AGL831

Abstract

AGL831 Abstract A seismic survey was performed in Southeastern Idaho from 1979-1980. The purpose of this geophysical study was to try to acquire data over a seismically opaque layer, one which is overlain by soft, high porosity volcanic tuffs and ash flows. A CDP line, Line 999 was processed and analyzed in order to investigate the effects of the surficial volcanic layer. Regional geology around the survey area was studied for interpreting the seismic data. One cross-section of a 3D survey area, which is parallel and close to Line 999, is shown and compared with 2D data. Several reasons are given to explain why the 3D migrated data do not produce the best results. An interpretation was made by relating the seismic data to well logs around the survey area. Two different geological models are presented; both of them are suitable models based on the available information.


AGL832

Abstract

Complex seismic trace attributes including the amplitude of the envelope, instantaneous phase, instantaneous frequency, and apparent polarity are computed and displayed from theoretical and scaled physical model data. The models were chosen so the seismic data from them could demonstrate the utility of attribute displays and their analysis when developing an interpretation. Vertical and horizontal attribute sections are presented which show their possible uses for delineating unconformities and fault blocks and generating isochron contour maps. The instantaneous frequency attribute is shown to be sensitive to waveform interferences and produces characteristic patterns for pinch out models. The importance of source wavelets, color codes and threshold parameters are demonstrated. Evaluation of elastic wave equation modeling programs is carried out by comparing complex trace attributes from synthetic and scaled physical model data. Lithologies of exploration interest are modeled using an elastic modeling program and their complex trace attributes are examined. Attribute displays are shown to aid the analysis of waveshape variation with angle of incidence in pre-stack common midpoint gathers. These variations might be able to be used for predicting lithologies and porefill material.


AGL833

Abstract

Concurrency control is the activity of coordinating concurrent accesses to a database in a multiuser database management system (DBMS). By preserving database consistency, concurrency control ensures that all alterations to the database are serializable (serializability is a situation in which concurrent operations on a database result in a computationally equivalent state of the database, compared with executing the operations in a serial fashion). The concurrency control problem is very important in a distributed DBMS (DDBMS) because: users may access data stored in many different computers in a distributed system, and a concurrency control mechanism at one computer cannot know about interaction at other computers. Concurrency control has been actively investigated for the past several years. Many concurrency control algorithms have been proposed for DDBMS and several have been, or are being, implemented. It is difficult to compare the performances of the many proposed algorithms. Naturally, each author proclaims his or her approach as the best, but there is little compelling evidence to support these claims. This thesis reviews the currently available algorithms concerning the concurrency control in DDBMS and evaluates their performance through simulation. The simulation software was developed to evaluate the performance of the DDBMS with different concurrency control mechanisms based on the timestamp technique. The results from the simulation are discussed and the conclusions are presented.


AGL834

Abstract

The Fast Fourier Transform (FFT) is an efficient algorithm to compute the discrete Fourier transform. The objective of this thesis is to analyze a variety of problems which lead to inaccurate results in standard FFT differentiation techniques. Methods which improve computational accuracy are also reviewed. Two main approaches are followed in order to improve the accuracy of the estimated derivative. The Fourier coefficients of the function are estimated more accurately in the first approach. The second approach is to improve the convergence of the Fourier series of the function. The methods discussed are tested using FFT routines available on the FPS 100 array processor. The results indicate that the latter approach leads to a higher accuracy.


AGL835

Abstract

This thesis describes a physical modeling study of seismic reflections from thin beds. Three models representing common thin bed situations were used in the study. In the first model, we studied the reflections from a homogeneous thinning bed embedded in a low velocity material, to determine amplitude and waveshape changes associated with changes in the bed thickness. In the second model, we studied the reflections from a thin bed which is composed of interlayering of high and low velocity materials of the same thickness, to investigate how reflections from a series of strata differ from reflection from a massive bed. In the third model, we extended the second model to study the reflections when the layers composing the thin bed are not of the same thickness, to verify the conclusion of numerical modeling that reflection amplitude and waveshape are not sensitive to how layers are distributed as long as the overall interval is thin. The results from the first model mostly agree with theoretical predictions published in the literature. In the second and third models the results show that not only interference but also other factors are important in constructing the reflection when the overall interval is thin. We also found that the waveshape is affected by the distribution of the layers in the thin bed, in contrast to the conclusion of numerical modeling published in the literature. We extended models two and three to model a concept of transgressive sands onto an unconformity, which relates to the question as to whether seismic reflections follow time or facies lines. The seismic sections show the attitude of most reflections are those of time lines.


