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    • 专利摘要:
    seismic exploration methods above subsurface region a seismic data collection system and method is provided here for terrestrial and marine data using non-impulsive narrowband low-frequency monochromatic sources designed to optimize migration/inversion capability of algorithms for imaging the earth's subsurface, in particular, full waveform inversion.
    公开号:BR112013014556B1
    申请号:R112013014556-0
    申请日:2011-12-16
    公开日:2021-08-24
    发明作者:Joseph Anthony Dellinger；John T. Etgen；Graham Anthony Openshaw
    申请人:Bp Corporation North America Inc；
    IPC主号:
    专利说明:

    CORRELATED CASE DESCRIPTIVE REPORT
    [001] This Application claims the benefit of Provisional Patent Application Serial Number 61/423,962 filed December 16, 2010, and incorporates said Provisional Application by reference to this disclosure, as fully defined herein. TECHNICAL FIELD
    [002] This invention relates to the general subject of seismic exploration and, in particular, to methods for acquiring seismic signals that are representative of subsurface for waveform inversion purposes in the frequency domain. BACKGROUND OF THE INVENTION
    [003] A seismic survey represents an attempt to image or map the Earth's subsurface, sending sound energy down to the ground and recording the “echoes” that return from the rock layers below. The source of sound energy that comes from underneath can come, for example, from explosions or seismic vibrators on land, or pressure guns in marine environments. During the seismic survey, the energy source is placed at various locations near the earth's surface above a geological structure of interest. Each time the source is activated, it generates a seismic signal (sound wave) that travels down through the earth, is reflected, and, upon its return, is recorded at a large number of locations on the surface. The combinations of multiple sources/records are then combined to create an almost continuous subsurface profile that can span many kilometers. In a two-dimensional (2-D) seismic survey, the record sites are generally established along a single line, whereas in a three-dimensional (3-D) seismic survey, the record sites are generally distributed over the entire surface. in a grid pattern. In simpler terms, a 2-D seismic line can be thought of as giving a cross-sectional (vertical slice) image of the earth layers as they exist directly below the record sites. A 3-D survey produces a “cube” or date volume, which is, at least conceptually, a 3-D image of the subsurface that lies beneath the survey area. In reality, both 2-D and 3-D surveys interrogate some volume of land seated beneath the area covered by the survey, and the processing of the recorded data is then implemented to produce an interpretable image. Finally, a 4-D survey (or time span) is one that is taken against the same subsurface target two or more different times. This can be done for many reasons, but often it is done to measure changes in subsurface reflectivity over time that can be caused, for example, by the progress of a water flood, movement of a gas/oil contact, or oil/water etc. Obviously, if successive images of the subsurface are compared any changes that are observed (assuming differences in source signature, receivers, recorders, ambient noise conditions etc. are accounted for) will be attributed to the progress of the processes of subsurface that are in operation.
    [004] The conventional seismic survey is composed of a very large number of records or individual seismic traces. These are typically 10 to 20 seconds long, so there is enough time for the echoes of interest to return before the source is dismissed again. Chapter 1, pages 9-89, of Seismic Data Processing by Ozdogan Yilmaz, Society of Exploration Geophysicists, 1987, contains general information relating to conventional 2-D processing and that disclosure is incorporated herein by reference. General information regarding 3-D data acquisition and processing can be found in Chapter 6, pages 384-427, of Yilmaz, the disclosure of which is also incorporated herein by reference.
    [005] A conventional seismic trace is a digital record of acoustic energy reflecting from heterogeneities or discontinuities in the subsurface, a partial reflection that occurs each time there is a change in the elastic properties of the subsurface materials. Digital samples are typically acquired at 0.002 second (2 milliseconds or “ms”) intervals, although 4 millisecond and 1 millisecond sampling intervals are also common. Each discrete sample in the conventional digital seismic trace is associated with a travel time and, in the case of reflected energy, a two-way travel time from the source to the reflector and back again to the surface, assuming, of course, that the source and receiver are located on the surface. Many variations of the conventional receiver-source arrangement are used in practice, eg VSP (vertical seismic profiling) surveys, ocean floor surveys etc. In addition, the surface location associated with each trace in a seismic survey is carefully tracked and is usually made a part of the trace itself (as part of the trace header information). This allows the seismic information contained within the traces to then be correlated with specific surface and subsurface locations, thus providing a means to affix and bypass seismic data - and attributes extracted from them - on a map (ie, from " mapping”).
