Processing the Artificial Edge-Effects for Finite-Difference Frequency-Domain in Viscoelastic Anisotropic Formations

被引:2
作者
Yang, Jixin [1 ,2 ,3 ]
He, Xiao [1 ,2 ,3 ]
Chen, Hao [1 ,2 ,3 ]
机构
[1] Chinese Acad Sci, Inst Acoust, State Key Lab Acoust, Beijing 100190, Peoples R China
[2] Univ Chinese Acad Sci, Sch Phys Sci, Beijing 100049, Peoples R China
[3] Beijing Engn Res Ctr Sea Deep Drilling & Explorat, Beijing 100190, Peoples R China
来源
APPLIED SCIENCES-BASEL | 2022年 / 12卷 / 09期
基金
中国国家自然科学基金;
关键词
frequency-domain modeling; anisotropy; viscoelastic; edge-effect removing; PERFECTLY MATCHED LAYER; WAVE-PROPAGATION; MEDIA; TOMOGRAPHY; REFLECTION; SIMULATION; INVERSION; MIGRATION; PML;
D O I
10.3390/app12094719
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
Real sedimentary media can usually be characterized as transverse isotropy. To reveal wave propagation in the true models and improve the accuracy of migrations and evaluations, we investigated the algorithm of wavefield simulations in an anisotropic viscoelastic medium. The finite difference in the frequency domain (FDFD) has several advantages compared with that in the time domain, e.g., implementing multiple sources, multi-scaled inversion, and introducing attenuation. However, medium anisotropy will lead to the complexity of the wavefield in the calculation. The damping profile of the conventional absorption boundary is only defined in one single direction, which produces instability when the wavefields of strong anisotropy are reflected on that truncated boundary. We applied the multi-axis perfectly matched layer (M-PML) to the wavefield simulations in anisotropic viscoelastic media to overcome this issue, which defines the damping profiles along different axes. In the numerical examples, we simulated seismic wave propagation in three viscous anisotropic media and focused on the wave attenuation in the absorbing layers using time domain snapshots. The M-PML was more effective for wave absorption compared to the conventional perfectly matched layer (PML). In strongly anisotropic media, the PML became unstable, and prominent reflections appeared at truncated boundaries. In contrast, the M-PML remained stable and efficient in the same model. Finally, the modeling of the stratified cross-well model showed the applicability of this proposed algorithm to heterogeneous viscous anisotropic media. The numerical algorithm can analyze wave propagation in viscoelastic anisotropic media. It also provides a reliable forward operator for waveform inversion, wave equation travel-time inversion, and seismic migration in anisotropic viscoelastic media.
引用
收藏
页数:16
相关论文
共 31 条
[1]   REVERSE TIME MIGRATION [J].
BAYSAL, E ;
KOSLOFF, DD ;
SHERWOOD, JWC .
GEOPHYSICS, 1983, 48 (11) :1514-1524
[2]   An efficient frequency-domain full waveform inversion method using simultaneous encoded sources [J].
Ben-Hadj-Ali, Hafedh ;
Operto, Stephane ;
Virieux, Jean .
GEOPHYSICS, 2011, 76 (04) :R109-R124
[3]   A PERFECTLY MATCHED LAYER FOR THE ABSORPTION OF ELECTROMAGNETIC-WAVES [J].
BERENGER, JP .
JOURNAL OF COMPUTATIONAL PHYSICS, 1994, 114 (02) :185-200
[4]   Application of the perfectly matched absorbing layer model to the linear elastodynamic problem in anisotropic heterogeneous media [J].
Collino, F ;
Tsogka, C .
GEOPHYSICS, 2001, 66 (01) :294-307
[5]  
Dai W, 2011, GEOPHYSICS, V76, pR135, DOI [10.1190/geo2010-0159.1, 10.1190/GEO2010-0159.1]
[6]  
DALEY PF, 1977, B SEISMOL SOC AM, V67, P661
[7]   GEOPHYSICAL DIFFRACTION TOMOGRAPHY [J].
DEVANEY, AJ .
IEEE TRANSACTIONS ON GEOSCIENCE AND REMOTE SENSING, 1984, 22 (01) :3-13
[8]   An unsplit complex frequency-shifted perfectly matched layer for second-order acoustic wave equations [J].
Fang, Xiuzheng ;
Niu, Fenglin .
SCIENCE CHINA-EARTH SCIENCES, 2021, 64 (06) :992-1004
[9]   Acoustic VTI modeling using high-order finite differences [J].
Hestholm, Stig .
GEOPHYSICS, 2009, 74 (05) :T67-T73
[10]  
Jeong W., 2011, SEG TECHNICAL PROGRA, P2654