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    • 专利摘要:
    Seismic Acquisition Methods and to minimize the Output Amplitude During Seismic Acquisition and Seismic System. The maximum power of a seismic source arrangement (110) can be reduced by activating the individual seismic sources (112) in these seismic source arrangements in a pattern, that is, extended in time instead of through the conventional simultaneous activation currently employed from a large number of individual seismic sources. The methods are described which consider triggering data with standardized sources and can use sparse inversion method to create data with approximately the same image quality as that of conventional sources. In this way the maximum impulse power of a seismic source arrangement can be reduced by an amplitude factor of about 10 in the examples shown here, corresponding to a reduction of about 20db while maintaining virtually the same quality of the seismic image. . The described methods can be used in combination with any simultaneous delivery technique. In addition, the described methods can be used with a plurality of font arrangements.
    公开号:BR112013014328B1
    申请号:R112013014328-2
    申请日:2011-12-09
    公开日:2021-01-19
    发明作者:Allan A. Ross；Raymond Lee Abma
    申请人:Bp Corporation North America Inc.；
    IPC主号:
    专利说明:

    DESCRIPTIVE REPORT REFERENCE RELATED REQUESTS
    [0001] This order claims the benefit of United States Provisional Order Serial No. 61 / 421.274, filed on 9th of 2010, and United States Provisional Order Serial No. 61 / 503,407, filed on June 30, 2011, and are incorporated herein by reference in their entirety for all purposes. DECLARATION REGARDING FEDERALLY SPONSORED DEVELOPMENT OR RESEARCH
    [0002] Not applicable. BACKGROUND Field of the Invention
    [0003] This invention generally refers to the field of geophysical exploration. More specifically, the invention relates to a standardized method of seismic firing for marine applications. Background of the Invention
    [0004] In marine seismic surveys, a source of seismic energy is used to generate seismic energy in the form of waves or acoustic pulses in a body of water such as a lake or the ocean. Seismic energy travels downward in the water, through the bottom of the water, and through the underground formations underlying the water base. Part of the energy that passes through the underground formations underlying the water base is reflected above them at the limits of acoustic impedance in the Earth's formations. Upward path energy is detected by sensors such as hydrophones towed on one or more streamer cables arranged close to the water surface, or by sensors arranged on cables along the bottom of the water. The sensors convert the detected energy to electrical or optical signals. The electrical or optical signals are then conditioned and interpreted to provide information both for the composition and the structure of the Earth's various underground formations. Such information is used particularly to determine the possibility that such Earth formations may contain mineral deposits such as hydrocarbons.
    [0005] Several different types of seismic energy sources have been used in the past to produce seismic energy in a manner required in marine seismic surveys. For example, explosives were used as a source of marine seismic energy. Another type of marine seismic energy source, called a gas gun, includes detonating fuel gases in a chamber and then expelling the resulting gas charge in the water to produce the seismic energy. In the acquisition of marine seismic data, an air gun is the most used seismic or acoustic source. In such air guns the sound is generated by allowing the high pressure air (100-200 atmospheres) to escape through the orifice openings in the air gun.
    [0006] A single air gun produces a systemic pulse having acoustic energy related to a complex pressure interaction between the air bubble and the water that causes the bubbles to oscillate when they rise to the surface of the water. Such an interaction can produce external bursts of seismic energy following the initial burst of energy. The amplitude and periodicity of these external bursts generated by the bubbles depend, among other factors, on the depth of the gun in the water and the size of the pressurized air chamber in the gun. As such, it is common to use an arrangement of airguns having several different chamber sizes, and to fire such pistols simultaneously. Such firing of an air gun array provides several advantages over firing a single air gun. First, the total amount of energy being transmitted into the Earth's subsoil for each seismic “shot” is increased. In addition, the different chamber sizes for the various pistols will produce different bubble responses, causing the bubble responses to tend to cancel each other out. The directivity of the energy source to the water base can be improved, because except directly below the source matrix, some frequencies in the seismic energy will be attenuated by the spatial distribution of the pistols in the layout. In this way, conventional air gun arrangements simultaneously discharge all air guns in the arrangement. This generates a strong signal with a more impulsive signal than any single air gun.
    [0007] The design of conventional marine air gun arrangements is generally fixed for the duration of a seismic survey. While some attributes of the air gun arrangement can be changed in processing, more processing flexibility in forming the source signal is desirable. Conventional air gun arrangements generate a strong impulsive signal (see, Figure 5). In addition to generating a seismic signal underground, the impulse can create noise interference with other seismic surveys, the mechanical vibration of the towing vessel's hull and the fatigue of the crew.
    [0008] Consequently, there is a need for a method and system for seismic acquisition that will allow the reconstruction of a seismic source arrangement in processing allowing for more flexibility than a conventional fixed air gun arrangement, while maintaining the signal strength. BRIEF SUMMARY
    [0009] These and other needs in the art are addressed in a modality by a seismic acquisition method comprising individually triggering the seismic sources within a seismic source arrangement over time. The motivation behind the presented methods is to reduce the impact on marine mammals, reducing the acoustic output of seismic sources. The maximum output of an arrangement can be reduced by firing the individual seismic sources (for example, air guns) in a pattern that extends over time instead of the conventional simultaneous firing currently employed from a large number of individual seismic sources. Individually by triggering the seismic sources within the array over time, the range of the array can be reduced. The methods are described which consider the seismic data acquired from the random firing patterns, and use a sparse inversion method to create data with approximately the same image quality as that of conventional sources. In this way the output of a seismic source arrangement can be reduced by an amplitude factor of about 10 in the examples shown here, corresponding to a reduction of about 20 dB while maintaining virtually the same quality of seismic image. The methods described here are contrary to conventional techniques because typically other seismic methods seek to maximize the amplitude to increase the quality of the seismic image. In contrast, the methods seek to minimize the amplitude, while still maintaining the quality of the seismic image through innovative processing techniques. Standardized seismic shots can result in lower maximum sound pressure levels than conventional marine air gun arrangements while maintaining approximately the same energy.
