Please wait a minute...
E-mail Alert Rss
 
物探与化探  2025, Vol. 49 Issue (3): 620-630    DOI: 10.11720/wtyht.2025.1365
  方法研究信息处理仪器研制 本期目录 | 过刊浏览 | 高级检索 |
基于L1-2范数约束的叠前多分量地震数据直接反演纵横波速度比方法
韩磊1(), 李景叶1, 耿伟恒2, 王永平1, 杨骐羽1, 张宇宁1
1.中国石油大学(北京) 地球物理学院,北京 102249
2.清华大学 信息科学与技术学院,北京 100084
A method for calculating the P-to-S-wave velocity ratio through direct inversion of prestack multi-component seismic data based on the L1-2 norm constraint
HAN Lei1(), LI Jing-Ye1, GENG Wei-Heng2, WANG Yong-Ping1, YANG Qi-Yu1, ZHANG Yu-Ning1
1. College of Geophysics,China University of Petroleum(Beijing),Beijing 102249,China
2. School of Information Science and Technology,Tsinghua University,Beijing 100084,China
全文: PDF(7321 KB)   HTML
输出: BibTeX | EndNote (RIS)      
摘要 

纵横波速度比是判别岩性、描述储层特征、识别气藏的重要工具。通过PP波地震数据直接反演纵波速度和横波速度的技术已经相对成熟,但分别反演纵横波速度后再求取其比值会产生累积误差。相比之下,PS波中包含横波速度信息,联合反演能够提高纵横波速度比的反演精度。本文引入了L1-2范数以提高反演结果的分辨率。相较于L1范数和L2范数,L1-2范数更稀疏,可以得到分辨率更高的反演结果。首先,通过推导线性化的PP波和PS波正演近似公式并分析其精度。然后,基于贝叶斯理论,引入L1-2范数构建直接反演纵横波速度比的目标函数,通过求解该目标函数,获得纵横波速度比的反演结果。定量对比相关系数表明,基于L1-2范数的反演结果优于L1范数和L2范数,直接反演结果优于间接反演结果,联合反演的结果优于单独反演的结果。合成数据和实际资料的反演验证了所提方法的有效性和可行性。

服务
把本文推荐给朋友
加入引用管理器
E-mail Alert
RSS
作者相关文章
韩磊
李景叶
耿伟恒
王永平
杨骐羽
张宇宁
关键词 纵横波速度比L1-2范数多波多分量地震数据直接反演    
Abstract

The ratio of compressional to shear wave velocities(hereafter referred to as the P-to-S-wave velocity ratio) is an essential parameter for lithology discrimination,reservoir characterization,and gas reservoir identification.Direct inversion of PP-wave seismic data to derive the P- and S-wave velocities has been a well-established technique.However,calculating the P-to-S-wave velocity ratio using the P- and S-wave velocities obtained through individual inversion may lead to cumulative errors.In contrast,since PS-wave data inherently contain S-wave velocity information,the joint inversion of PS-wave data can significantly improve the accuracy of the P-to-S-wave velocity ratio.This study employed the L1-2 norm to enhance the resolution of inversion results.Compared to the L1 and L2 norms,the L1-2 norm yielded sparser solutions with higher resolution.First,this study derived and assessed the accuracy of linearized forward modeling approximate formulas for PP- and PS-waves.Second,based on Bayesian theory,this study incorporated the L1-2 norm to construct an objective function for the direct inversion of the P-to-S-wave velocity ratio.Third,the objective function was solved to obtain the inversion result for the P-to-S-wave velocity ratio.The quantitative comparison of the correlation coefficients demonstrates that the inversion results based on the L1-2 norm outperform those based on the L1 or L2 norm,direct inversion is superior to indirect inversion,and joint inversion provides better results than individual inversion.Finally, the effectiveness and feasibility of the proposed method in this study were validated through inversions of synthetic and field data.