AGL836

Abstract

The physical seismic modeling system at the AGL has been utilized to measure ultrasonic wave attenuation and dispersion in (1) homogeneous materials (Plexiglas and silicone rubbers) used to construct geologic models and (2) geologically more realistic two-phase materials (fluid-saturated sands and fluid-solid suspensions). Such measurements are necessary to better understand physical model data, and the data for two-phase media are helpful in evaluating theories for wave propagation in heterogeneous media. A procedure has been developed which successfully synthesizes the effect of a plane wave by summing the responses to point sources arranged in a planar grid. This data collection procedure provides a way to increase the signal/noise ratio in a more physically meaningful and helpful way than other collection schemes. It should also prove useful for studies in other areas. The P-wave velocities for silicone rubber-sand (fluid-solid) mixtures are predicted very well as a function of inclusion concentration by considering them to be composed of spherical inclusions suspended in an ideal fluid matrix. The spectral amplitude ratio and phase difference techniques yielded the spatial attenuation coefficient and the phase velocity as functions of frequency. The greatest attenuation and dispersion were observed for the rubber-sand mixtures; relative motion between matrix and inclusions is hypothesized as the principal attenuation mechanism. The fluid-saturated sandpacks exhibited intermediate Qs and dispersion rates, while the silicone rubbers were highly nonattenuative and nondispersive. For Plexiglas, attenuation and dispersion were relatively high; this was the only material for which Q appeared frequency-dependent. The envelope and instantaneous frequency attributes are found to be more useful than other time-domain pulse characteristics, especially in estimating Q and variation of pulse peak frequency. A complex propagation operator was applied to pulses in the frequency domain. Waveforms predicted for nondispersive, constant-Q propagation agree well with observed waveforms for constant-Q media, but not so well for Plexiglas. An accurate method of determining the peak-frequency Q has been developed which iteratively models the effects of propagation with different trial Q values.


AGL837

Abstract

For a given geological model, the relationships (temporal, spatial and causal) between the layers in the model, the raypaths and the seismic wavefronts radiating from a point source can be preserved by means of a linked tree data structure. Each node in the tree represents a seismic hologram a collection of rays along the boundary of a geological layer, defining the propagation of a particular seismic wavefront through that layer. These structures used in combination with ray tracing algorithms and interactive computer graphics open the possibility for many advanced interactive, animated displays, including the ability to interactively identify every event in the display as to its origin and history. The techniques for building such data structures and for building the associated graphic displays are described. An algorithm for reconstructing the seismic wavefronts and arrival time curves using polynomial splines is developed. These procedures are demonstrated for several geological models and the results compared with data obtained from a physical modeling experiment.


AGL821

Abstract

A Fourier or pseudo-spectral forward modeling algorithm for solving the 2-D acoustic wave equation is presented. Time derivatives which appear in the wave equation are calculated by second order finite differencing, whereas spatial derivatives are calculated by Fast Fourier Transforms (FFT). The scheme requires fewer spatial grid points than finite difference methods to achieve the same accuracy. This method is tested against known analytic solutions and physical modeling results. The Exploding Reflector concept (Loewenthal et al., 1976) is examined for the modeling of zero source-to-receiver offset sections. The acoustic wave equation is compared with a one-way wave equation which represents the upgoing wavefield only. The one-way wave equation used is not derived through an expansion and, therefore, can represent dips up to 90 degrees. There is apparently no simple counterpart of this equation in the space domain and it can be conveniently implemented only by a Fourier method. The inverse problem (migration) is investigated using the complementary version of the one-way wave equation employed for modeling. Also a novel alternative of carrying out the migration through a reverse time extrapolation is examined. This method is tested using synthetic data. A new two way non-reflecting wave equation is derived, which gives highly reduced reflection coefficients at material boundaries. This new equation is used in both zero source to receiver offset modeling and reverse time depth migration. The examples show that this equation is capable of simulating raypaths which bend beyond the horizontal due to refraction associated with large velocity gradients. It should be useful for the modeling or migration of primary reflections from the underside of complex structures such as overhanging salt domes or steep thrust faults.