    [0010] In one embodiment, a seismic acquisition method comprises the positioning of a first seismic source arrangement comprising a plurality of seismic sources over a seismic survey region, the seismic source arrangement generating an output amplitude. The method also comprises activating the first seismic source arrangement according to one of a plurality of different trigger patterns, the trigger patterns comprising a plurality of different time intervals between the activation of each seismic source in the first seismic source arrangement. Each trigger pattern is optimized to minimize the output amplitude. The method also comprises recording a plurality of seismic signals reflected from one or more underground formations.
    [0011] In one embodiment, a method for minimizing the output amplitude during seismic acquisition comprises positioning a seismic source arrangement comprising a plurality of seismic sources over a seismic survey region, the seismic source arrangement generating an output amplitude. In addition, the method comprises generating one or more trigger patterns. Each firing pattern comprises a plurality of time intervals between the firing of each seismic source in the seismic source arrangement. The time intervals are calculated according to an algorithm to minimize the amplitude of the output. The method also comprises activating the seismic sources within the seismic source arrangement according to one or more trigger patterns to minimize the output amplitude of the seismic source arrangement.
    [0012] In yet another embodiment, a seismic system comprises a first seismic source arrangement comprising a plurality of impulsive seismic sources. The seismic source arrangement generates an output comprising an amplitude. The system also comprises a controller operatively coupled to the seismic source arrangement. The controller is programmed to activate the seismic sources according to one of a plurality of trip patterns. Each trigger pattern is optimized to reduce the output amplitude
    [0013] The foregoing has very broadly defined the technical characteristics and advantages of the invention so that the detailed description of the invention that follows can be better understood. Additional features and advantages of the invention will be described below which constitute the purpose of the Claims of the invention. It should be considered by those skilled in the art that the specific concept and modalities described can easily be used as a basis for modifying or designating other structures to accomplish the same purposes as the invention. It should also be taken into account by those skilled in the art that such equivalent constructions do not depart from the spirit and scope of the invention as set out in the appended Claims. BRIEF DESCRIPTION OF THE DRAWINGS
    [0014] For a detailed description of the preferred embodiments of the invention, reference will now be made to the accompanying drawings.
    [0015] Figure 1 illustrates a modality of the seismic acquisition method;
    [0016] Figure 2 illustrates a modality of a seismic system to implement the described method;
    [0017] Figure 3 illustrates the signatures of the 10 air guns used to build the layout with 33 guns. The volumes are 40, 70, 80, 100, 120, 140, 175, 200, 250, and 350 cubic inches, which can be used with the method modalities. (time scale is in the number of samples of 2 msec.);
    [0018] Figure 4 illustrates the time signatures of three standardized shots, each consisting of 33 shots from a single pistol. (The time scale is the number of samples of 2 msec.);
    [0019] Figure 5 illustrates the signature of a conventional air gun using the 33-gun layout. (The time scale is the number of 2 ms sample intervals);
    [0020] Figure 6 illustrates a modality of the seismic acquisition method with continuous firing patterns;
    [0021] Figure 7 illustrates the impulse response of standard air gun arrangements.
    [0022] Figure 8 illustrates the impulse response of the air gun arrangement calculated after the sparse inversion;
    [0023] Figure 9 illustrates the impulse response of a standard air gun arrangement;
    [0024] Figure 10 illustrates the difference between the data in Figures 8 and 9 showing the reconstruction error;
    [0025] Figure 11 illustrates the acquisition of a standardized shot in a 3D synthetic;
    [0026] Figure 12 illustrates the calculated data derived from the 3D data from standardized source in Figure 8;
    [0027] Figure 13 illustrates the 3D data conventionally acquired;
    [0028] Figure 14 illustrates the difference between Figures 9 and 10 showing the reconstruction error;
    [0029] Figure 15 illustrates the impulse response of the 9 standardized shots used to generate Figure 8. (Horizontal axis is the number of samples of 2 msec);
    [0030] Figure 16 illustrates the spectra of the nine standardized shots shown in Figure 12 with the spectra of the desired signatures observed in Figure 2 shown as the base spectrum;
    [0031] Figure 17 illustrates the data spectra resulting from the inversion of standardized data and 3D data conventionally acquired;
    [0032] Figure 18 illustrates standardized trigger data for a 2D data set;
    [0033] Figure 19 illustrates the calculated data from the 2D standardized trigger data seen in Figure 15;
    [0034] Figure 20 illustrates data conventionally acquired from the 2D data set;
    [0035] Figure 21 illustrates the difference between 2D data sets calculated and conventionally acquired;
    [0036] Figure 22 illustrates the data spectra resulting from the inversion of standardized data and 2D data conventionally acquired;
    [0037] Figure 23 illustrates a modality of a computer system for use with the described methods. NOTATION AND NOMENCLATURE
    [0038] Certain terms are used throughout the following description and Claims to refer to the components of the particular system. This document is not intended to distinguish between components that differ in name, however, not in function.