Key wordsP-to-S-wave velocity ratio    L1-2 norm    multi-wave multi-component seismic data    direct inversion
收稿日期: 2024-10-25      修回日期: 2025-02-13      出版日期: 2025-06-20
ZTFLH:  P631.4  
基金资助:中国石油天然气集团有限公司项目“物探应用基础实验和前沿理论方法研究”(2022DO0604-04)
作者简介: 韩磊(1998-),男,中国石油大学(北京)博士在读,主要研究方向为地震反演。Email:hl981019@163.com
引用本文:   
韩磊, 李景叶, 耿伟恒, 王永平, 杨骐羽, 张宇宁. 基于L1-2范数约束的叠前多分量地震数据直接反演纵横波速度比方法[J]. 物探与化探, 2025, 49(3): 620-630.
HAN Lei, LI Jing-Ye, GENG Wei-Heng, WANG Yong-Ping, YANG Qi-Yu, ZHANG Yu-Ning. A method for calculating the P-to-S-wave velocity ratio through direct inversion of prestack multi-component seismic data based on the L1-2 norm constraint. Geophysical and Geochemical Exploration, 2025, 49(3): 620-630.
链接本文:  
https://www.wutanyuhuatan.com/CN/10.11720/wtyht.2025.1365      或      https://www.wutanyuhuatan.com/CN/Y2025/V49/I3/620
Fig.1  单独PP波、联合PP-PS波直接反演纵波速度(a)、横波速度(b)、密度(c)
数据类型 单独PP反演 联合PP+PS联合反演
反演参数 纵波速度 横波速度 密度 纵波速度 横波速度 密度
相关系数 0.8723 0.8259 0.9067 0.9423 0.8697 0.9619
Table 1  不同数据类型反演结果的相关系数
地层 Vp/(m·s-1) Vs/(m·s-1) ρ/(g·cm-3)
页岩 2540 1250 2.30
含气砂岩 2980 1525 2.42
Table 2  第一类典型AVO模型
地层 Vp/(m·s-1) Vs/(m·s-1) ρ/(g·cm-3)
页岩 2776 1780 2.35
含气砂岩 2700 1740 2.34
Table 3  第二类典型AVO模型
地层 Vp/(m·s -1) Vs/(m·s-1) ρ/(g·cm-3)
页岩 3000 1280 2.30
含气砂岩 2450 1265 2.12
Table 4  第三类典型AVO模型
Fig.2  3种典型AVO模型的PP波反射系数对比
Fig.3  3种典型AVO模型的PS波反射系数对比
Fig.4  无噪正演合成的PP波(a)和PS波(b)地震记录
Fig.5  不同分布的一维概率密度函数对比
Fig.6  L0范数(a)、L1范数(b)、L2范数(c)、L1-2范数(d)的二维图像
Fig.7  无噪数据反演结果
a—PP单独反演;b—PP+PS联合反演
Fig.8  SNR=10正演合成地震记录
a—PP波地震记录;b—PS波地震记录
Fig.9  SNR=10数据反演结果
a—PP单独反演;b—PP+PS联合反演
Fig.10  SNR=4正演合成地震记录
a—PP波地震记录;b—PS波地震记录
联合PP+PS直接反演 单独PP直接反演 联合PP+PS间接反演
L1 L2 L1-2 L1 L2 L1-2 L1 L2 L1-2
SNR=4 0.9326 0.9300 0.9592 0.9123 0.9050 0.9454 0.9073 0.9017 0.9342
SNR=10 0.9815 0.9529 0.9841 0.9257 0.9228 0.9536 0.9219 0.9162 0.9425
Table 5  反演结果相关系数对比
Fig.11  SNR=4数据反演结果
a—PP单独反演;b—PP+PS联合反演
Fig.12  SNR=10(a)和SNR=4(b)数据PP单独反演结果
Fig.13  PP波(a)和PS波(b)部分叠加地震剖面
Fig.14  井旁道PP波单独反演结果(a)和井旁道PP波、PS波联合反演结果(b)
Fig.15  L1-2范数约束的叠前单独PP波地震数据直接反演纵横波速度比
Fig.16  L1-2范数约束的叠前联合PP波、PS波地震数据直接反演纵横波速度比
数据类型 单独PP反演 联合PP+PS联合反演
约束方法 L1范数 L2范数 L1-2范数 L1范数 L2范数 L1-2范数
相关系数 0.3133 0.3019 0.5350 0.4514 0.4359 0.6535
Table 6  反演结果相关系数对比
[1] Granli J R, Arntsen B, Sollid A, et al. Imaging through gas-filled sediments using marine shear-wave data[J]. Geophysics, 1999, 64(3):668-677.
[2] Tsvankin I, Gaiser J, Grechka V, et al. Seismic anisotropy in exploration and reservoir characterization:An overview[J]. Geophysics, 2010, 75(5):75A15-75A29.
[3] Dave H. Dynamic warping of seismic images[J]. Geophysics, 2013, 78(2):S105-S115.
[4] Geng W H, Chen X H, Li J Y, et al. Warped P-SV wavelet distortion correction using a time-frequency adaptive shaping filter[J]. Geophysics, 2023, 88(2):V101-V112.
[5] 张天悦, 林凯, 文晓涛, 等. 应用Lp拟范数稀疏约束的纵横波速比直接反演[J]. 石油地球物理勘探, 2024, 59(2):230-237.
[5] Zhang T Y, Lin K, Wen X T, et al. Direct inversion of P-wave to S-wave velocity ratio by Lp quasi-norm sparse constraints[J]. Oil Geophysical Prospecting, 2024, 59(2):230-237.
[6] 程冰洁, 徐天吉, 梁群, 等. 多波速度比参数含气性识别研究与应用[J]. 石油地球物理勘探, 2014, 49(2):307-315,220-221.
[6] Cheng B J, Xu T J, Liang Q, et al. Gas identification using multi-wave velocity ratio parameters[J]. Oil Geophysical Prospecting, 2014, 49(2):307-315,220-221.