AGL822

Abstract

A 3D acoustic wave equation modeling program was designed and implemented on the CDC Cyber 205 vector processor. The program was designed to handle a 256x256x128 spatial grid and approximately 3000 time steps within 40 hours of computing time. The Fourier method was selected as the computational basis of the 3D modeling program. Some basic features of vector processors are introduced such as pipelining, vector instructions . . .etc. A brief overview of the Cyber 205 system and the algorithm used in solving the wave equation are also discussed. The design of the 3D forward modeling program has the following properties (1) Halfword (32-bit) storage and computation. (2) Four- way concurrent I/O management (SLICE4). (3) Dynamic startup computation involving only those spatial points at which wave activity is present. The measured times and snapshots of the test models are presented. Factors affecting the computing time and improvements of the 3D forward modeling program are also discussed.


AGL823

Abstract

The Multi-channel Wavelet Extraction System (MWES) is a generalization of the algorithm developed by Thomas (1976). It is a deterministic technique which makes use of the velocity function and the offset distance to determine the phase of the seismic wavelet. When the normal move-out correction is known, the system appears to recover a consistent wavelet estimate. Several rules of thumb are discussed for quantifying the input parameters necessary for running the MWES in terms of the properties of the input data. These rules of thumb are clarified by synthetic results. The MWES overcomes problems related with real field data analysis such as additive noise introduced into the traces and errors in stacking-velocity estimation. An application of the System to real field data analysis demonstrates advantages of the method with respect to the traditional algorithms for seismic deconvolution.


AGL824

Abstract

A generalization of the simplex algorithm for solving linear programming problems is presented. In each iteration of the simplex algorithm the objective function is improved by proceeding from one vertex to an adjacent vertex along a one dimensional facet (an edge) of the convex polytope of feasible solutions. We exhibit a k-dimensional analog of this where k>1 is chosen so as to yield a steep descent. It is anticipated that the faster rate of convergence to the optimal solution will more than offset the extra work done to select a higher dimensional facet, resulting in a reduction of overall computational effort. We have implemented this method by modifying an existing program written in vector FORTRAN for CDC CYBER 203/205. The original program used the simplex algorithm to solve transportation problems which form an important special class of linear programming problems. We discuss some details of this implementation and report some favorable numerical results comparing the timings for the simplex method and our generalization of the simplex method for some randomly generated transportation problems involving upto 10,000 variables. Suggestions are given for future research.


AGL811

Abstract

Velocity analysis is an important step in seismic processing for final proper interpretation. Three sets of computer programs have been designed and tested for the analysis of velocity based on 3D seismic data. These computer programs can be used with any set of 2D or 3D data provided the source and receiver coordinates have been written in the header of each trace. Program set A modifies Owusu&180;s (1981) velocity analysis algorithm which is based on 3D migration. Program set B gives attributes for a fixed velocity and variable arrival time. Each event has to be analyzed separately. Program set C displays any selected event as a function of offset from source to receiver. This allows one to analyze the distribution of energy among offsets and hence to select weights for the offsets that will improve resolution for the output from program set A or program set B. Two physical models demonstrate the use of these computer programs. The first model is a stack of 9 layers of RTV materials. A single multi-fold CDP (Common Depth Point) line tests these programs for the 2D case. The second model is a modified GULF model (SALGLF-5). Areal coverage data on the second model tests these programs for the 3D case.


AGL812

Abstract

In recent years the acquisition, processing and interpretation of 3D seismic data, for the purpose of locating gas and oil reservoirs, have become practical. A typical seismic survey will sample a 25 square mile area with about 2 million seismic recordings, each containing 4000 time samples. The processing reconstructs these data by a 3D convolution into a regular grid of data that represents the acoustic impedance distribution in the earth for a volume of about 50 cubic miles. The interpretation requires that this volume be searched and correlated with geologic information. This thesis explores one way in which the volume can be searched and visualized, which may aid the interpreter. The concept is based on steroscopic perception, and was originally proposed for the interpretation of volume data for medical applications. The illusion of looking at a 3D volume can be obtained by fusing a stereoscopic pair of pictures. Each picture can be made by projecting each data point of the volume into a plane from a point where the eye is placed. The data values along any projection line can be summed to form the picture, or only a segment along the line can be selected. By selective projection, the volume can be searched and obscuring layers removed. This thesis describes a VAX 11/780 computer program which generated stereoscopic images from standard seismic data, and illustrates the concept of 3D perception with synthetic and physical model data. The physical model simulated 5 stratigraphic traps in a marine environment, and the data simulated a survey over the traps consisting of a 128 x 128 grid of seismic recordings. The raw data were 3D migrated and the resulting volume was projected into stereoscopic pairs of images. The data conversions required to display the images on a RAMTEK graphic system are explained. The stereoscopic pictures show the synthetic and physical models in their true spatial positions. A comparison of the raw data and the 3D migrated data demonstrates the increase in lateral resolution achieved by the 3D processing. Projection of the envelope function of the seismic traces is shown to give improved depth perception compared with projection of the positive amplitudes. The following lines of research are suggested by this investigation: (1) to develop an interactive stereoscopic display so that the data volume projected can be selected and enhanced interactively, (2) to rewrite the algorithm for orthogonal projection, or for vector processing computer, so that the computation time is reduced, (3) to project contour plots of constant phase angle, (4) to investigate the use of other seismic attributes of the data such as instantaneous frequency or velocity and (5) to investigate enhancement techniques for visualizing faults or for picking geologic horizons.