    [006] Conventional seismic acquisition and processing has advanced considerably over the previous decades, but the fundamental paradigm described above of the “echoes” record and their use of time to locate discontinuities on Earth has remained essentially unchanged. Full Waveform Inversion (FWI) is a time- or frequency-based seismic processing technique that provides a more general paradigm for imaging subsurface structures: instead of relying solely on reflected or scattered waves that echo from discontinuities On Earth, FWI also makes use of transmitted/refracted waves that travel downwards, then return to become horizontal, and finally upwards to emerge as rising seismic waves (possibly at a considerable distance from your origin). Subsurface structures on Earth advance, retard, and/or distort these transmitted/refracted diving waves with their presence, and resolve the FWI to their location and feature properties print these outputs on the data. See, for example, the teachings of Sirgue, et al., in US Patent Application 11/756,384, filed May 31, 2007, the disclosure of which is fully incorporated herein by reference, as defined herein. FWI has recently gone from being an academic curiosity to finding widespread industrial application. See, for example, Sirgue, et al., 2010, Full waveform inversion: the next leap forward in image at Valhall, first volume of Break 28, page 65, the disclosure of which is fully incorporated herein by reference, as defined herein.
    [007] Frequency domain algorithms, in particular the FWI algorithm mentioned above, require input seismic data that is very different from what is conventionally recorded: they work in monochromatic wave fields. Conventional seismic data must be converted into a form of these algorithms that can be used by Fourier transform from time to frequency domain (with proper windowing and taper), after which the individual frequencies are selected for use. Sirgue's frequency domain FWI algorithm detects subsurface structures by the perturbations they create in the amplitude and phase of these monochromatic wave fields.
    [008] Note the fundamental paradigm shift here: instead of an impulsive source followed by listening to (record) discrete echo return, mathematically for the purpose of understanding the FWI algorithm the source can now be considered to be a continuous pure tone (ie, a monochromatic source) that excites standing waves on Earth. Unknown subsurface structures are detected by analyzing how the amplitude and phase of these standing waves differ from what was expected. By making use of transmitted/refracted diving waves, FWI can detect structures that do not generate a classic impulsive “echo”.
    [009] Thus, current practices when performing FWI in the frequency domain on vibrator (vibration) data over the earth are unnecessarily reversed: seismic waves are generated using a swept frequency source, reflected/refracted waves are detected with a receiver and the resulting data is then processed to approximate data from a traditional impulsive source. The “impulsive” seismic data is then processed to resemble data from a monochromatic source, as required by the frequency domain inversion algorithms.
    [0010] In fact, it has been shown that FWI in the frequency domain requires only a small number of discrete frequencies well separated in order to produce a good result. See, for example, Sirgue, L., and Pratt, RG, 2004, Efficient Wave Inversion and Imaging: A Strategy for the Selection of Geophysics Temporal Frequencies, volume 69, page 231, the disclosure of which is fully incorporated herein by reference. , as defined at this point. Thus, with conventional acquisition followed by FWI in the frequency domain, a large part of the energy produced by traditional broadband sources is wasted: it is in frequencies that are not used by the processing algorithm.
    [0011] Note that without low-frequency broad displacement data containing the transmitted/refracted waves discussed above, full waveform inversion often fails and cannot resolve subsurface structures (ie, may produce a useless result). Unfortunately, traditional seismic sources do not provide the low frequency waves, which are generally desired, and more particularly the low frequency data, which can be used when full waveform inversion is performed.
    [0012] In particular, the most popular impulsive sources, dynamite on land or pressure guns at sea, produce relatively little low frequency energy. The conventional way to provide more low-frequency energy for a seismic survey is to produce more energy at all frequencies, which is often impractical for cost, safety, and engineering considerations. Swept frequency sources such as vibrators allow more control of the frequencies of the emitted acoustic waves, thus, they may provide a more promising method for generating low frequency waves.
    [0013] Currently, the practice of ground vibrators is to generate a broadband sweep. The “chirp” emitted vibrator source is then correlated with the recorded seismic data to produce data traces that approximate those generated by an impulsive seismic source. Unfortunately, creating a reliable high-output, wideband, swept-frequency vibrator proved to be a challenge for low-frequency waves below about 3Hz. Several solutions have been proposed, the simplest of which is the use of a massive vibrator and driving it with a non-linear sweep, so that the vibrator spends more time producing the lowest frequencies. See, for example, Baeten, in Patent Application WO 2010/037840 A1, filed October 2, 2009, the disclosure of which is fully incorporated herein by reference as if set out herein.
