14. Case Studies of Multicomponent Seismic Data for Fracture Characterization: Austin Chalk Examples

Shear wave studies of multicomponent seismic data were done along the Austin Chalk trend in Texas. Six surface seismic lines of four-component shear wave data from Pearsall and Giddings fields and three zero-offset vertical seismic profiles (VSPs) from three sites with different production rates were studied to demonstrate the applications of shear wave splitting for fracture reservoir delineation. The three seismic lines (l-3) from Pearsall field formed a classic experiment for studying shear wave splitting. They have different (line) azimuth with respect to the regional fracture strike (parallel, perpendicular, and at -4O”, respectively), are in areas with different hydrocarbon production, and have different split shear wave behavior. The anisotropy along line 1 is small, which correlates with the absence of nearby commercial production. There is an increasing trend in anisotropy from line 2 to 3, which correlates with line 2 being close to and line 3 being within the producing Austin Chalk acreage. The trend of anisotropy variation along line 3 also correlates with the distribution of producing oil wells along that line. In particular, production from the three horizontal wells (Wl-W3) drilled nearby correlates with the variation in shear wave polarization, time delay, and amplitude. Line 4 from Giddings field had a horizontal well drilled on it, and mud logs were obtained for identifying fracture zones. The fracture swarms identified by the mud logs are coincident with the dim spots identified from the section of the slow split shear wave. Lines 5 and 6, also from Giddings field, demonstrate classic S, dim spot and S, versus S2 mistie behavior, respectively. The three VSPs, from three wells with different production rates, show different shear wave responses. VSP 1, from a nonproductive well, shows minimal shear wave time delay and no amplitude anomalies. VSP 2, from a water-producing well, shows some amount of splitting but no anomalies in shear wave attributes. VSP 3, from an oil-producing well, shows clear shear wave splitting and anomalies in shear wave amplitudes. Amplitude corrections are necessary for preserving and recovering shear wave anisotropy information associated with the target, and the linear transform technique (LTT) simplifies the processing sequence for examining anisotropy in shear wave reflection data. Stacked polarization logs can be used for identifying local variations in polarization (often associated with local variations in crack geometry) and for better imaging of subsurface structure, as in line 3.

[1]  X. Li Detecting Polarization Changes with Depth in Multicomponent Reflection Surveys , 1995 .

[2]  Xiang-Yang Li,et al.  Interpreting Data Matrix Asymmetry And Polarization Changes With Depth In Multicomponent Reflection Surveys , 1995 .

[3]  L. Thomsen,et al.  Shear‐wave anisotropy and coalbed methane productivity , 1995 .

[4]  S. Crampin,et al.  Interpreting data matrix asymmetry in near-offset, shear-wave VSP data , 1994 .

[5]  Xiang-Yang Li,et al.  Amplitude corrections for multicomponent surface seismic data , 1994 .

[6]  S. Crampin,et al.  Approximations to Shear-Wave Velocity and Moveout Equations in Anisotropic MEDIA1 , 1993 .

[7]  S. Crampin,et al.  Variation of reflection and transmission coefficients with crack strike and crack density in anisotropic media , 1993 .

[8]  S. Crampin,et al.  Interpreting non-orthogonal split shear waves in multicomponent VSPs , 1993 .

[9]  Stuart Crampin,et al.  Linear‐transform techniques for processing shear‐wave anisotropy in four‐component seismic data , 1993 .

[10]  W. Rizer,et al.  VELOCITY AND ATTENUATION ANISOTROPY CAUSED BY MICROCRACKS AND MACROFRACTURES IN A MULTIAZIMUTH REVERSE VSP , 1993 .

[11]  Xiang-Yang Li Shear-wave splitting in reflection surveys theory, methods and case studies , 1992 .

[12]  S. Crampin,et al.  Viability of shear-wave amplitude versus offset studies in anisotropic media , 1991 .

[13]  M. C. Mueller,et al.  Prediction of lateral variability in fracture intensity using multicomponent shear-wave surface seismic as a precursor to horizontal drilling in the Austin Chalk , 1991 .

[14]  Stuart Crampin,et al.  A decade of shear-wave splitting in the Earth's crust: what does it mean? what use can we make of it? and what should we do next? , 1991 .