AGL813

Abstract

Traditional seismic imaging methods send pulse-like acoustic waveforms into the subsurface and record the echoes. A large degree of data redundancy is collected and wasted just to improve the output signal-to-noise ratio to a limited amount. This study examines an alternative way in seismic data acquisition, the sign-bit Vibroseis method. The objective is to evaluate the method for 3D imaging applications; in particular, the holographic method. Acoustical holography is identified as any image focusing scheme that performs spatial correlations either implicitly or explicitly. One particular implementation, the multifrequency acoustical holography, has been suggested for seismic imaging. This method requires broadband yet coherent input data, which is readily supplied by the Vibroseis sweep signals and the associated temporal correlation procedure. The multifrequency holographic method is compared with another similar approach, the lensless Fourier transform holographic method. Also compared are other 3D wave equation imaging algorithms, such as the Kirchhoff summation migration, the frequency domain migration, the finite difference migration, the Fresnel imaging, the Fraunhofer imaging and the wave vector diversity method. Fundamental differences and similarities among these algorithms are compared on a theoretical basis. The 3D Kirchhoff migration is also implemented in a more efficient process, the two-step method. This approach approximates the 3D full-blown integration by two 2D integrations. The resulting aberrations are tolerable. Both the Vibroseis sweep and the sign-bit recording technique are recognized as information encoding and compressing processes. The benefits of these processes are to have less critical requirements for the input dynamic range and higher utilization of the redundantly collected data. Data retrieval of the sign-bit Vibroseis data is performed by either linear processes, such as pilot-correlation and vertical stacking, or some nonlinear processes, such as CDP stacking and migration. All nonlinear processes involve distortions due to hard-limiting. Mathematical analyses are done to derive the relationship between the input and output dynamic ranges. Distortions are pointed out. Synthetic traces are generated to compare the results of sign-bit and 16-bit recordings under the assumption of some simple noise models. Tank experiments are performed to collect 3D reflection data from physical models, using a pulse-like source and a Vibroseis simulating sweep source. The sign-bit version of the Vibroseis- simulating data is correlated, migrated, and compared with the 16-bit Vibroseis data and the pulse-echo data.


AGL814

Abstract

In this research, interpretations based on theoretical and physical modeling data are given in the hope that they can be useful to the seismic interpreter for discerning pitfalls in real data. Recognition of these pitfalls could be an additional aid in the area of seismic interpretation. As for the theoretical modeling, several interpretational pitfalls were identified when a systematic analysis was carried out with respect to three basic geological structures: basins, domes and partial reflectors. The pitfalls identified include: apparent pinchouts and grabens which were related to the profile line direction; extra reflection layers related to the depth of the model and the areal size of the structure; cross-stratifications related to the profile line direction and the areal size of the structure; faults or extra events related to the processing flow; apparent ambient noise related to structural dip change; etc. As for physical modeling, both the lateral and vertical velocity variations in a 3-D environment were evaluated and several pitfalls were identified. These pitfalls include: a dim spot which was related to an overlying high-velocity lens; a bright spot related to an overlying low velocity lens; an apparent velocity pullup where actually a velocity pushdown should be observed; a low frequency disturbed zone under the lens having a high velocity contrast; the thick lens effect which distorted the appearance of the true structure; the wave conversion within sharply curved 3-D structures which is yet an unsolved problem of converted wave; ghost events which result from wavelet processing; etc. Also in this research, three different velocity analysis algorithms were developed and evaluated for areally gathered seismic data. The first velocity algorithm was designed for data gathered by closely spaced conventional CDP lines. An optimum stacking velocity along with the apparent dip were obtained. The second velocity algorithm was designed for areal common-mid-point data. A migration velocity along with strike and dip were obtained. The third velocity algorithm was designed for multi-midpoint data such as would be gathered in a crooked-line survey. An optimum stacking velocity as a function of dip and strike and a final migration velocity were obtained. These velocity algorithms offered a new processing flow which was applied on the crooked-line data using the output parameters derived from the third velocity algorithm. A satisfactory depth reconstruction was obtained and it proved that the processing flow and velocity algorithm were correct.