    [0039] In the following description and in the Claims, the terms "including" and "comprising" are used in an open manner, and should therefore be interpreted to mean "including, but not limited to ...". In addition, the term "coupled" or "coupled" is intended to mean a direct or indirect connection. Thus, if a first device is coupled to a second device, that connection can be through a direct connection, or through an indirect connection via other devices and connections.
    [0040] As used here, “continuous record” can refer to the recording of seismic data through the time intervals that occur between conventional seismic records. A single continuous record is as long as many conventional seismic records and thus contains the seismic arrivals generated by the start of many seismic sources. A continuous record can take up to many hours in duration (even in a geological environment where seismic records need only be a few seconds) and may, however, not need to be carved into numerous shorter records, contiguous with each other, or if overlapping, or even discarding certain time windows of the continuous record.
    [0041] As used here, an “array” or “array of seismic source” can refer to multiple or a plurality of individually spaced or grouped individual seismic sources, with the effect of acting as a single seismic source.
    [0042] As used here, "independent simultaneous supply" can refer to multiple or a plurality of seismic sources or source arrangements activated independently with no or very little coordination between them.
    [0043] As used here, “trigger pattern” or “standardized source” can synonymously refer to a seismic acquisition method, where instead of discharging all sources in a seismic source arrangement substantially simultaneously, seismic sources are discharged in a programmed, random or pseudo-random pattern with delays or intervals between each source activation. Some sources can burn simultaneously, such as "source clusters" (for example, 2, 3, or 4 sources of identical volume closely grouped), or in cases where a specific objective was sought while simultaneously firing some of the various sources in the array .
    [0044] As used here, "non-continuous recording" can refer to the practice in seismic exploration of specifying the duration of a seismic record for the time window required to record all seismic waves of interest from the beginning of a seismic source. Typically, the start of the record is synchronized with the start of the seismic source and ends with the arrival at the seismic sensors of the last seismic arrivals that are of interest (usually deeper and more distant) in the seismic exploration of the particular geological environment (in addition to a surplus to allow for miscalculation, data processing, etc.). The repetition interval of the sources is generally longer than the duration of the recording, and the intervals between the records represent time of the unregistered wall clock; the time interval also allows the residual energy of the previous shot to be attenuated.
    [0045] As used here, “auto simultaneous supply” can refer to repeatedly activating or starting a single seismic source or source arrangement so that the triggering records obtained overlap in time with the previous triggering record or the recording of next shot, or both. This is the method for firing multiple shots from a single pistol or pistol array where the expected stroke length is greater than the time between shots. For example, if 10mseconds are desired, shots can be taken every 5 seconds, and overlapping shots are separated in processing.
    [0046] As used here, "simultaneous supply technique" can refer to any seismic supply or acquisition method where more than one seismic source or source arrangements are burned or activated in parallel. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
    [0047] Figure 1 schematically illustrates a modality of a seismic acquisition method. In general, the method consists of burning individual seismic sources 112 within an array 110 of such sources according to one of a plurality of different trigger patterns 201, 202. The trigger patterns 201, 202 shown in Figure 1 are for illustrative purposes only and should not be construed as limiting in any way. As shown in Figure 1, the seismic source arrangement 110 includes a plurality of individual seismic sources, where S1 through S8 represent each seismic source 112 within arrangement 110. Although seismic sources S1 through S8 are shown as air guns, as will be described in greater detail below, any number, volume and type of seismic sources 112 can be included in an arrangement 110. As an example, Figure 1 shows an arrangement 110 where S1 and S2 represent the same large-volume air gun, S3 to S5 are the same medium-volume air guns, and S6 to S8 are the same small-volume air guns.
    [0048] Trigger patterns 201, 202 can be previously generated and loaded into a controller, which controls the burning of seismic sources or can be generated in real time by the controller itself. Trigger patterns generally comprise a set of random delays or time intervals between firing or activating each seismic source 112. In addition, each trigger pattern is optimized to minimize the output amplitude. In each trigger pattern, each seismic source 112 can burn at different times or alternatively, some seismic sources 112 in arrangement 110 can burn at the same time. An algorithm or program can be used to generate the optimized random trigger patterns within certain limits, which are described in more detail below. Seismic signals acquired from these firing patterns or standardized firing can be processed by any method known to those of skill in the art. In one embodiment, as shown in Figure 1, there may be a time delay, tD, between the trigger patterns, 201, 202. The time delay, tD, can be any suitable nonzero time period. In one embodiment, the time delay, to, can be varied or can remain consistent. The time delay can be varied randomly, pseudo-randomly, or according to a pattern. In addition, although Figure 1 only shows a trigger pattern 201 followed by a second trigger pattern 202, in practice, the subsequent different trigger patterns are successfully initiated or activated many times during a full seismic acquisition program. However, in some modalities, it is anticipated that the same trigger pattern can be used with varying time delays between the same trigger pattern.
