Dispersion characteristics of Scholte waves on horizontal layered seabed
YU Pengfei1, CHEN Junlin1, JIANG Jiameng1, YANG Xiaohui2
1. College of Oceanography, Hohai University, Nanjing, Jiangsu 210024, China; 2. Sinopec Geophysical Research Institute, Nanjing, Jiangsu 211103, China
Abstract:Scholte waves propagate along the seafloor fluid-solid interface and exhibit typical dispersion characteristics. The dispersion properties of Scholte waves can be utilized for the inversion of the shear wave velocity of the shallow seabed, making it an effective tool for seabed shear wave velocity modeling. It is of critical importance to establish the theoretical model of Scholte wave dispersion. In this study, a horizontal layered model of seawater-seabed elasticity is developed based on a real seawater-seabed environment. The dispersion equation and displacement equation for Scholte waves in this model are derived using the continuity conditions of boundary stress and displacement. The influence of seawater depth and seabed property parameters on the dispersion characteristics of Scholte waves is analyzed. Experimental results using a 6-layer seawater–seabed model show that: ①Regardless of the seabed is hard or soft, Scholte waves exhibit distinct dispersion characteristics. In the case of a hard seabed, the energy of Scholte waves is mainly concentrated in the seawater, with the fundamental mode having the weakest energy and the second mode having the strongest energy. As the seawater depth increases, the dispersion characteristics of Scholte waves weaken. For the soft seabed model, the energy of Scholte waves on the solid seabed significantly increases, and the seawater depth has little effect on Scholte wave dispersion characteristics. ②Compared with deep-water environments, Scholte waves have stronger energy and more pronounced dispersion characteristics in shallow water. Therefore, utilizing Scholte waves for inverting the shallow seabed shear wave velocity in shallow water environments yields higher accuracy and reliability. Finally, based on an actual seabed elastic geological model of a working area in the East China Sea, multi-component seismic data are simulated, and dispersion curves are extracted. A comparison analysis between the theoretically calculated dispersion curves and the extracted dispersion curves shows a good agreement, confirming the accuracy of our theoretical approach.
STEWART R R, GAISER J E, BROWN R J, et al. Converted-wave seismic exploration:methods[J].Geophysics, 2002, 67(5):1348-1363.
[2]
BOUSKA J. Advantages of wide-patch, wide-azimuth ocean-bottom seismic reservoir surveillance[J].The Leading Edge, 2008, 27(12):1662-1681.
[3]
MAVER K G. Ocean Bottom Seismic:strategic technology for the oil industry[J].First Break, 2011, 29(12):75-80.
[4]
张永刚, 王赟, 王妙月. 目前多分量地震勘探中的几个关键问题[J].地球物理学报,2004.47(1):151-155.ZHANG Yonggang, WANG Yun, WANG Miaoyue. Some key problems in the multi-component seismic exploration[J].Chinese Journal of Geophysics, 2004, 47(1):151-155.
[5]
李向阳, 王九拴. 多波地震勘探及裂缝储层预测研究进展[J].石油科学通报, 2016, 1(1):45-60.LI Xiangyang, WANG Jiushuan. Recent advances in multicomponent seismic and fractured reservoir characterization[J].Petroleum Science Bulletin, 2016, 1(1):45-60.
[6]
EWING W M, JARDETZKY W S, PRESS F. Elastic Waves in Layered Media[M].McGraw-Hill, New York, 1957.
[7]
PADILLA F, DE BILLY M, QUENTIN G. Theoretical and experimental studies of surface waves on solid-fluid interfaces when the value of the fluid sound velocity is located between the shear and the longitudinal ones in the solid[J].The Journal of the Acoustical Society of America, 1999, 106(2):666-673.
[8]
卓乐芳. 固体-液体层分界面处的P、SV型面波[J].西安工程学院学报, 1999, 21(3):71-73.ZHUO Lefang. P、SV typal surface waves at the interface of solid-aliquid layer[J].Journal of Xi'an Engineering University, 1999, 21(3):71-73.
