Borehole Acoustics and Logging and Reservoir Delineation Consortia Annual Report 1998 Earth Resources Laboratory Department of Earth, Atmospheric, and Planetary Sciences Massachusetts Institute of Technology Cambridge, MA 02139 We would like to express our sincere appreciation to Sue Thrbak and Lori Weldon, without whose work the publication of this annual report would not be possible. Copyright © 1998 Massachusetts Institute of Technology Earth Resources Laboratory Copying is permitted only for internal purposes of the sponsors of the M.LT. Borehole Acoustics and Logging and Reservoir Delineation Consortia This report was typeset at ERL in Computer Modern Roman using 'I'gX. Borehole Acoustics and Logging and Reservoir Delineation Consortia Annual Report 1998 Principal Investigator M. N. Toksiiz Contributors A. Al-Dajani T. Alkhalifah H. J. Alshammery C. 1. Burch D. R. Burns M. G. Imhof M. L. Krasovec O. V. Mikhailov F. D. Morgan J. F. Olson J. H. Queen P. M. Reppert W. L. Rodi F. Shen J. Sierra M. N. Toksiiz Z. Zhu Report Editors D. R. Burns E. A. Henderson K. Jesdale Table of Contents 1. EXECUTIVE SUMMARY-CHARACTERIZATION OF RESERVOIR FLUID FLOW PROPERTIES by Daniel R. Burns and M. Nafi Toksoz Introduction. . . . . . . . . . . . . . . Fluid Flow Induced by Seismic Waves Fluid Flow Directionality . Scattering and Scale Effects Work in Progress . . . . . . 1-1 1-2 1-3 1-4 1-4 2. NEAR-SURFACE SCATTERING FROM HIGH VELOCITY CARBONATES IN WEST TEXAS by Matthias G. Imhof, M. Nafi Toksoz, Charles I. Burch, and John H. Queen Abstract . . . . . . . 2-1 Introduction. . . . . 2-1 2-3 West Texas Dataset Irregular Topography. 2-6 Near-Subsurface Heterogeneities 2-7 Discussion and Conclusions 2-8 Acknowledgments. . . . . . . . . 2-9 References. . . . . . . . . . . . . 2-10 Appendix A: Boundary Element Method. 2-12 Appendix B: Elastic Multipole Expansions. 2-13 Appendix C: Asymptotic Elastic Free Surface 2-15 Figures 2-21 3. SCALE AND FREQUENCY DEPENDENCE OF REFLECTION AND TRANSMISSION COEFFICIENTS by Matthias G. Imhof Abstract. . . Introduction . 3-1 3-1 M~~d.. 3~ Example. . Conclusions 3-4 3-5 v Acknowledgments. References . Figures 3-6 3-7 3-8 4. SENSITIVITY ANALYSIS OF AMPLITUDE VARIATION WITH OFFSET (AVO) IN FRACTURED MEDIA by Mary L. Krasovec, William L. Rodi, and M. Nafi Toksiiz Abstract . . . . . . . Introduction. . . . . . . The Forward Model .. Results and Discussion. Conclusions . . . . Acknowledgments. References . Figures 4-1 4-1 4-2 4-4 4-5 4-5 4-6 4-7 5. SCATTERING CHARACTERISTICS IN HETEROGENEOUS FRACTURED RESERVOIRS FROM WAVEFORM ESTIMATION by Feng Shen and M. Nafi Toksiiz Abstract . . . . . . . . . . . . . . . . . Introduction. . . . . . . . . . . . . . . Signal Parameter Estimator Function Conclusions . . . . Acknowledgments. . . . . . . . . . . . References. . . . . . . . . . . . . . . . Appendix: Signal Parameter Estimation Figures 5-1 5-2 5-4 5-10 5-11 5-12 5-14 5-17 6. SHEAR WAVE BIREFRINGENCE IN REVERSE VSP: AN APPROACH TO 3-D SURFACE P TO S CONVERTED WAVES by Jesus Sierra and John H. Queen Abstract . Introduction. . . . . . . . . . . . . . . . Propagator Matrix Method . . . . . . . Interpretation of the Propagator Matrix Synthetic Data and Application. P to S Converted Waves Conclusions . . . . Acknowledgments. . .. References. . . . . . . . Appendix: Simulated Annealing Figures . 6-1 6-2 6-2 6-4 6-5 6-6 6-7 6-8 6-9 6-11 6-13 VI ( 7. REFLECTION MOVEOUT INVERSION FOR HORIZONTAL TRANSVERSE ISOTROPY: ACCURACY AND LIMITATION by AbdulFattah AI-Dajani and Tariq Alkhalifah Abstract. . . . . . . . . . . . . . . Introduction. . . . . . . . . . . . . Reflection Moveout in HTI Media. The Inverse Problem. . . . . . . . Error Analysis The Inverse Problem in Layered Media. Discussion and Conclusions Acknowledgments. . . . . . . . . . . References. . . . . . . . . . . . . . . Appendix: Sign of HTI Parameters. Figures 7-1 7-2 7-3 7-4 7-5 7-12 7-16 7-18 7-19 7-20 7-22 8. BOREHOLE ELECTROSEISMIC MEASUREMENTS IN DOLOMITE: IDENTIFYING FRACTURES AND PERMEABLE ZONES by Oleg V. Mikhailov and M. Nafi Toksoz Abstract. . . . . . . . . . . 8-1 Introduction. . . . . . . . . 8-1 The Physical Phenomenon. 8-2 The Theoretical Model. 