    [0049] Figure 2 illustrates a modality of a seismic system 100 that can be used to implement the methods described here. The seismic system can include the seismic arrangement 110, the seismic sources 112, a seismic vessel 120 towing the arrangement 110, and a controller 130 for controlling the timing of the seismic sources. The seismic vessel 120 can position the seismic arrangement 110 over a desired seismic survey region of the earth. Seismic sources 112 can be any seismic source known to those of skill in the art. Controller 130 may be preloaded with trigger patterns or routines for arrangement 110. Alternatively, controller 130 may have a processor that determines trigger patterns in real time. Controller 130 communicates with and controls the burning of seismic sources 112. Controller 130 may be located on vessel 120 or located on arrangement 110 underwater. Although Figure 2 describes a marine seismic system 100, it is expected that the one described
    [0050] As already mentioned, seismic sources can be any seismic source known to those with experience in the art. In one embodiment, the seismic source can be a source that repeatedly emits a single pulse of energy when opposed to a continuous sweep of energy. As used here, such seismic sources are referred to as impulsive seismic sources. More particularly, examples of suitable impulsive seismic sources may include, without limitation, air guns, gas injectors, water guns, charges, explosives, combinations thereof, and the like. While method modalities are primarily directed towards impulsive sources, other more impulsive or non-impulsive sources can also be employed, such as without limitation, vibrators, resonators, sirens, and combinations thereof.
    [0051] Figure 3 shows the individual signatures of a typical arrangement of impulsive seismic sources (for example, air guns), which can be used in conjunction with the described methods. In addition, although the methods described here are primarily intended for marine applications, they can also be applicable in land-based seismic operations. Figure 5 describes an example of signing an impulsive seismic source arrangement comprising air guns. In particular, Figure 3 shows an exemplary embodiment of an air gun arrangement with 10 different volumes of air guns. In this embodiment, an array of 33 pistols can include 4 pistols of 40 cubic inches each, 2 pistols of 70 cubic inches each, 3 pistols of 80 cubic inches each, 8 pistols of 100 cubic inches each, 4 pistols of 120 cubic inches each, 4 pistols of 140 cubic inches each, 2 pistols of 175 cubic inches each, 2 pistols of 200 cubic inches each, 2 pistols of 250 cubic inches each, and 2 pistols of 350 cubic inches each. However, any suitable arrangement of marine seismic sources can be used in conjunction with the modalities of the methods described. In addition, in modes using air guns, air guns can be of any suitable volume. In particular, air guns can have volumes ranging from about 1 cubic inch to about 1,000 cubic inches, alternatively from about 40 cubic inches to about 350 cubic inches, alternatively from about 80 cubic inches to about 500 inches cubic. In one embodiment, at least two of the seismic sources generate energy in different frequency ranges or generate different output amplitudes. In modes with air gun arrangements, this means that at least two of the air guns have different volumes between them. However, method modalities can also be used with air gun layouts all having the same volume. In addition, any number of seismic sources can be used in the arrangement.
    [0052] The maximum amplitude of the seismic source arrangement can generally be reduced by about a tenth of that of the conventional signature (ie, simultaneous firing) or about a 20 dB reduction in the examples shown here. However, the maximum amplitude can be reduced by any desired amount. The maximum amplitude of the standardized seismic source signature is approximately that of the largest source in the arrangement.
    [0053] There are several parameters in the generation of a trigger pattern. In particular, there is, without limitation, the duration of the firing pattern which is the time duration from burning the first seismic source to burning the last seismic source, the order in which the sources burn, and the time intervals between fires. and the desired breadth of any of the standardized individual arrangements. It is taken into account that any suitable value can be used for these parameters. In the embodiments, the duration of the firing pattern can vary from about 1 second to about 4 seconds, alternatively from about 7 seconds to about 2 seconds, alternatively from about 3 seconds to about 10 seconds. The time interval between burns can vary from about 50 milliseconds to about 500 milliseconds, alternatively from about 150 milliseconds to about 250 milliseconds, alternatively from about 250 milliseconds to about 1 second.
    [0054] Preferably, the patterns are different with respect to each other so that the notches in the adjacent standardized shot spectra do not overlap significantly. Sufficient patterns must be created to allow significant randomness in adjacent patterns. That is, the sequential firing patterns can all be different from each other. However, in some modalities, some or all of the patterns may be the same. Any number of trigger patterns can be generated and used with the described methods. This number can be limited by the number of sources in the arrangement and also in the restrictions and parameters chosen for the triggering patterns.
    [0055] The duration of time that the shots are burned is controlled by the limits in the maximum desired amplitude in each firing pattern signature and the required firing resolution. If a firing time duration is too short, the maximum amplitude of single pistol shots will tend to stack constructively, and the maximum amplitude of this pattern may not be reduced to much less than the conventional air gun arrangement. If the duration of the burning time pattern is too long, the rebuilt shot is spotted in space due to the vessel's course. The order of the pistol shots and the time between them can be used to isolate the larger pistols in the standard sequence to minimize the stacking of single gun outputs and prevent the amplitude of the standard shot from being minimized.
    [0056] The sequencing of the pistols in any individual source pattern is related to the notches in the spectra of the individual patterns. The notches in the spectra should cover as many different frequency bands as possible. Since the sequencing of individual sources in any given pattern also controls the maximum amplitude of any individual pattern, the burning time for each source must be carefully calculated and controlled.
    [0057] The combination of inversion for standardized trips and inversion for simultaneous trip separation opens up the possibility of alternative acquisition source methods. For example, in one embodiment, as shown in Figure 6, the method can include continuous shooting, which can also be referred to as "continuous standard shooting" or "continuous shooting patterns". In contrast, modalities that involve a time interval between triggering patterns can be referred to as discrete standardized triggering or discrete triggering patterns as shown in Figure 1. Specifically, instead of triggering a triggering pattern, having a delay, tD , and then triggering a different trigger pattern, the delay is removed and a trigger pattern is immediately followed by another trigger pattern. That is, tD will essentially be zero for standard continuous shooting. As such, in some modalities, there may be intervals of several seconds between the two firing patterns, however, it is not necessary to have one. When standardized and sequenced shots are used with a continuously varied source pattern while moving along a firing line, the firing can be divided into reconstructed shots with a large or small spatial extent. The reconstructed trigger spacing can now become a processing parameter. For shallow high-resolution images the reconstructed shot spacing can be established as small as possible. For deep image targets or in noisy areas, larger reconstructed shot spacing can be used to produce better signals. For air guns or impulsive sources, the minimum font spacing would be the current interval between shots and individual fires, although if this interval is irregular, interpolation can be used to reduce the spacing of the shot as well. Without being limited to theory, the maximum derivative reconstructed firing interval may depend on the spatial resolution required to image the desired targets.
