress imaging technique name is proposed for this new free surface boundary condition (VGR stands for ‘vertical grid-size reduction’). To study the performance of the proposed VGR-stress imaging technique, it was implemented in a newly developed second order accurate in time and fourth-order accurate in space (2, 4) staggered grid SH-wave finite-difference (FD) algorithm with variable grid size. It was confirmed that the effective thickness (ETH) of first soil layer becomes less by one-half of vertical grid size than the assigned thickness (ATH), if stress imaging technique is used as a free surface boundary condition. The qualitative and quantitative results of various numerical experiments revealed that the proposed VGR-stress imaging technique is better than the stress imaging technique since it is free from the thickness discrepancy arising due to the use of images of stress components across the free surface. On the basis of iterative numerical experiments, it was confirmed that the stability condition for this FD scheme with variable grid size is fracVS Dt min(Dx,Dz) £ 0.71. frac{{V_{S} Delta t}} {{min (Delta x,Delta z)}} le 0.71. It was also inferred that at least five to six grid points per shortest wavelength are required to avoid the grid dispersion. The maximum grid-spacing ratio up to 12.5 or even more did not affect the accuracy of (2,4) SH-wave algorithm. The obtained reduction of 10.46 and 5.38 folds in the requirement of computational memory and time for a particular basin-edge model, as compared with the homogeneous grid size, reflects the efficacy of the new FD algorithm.
机译:本文提出了一种实现无平面表面边界条件的新方法。它基于自由表面边界条件的显式计算过程中自由表面上方的垂直网格大小减小。该技术与众所周知的应力成像技术非常相似。针对这种新的自由表面边界条件,建议使用VGR应力成像技术名称(VGR代表“垂直网格尺寸减小”)。为了研究所提出的VGR应力成像技术的性能,它是在新开发的时间上精确的二阶和空间(2,4)交错网格SH波有限差分(FD)算法中实现的。可变的网格大小。如果将应力成像技术用作自由表面边界条件,则可以确定的是,第一土壤层的有效厚度(ETH)减小了垂直网格尺寸的一半,而不是指定的厚度(ATH)。各种数值实验的定性和定量结果表明,所提出的VGR应力成像技术优于应力成像技术,因为它没有因使用自由表面上的应力分量图像而引起的厚度差异。在迭代数值实验的基础上,确定了该可变网格尺寸FD方案的稳定性条件为fracV S Dt min(Dx,Dz)£0.71。 frac {{V_ {S} Delta t}} {{min(Delta x,Delta z)}} le 0.71。还可以推断,每个最短波长至少需要5至6个栅格点,以避免栅格分散。高达12.5甚至更高的最大网格间距比不会影响(2,4)SH波算法的准确性。与均匀网格大小相比,特定盆地边缘模型在计算内存和时间上的需求减少了10.46倍和5.38倍,这反映了新FD算法的有效性。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号