    [0014] The situation is similar at sea. For marine swept frequency sources (marine vibrators, resonators, water sirens, etc.), the conventional practice is to generate a relatively wide band sweep. The “chirp” emitted source is then correlated with the recorded seismic data to produce a seismic trace that is conceptually equivalent to one generated by an impulsive seismic source such as a pressure gun (but without the production of the seismic energy pressure gun at frequencies above about 100 Hz that are not used for seismic imaging). Creating a reliable, high-throughput, broadband swept frequency source for marine use has proven to be a challenge, particularly at frequencies lower than those that conventional pressure guns can generate (eg, the frequencies of about 4 Hz or less).
    [0015] Thus, if the objective is to acquire data associated with low frequency reflected/refracted waves for FWI in the frequency domain or other uses, current industry practices have several disadvantages. As discussed above, frequency domain FWI performed on conventionally acquired wideband seismic data discards much of the generated data and most of the energy produced by the source is thus wasted (either from a swept frequency source or impulsive), which is obviously inefficient.
    [0016] Potentially more problematic, the use of impulsive broadband sources introduces approximations that can degrade the final result. Full waveform inversion in the frequency domain uses a theory based on monochromatic standing wave patterns. Frequency domain FWI algorithms such as those discussed above achieve computational practicality by approximating these excited source wave fields using monochromatic conical sine wave sources modeled in the time domain. The resulting data is then from discrete Fourier transforms and a single frequency is extracted. The recorded wideband field data is similarly discrete Fourier transform and the same single frequency is extracted. The inversion process then attempts to find an Earth model that best matches the amplitude and/or phase of the modeled monochrome data with the amplitude and/or phase derived from the impulsive broadband data recorded for that frequency. The tapered monochrome fonts used in computer models typically have a very different signature from the broadband fonts used in the field. This introduces an approximation, which is only partially smoothed by the Fourier transform step, of both real and modeled data and extracts the same single frequency.
    [0017] The aim of an inversion algorithm is to produce a computational model of subsurface structures, which correctly predicts the subsurface structures of interest on the real Earth. Logically, the better the computational modeling of how waves are generated, recorded and processed matches what happened on the real Earth, the better the result of the inversion of the algorithm can be. To produce a better inversion result, it is desirable to match seismic data acquisition and processing and computer modeling on the computer as closely as possible. This can be achieved by modifying computer modeling to better fit what happened on the real Earth. This could also be achieved by modifying the acquisition and processing of field data to correspond with computer modeling.
    [0018] Finally, in addition to all these shortcomings of existing practice, conventional seismic sources often do not produce enough energy during the lifetime of a conventional seismic trace to generate low-frequency transmitted/refracted diving waves recordable in very large displacements desirable for full waveform inversion.
    [0019] Typically, the trace lengths used in existing seismic surveys are based on the limitations of a conventional imaging paradigm that FWI in the frequency domain does not use. Without being bound by theory, the monochromatic standing waves used through a frequency domain algorithm repeat indefinitely. Data generated by a monochrome font does not have a natural maximum record length beyond which no other useful data can be received. Consequently, the signal-to-noise ratio can be increased by obtaining signals over a longer period, allowing sources to radiate for longer periods of time.
    [0020] Existing methods for using very long sweeps to generate more energy from existing low-amplitude sources require sources with precisely controllable emitted waveforms. See, for example, Meunier, US Patent Application 6,714,867 B2, filed February 9, 2001, the description of which is fully incorporated herein by reference as if set forth herein. Such control can be difficult to achieve in practice, especially at low frequencies.
    [0021] Hitherto, as is well known in seismic processing and acquisition techniques, there is a need for an efficiently optimized low-frequency data acquisition system and method for use with inversion algorithms, in particular , full waveform inversion in the frequency domain. Therefore, it must now be recognized, as recognized by the present inventors, that there is, and has been for some time, a very real need for a method of seismic data acquisition and processing that can address and solve the problems described above. .