    [0058] The standardized source method or firing pattern can be used to collapse an array of standard impulsive seismic sources into a much shorter layout by burning the impulsive seismic sources in front of the arrangement, followed by the impulsive seismic sources behind, since they occupied the same location as the impulsive seismic sources in the front when they burned. However, the seismic source arrangement can be of any length. In the modalities, the arrangement of the seismic source can vary from about 1 meter to about 100 meters in length, alternatively 5 meters to about 50 meters, alternatively from about 5 meters to about 20 meters. The pattern would continue as the last impulsive seismic sources occupied the same location as the frontal impulsive seismic sources when they burned.
    [0059] In other modalities, the firing patterns can be combined with any known suitable technique of simultaneous seismic acquisition or supply by those with experience in the technique. Examples of simultaneous seismic firing techniques include, without limitation, independent simultaneous supply, simultaneous self-supply with one or more sources / arrangements, or combinations thereof. More detailed descriptions of such techniques are described in United States Patent Applications Nos. 12 / 542,433, entitled “Method for Separating Independent Simultaneous Sources” and 12 / 851,590, entitled “Method for Separating Independent Simultaneous Sources”, incorporated herein by reference in their entirety for all purposes. In one embodiment, a single source arrangement can be used with discrete trigger patterns in conjunction with simultaneous auto supply. That is, the arrangement can activate discrete trigger patterns with a time interval between each trigger pattern. However, the delay or time interval, tD, between the trigger patterns can be such that the trigger records obtained overlap.
    [0060] In one embodiment, a plurality of arrangements can be employed where a first source arrangement is firing with firing patterns and at least a second arrangement is firing with a method of simultaneous auto supply or with a conventional firing technique (i.e. ie, the consistent or equal period or time delays between triggering patterns). The first and second arrangements can be synchronized or not synchronized with each other.
    [0061] In other modalities, firing patterns are not used. Instead, two or more seismic sources or source arrangements can be employed where each seismic source or source arrangement can each be burning with alternative techniques of simultaneous seismic firing including without limitation, independent simultaneous supply, auto simultaneous supply with one or more sources / provisions or combinations thereof.
    [0062] In another exemplary embodiment, a first arrangement may be firing with firing patterns and at least a second and third arrangement may be firing using an independent simultaneous delivery technique, where all arrangements can be synchronized, unsynchronized, random or pseudo-random with respect to one another. It is taken into account that any number of sources or source arrangement can be used where each source or source arrangement can be triggered with any combination of simultaneous acquisition or supply techniques such as without limitation, discrete trigger patterns, continuous trigger patterns , independent simultaneous supply, auto simultaneous supply, or combinations thereof. When a plurality of sources or source arrangement is used, each source or source arrangement can also combine different techniques of simultaneous triggering, if possible, such as triggering patterns in conjunction with simultaneous auto supply.
    [0063] In an exemplary embodiment, a plurality of provisions can be used where each of the provisions can be burned or activated independently of one another. In addition, each activation of one disposition may use a different trigger pattern than the other disposition. The arrangements can be coordinated / synchronized with others or not synchronized. This is a variation of independent simultaneous supply, as previously defined. In one embodiment, the plurality of arrangements may also each be triggering the continuous trigger patterns, where there is no delay or gap between the trigger patterns. In yet another embodiment, a first arrangement can fire with discrete firing patterns and a second arrangement can fire with continuous firing patterns.
    [0064] This flexibility in the firing interval or time may not be confined to the in-line direction. If the font arrangement has a cross-line extension, burning the fonts in a standardized manner in the direction of the cross-line will allow the same freedom in choosing the cross-line stroke spacing.
    [0065] Other applications of standardized shooting include, but are not limited to, noise mitigation, beam orientation, low frequency generation, encoded pulse sequences (such as miniSosie), final spatial resolution, amplitude modulation, array layout time domain sources, with both pseudo-random and standardized firing sequences. The attenuation of the phantom surface reflection can be achieved by firing a single pistol or multiple pistols, followed by the firing of the second pistol or second multiplicity of pistols under the bubble or bubble elevation of the first pistol or first multiple pistols.
    [0066] If the fountains can be prepared for rapid re-firing or redrawing, the physical dimensions of the layout can be reduced. In one embodiment, a single impulsive seismic source within the array can fire multiple times in a firing pattern.
    [0067] In yet another modality, referring again to Figure 2, the seismic source groupings 114 can be used. That is, two or more seismic sources of the same volume can be controlled as a “cluster” and easily adapted so that each cluster is fired as a single pistol in the firing pattern. More particularly, the use of an exemplary arrangement in Figure 1 as an example, sources S1 and S2 can be activated simultaneously and sources S3 through S5 can be activated simultaneously. Similarly, any number of pistols, such as a subdisposition, can be elements of the pattern and fired simultaneously. Again using the arrangement in Figure 1 as an example to illustrate the principle and without being limited, sources S1 and S8 can be activated simultaneously and sources S3 and S7 can be activated simultaneously in an exemplary trigger pattern. Sub-dispositions can include any different combination and number of seismic sources within the layout.