AGL815

Abstract

The problem of determining the proper subsurface velocity model has been an area of active concern since the inception of acoustic remote sensing methods. The co-problem of determination of structural parameters, strike and dip, has also generated a great deal of research. The relatively recent development of computerized acoustic imaging techniques has placed an even greater emphasis on the need for accurate models of the subsurface velocity structure. Once one has recognized the complementary nature of the velocity analysis and optimal migration problems, which will be demonstrated, a number of physically obvious solutions become apparent. Through the use of general techniques of image formation, two algorithms that yield both optimum velocity for migration, and strike and dip parameters will be presented. The formation and evaluation of acoustic images is of prime importance to the methods employed. The particular images of interest are the source image for field gathers and the common reflection point for common midpoint gathers. Through the utilization of approximate forms of the Rayleigh-Sommerfeld Diffraction formula, acoustic images for these types of recordings are focused for a range of parameters (velocity, dip, and strike), the image of highest intensity corresponding to the best bit set of trial parameters. These procedures are undertaken in the space-temporal frequency domain. Results from analyses on theoretical and physical model data are used to demonstrate the effectiveness of the techniques. These are presented as a series of parameter spectra for each of the search variables; velocity, strike, and dip. The accuracy and reliability of the results, as expected, were seen to depend on the range of offset and number of traces in the aperture, the size of the aperture with respect to image depth, and the grid density of the analysis parameters. The successful extraction of the actual model parameters involved in the tests performed has demonstrated the effectiveness of the methods employed.


AGL816

Abstract

Many of the existing seismic velocity estimation techniques use common depth point (CDP) data, and are based on a horizontally layered media assumption. These techniques have a degraded performance in areas of complex geology. The primary causes of such a degradation are the effects of structure, diffraction effects, and 3-D sideswipe energy that gets superimposed on the CDP data. The geometrical effects on the velocity needed to stack CDP data over a curved reflector were studied using a mathematical surface of second degree in x and y. The velocities were found to vary as a function of the profile direction, as a function of the depth of the reflector, and as a function of the principal radii of curvature. To overcome the geometrical effects, a 3-D stacking velocity for an arbitrary 3-D areal coverage was defined based on the first of two-step approximation to 3-D migration. The method of velocity analysis eliminates many of the difficulties associated with a 3-D subsurface. This is so because it basically extracts a true 2-D profile (without sideswipe) from 3-D multi-fold data and computes the corresponding stacking velocity. The velocity estimate obtained is still dependent on the dip and curvature of the reflector in the plane of the profile, although the cross-dip and cross-curvature effects have been eliminated. The analysis was demonstrated using physical model data obtained in a 3-D tank experiment. To overcome the still persistent effects, an algorithm based on a complete 3-D migration, without any approximations, was developed. In the conventional use of migration for velocity analysis, each input trace of N samples, is migrated for each of M constant velocity functions requiring about N x M moveout calculations. The algorithm used here, transforms the input traces into a logarithmic space and scans for constructive interference at a number of depth locations along the proposed axis of a well. From the formulation, a constant shift is calculated for a particular trace, for each depth scanned. This reduces the number of calculations to about N. The algorithm was tested on a number of computer generated 3-D model data and also on a 3-D physical model data. It was found that by having the data cover an area that includes the normal incidence point of a reflector, a velocity estimate was obtained which was independent of structure. The method also worked where random noise was superimposed on the data with a signal-to-noise ratio of about 1:300. It also worked when the transformed data was converted to sign bit only.