    [0022] Before proceeding with a description of the present invention, however, it should be noted and remembered that the description of the invention which follows, together with the accompanying drawings, should not be interpreted as limiting the invention to examples (or preferred embodiments ) shown and described. This is so because those skilled in the art to which the invention pertains will be able to conceive of other forms of the present invention within the scope of the appended Claims. In particular, the acquisition methodology may prove useful for obtaining low frequencies for algorithms other than full waveform inversion in the frequency domain, for example, full waveform inversion in time domain. SUMMARY OF THE INVENTION
    [0023] According to a preferred aspect of the present invention a system and a method for acquiring additional data beyond those normally acquired in a seismic survey are provided for the purpose of improving the processing thereof.
    [0024] According to a first preferred embodiment, one or more narrowband or monochromatic low frequency "sweeps" will be acquired using a frequency controlled, tunable or other customizable seismic source (for example, a ground vibrator that can be configured to produce a signal that is largely confined to a single target frequency, or within a narrow frequency range), with the selected narrow frequency ranges or frequency ranges having been chosen to improve the calculation of a complete waveform inversion . In this way, a methodology for the acoustic waves emitted by the source is used in the field that corresponds to the method used in the computer processing algorithm. Typically, the frequencies used would be lower than could possibly be acquired using conventional wideband seismic sources (ie, below about 4 Hz).
    [0025] The source(s) will emit the monochromatic waves for at least a sufficient period of time to achieve a target signal-to-noise ratio for the signals recorded at maximum desired register shifts that are used for full waveform inversion of desired target subsurface structures. The recorded data trace lengths must be long enough to accommodate the longer emission times or, alternatively, the recording must be continuous.
    [0026] Note that the present invention does not require a monochromatic source to precisely maintain a particular source frequency. As a rule of thumb, if the sufficient period of time to develop a sufficient signal-to-noise ratio is T, then a source that maintains a frequency accuracy of about ±1/T Hz is still monochromatic for all practical purposes. A small frequency shift can often be as closely approximated as a phase shift from a monochromatic source. Conventional practice is for full waveform inversion algorithms in the frequency domain to resolve the unknown source phase so that it does not present any additional algorithmic complications. Therefore, relatively minor deviations from the target frequency are not detrimental to the functioning of the invention.
    [0027] A narrowband source that emits power over a bandwidth greater than ± 1/T Hz, but still less than two or more octaves of a typical wideband source, may also be useful for some applications, for example, complete waveform inversion in the time domain. The signal-to-noise ratio depends on both signal strength and noise strength. Natural background noise is typically wideband, so the narrower the signal's bandwidth, the less background noise falls within its bandwidth and thus less signal energy and shorter integration time. enough signal to achieve the desired signal-to-noise ratio. Monochromatic fonts are merely a borderline case of a broader category of narrowband fonts.
    [0028] A scaled frequency source is monochromatic for periods of "T" (the period of time to build the signal-to-noise ratio) or more seconds, at which time it changes to a new frequency, which also remains for “T” or more seconds before changing again, and so on, eventually going back to the original frequency and starting the cycle again. Instead of abruptly changing frequencies, the source may decrease its amplitude and cease emission, then increase the amplitude at the new frequency, or they may "sweep" from one monochromatic frequency to another over a substantially period of time. shorter than the “T”.
    [0029] The waves emitted by the monochromatic or narrowband source can be monitored and recorded continuously. The resulting data will be used to create an optimal source wave field in the modeling step of the inversion algorithm used to process the data. That is, instead of precisely controlling the amplitude, frequency and phase of the waves emitted by the source(s) in an attempt to mimic in the field an idealized source assumed by standard processing algorithms, the amplitude, frequency and phase of the waves emitted by the source(s) are recorded and the model source(s) in the algorithm is(are) adjusted to match these. The location of each source as it radiates must also be recorded so that this information can also be used in modeling.
    [0030] In practice, low frequency, monochromatic or stepped narrowband earth vibrators would be used to complement, not replace, current high frequency wide bands. Conventional high-frequency and low-frequency surveys can be purchased separately or simultaneously.
    [0031] According to another preferred embodiment, an invention substantially the same as described above is provided, but in which marine seismic data is recorded. Narrowband, monochromatic or stepped frequency sources can radiate continuously as they are carried through water in order to maximize the amount of energy produced. The source waves emitted, the reflected/refracted waves received and the source and receiver positions can also be recorded continuously. In this case, the modeling step of the complete waveform inversion algorithm (either in time domain or frequency domain) can include a motion source, mimicking the motion of the real source.