    [0068] In one embodiment, an algorithm or computer program can be used to produce a set of ideal trigger patterns to be used to control the trigger time interval. Trips from each seismic source are randomly sequenced in the trip time window. The resulting trigger pattern is then examined for maximum amplitude. If the maximum amplitude is significantly greater than that of the larger air gun, the timing of the pistol firing times and order are re-performed and the maximum amplitude can be examined again. This process is repeated until a trigger pattern is found with the desired amplitude. In the 2D examples below, about 0.5 percent of the generated random patterns were suitable for use. The process can be repeated for as many patterns as necessary. In another embodiment, the algorithm or computer program that can be used to produce a set of ideal trigger patterns can also examine the trigger pattern or generate the ideal time intervals to allow for the optimal separation of seismic signals at the same time. minimizing the output amplitude.
    [0069] The number of patterns should preferably be large enough to prevent unwanted overlapping of the notches in the spectra within the spatial data processing window. The testing of the limits for overlapping the spectra can be done by processing simulated standardized shots to check the accuracy of the reconstruction. In particular, performing the inversion using the patterns calculated at one point is likely to show any weaknesses in the generated patterns. The results of an example of such a test are shown in Figures 7 to 9.
    [0070] The inversion method used to process seismic data acquired using the described methods is similar to the methods previously described for the separation of the simultaneous shots. (See Abma, RL, Manning, T, Tanis, M., Yu, J, and Foster, M., [2010] High Quality Separation of Simultaneous Sources by Sparse Inversion, 72nd Annual Conference and Exhibition, EAGE, Extended Abstracts and Request United States Patent No. 12 / 542,433, incorporated herein by reference for all purposes in its entirety). As such, the use of standard air guns as a source can be replaced by that of other sources, for example, Vibroseis sources with different sweeps in a terrestrial environment, and the process will not change significantly. In other words, although the methods described here are aimed at marine seismic sources, the methods described are also applicable in a terrestrial environment with land or land seismic sources.
    [0071] Figure 7 shows the impulse responses of a set of standardized shots along a trigger line. The maximum amplitude produced by standardized shots is much smaller than that of the conventional air gun arrangement shown in Figure 9. The result of the inversion process seen in Figure 8 is almost exactly that of the conventional air gun arrangement. The difference between the impulse responses in Figures 8 and 9 is shown in Figure 10, which shows virtually no difference in response.
    [0072] These standards cannot be processed by conventional methodologies for acquisition sources since the individual standards cannot be decoded separately. However, traditional codes can be used instead of the random patterns used here.
    [0073] Normally, the conversion of the impulse from one source to another is done by a method of pairing or deconvolution. This involves inverting the d «A m (1) system
    [0074] where d is the known or acquired data, m is the desired data, and A is the convolution operator. In creating firing patterns for airguns, the small waves in Figure 3 are spread over time to create small, prolonged waves as seen in Figure 4. The dispersion of these small waves over time creates indentations in the spectra of small waves. The notches that correspond to the null space of the matrix A. The reconstruction of the data in these notches in individual lines is difficult or impossible in real data, and attempts to then make the results in the noise generated by the inversion.
    [0075] To eliminate the null space, another restriction can be introduced, that of the spatial continuity of the data. Since the propagation of seismic waves through even the most irregular subsoil typically creates continuous wave fields, this continuity can be used to restrict solutions. This changes Equation 1 to d «A C m (2)
    [0076] where C is an operator that ensures that m is spatially continuous. Multidimensional Fourier transformations can be used with thresholding to calculate a continuity operator. Other coherence criteria can be used, such as the curvelet method suggested in Lin and Herrmann (2009). With sufficient interactions, thresholding of curvelets can produce results similar to those of the methods described above, but thresholding in the FK space is likely to be more effective and faster than the corresponding curvelet methodology. Examples of alternative methods of incorporating the assumption of a coherent wave field into the inversion would include several random transformations and error prediction filters.
    [0077] The inversion process used to solve m may be similar to that of the POCS (Projection Onto Convex Sets) interpolation method used by Abma R., and Kabir, N. [2006] 3D interpolation of irregular data with a POCS algorithm , Geophysics, 71, E91-E97, hereby incorporated by reference in their entirety for all purposes. Other inversion methods known to those with experience in the art, such as without limitation, the Spectral Projected Gradient LI Solver (SPGLl), can also be used to solve Equation 2. However, any suitable solver known to those with experience in the technique can be used to solve Equation 2.
    [0078] In general, a method of processing data acquired by the described method may include the use of a Fourier transformation method such as a Fast Fourier Transformation (FF) to remove a response from the pattern. The subsequent set of data may be arranged to allow measurement of coherence. A two-dimensional (2D) or three-dimensional (3D) Fourier transformation can be applied to the data set. The resulting data set can be limited and then inverted to create an inverted data set. The pattern response can be applied to the inverted data set to generate a new model. The new model is subtracted from the original seismic data set to form a residual data set. The residual data set can then be used as the input for the next iteration.
    [0079] Figure 23 illustrates, according to an example of a modality, the computer system 20, which can perform the operations described in this specification to process the seismic data acquired by the described methods or to generate the trigger patterns. In this example, system 20 is as performed by a computer system including workstation 21 connected to server 30 via a network. Certainly, the particular construction and architecture of a computer system useful in conjunction with this invention can vary widely. For example, system 20 can be realized by a single physical computer, such as a conventional personal computer or workstation, or alternatively by a computer system implemented in a distributed manner over multiple physical computers. Consequently, the generalized architecture illustrated in Figure 3 is provided by way of example only.