AGL817

Abstract

Three-dimensional (3D) migration applied to 3D seismic data provides a reliable image of the subsurface and excludes misleading effects of sidewipe events which occur when complicated 3D subsurface structures are explored by conventional 2D methods. Several types of 3D migration methods have been developed at the Allied Geophysical Laboratories at the University of Houston. This thesis aims at investigating another way to migrate 3D seismic data. Integration of the input data over diffraction surfaces is done in two steps, first by integration at constant time and then over a range of time. The values of the input data on the surfaces are obtained from the input samples by trigonometric interpolation. For constant velocity laterally the contribution of each input time slice to each output time slice is obtained by convolution with a space invariant 2D operator constructed from the interpolation weights. The convolution is implemented by multiplication in the Fourier domain. Results for synthetic and scaled physical model data are compared with results using well-establishing 3D migration programs. It is concluded that a tapered weighting function over the diffraction surface is necessary to avoid false events caused by a sharp truncation of the integration. The Fortran program for a VAX 11/780 is included.


AGL818

Abstract

In the past, the Kirchhoff method has been used both in a forward mode to generate synthetic seismic sections and in a backward mode to migrate field data. This work addresses the practical implementation of either mode through a unified treatment of Kirchhoff´s integral solution of the acoustic wave equation. Laboratory- collected data have played an important part in this analysis since solutions for practical forward modeling and migration problems require extensive numerical calculations and these must be verified. These data have confirmed several theoretical considerations which show how problems in one mode of the Kirchhoff method are solved with the other mode. For example, downward continuation of surface-recorded wavefields for migration depends heavily on several features of the integration aperture, such as aperture size and shape, sampling, and weight functions, and these are readily related to forward modeling techniques. Migration noises in the form of ghosts and halos are easily evaluated with forward modeling, and hence, modeling results serve as a basis for their removal. Theoretical considerations for forward modeling lead to a set of design criteria for migration. On the other hand, a problem inherent in forward modeling is the proper selection of Green´s functions, and these are easily evaluated through migration techniques using image positions of sources and receivers. Horizontal resolution in migration is related to the Rayleigh criterion of optics, and at the same time it is related to scattering of small thin right-circular cylinders in forward modeling. Theoretical and physical model studies have been conducted for several new field acquisition and migration display schemes with results that have been confirmed with laboratory measurements.


AGL819

Abstract

One of the least investigated and most tedious and error-prone tasks associated with computer graphics is producing a description of a complex object in a form suitable for manipulation by a graphics system. The information required for this description is generally of two types: (1) 3-D coordinates of certain points, and (2) some organization of these points into sets describing portions of the surface, usually as polygonal faces. This is accomplished in two distinct stages, one for each of the two types of information, or by alternating between the two. Several means of automating the first stage, the collection of coordinates, have been suggested. This discussion centers on the second stage, that of generating polygonal descriptions of the surface. Several existing object description methods are described and their benefits and limitations discussed. A very general algorithm, assuming only knowledge of the point co-ordinates is presented. This algorithm can be modified to use any one of a large class of cost functions in choosing from among the many topologically legitimate surfaces possible. This algorithm is analyzed for its worst case execution speed using standard techniques. A discussion of how to evaluate the quality of the approximations generated by this algorithm (or any other for the same purpose) is pursued, resulting in a metric and two algorithms useful in computing it. One algorithm computes the intersection (and symmetric difference) of two polyhedra. The other algorithm computes the volume of an arbitrary polyhedron (or set of polyhedra). Finally, several extensions to the main algorithm are presented. The theme of these extensions is the incorporation of additional knowledge which may be available.


AGL8110

Abstract

The forward modeling technique developed by Trorey in 1970 can be cast in the form of a matrix equation that linearly relates subsurface reflection coefficients to CDP (Common Depth Point) data. The proposed inversion attempts to solve these matrix equations for the unknown reflection coefficients. The complete inversion procedure can be described in five steps: I) divide the subsurface into a rectangular grid and then guess an initial model by assigning reflection coefficients at the grid points; II) calculate the weighting of each grid element with respect to each CDP position; III) forward construct the seismogram based on the initial model; IV) subtract this calculated result from the corresponding observed data, resulting in the so called error vector; V) solve a system of equations by minimizing the error vector in a least-squares sense while subject to the constraints that the distance of the result from the true model is fixed. The result can be improved iteratively by repeating the procedure from III to V. In the processing, a 2-D operation block is chosen which, depending on the complexity of the subsurface, should have the proper size. This size must be large enough to cover the necessary diffraction and small enough to be computationally efficient. The whole seismic section is covered by these blocks with some overlapping on the edges. The most time consuming step in the processing is to calculate the inverse operator for the chosen operation block. This inverse operator changes slowly in both vertical and horizontal direction for a regular subsurface; thus, the processing time can be reduced when a matrix factorization technique is used. The proposed inversion algorithm has been tested with a set of synthetic traces, physical tank data, and field data. Of particular note in this paper is that a forward construction and backward reconstruction pair are explicitly presented.


