[an error occurred while processing this directive] Global Geology 2019, 22(2) 112-120 DOI:   10.3969/j.issn.1673-9736.2019.02.06  ISSN: 1673-9736 CN: 22-1371/P

����Ŀ¼ | ����Ŀ¼ | ������� | �߼�����                                                            [��ӡ��ҳ]   [�ر�]
����
��չ����
������Ϣ
Supporting info
PDF(351KB)
[HTMLȫ��]
�����[PDF]
�����
�����뷴��
�ѱ����Ƽ�������
�����ҵ����
�������ù�����
����
Email Alert
���·���
���������Ϣ
���Ĺؼ����������
finite difference method
staggered grid
forward modeling
3D acoustic-elastic coupled media
transversely isotropic medium
���������������
PENG Changhua
WANG Deli
ZHOU Jinju
PubMed
Article by Peng C
Article by Wang D
Article by Zhou J
3D numerical simulation in acoustic-elastic coupled media with staggered-grid finite-difference method
PENG Changhua, WANG Deli, ZHOU Jinju
College of Geo-Exploration Science and Technology, Jilin University, Changchun 130026, China
ժҪ�� Acoustic-elastic coupled media is often encountered in most marine explorations, and accurate simulation of acoustic-elastic coupled media is of great significance. At present, the study of acoustic-elastic coupled media still assumes that the solid of the acoustic-elastic coupled media is isotropic, but this assumption is not in accordance with the actual situation. In this paper, we derive the solid media of acoustic-elastic coupled media from isotropic media to anisotropic media, and propose an acoustic-elastic coupled medium based ontransverse isotropic media with vertical symmetric axes (VTI) to improve the accuracy of forward modeling. Based on the relationship between the Thomsen parameter and the coefficient matrix of the anisotropic elastic wave equation, we transform the Thomson parameter into a velocity model with anisotropic properties. We use a staggered grid finite difference method to simulate the propagation of a wavefield in a three-dimensional acoustic-elastic coupled media. We obtain the snapshots of the wave field when the solid of the acoustic-elastic coupled media is an isotropic medium and a VTI media. When the solid of the acoustic-elastic coupled media is considered VTI media, we can observe the qP wave and qS wave that cannot be observed in the isotropic medium from the wave field snapshot. We can also find that the seismic records obtained by the method we use are more realistic. The algorithm proposed in this paper is of great significance for high-precision ocean numerical simulation.
�ؼ����� finite difference method   staggered grid   forward modeling   3D acoustic-elastic coupled media   transversely isotropic medium  
3D numerical simulation in acoustic-elastic coupled media with staggered-grid finite-difference method
PENG Changhua, WANG Deli, ZHOU Jinju
College of Geo-Exploration Science and Technology, Jilin University, Changchun 130026, China
Abstract: Acoustic-elastic coupled media is often encountered in most marine explorations, and accurate simulation of acoustic-elastic coupled media is of great significance. At present, the study of acoustic-elastic coupled media still assumes that the solid of the acoustic-elastic coupled media is isotropic, but this assumption is not in accordance with the actual situation. In this paper, we derive the solid media of acoustic-elastic coupled media from isotropic media to anisotropic media, and propose an acoustic-elastic coupled medium based ontransverse isotropic media with vertical symmetric axes (VTI) to improve the accuracy of forward modeling. Based on the relationship between the Thomsen parameter and the coefficient matrix of the anisotropic elastic wave equation, we transform the Thomson parameter into a velocity model with anisotropic properties. We use a staggered grid finite difference method to simulate the propagation of a wavefield in a three-dimensional acoustic-elastic coupled media. We obtain the snapshots of the wave field when the solid of the acoustic-elastic coupled media is an isotropic medium and a VTI media. When the solid of the acoustic-elastic coupled media is considered VTI media, we can observe the qP wave and qS wave that cannot be observed in the isotropic medium from the wave field snapshot. We can also find that the seismic records obtained by the method we use are more realistic. The algorithm proposed in this paper is of great significance for high-precision ocean numerical simulation.
Keywords: finite difference method   staggered grid   forward modeling   3D acoustic-elastic coupled media   transversely isotropic medium  
�ո����� 2018-08-12 �޻����� 2018-10-25 ����淢������  
DOI: 10.3969/j.issn.1673-9736.2019.02.06
������Ŀ:

Supported by Major Project of National Science and Technology of China (No.2016ZX05026-002-003) and National Natural Science Foundation of China (No.41374108).

ͨѶ����:
���߼��:
����Email:

�ο����ף�
Bae H S, Shin C, Cha Y H,et al. 2010.2D acoustic-elastic coupled waveform inversion in the Laplace domain. Geophysical Prospecting,58:997-1010.
Basaldua-Sanchez J E, Samayoa-Ochoa D, Rodriguez-Sanchez J E,et al. 2013. Diffraction of elastic waves in fluid-layered solid Interfaces by an integral formulation:Journal of Applied Mathematics,1-9. DOI:10.1155/2013/469428
Choi Y, Min D J, Shin C. 2008. Two-dimensional waveform inversion of multi-component data in acoustic-elastic coupled media.Geophysical Prospecting.56:863-881.
De Basabe J D, Sen M K. 2015. A comparison of finite-difference and spectral-element methods for elastic wave propagation in media with a fluid-solid interface.Geophysical Journal International,200:278-298.
De Hoop A T, Van der Hijden J H M T. 1983. Generation of acoustic waves by an impulsive line source in a fluid/solid configuration with plane boundary.The Journal of the Acoustical Society of America.74(1):333-342.
Gaiser J, Moldoveanu N, Macbeth C, et al. 2001. Multicomponent technology:the players, problem, applications, and trends:summary of the workshop sessions.The Leading Edge,20(9):974-977.
Hou G, Wang J, Layton A. 2012. Numerical methods for fluid-structure interaction-a review.Communications in Computational Physics,12(2):337-377.
Kim M H, Choi Y, Cha Y H,et al. 2009.2D frequency-domain waveform inversion of coupled acoustic-elastic media with an irregular interface.Pure and Applied Geophysics,166(12):1967-1985
Komatitsch D, Barnes C, Tromp J. 2000. Wave propagation near a fluid-solid interface:a spectral element approach.Geophysics.65(2):623-631.
Li L, Hao C T. 2011. Constraints on anisotropic parameters in transversely isotropic media and the extensions to orthor-hombic media.Chinese Journal of Geophysics.54(6):798-809. (in Chinese with English abstract)
Maver K G. 2011. Ocean bottom seismic:strategic technology for the oil industry.First Break.29:75-80.
Minkoff S E. 2002. Spatial parallelism of a 3D finite difference velocity-stress elastic wave propagation code.Society for Industrial and Applied Mathematics.24(1):1-19.
Ravasi M, Curtis A. 2013. Elastic imaging with exact wavefield extrapolation for application to ocean-bottom 4C seismic data.Geophysics,78(6):265-284.
Van Vossen R, Robertsson J O A, Chapman C H. 2000. Wave propagation near a fluid-solid interface:a spectral element approach.Geophysics,65(2):623-631.
Virieux J. 1986. P-SV wave propagation in heterogeneous media:velocity-stress finite-difference method. Geophysics,51, 889-901.
Zienkiewicz O C, Taylor R L, Zhu J Z. 2005. The finite element method:its basis and fundamentals. Oxford:Elsevier, 634-637.
�������������

Copyright by Global Geology