    [0080] As shown in Figure 23 and as mentioned above, system 20 can include workstation 21 and server 30. Workstation 21 includes central processing unit 25, coupled to the system bus. Also connected to the BUS system bus is the input / output interface 22, which refers to those interface resources through which the interface of peripheral functions P (for example, keyboard, mouse, monitor, etc.) with the other constituents of workstation 21. Central processing unit 25 refers to the data processing capacity of workstation 21, and as such can be implemented by one or more CPU cores, coprocessing circuit and the like. The particular construction and central processing unit capacity 25 are selected according to the application needs of the workstation 21, such needs including, at a minimum, performing the functions described in this specification, and also including such other functions as can be run by the computer system. In the architecture of the allocation system 20 according to this example, the system memory 24 is coupled to the BUS system bus, and provides memory resources of the desired type useful as data memory to store the input data and the processing results executed by the central processing unit 25, as well as the program memory to store the instructions of the computer to be executed by the central processing unit 25 in carrying out these functions. Certainly, this memory arrangement is only an example, it being understood that system memory 24 can implement such data memory and program memory in separate physical memory resources, or distributed completely or in part outside the workstation 21. In addition in addition, as shown in Figure 2, measurement inputs 28 that are acquired from laboratory or field tests and measurements are included via the input / output function 22, and stored in a memory resource accessible to workstation 21, locally or via the network interface 26.
    [0081] The network interface 26 of workstation 21 is a conventional interface or adapter through which workstation 21 accesses network resources on a network. As shown in Figure 2, the network resources that workstation 21 accessed through network interface 26 include server 30, which resides on a local area network, or a wide area network, such as an intranet, a virtual private network, or over the Internet, and which is accessible to workstation 21 by means of one of these network arrangements and by corresponding wired or wireless communication devices (or both). In this embodiment of the invention, server 30 is a computer system, of a conventional architecture similar, in a general sense, to that of workstation 21 and, as such, includes one or more central processing units, system buses and resources memory, network interface functions, and the like. In accordance with this embodiment of the invention, the server 30 is coupled to the program memory 34, which is a computer-readable medium that stores executable computer program instructions, according to which the operations described in this specification are carried out by the control system. allocation 30. In this embodiment of the invention, these computer program instructions are executed by the server 30, for example, in the form of an “internet-based” application, under input data communicated from workstation 21, to create the output data and results that are communicated to workstation 21 to the monitor or output by peripherals P in a form useful to the human user of workstation 21. In addition, library 32 is also available for server 30 ( and, perhaps, workstation 21 over the wide area network or local area), and stores such reference information or file since it can be useful in the allocation system 20. The library oteca 32 may reside on another local area network, or alternatively be accessible via the Internet or some other wide area network. It is taken into account that library 32 may also be accessible to other associated computers on the entire network.
    [0082] Certainly, the particular or local memory resource in which the measurements, library 32, and program memory 34 physically reside can be implemented in various locations accessible to the allocation system 20. For example, this program data and instructions they can be stored in local memory resources on workstation 21, on server 30, or in memory resources accessible over the internet for these functions. In addition, each of these data and program memory resources can alone be distributed among multiple locations. It is taken into account that those skilled in the art will be easily able to implement the storage and retrieval of the applicable measurements, models, and other useful information in conjunction with this embodiment of the invention, in a manner suitable for each particular application.
    [0083] According to this modality, for example, system memory 24 and program memory 34 store computer instructions executable by central processing unit 25 and server 30, respectively, to perform the functions described in this specification, whereby triggering patterns can be generated and also seismic data can be processed. These computer instructions can be in the form of one or more executable programs, or in the form of source code or higher level code from which one or more executable programs are derived, assembled, interpreted or compiled. Any of several computer protocols or languages can be used, depending on the way in which the desired operations are to be performed. For example, these computer instructions can be written in a conventional high-level language, such as a conventional linear computer program, or arranged for execution in an objective-oriented manner. These instructions can also be incorporated into a higher level application. For example, an executable network-based application can reside in program memory 34, accessible to server 30 and client computer systems such as workstation 21, receive input from the client system in the form of a spreadsheet, execute algorithm modules on an internet server, and provide output to the client's system in some convenient printed or display form. It is taken into account that those skilled in the art having reference to this description will be easily able to carry out, without undue experimentation, this embodiment of the invention in a manner suitable for the desired installations. Alternatively, these software instructions executable by the computer can be resident anywhere on the local area network or wide area network, or capable of being downloaded from higher-level locations or servers, through information encoded in an electromagnetic vehicle signal through some network interface or input / output device. Software instructions executable by the computer may have been originally stored on a removable or non-volatile computer-readable storage medium (for example, a DVD disc, flash memory, or the like), or are capable of being downloaded as information encoded in an electromagnetic vehicle signal, in the form of a software package from which the software instructions executable by the computer were installed by the allocation system 20 in the conventional manner for software installation. Example
    [0084] A modeled or synthetic example of a 3D data set with standardized trigger acquisition is shown in Figure 11. Figure 12 shows the data calculated to pair the conventional trigger and Figure 13 shows the conventional result. Figure 14 shows the difference between the data shown in Figures 12 and 13.
