Imaging faults and fractures with the difference of fast and slow shear-wave splitting reflectivity, Δγ(S): 3D/9C survey in Midland Basin, West Texas, and 3D/3C survey in Washakie Basin, Wyoming

James Gaiser, H. Malcotti, Ranjan Dash, James DiSiena, Gary Murphy
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Abstract

One of the most important applications of shear-wave (S-wave) seismic exploration has been in reservoir fracture characterization. While many advancements have been made over the past 30 years to compute and correct for the long-wavelength kinematics of S-wave splitting (SWS) (fast S-wave polarization directions and slow S-wave time delays), practically no progress has been made in imaging the short-wavelength reflectivity of fractures directly with Δγ(S). This property is the contrast in the SWS anisotropy parameter, γ(S), and represents the reflection amplitude at vertical incidence for changes in fracture density and orientation across an interface. In this article, we examine the Lupin nine-component survey in Midland Basin, Texas, for the technical reliability of imaging fractures in depth with converted P to S waves (PS waves) guided by pure-mode horizontal shear waves and vertical shear waves. Final Δγ(S) amplitude maps for each mode show sensitivity to fractures, faults, and the maximum horizontal stress direction. These maps are computed from the difference between fast and slow S-wave stacks (after SWS analysis and correction) and P-wave amplitude variation with offset gradient stacks. The S-wave difference maps identify an east–west lineament, possibly a strike-slip fault or fracture corridor, that is not observed by P-wave depth slices. Pure-mode S waves and PS waves are orders of magnitude more sensitive to Δγ(S) than P waves. We also review the development of Δγ(S) and find that it has been relatively unexploited by the exploration industry. In addition, we demonstrate that Δγ(S) can be obtained directly from the objective function of the transverse energy to correct for SWS, and show a four-component Alford rotation example from a previous PS-wave survey in the Washakie Basin, Wyoming.
利用快慢剪切波分裂反射率Δγ(S)的差异成像断层和裂缝:西得克萨斯州米德兰盆地的三维/九维测量和怀俄明州瓦沙基盆地的三维/三维测量
剪切波(S 波)地震勘探最重要的应用之一是储层裂缝特征描述。过去 30 年中,在计算和校正 S 波分裂(SWS)的长波运动学(快速 S 波极化方向和慢速 S 波时间延迟)方面取得了许多进展,但在用Δγ(S) 直接成像裂缝的短波反射率方面几乎没有取得任何进展。这一特性是 SWS 各向异性参数 γ(S) 的对比,表示在垂直入射时,断裂密度和方向在界面上发生变化时的反射幅度。在本文中,我们研究了德克萨斯州米德兰盆地的 Lupin 九分量勘探,利用纯模式水平剪切波和垂直剪切波引导的 P 波到 S 波(PS 波)转换,对裂缝进行深度成像的技术可靠性。每种模式的最终Δγ(S)振幅图显示了对断裂、断层和最大水平应力方向的敏感性。这些振幅图是根据快速和慢速 S 波叠加(经过 SWS 分析和校正)以及 P 波振幅变化与偏移梯度叠加的差值计算得出的。S 波差值图确定了一条东西向线状构造,可能是一条走向滑动断层或断裂走廊,P 波深度切片没有观测到这一构造。纯模式 S 波和 PS 波对 Δγ(S)的敏感度要比 P 波高几个数量级。我们还回顾了 Δγ(S)的发展历程,发现勘探行业对它的利用相对较少。此外,我们还证明Δγ(S)可以直接从横向能量的目标函数中获得,以校正SWS,并展示了以前在怀俄明州瓦沙基盆地进行的PS波勘探中的一个四分量阿尔福德旋转实例。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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