8-2 Field Experiments 8-3 mcldD~a. ~3 Discussion . . . . . Conclusions . . . . Acknowledgments. References. Figures 8-6 8-6 8-6 8-7 8-8 9. ELECTROSEISMIC LOGGING FOR THE DETECTION AND CHARACTERIZATION OF PERMEABLE ZONES: FIELD MEASUREMENTS AND THEORY by Oleg V. Mikhailov, Daniel R. Burns, and M. Nafi Toksoz Abstract. . . . . . . . . . . . . . . . . . . . . . . . . . Introduction. . . . . . . . . . . . . . . . . . . . . . . . Electrical Field Induced by a Borehole Stoneley Wave Electroseismic Logging Technique . . . . . . . . . . . . Field Experiment . . . . . . . . . . . . . . . . . . . . . Preliminary Analysis of the Stoneley-Wave-Induced Electrical Signals Theoretical Model for the Stoneley-Wave-Induced Electrical Potential Comparison of the Field Data and Theory: Amplitude-Versus-Frequency Dependence of the Stoneley-Wave-Induced Electrical Potential vii 9-1 9-1 9-2 9-3 9-5 9-8 9-10 9-15 Discussion . . . . . Conclusions . . . . Acknowledgments. References . . . . . Appendix A. Analysis of the Mysterious Electrical Signal M-M Appendix B. Relationships Bet\veen the Amplitude ofthe Electrical Potential Oscillation and the Amplitudes of the Signals Measured Using the 4-Electrode and the 2-Electrode Arrays Figures 9-15 9-17 9-17 9~ 19 9-21 9-22 9-24 lO.SEISMOELECTRIC LABORATORY MEASUREMENTS IN A BOREHOLE by Zhenya Zhu and M. N afi Toksoz Abstract. . . . . . . . . . . . . . . . Introduction. . . . . . . . . . . . . . . Borehole Models and Measurements . Results in Fractured Borehole Models Results in Sandwiched Borehole Models Conclusions . . . . Acknowledgments. References. Figures 10-1 10-1 10-2 10-3 10-5 10-6 10-6 10-7 10-8 l1.LABORATORY STUDY OF FREQUENCY DEPENDENT STREAMING POTENTIALS by Philip M. Reppert and F. Dale Morgan Abstract. . . Introduction. . . . . . . Theory. . . . . . . . . . Experimental Approach Discussion and Applications. Conclusions . . . . Acknowledgments. References . Figures 11-1 11-1 11-2 11-4 11-5 11-6 11-6 11-7 11-8 12.INTERVAL ATTENUATION ESTIMATION by Hafiz J. Aishammery and M. Nafi Toksoz Abstract. . . . . Introduction. '. . . . . . Definition of Q . . . . . Spectral Ratio :rvIethod . Q Estimation Accuracy 12-1 12-1 12-2 12-3 12-4 V III Water Tank Experiment Conclusions . . . . Acknowledgments. References . Figures . 12-6 12-9 12-10 12-11 12-12 13.TOWARD THE SIMULATION OF ATTENUATION: OSCILLATORY FLOW IN POROUS ROCK by John F. Olson Abstract . Introduction . Simulation Method . Preliminary Results Conclusions . . . . Acknowledgments. References . Figures . 14.DISPERSION ANALYSIS OF CROSS-DIPOLE DATA by Xiaojun Huang, Daniel R. Burns, and M. Nafi Toksoz Abstract . Introduction. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Flexural Dispersion and Formation Anisotropy . . . . . . . . . . A New Rotation Method for Mismatched Sources and Receivers. Application to Four-Component Cross-Dipole Data. Effects of Rotation on Dispersion Analysis . Conclusions . . . . Acknowledgments. . . -.' References . Figures . IX 13-1 13-1 13-2 13-4 13-6 13-7 13-8 13-9 14-1 14-2 14-3 14-4 14-7 14-9 14-9 14--':10 14-11 14-12 EXECUTIVE SUMMARY-CHARACTERIZATION OF RESERVOIR FLUID FLOW PROPERTIES Daniel R. Burns and M. Nafi Toksoz Earth Resources Laboratory Department of Earth, Atmospheric, and Planetary Sciences Massachusetts Institute of Technology Cambridge, MA 02139 INTRODUCTION The characterization of subsurface fluid flow is the key to exploration, production, and management of oil, gas, geothermal, and groundwater reservoirs. From a research perspective the question then becomes how can we measure or estimate the spatial variations in physical properties which control the flow of these fluids? Ideally we would like to be able to remotely identify fluid type and provide accurate estimates of in-situ porosity and permeability values in three dimensions. In some situations this may be possible, but in others such a goal may not be attainable. If accurate estimates of these physical properties cannot be achieved, there may still be important and useful related information available. For example, being able to provide accurate estimates of the direction of maximum fluid flow may be a very important piece of information for field development and drilling decisions. The Earth Resources Laboratory has focused on developing methods for using seismic waves to estimate flnid flow properties. Seismic waves provide higher resolution data than potential field measurements, can be polarized for anisotropy measurements, can be used in surface and borehole applications. and ERL has significant experience in the physics and modeling of wave propagation ill complex media. Our report this year provides results in three specific areas related t.o our overall goal of fluid flow characterization. The first. involves research into methods which utilize t.he actual motion, induced by seismic waves, of fluids ill porous rock. The passing of a seismic wave t.hrough a rock cont.aining a viscous fluid result.s in relative motion between t.he fluid and the solid matrix. This mot.ion dissipates seismic energy resulting in the att.enuat.ion of the passing wave. The motion of the fluid, which contains ions, also creates an elect.rical field which can be measured. We present result.s in both of these areas in this report. A second research area is the measurement of flow direct.ionality. 