    [0032] Of course, the acquisition of auxiliary information of this type has the potential to significantly improve the quality of subsurface images produced by processing seismic data, which, in turn, would improve the chances of discovering economic quantities of oil and/or gas.
    [0033] In some embodiments, a low frequency survey will be used to improve a previously acquired subsurface model derived from conventional broadband high frequency data.
    [0034] According to another aspect of the present invention, there is provided a method of seismic exploration above a region of the subsurface containing structural or stratigraphic characteristics favorable to the presence, migration or accumulation of hydrocarbons, comprising the steps of: selecting at least a narrowband frequency range; providing at least one narrowband seismic source for each of said at least one selected narrowband frequency band, each of said narrowband seismic energy source emitting seismic energy at least approximately within a band of frequency band close matching; performing a narrowband seismic survey with each of said at least one narrowband seismic source, thereby creating a narrowband seismic survey; combining at least a portion of said narrowband seismic survey together with a wideband survey collected close to said narrowband seismic survey, thereby forming an advanced survey; and, using at least a portion of said advanced survey to explore for hydrocarbons in said subsurface region.
    [0035] In another modality, a seismic exploration method is provided above a subsurface region containing structural or stratigraphic characteristics favorable to the presence, migration or accumulation of hydrocarbons, comprising the steps of: selecting at least a discrete frequency; providing at least one monochromatic seismic source for each of said at least one selected discrete frequency, each of said narrowband seismic sources emitting seismic energy at a frequency at least approximately equal to said corresponding discrete frequency; performing a narrowband seismic survey using each of said at least one monochromatic seismic source, thereby creating a narrowband seismic survey; combining at least a portion of said narrowband seismic source together with a wideband survey collected near said narrowband seismic source, thus forming an advanced survey; and using at least a portion of said advanced survey to explore hydrocarbons in said subsurface region.
    [0036] In other modalities, the conventional wideband and low frequency narrowband seismic surveys will be continuously recorded by some of the same receivers and the higher frequency broadband, the low frequency narrowband and the ambient noise signals registered by these receivers will be separated before further processing.
    [0037] Still in other modalities, the timing of the shots in the higher frequency wideband survey will be adjusted according to the phase of the higher frequency narrowband source in the low frequency survey, in order to mitigate the interference between the two surveys.
    [0038] In still other embodiments, the wave fields emitted from one or more narrowband low frequency sources will be recorded and the information will be used to improve the processing of narrowband seismic data.
    [0039] In yet another modality, only the phase and amplitude of the near monochromatic narrowband low frequency source(s) will be recorded.
    [0040] In yet another modality, a seismic exploration method is provided above a region of structural or stratigraphic characteristics favorable to the presence, migration or accumulation of hydrocarbons, comprising the steps of selecting a plurality of distinct frequencies; providing at least one monochromatic seismic source corresponding to each of said plurality of selected discrete frequencies, each of said at least one monochromatic seismic source emitting seismic energy at a frequency at least approximately equal to said corresponding discrete frequency; performing a narrowband seismic survey using each of said at least one monochromatic seismic sources, thereby creating a narrowband seismic survey; using at least a portion of said narrowband seismic survey to calculate a complete waveform inversion dataset; and, using at least a portion of said complete waveform inversion dataset to scan for hydrocarbons in said subsurface region.
    [0041] The foregoing has outlined, in general terms, the most important features of the invention disclosed herein so that the detailed description which follows can be more clearly understood, and so that the present inventors' contribution to the art can be better taken into account. The present invention is not to be limited in its application to the details of construction and arrangements of components shown in the following description or illustrated in the drawings. Rather, the invention is capable of other embodiments and of being practiced and carried out in various other ways that are not specifically enumerated herein. In particular, other algorithms (in addition to full waveform inversion in the frequency domain) can benefit from supplementing existing wideband seismic data with low frequency data generated by narrowband, monochromatic, or scaled frequency sources. Finally, it is to be understood that the phraseology and terminology employed herein are for descriptive purposes and are not to be considered as limiting, unless the Descriptive Report specifically so limits the invention. BRIEF DESCRIPTION OF THE DRAWINGS
    [0042] Other objects and advantages of the invention will be apparent after reading the following detailed description and after reference to the drawings in which:
    [0043] FIG. 1 illustrates an embodiment of a survey system for deploying the present invention in a marine environment.