[7] Compton S, Hale D. Estimating VP/VS ratios using smooth dynamic image warping[J]. Geophysics, 2014, 79(6):V201-V215.
[8] Zhi L X, Chen S Q, Song B S, et al. Nonlinear PP and PS joint inversion based on the exact zoeppritz equations:A two-stage procedure[J]. Journal of Geophysics and Engineering, 2018, 15(2):397-410.
[9] Donoho D L. Compressed sensing[J]. IEEE Transactions on Information Theory, 2006, 52(4):1289-1306.
[10] Zhang R, Castagna J. Seismic sparse-layer reflectivity inversion using basis pursuit decomposition[J]. Geophysics, 2011, 76(6):R147-R158.
[11] Yin P H, Lou Y F, He Q, et al. Minimization of L1-2 for compressed sensing[J]. SIAM Journal on Scientific Computing, 2015, 37(1):A536-A563.
[12] 耿伟恒, 陈小宏, 李景叶, 等. 基于L1-2正则化的地震波阻抗“块” 反演[J]. 石油地球物理勘探, 2022, 57(6):1409-1417,1260-1261.
[12] Geng W H, Chen X H, Li J Y, et al. Seismic“blocky” acoustic impedance inversion based on L1-2 regularization[J]. Oil Geophysical Prospecting, 2022, 57(6):1409-1417,1260-1261.
[13] 聂文亮. 非凸L1-2正则化地震反演方法研究[D]. 成都: 成都理工大学, 2021.
[13] Nie W L. Research on nonconvex L1-2 regularization seismic inversion method[D]. Chengdu: Chengdu University of Technology, 2021.
[14] Aki K, Richards P G. Quantitative seismology theory and methods[M]. San Francisco: W.H. Freeman,1980.
[15] 刘应天, 李勇, 廖章权, 等. 基于弹性阻抗的高精度纵横波速比直接反演方法研究与应用[J]. 地球物理学进展, 2024, 39(3):1152-1163.
[15] Liu Y T, Li Y, Liao Z Q, et al. Study and application of high-precision direct inversion method of P-to-S-wave velocity ratio based on elastic impedance[J]. Progress in Geophysics, 2024, 39(3):1152-1163.
[16] Wang P, Hu T Y. AVO approximation for PS-wave and its application in PP/PS joint inversion[J]. Applied Geophysics, 2011, 8(3):189-196.
[17] Ramos A C B, Castagna J P. Useful approximations for converted-wave AVO[J]. Geophysics, 2001, 66(6):1721-1734.
[18] 张世鑫, 印兴耀, 张繁昌. 基于三变量柯西分布先验约束的叠前三参数反演方法[J]. 石油地球物理勘探, 2011, 46(5):737-743,836,663.
[18] Zhang S X, Yin X Y, Zhang F C. Prestack three term inversion method based on Trivariate Cauchy distribution prior constraint[J]. Oil Geophysical Prospecting, 2011, 46(5):737-743,836,663.
[19] 周林, 廖建平, 李景叶, 等. 基于精确Zoeppritz方程的储层含油气性预测方法[J]. 地球物理学报, 2021, 64(10):3788-3806.
doi: 10.6038/cjg2021P0099
[19] Zhou L, Liao J P, Li J Y, et al. Prediction method of reservoir oil-gas potential based on exact Zoeppritz equations[J]. Chinese Journal of Geophysics, 2021, 64(10):3788-3806.
[20] 周林, 廖建平, 袁成, 等. 基于精确Zoeppritz方程的时移地震流体动态监测[J]. 地球物理学进展, 2022, 37(5):2118-2128.
[20] Zhou L, Liao J P, Yuan C, et al. Time-lapse seismic inversion for fluid dynamic monitoring based on the exact Zoeppritz equations[J]. Progress in Geophysics, 2022, 37(5):2118-2128.
[1] 汪舒, 王锐, 杨家义, 赵卫升, 廖建. 基于非平稳褶积模型的泊松阻抗及裂缝参数叠前地震各向异性高分辨率直接反演方法[J]. 物探与化探, 2025, 49(3): 642-652.
[2] 李灿, 归平军. 纵横波速度比在东胜气田致密低渗储层流体识别中的应用[J]. 物探与化探, 2019, 43(3): 536-542.
[3] 冉然, 宋建国. 基于Zoeppritz方程的纵横波模量反演[J]. 物探与化探, 2017, 41(4): 707-714.
[4] 李红梅. 弹性参数直接反演技术在储层流体识别中的应用[J]. 物探与化探, 2014, 38(5): 970-975.
[5] 蒋邦远. 剩余视纵向电导比定义—— TEM新导出参数ΔSτrt及一维直接反演特性[J]. 物探与化探, 2012, 36(1): 59-64.
[6] 安玉林. 起伏地形上规则二度体复重磁场正演和直接反演[J]. 物探与化探, 2003, 27(1): 33-38.
[7] 蒋邦远, 张杰. TEM中心回线测深解释新参数Δn的数学模型研究[J]. 物探与化探, 2002, 26(6): 478-482.
Viewed
Full text


Abstract

Cited

  Shared   
  Discussed   
京ICP备05055290号-3
版权所有 © 2021《物探与化探》编辑部
通讯地址:北京市学院路29号航遥中心 邮编:100083
电话:010-62060192;62060193 E-mail:whtbjb@sina.com , whtbjb@163.com