    [0085] Note that the amplitudes of the data in Figure 8 are considerably smaller than those in Figures 12 and 13, and that the data in Figure 11 are much less coherent than those in Figures 12 and 13. This is due to the extended signatures of the randomly assigned font patterns used here. Each shot was assigned to a random pattern in Figure 15. Figure 16 shows the spectra of the nine patterns as well as the spectra of the desired impulses seen in Figure 5. At the same time that each of the nine patterns shows significant notches and irregularities in their spectra, the spectra of the calculated data match those of the conventionally acquired data observed in Figure 17, indicating that the inversion was a success.
    [0086] At the same time that the modalities of the invention have been shown and described, modifications of them can be made by someone skilled in the art without departing from the spirit and teachings of the invention. The modalities described and the examples provided here are exemplary only and are not intended to be limiting. Many variations of modifications of the invention described here are possible and are within the scope of the invention. Consequently, the scope of protection is not limited by the description presented above, however, it is only limited by the Claims that follow such scope including all equivalents of the subject matter of the Claims.
    [0087] The description of a reference is not an admission that it is the prior art to the present invention, especially any reference that may have a publication date after the priority date of this application. The description of all patents, patent applications, and publications cited here, is hereby incorporated here by reference in their entirety, insofar as they provide exemplary, procedural or other supplementary details to those presented here.
    权利要求:
    Claims (11)
    [0001]
    1 - Seismic Acquisition Method, characterized by the fact that it comprises: (a) positioning a first seismic source arrangement comprising a plurality of seismic sources over a seismic survey region, the seismic source arrangement generating an output amplitude when all the plurality of seismic sources referred to is activated simultaneously; (b) choosing a plurality of different trigger patterns, each of said plurality of trigger patterns having a pattern output amplitude associated with it, wherein the referred pattern output amplitude is a maximum amplitude of the seismic source arrangement referred when the referred seismic source arrangement is activated according to the associated associated firing pattern and, where (i) each of the plurality of different referred firing patterns is less than 10 seconds long and greater than 0.5 seconds of duration; (ii) each of the plurality of different trigger patterns referred to is chosen so that the output amplitude of the associated associated pattern is less than the output amplitude of the referred source; and, (iii) each of the referred trigger patterns creates a plurality of notches in a frequency spectrum of any seismic data recorded from them; (c) activate the first seismic source arrangement according to one selected from a plurality of different trigger patterns; (d) performing step (c) at least twice for at least two different units selected from the plurality of trigger patterns; (e) record a plurality of seismic signals reflected from one or more underground formations; and, (f) processing the plurality of seismic signals referred to using a sparse inversion to produce processed seismic signals for use in seismic exploration, in which the sparse inversion referred to is obtained by solving d * = AC m to m, where d is a set of data acquired from recording the plurality of seismic signals in (e), m are the processed seismic signals, C is an operator that ensures that m is spatially continuous and A is a convolution operator chosen in such a way that the said notches correspond to a null space of A.
    [0002]
    2 - Seismic Acquisition Method, according to Claim 1, characterized by the fact that at least two of the seismic sources within the first seismic source arrangement generate energy with different frequency ranges.
    [0003]
    3 - Seismic Acquisition Method, according to Claim 1, characterized by the fact that each trigger pattern further comprises an order to activate each seismic source, where the order for each trigger pattern is different from each other.
    [0004]
    4 - Seismic Acquisition Method according to Claim 1, characterized by the fact that at least one of the plurality of different trigger patterns comprises a plurality of different time intervals between an activation of each seismic source within the first arrangement of seismic sources, and where the plurality of different time slots in at least one of the plurality of different trigger patterns are pseudo-randomly varied.
    [0005]
    5 - Seismic Acquisition Method, according to Claim 1, characterized by the fact that seismic sources are impulsive sources.
    [0006]
    6 - Seismic Acquisition Method, according to Claim 1, characterized by the fact that seismic sources are marine sources.
    [0007]
    7 - Seismic Acquisition Method, according to Claim 1, characterized by the fact that seismic sources are terrestrial sources.
    [0008]
    8 - Seismic Acquisition Method, according to Claim 1, characterized by the fact that it comprises towing the set of seismic sources underwater behind a seismic vessel.
    [0009]
    9 - Seismic Acquisition Method, according to Claim 1, characterized by the fact that seismic sources comprise air guns, explosives, gas guns or combinations thereof.
    [0010]
    10 - Seismic Acquisition Method, according to Claim 9, characterized by the fact that pneumatic pistols comprise different volumes.
    [0011]
    11. Seismic Acquisition Method according to Claim 1, characterized by the fact that at least one of the plurality of different trigger patterns reduces their associated pattern output amplitude by at least 20 dB when compared to the source's output amplitude.
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    法律状态:
    2018-12-18| B06F| Objections, documents and/or translations needed after an examination request according art. 34 industrial property law|
    2020-02-04| B06U| Preliminary requirement: requests with searches performed by other patent offices: suspension of the patent application procedure|
    2020-12-15| B09A| Decision: intention to grant|
    2021-01-19| B16A| Patent or certificate of addition of invention granted|Free format text: PRAZO DE VALIDADE: 20 (VINTE) ANOS CONTADOS A PARTIR DE 09/12/2011, OBSERVADAS AS CONDICOES LEGAIS. |
    优先权:
    申请号 | 申请日 | 专利标题
    US42127410P| true| 2010-12-09|2010-12-09|
    US61/421,274|2010-12-09|
    US201161503407P| true| 2011-06-30|2011-06-30|
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    PCT/US2011/064144|WO2012078978A1|2010-12-09|2011-12-09|Seismic acquisition method and system|
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