[9]
CARCIONE J M, HELLE H B. The physics and simulation of wave propagation at the ocean bottom[J].Geophysics, 2004, 69(3):825-839.
[10]
BOHLEN T, KUGLER S, KLEIN G, et al. 1.5D inversion of lateral variation of Scholte-wave dispersion[J].Geophysics, 2004, 69(2):330-344.
[11]
RAUCH D, KUPERMAN W A,JENSEN F B. Experimental and Theoretical Studies of Seismic Interface Waves in Coastal Waters[M]. Bottom-Interacting Ocean Acoustics, Springer, Boston, MA, 1980, 307-327.
[12]
SCHOLTE J G. The range of existence of Rayleigh and Stoneley waves[J].Geophysical Journal International, 1947, 5(S5):120-126.
[13]
TOMAR G, STUTZMANN E, MORDRET A, et al. Joint inversion of the first overtone and fundamental mode for deep imaging at the Valhall oil field using ambient noise[J].Geophysical Journal International, 2018, 214(1):122-132.
[14]
GLORIEUX C, VAN DE ROSTYNE K, GUSEV V, et al. Nonlinearity of acoustic waves at solid-liquid interfaces[J].The Journal of the Acoustical Society of America, 2002, 111(1):95-103.
[15]
WOEZEL J L, EWING M, PEKERIS C L. Explosion Sounds in Shallow Water[M].University of Pittsburgh Press, Pittsburgh, 1948.
[16]
MUYZERT E. Scholte wave velocity inversion for a near surface S-velocity model and PS-statics[C].SEG Technical Program Expanded Abstracts, 2000, 19:1197-1200.
[17]
WANG Y, LI Z, YOU Q, et al. Shear-wave velocity structure of the shallow sediments in the Bohai Sea from an ocean-bottom-seismometer survey[J].Geophysics, 2016, 81(3):ID25-ID36.
[18]
WANG Y, LI Z, GENG J, et al. Seismic imaging of S-wave structures of shallow sediments in the East China Sea using OBN multicomponent Scholte-wave data[J].Geophysics, 2020, 85(6):EN87-EN104.
[19]
WANG Y, YOU Q, HAO T. Estimating the shear-wave velocities of shallow sediments in the Yellow Sea using ocean-bottom-seismometer multicomponent Scholte-wave data[J].Frontiers in Earth Science, 2022, 10:812744.
[20]
SPICA Z J, NISHIDA K, AKUHARA T, et al. Marine sediment characterized by ocean-bottom fiber-optic seismology[J].Geophysical Research Letters, 2020, 47(16):e2020GL088360.
[21]
CHENG F, CHI B, LINDSEY N J, et al. Utilizing distributed acoustic sensing and ocean bottom fiber optic cables for submarine structural characterization[J].Scientific Reports, 2021, 11(1):5613.
[22]
LIOR I, SLADEN A, RIVET D, et al. On the detection capabilities of underwater distributed acoustic sensing[J].Journal of Geophysical Research:Solid Earth, 2021, 126(3):e2020JB020925.
[23]
梁志强. 层状介质中多模式面波频散曲线研究[D].陕西西安:长安大学, 2006.LIANG Zhiqiang.Study on Multi-Modes Surface Wave Dispersion Curves in Bedding Media[D].Chang'an University, Xi'an, Shanxi,2006.
[24]
邵广周. 多阶模式瑞利波频散特征与反演研究[D].陕西西安:长安大学, 2009.SHAO Guangzhou. Study on Multiple-Mode Dispersion Characteristics of Rayleigh Waves and it's Inversion[D].Chang'an University, Xi'an, Shanxi, 2009.