1-1 Burns The presence of open fractures with a preferred orientation will control the direction of fluid flow in a reservoir. Such fractures will also have a large effect on the elastic properties of the reservoir rock. The resulting elastic anisotropy may be observable in both surface seismic data as well as borehole acoustic logs. We present several papers on the effects of anisotropy on surface seismic data and AVO signatures, as well as on dipole sonic logs. Finally, because fluid flow is only one of the many factors which effect seismic waves, we must continue to improve our understanding of wave propagation in complex media. We present two such papers which look at scattering and scale dependent issues. The way in which property variations at different spatial scales affect seismic waves is an important research area that we will continue to investigate in the coming year. The following sections provide a more detailed summary of the results in each of these three broad areas. FLUID FLOW INDUCED BY SEISMIC WAVES A seismic wave impinging on a fluid-filled porous rock results in relative motion between the viscous fluid and the solid matrix. This motion may be bulk flow or local '~quirt' flow. Although there is evidence of both types of mechanisms from laboratory studies of rock samples, the way that fluid moves in a porous rock when a seismic wave passes is not well understood. Regardless of the mechanism, such relative motion results in attenuation of the seismic wave, with the frequency dependence of that attenuation being related to the type of fluid flow mechanism at work. Olson presents a numerical modeling approach that allows us to visualize such fluid motion. His results provide an exciting glimpse into the complexity of fluid flow in rocks, and will help us to understand the dominant attenuation mechanisms in different rocks. The use of surface seismic data to estimate fluid flow properties based on attenuation measurements is much more difficult. In order to use reflection data to estimate variations in reservoir attenuation, we must be able to isolate any amplitude changes to a specific interval of interest. Alshammery and Toksoz present results from a laboratory study in which they estimate the quality factor of several materials based on a comparison of the reflections from the top and base of a slab suspended in a water tank. The Q estimates they obtain are in good agreement with the actual values, but they point out that overburden attenuation may degrade the estimates as a function of source receiver offset due to different travel path lengths. When a seismic wave induces fluid flow, a streaming electrical current is produced. This current is caused by the adsorption of charged ions to the surface of the solid grains, and the resulting charge excess in the pore fluid. The relative motion of this fluid creates an electrical field which can be measured. This electroseismic effect provides another way to measure remotely the movement of fluids in a reservoir. Mikhailov et al. present field observations of this phenomenon in a borehole logging mode. They show that the effect can be measured in the field in sedimentary rocks (dolomite), and that the effect can be related to the interconnected porosity in the formation. They also find that by 1-2 ( Executive Summary making the measurement over a range of frequencies, it may be possible to estimate the permeability of the formation. Zhu and Toksoz likewise study the electroseismic logging technique in laboratory scale models. Their results indicate that this effect can be used to identify open fractures, and that the amplitude of the signal is related to the fracture aperture. Finally, Reppert and Morgan provide laboratory measurements of the streaming potential caused by fluid motion through porous materials. They measured the effect for a capillary tube, a porous filter, and a sample of Boise Sandstone over a frequency range which covered the critical frequency for each material. Their estimates for the average pore diameter based on the critical frequency are in good agreement with the actual values, and support the idea that the measurement of electroseismic data over a range of frequencies may provide a means of estimating