    [0044] FIG. 2 contains a high-level summary of some steps of an embodiment of the present invention that would be suitable for use with the marine survey method shown in Figure 1.
    [0045] FIGs. 3A and 3B contain additional details of the steps in Figure 2. DETAILED DESCRIPTION
    [0046] Although this invention is capable of the embodiment in many different forms, some specific embodiments of the present invention are shown in the drawings, and will be described hereinafter in detail. It is to be understood, however, that the present disclosure is to be considered an exemplification of the principles of the invention and is not intended to limit the invention to the specific embodiments or algorithms so described. MODALITIES OF ILLUSTRATIVE EXAMPLES OF THE INVENTION
    [0047] Figure 1 illustrates a marine acquisition geometry suitable for implementing the present invention. In some embodiments, a seismic survey will be conducted in ocean 10O on a subsurface target of geological interest 126, which lies below the seabed 125. A vessel 110 floating on the surface of ocean 120 will tow a conventional pressure weapon array 140 and a streamer 130 of receivers, eg hydrophones 132. These components comprise the “conventional broadband acquisition” part of the survey system.
    [0048] In the augmented survey system, the vessel 110 can tow one or more low-frequency narrowband or monochromatic sources 150, each of which contains a receiver or a sensor (not shown) that will record the emitted wave field by that source, as is often done. To enhance low-frequency recordings, ocean floor receivers 135 can be simultaneously deployed and used in conjunction with conventional streamer 130, or ocean floor receivers 135 can be used without streamers 130. These comprise the part of “ narrowband low frequency” of one embodiment of the present survey system.
    [0049] Pressure guns 140 can be towed in shallow depths in order to enhance their ability to generate higher frequency acoustic waves. Low frequency sources 150 are shown towed to greater depths; in some modalities each will be towed to a depth suitable for its frequency range. Thus, the lower the frequency of the monochrome or narrowband source, the deeper the depth. See, for example, Tenghamn, US patent application 2010/0118647 A1, filed November 7, 2008, or Laws et al., US Patent 7,257,049 B1, filed August 22, 2000, the disclosures of which are entirely herein. incorporated by reference as defined herein.
    [0050] Note that many variations of this acquisition system are possible and are well within the ability of one skilled in the art to design it. The present survey system could acquire 2-D, 3-D, or 4-D data. More than one pressure gun array could be used. Conventional sources may not be pressure guns, but could instead be any other wideband seismic source, such as the types discussed above, that would benefit from low frequency supplementation. More than one stream of receivers could be used. One or more low frequency sources can be used. Instead of one vessel towing all the components of the lifting system, the components can be supported by multiple vessels moving in choreographed formation. Low-frequency narrowband survey can be performed at the same time as conventional high-frequency wideband survey, either in a separate pass, or in multiple separate passes. Alternatively, a low-frequency narrowband survey can be used to complement a previously acquired conventional high-frequency wideband survey such that the original data is reprocessed with additional low-frequency data or a low-frequency narrowband survey. frequency can be acquired first, and a conventional high-frequency broadband survey later. Data can be recorded by streamers, ocean floor receivers, or both, or possibly even receivers in subsurface wells, or receivers suspended in the water column.
    [0051] Low frequency sources 150 can operate continuously. The low-frequency sources can each operate at a single frequency ("monochromatic" low-frequency sources) or cycled between two or more discrete frequencies ("step frequency" low-frequency sources), or swept into a range low-frequency narrowband devices designed to increase the range of frequencies produced by wideband sources (low-frequency “narrowband” sources). Sources can operate to produce waves of constant amplitude, or the amplitude of the waves can vary (funnel up and down).
    [0052] Figure 2 shows how the acquisition system shown in Figure 1 can be used in practice. Initially, a seismic survey will be designed. Note that, for illustrative purposes only, the discussion that follows will be directed primarily toward the design of a marine survey. Therefore, those of ordinary skill in the art will readily understand how the present approach can be altered if the survey is done on land.
    [0053] As shown in Figure 2, 210, a conventional pressure gun lift can be designed in such a way that it is purchased in conjunction with the low frequency lift. The principles of conventional survey design are well established and will not be discussed here. Note that the steps in Figure 2 are explained in more detail in Figures 3A and 3B.