[25]
罗夏云, 程广利, 张明敏, 等. 浅海Scholte波的频散特性研究[J].兵工学报, 2018, 39(9):1786-1794.LUO Xiayun, CHENG Guangli, ZHANG Mingmin, et al. Research on dispersion characteristics of Scholte wave in shallow sea[J].Acta Armamentarii, 2018, 39(9):1786-1794.
[26]
祝捍皓, 郑红, 林建民, 等. 海洋环境参数对Scholte波特性的影响[J].上海交通大学学报, 2016, 50(2):257-264.ZHU Hanhao, ZHENG Hong, LIN Jianmin, et al. Influence of ocean environment parameters on Scholte wave[J].Journal of Shanghai Jiaotong University, 2016, 50(2):257-264.
[27]
雷左, 孟路稳, 金丹, 等. 基于两种海底介质的地震波传播特性研究[J].海军工程大学学报, 2017, 29(6):13-17.LEI Zuo, MENG Luwen, JIN Dan, et al. Propagation characteristics of seismic waves based on two kinds of seabed medium[J].Journal of Naval University of Engineering, 2017, 29(6):13-17.
[28]
ALI H B, BIBEE L D. The influence of sediment layering and geoacoustics on the propagation of Scholte interface waves[C].Proceedings of OCEANS'93, 1993, I105-I113.
[29]
QI Q. Attenuated leaky Rayleigh waves[J].The Journal of the Acoustical Society of America, 1994, 95(6):3222-3231.
[30]
VINH P C. Scholte-wave velocity formulae[J].Wave Motion, 2013, 50(2):180-190.
[31]
DONG Y, PIAO S, GONG L, et al. Scholte wave dispersion modeling and subsequent application in seabed shear-wave velocity profile inversion[J].Journal of Marine Science and Engineering, 2021, 9(8):840.
[32]
CARLSON R L, SCHAFTENAAR C H, MOORE R P. Causes of compressional-wave anisotropy in carbonate-bearing,deep-sea sediments[J].Geophysics, 1984, 49(5):525-532.
[33]
BERGE P A, MALLICK S, FRYER G J, et al. In situ measurement of transverse isotropy in shallow-water marine sediments[J].Geophysical Journal International,1991,04(2):241-254.
[34]
BUCKINGHAM M J.Compressional and shear wave properties of marine sediments:comparisons between theory and data[J].Journal of the Acoustical Society of America, 2005, 117(1):137-152.
[35]
HAMILTON E L. Sound velocity gradients in marine sediments[J].The Journal of the Acoustical Society of America, 1979, 65(4):909-922.
[36]
GARDNER G H F, GARDNER L W, GREGORY A R. Formation velocity and density: the diagnostic basics for stratigraphic traps[J].Geophysics, 1974, 39(6):770-780.
[37]
KOMATITSCH D, TROMP J. Spectral-element simulations of global seismic wave propagation-I. Validation[J].Geophysical Journal International, 2002, 149(2):390-412.
[38]
KOMATITSCH D, TROMP J. Spectral-element simulations of global seismic wave propagation-Ⅱ. Three-dimensional models, oceans, rotation and self-gravitation[J].Geophysical Journal International, 2002, 150(1):303-318.
[39]
夏江海, 高玲利, 潘雨迪, 等. 高频面波方法的若干新进展[J].地球物理学报, 2015, 58(8):2591-2605.XIA Jianghai, GAO Lingli, PAN Yudi, et al. New findings in high-frequency surface wave method[J].Chinese Journal of Geophysics, 2015, 58(8):2591-2605.
[40]
GANJI V, GUCUNSKI N, NAZARIAN S. Automated inversion procedure for spectral analysis of surface waves[J].Journal of Geotechnical and Geoenvironmental Engineering, 1998, 124(8):757-770.
[41]
OLAFSDOTTIR E A, ERLINGSSON S, BESSASON B. Tool for analysis of multichannel analysis of surface waves (MASW) field data and evaluation of shear wave velocity profiles of soils[J].Canadian Geotechnical Journal,2018,55(2):217-233.