permeability. FLUID FLOW DIRECTIONALITY Although we are most interested in obtaining direct indicators of in-situ permeability variations, information about the direction of fluid flow can be critically important for reservoir development decisions. The presence of aligned fractures results in elastic anisotropy which can be characterized by seismic measurements. AVO measurements as a function of azimuth can provide information about the orientation of fractures and the fracture density which is related to the fluid volume and permeability. Krasovec et al. studied the sensitivity of AVO parameters to fracture density, pore fluid, and lithology variations. They found that the 'c' parameter in a three-term Shuey-type parameterization of the AVO behavior is particularly sensitive to fracture density variations for vertical fractures. Shen et al., using 3-D finite difference models and field data, found that the spectral characteristics of reflections from the top and base of a fractured reservoir contain information about fracture density and the correlation scale lengths of the fracture distribution. They used a high resolution spectral analysis technique to study variations in the spectral signatures of reflections as a function of offset. Their results indicate that scattering from fractures aligned normal to the propagation path results in more energy at higher frequencies as a function of offset than would be seen for data acquired in areas without fractures or along the fracture strike. Al-Dajani and Alkhalifah investigate the effect of an HTI medium on the normal moveout of seismic reflections as a function of azimuth. If measurements are available for several source-receiver azimuths, the anisotropy parameter and symmetry axis direction can be obtained. Sierra and Queen present a method for estimating shear wave birefringence from 3-D surface P-S converted wave data based on an equivalent reverseVSP formulation. They show that it is possible, using a range of frequencies and offsets, to obtain information about 'subsurface anisotropy from converted wave data. In-situ anisotropy directions, due to aligned fractures, stress, or intrinsic material properties, can also be obtained from cross-dipole sonic logs. Huang et al. present a frequency domain rotation method that handles situations in which the two dipole sources are not matched. This method can improve the accuracy of the rotation of 1-3 Burns the data into fast and slow shear wave directions. Accurate rotation is also critical for analyzing differences in the dispersion characteristics of the fast and slow flexural modes. Differences between these dispersion curves may indicate variations in the propagation directions as a function of distance from the borehole. SCATTERING AND SCALE EFFECTS The characterization of fluid flow effects in reservoirs takes place within the context of complex subsurface geological conditions which scatter seismic energy. These scattering effects can provide us with information about the nature of small-scale heterogeneities which may impact reservoir production. However, if we are interested in the analysis of subtle fluid flow effects in seismic data, such scattering may be an unwelcome complication. Imhof et al. studied the effects of near-surface scattering on seismic reflection data. They found that for data acquired in West Texas, scattering was dominated by the presence of vugs and cavities in the near surface limestones. These heterogeneities set up a waveguide that trapped energy near the surface. Irregular topography and heterogeneous weathering layers did not appear to be important factors for this data. Imhof, in a second paper, studied the effect of different spatial scale heterogeneities on the reflection and transmission of seismic waves. Using wavelet transforms to filter different spatial scales from a sonic log, he calculated reflection and transmission coefficients as a function of frequency. The results indicate that transmission coefficients are generally independent of frequency and scale, while reflection coefficients are very sensitive to even the small-scale perturbations of slowness. WORK IN PROGRESS A number of other related projects are ongoing at ERL, including: geostatistics, fast wave propagation modeling and imaging algorithms (phase-screen type propagators; variable grid finite difference methods), hydrofracture imaging and monitoring, VSP while drilling, and a field acquisition research program that includes reverse VSP using a downhole vibrator source and surface 3-D seismic using random receiver layouts. 1-4 ( (