AGL801

Abstract

The seismic response of several coal depositional environments are examined by two sets of physical models. First, meandering-stream models provide tools for channel location by seismic methods, and they also document interpretational pitfalls. Undisturbed coal is discerned from channel eroded coal by: (1) the presence of 2-D and 3-D foci; (2) velocity induced pull-up or sag of the reflectors underlying the channels; and (3) amplitude analysis. However, the 2-D and 3-D foci are absent when an interface is placed between the channel walls and their respective centers of curvature. Also, if the velocity of the channel-fill is higher than the coal´s, the velocity pull-up displays a diffraction-like appearance, due to the channel´s refractive properties. Second, progradational delta coal models emphasize the effects of small, thin coal bodies upon the seismic response of an underlying, thick coal seam. Velocity pull-up, strong diffraction events and dim-spots from each overlying coal prevents mapping of the thick coal seam. 2-D studies on transitional coal-to-sand contacts and vertically-thinning beds highlight the subtle characteristics of certain coal depositional environments, by demonstrating that not only does a thinning coal bed have an amplitude tuning at (lambda)/4, but it also has a characteristic frequency response. The interrelationship of amplitude and frequency provides both an estimate of thickness and a clue as to the style of the coal´s vertical contact. The 2-D studies are extended to 3-D, to provide an estimate of total coal volume from reflection data. The thin-bed frequency and amplitude behavior is the same for spatial discs which are a fraction of a Fresnel disc. The measurable waveform for thin beds results from interference of reflections from the top and base, while for small bodies, it results from interference of the reflection and coherent edge diffraction. The tuned waveform, for both cases, is 90 degrees out of phase with the input wavelet. For coal bodies which are both thin and small, the amplitude still tunes at the characteristic fraction of a wavelength; however, the wavelength is defined by the spatially-altered frequency, not the input frequency. For this case, the tuned waveform is 180 degrees out of phase with the input wavelet.


AGL802

Abstract

A simple 2-D model for the acoustic impedance structure of the earth is proposed to model and migrate seismic data using a hybrid Kirchhoff-Trorey approach. The new technique is based upon the summation of fields from linear diffraction sources over space and time to obtain the total acoustic field (analogous to Kirchhoff integral theory). The time response of the linear diffraction sources has been derived by Trorey (1970). Accurate seismic responses of known acoustic impedance models of the earth can be simulated using this new theory. The inverse procedure (or migration) while conceptually simple to consider in the context of the 2-D earth model, is not a stable algorithm due to numerical error propagation problems. A discussion of the sources of these numerical errors is presented.


AGL803

Abstract

The sedimentary section in the southwestern abyssal Gulf of Mexico (7 to 10 km thick) is divided into 8 major depositional sequences. The sequence boundaries represent widespread unconformities or major changes in regional depositional conditions. These depositional sequences provide a framework for reconstructing the depositional history of the area. The pre-middle Cretaceous sedimentary section consists of detrital clastic sediments of varied provenance, deposited after the formation of the Gulf (probably early Mesozoic). However, the post-middle Cretaceous sediments were deposited in deep marine environments and essentially consists of a combination of pelagic and hemipelagic deposits and turbidites derived from the continental terraces to the west along eastern Mexico. The area experienced several major transgressions and regressions as evidenced by the presence of well-developed relict submarine channels and growth of submarine fan complexes. The youngest depositional sequence (Pleistocene) displays dune-like features with wavelength of 2-4 km and thickness of 10-50 m.