[15]  D. Michon,et al.  Anisotropy survey for reservoir definition , 1991 .

[16]  S. Crampin,et al.  EXTENSIVE‐DILATANCY ANISOTROPY: RELATIVE INFORMATION IN VSPs AND REFLECTION SURVEYS1 , 1991 .

[17]  Robert H. Tatham,et al.  Multicomponent seismology in petroleum exploration , 1991 .

[18]  T. Davis,et al.  Reservoir characterization by 3-D, 3-C seismic imaging, Silo field, Wyoming , 1990 .

[19]  Donald F. Winterstein,et al.  Velocity anisotropy terminology for geophysicists , 1990 .

[20]  L. Thomsen,et al.  Reflection shear-wave data collected near the principal axes of azimuthal anisotropy , 1990 .

[21]  K. K. Sekharan,et al.  Dispersion And Anisotropy In Laminated Versus Fractured Media: An Experimental Comparison , 1990 .

[22]  T. Davis,et al.  Three-dimensional multicomponent imaging of reservoir heterogeneity, Silo Field, Wyoming : Geophysics V56, N12, Dec 1991, P2048–2056 , 1991 .

[23]  N. Kuich Seismic Fracture Identification and Horizontal Drilling: Keys to Optimizing Productivity in a Fractured Reservoir, Giddings Field, Texas , 1989 .

[24]  Leon Thomsen,et al.  Reflection seismology over azimuthally anisotropic media , 1988 .

[25]  Stewart G. Squires,et al.  Interpretation of total wave field data over Lost Hills field, Kern County, California , 1988 .

[26]  S. Crampin Geological and industrial implications of extensive-dilatancy anisotropy , 1987, Nature.

[27]  John H. Spang,et al.  Fracture development and mechanical stratigraphy of Austin Chalk, Texas , 1987 .

[28]  Iain Bush,et al.  Estimating the internal structure of reservoirs with shear‐wave VSPs , 1986 .

[29]  R. M. Alford,et al.  Shear data in the presence of azimuthal anisotropy: Dilley, Texas , 1986 .

[30]  H. A. Willis,et al.  Azimuthal Anisotropy: Occurrence And Effect On Shear-Wave Data Quality , 1986 .

[31]  D. Winterstein,et al.  Supercritical reflections observed in P- and S- wave data , 1985 .

[32]  Stuart Crampin,et al.  Evaluation of anisotropy by shear‐wave splitting , 1985 .

[33]  G. Dohr Seismic shear waves , 1985 .

[34]  Bob A. Hardage,et al.  Vertical Seismic Profiling, Part A: Principles , 1985 .

[35]  R. Ensley Comparison of P- and S-wave seismic data: A new method for detecting gas reservoirs , 1984 .

[36]  Stuart Crampin,et al.  A review of wave motion in anisotropic and cracked elastic-media , 1981 .

[37]  J. Hudson Wave speeds and attenuation of elastic waves in material containing cracks , 1981 .

[38]  J. Dravis SEDIMENTOLOGY AND DIAGENESIS OF THE UPPER CRETACEOUS AUSTIN CHALK FORMATION, SOUTH TEXAS AND NORTHERN MEXICO , 1980 .

[39]  Paul G. Richards,et al.  Quantitative Seismology: Theory and Methods , 1980 .

[40]  S. Crampin,et al.  Seismic body waves in anisotropic media: Reflection and refraction at a plane interface , 1977 .

[41]  W. L. Stapp The Geology of the Fractured Austin and Buda Formations in the Subsurface of South Texas , 1977 .

[42]  R. Scott The Austin Chalk-Buda Trend of South Texas , 1977 .

[43]  Paul L. Stoffa,et al.  Vp/Vs—A POTENTIAL HYDROCARBON INDICATOR , 1976 .

[44]  R. L. Layden Big Wells Field, Dimmit and Zavala Counties, Texas , 1976 .

[45]  G. Gardner,et al.  Velocity And Attenuation Of Elastic Waves In Sands , 1968 .

[46]  A. W. Weeks Balcones, Luling, and Mexia fault zones in Texas , 1945 .