AGL791

Abstract

This thesis deals with the research work related to a consortium project on 3-D Seismic Data Acquisition, Processing, and Interpretation using a physical model. The research work encompassed three major areas. The first was the study of the candidate materials for the model construction. A number of materials were tested for their physical and ultrasonic characteristics. The second area was the ultrasonic characteristics. The second areas was the ultrasonic characterization of various avail-able transducers and the plotting of their pulse-mode beam patterns. These transducers were used as sources to generate sound signals and/or as receivers to collect the returned signals from the model surface. The data so obtained could be utilized, when processed, for the interpretation of the geological structure, or for making a hologram of the geological structure. The third area was the design of an ultrasonic receiver which would meet all or most of a set of desired characteristics in order to obtain the seismic data from the model. A waveguide type ultrasonic receiver was designed and constructed to meet these objectives. The waveguide receiver was characterized and its sensitivity was compared with other available receivers.


AGL792

Abstract

Wave-Vector Diversity is a new technique of imaging pioneered by Dr. N.H. Farhat. This involves a Fourier Optics approach to imaging, where the frequency sweep and the relative orientations of the sources and receivers produce diversity in the wave vector. This is also a new analytical approach to imaging. The super resolving features found in mammals such as bottle nosed dolphins, whales and bats, have been the prime motivation in the development of the theory. The theory which had been developed for a general case with a continuous frequency sweep, has been extended in this thesis, to a special case of ZSRO (zero-source-receiver-offset) imaging with a broad band pulse. It has been shown that for the use of FFT (Fast Fourier Transform) in reconstruction, the interpolation could be done in the temporal frequency spectra of traces instead of spatial or spatial frequency domains. The advantages of this type of interpolation have been discussed. Other special features and limitations of this new technique of imaging are also discussed towards the end of this thesis. Synthetic data analysis has been done for the case of ZSRO imaging with WVD (Wave-Vector Diversity) and the results are explained. Suggestions for future work are made.


AGL761

Abstract

The extraction of elastic parameters from seismic reflected data with the state-of-the-art indicates little success. The specific method tried was the inversion of the seismic reflection amplitude curve with respect to offset angle to yield the elastic parameters on either side of a plane reflection boundary. By numerically evaluating the partial derivatives of the reflection coefficient equation with respect to the elastic parameters, almost all the problems found could be explained. In fact, many of the conclusions by earlier investigators of the reflection coefficient curve such as Koefoed (1955) can also be easily explained by the partial derivatives. The inversion of the reflection coefficient curve for P-waves, when the acoustic impedance ratio is known, is not unique for incidence angles below the critical. This is because the two Poisson´s ratios approximately cancel each other´s effect on the reflection coefficient. However, when reflection amplitudes above and below the critical angle are inverted, then a unique solution of the problem is possible, but is highly sensitive to error. Once again, the acoustic impedance ratio is known. For SH-waves, the inversion of the reflection coefficient curve was unique, for the cases studied. A SH-error analysis indicates the inversion is more stable when the acoustic impedance ratio is known. Among the different propagation factors affecting the amplitude curve, and consequently the inversion problem, the most important factor is usually the geophone array.


AGL762

Abstract

In the stochastic deconvolution process, the assumption of a random reflectivity function can be replaced by the NMO curve and a CDP gather record. With this information, the seismic wavelet can be compressed. This compression method operates in a manner opposite to the NMO correction stretch. Shaping filters are interactively computed either in the time domain or in the frequency domain which subsequently compress the seismic wavelet. Based on the principles of the wavelet compression technique, the seismic wavelet can be extracted without making any assumption about the shape of the seismic wavelet. From an initial estimate of the seismic wavelet, the method computes interactively new estimations in order to minimize the energy error between the predicted seismic trace at various offsets and the field traces at the same offsets. The NMO-curve provides the information to predict the far traces from the near traces. Stability problems limit the process to wide band source signatures.



Wavelet Extraction Parameters of Homomorphic Deconvolution

Abstract

Homomorphic extraction of the seismic wavelet has been reported in the literature where the assumption that the wavelet cepstrum and reflectivity function cepstrum are separable by linear filtering has been made. This assumption however restricts the application of the technique to simple relectivity models. Thus it is desirable to design homomorphic wavelet extraction techniques that are not based on this assumption; this has been done by using two statistical methods.
    The first method uses the cepstrum of the seismic trace autocorrelation to estimate the cepstrum of the minimum-delay wavelet equivalent. If the reflectivity function is minimum-delay then mixed-delay wavelets can also be estimated .
    The second method involves teh cepstral averaging of seismic trace windows. It is shown that this procedure cancels the cepstrum of the reflectivity function and recovers the wavelet cepstrum. Both methods were tested with synthetic seismic traces.