    [0054] For low frequency data, the survey design can proceed as follows. Typically, a pressure gun array provides adequate data for emitted waves having a frequency above 3.5 Hz, but computer modeling of the application of waveform inversion in this geological configuration suggests that frequencies as low as 1, 4 Hz may be important for successful complete waveform inversion. The algorithm for selecting frequencies given in Sirgue, L., and Pratt, R.G., 2004, previously referenced, suggests that frequencies should be selected which are separated by a ratio of about - for this survey geometry. Thus, in the present example, three or more narrowband sources can be used, operating at 1.4, 2.0, and 2.8 Hz, respectively. (In this example, the near frequency would be 4Hz, but this frequency will be available from the data collected using the wideband sources, so a narrowband source cannot be used to acquire this frequency.).
    [0055] The theoretically optimal ratio between successive frequencies can be shown to be equal to
    where o is the maximum displacement and d is the depth of the target of interest. So, for example, consider a maximum displacement of 20 kilometers and a target depth of interest of 6 kilometers. Then,

    [0056] Thus, starting from 0.7 Hz and following the prescription identified above, the next frequency would be 1.36 Hz, followed by 2.64 Hz, followed by 5.14 Hz etc. The last frequency is susceptible within the range available from conventional sources such as pressure guns, so in this case only three frequencies would be used from a controlled frequency source: 0.7, 1.36, and 2.64 Hz. In practice, it may be desirable to be somewhat conservative, but this example still illustrates that only a few frequencies may be needed for realistic examples.
    [0057] It may still be desirable to choose to disturb the frequencies of monochromatic sources to avoid unwanted harmonic interference between the seismic sources. For example, if theory suggests that sources that emit 1.0 and 2.0 Hz waves should be employed, it may be preferable, instead of using 0.9 and 2.1 Hz, to avoid having a frequency conflict of source with the second harmonic of the other. Optionally the harmonic or subharmonic output of a “monochromatic” source can be boosted and the harmonics or subharmonics can be used as additional monochromatic sources. So, for example, a source can simultaneously generate waves with frequencies of 1.4 and 2.8 Hz.
    [0058] Next, a joint survey 220 may be conducted, although the invention may function similarly, if separate broadband and narrowband surveys are performed. Conventional lifting can proceed as usual, with the pressure guns being dispensed with as the pressure gun die passes over each desired trigger point location. If pressure guns emit waves with a detectable intensity, eg 2.8 Hz, the largest of the low frequency sources, it may be desirable to slightly modify the timing of each shot so that the wave component of 2.8 Hz of the carbine signal is programmed to be in phase with the waves produced by the 2.8 Hz monochrome low frequency source(s). Note, at the most, this would require delaying or advancing the trigger time by 1.4 seconds. Alternatively, the vessel speed can be adjusted so that the pressure guns arrive at their firing locations only at the desired point in cycling the monochrome source. Note that the energy of the acoustic signal produced from pressure guns drops off quickly at lower frequencies, so any unwanted interference will be greatly reduced to any lower low frequency sources.
    [0059] Narrowband low frequency sources can operate independently or simultaneously. Low frequency narrowband sources can operate continuously or discontinuously. Each narrowband low frequency source records the signal it is radiating, as this information will be used to perform the inversion.
    [0060] Receivers can be registered continuously. The locations of all sources and receivers will, in some modalities, also be recorded continuously.
    [0061] The recorded data will then typically be prepared for two uses: for conventional processing 230 and for full waveform inversion 240. If low-frequency sources are truly monochromatic, simple band filtering it may be enough to remove your reflected/refracted waves from the conventional dataset. If they generate harmonics that overlap in the frequency band of broadband sources, a more sophisticated prediction-and-subtraction filtering algorithm can be used (such as a design to remove 60 Hz Hum of AC from seismic data from the Earth). It is observed that, by definition, low frequency signals cycle slowly and thus cannot be sampled for a sufficient number of cycles to be well represented in conventional length traces. Thus, the separation of high-frequency and low-frequency datasets (along with any low-frequency ambient noise suppression) will likely be done before the data is split into conventional length traces. Furthermore, in some cases, conventionally acquired data will be combined with narrowband data to produce an advanced seismic dataset with a range of frequencies that would not be available if only conventional surveying had been used.
    [0062] Once the data has been prepared, inversion of the complete waveform 260 can, in some embodiments, be performed first. This is usually done in stages from low frequencies and working towards higher and higher frequencies. Therefore, in this arrangement, data from the narrowband low frequency sources will be processed first, starting with the lowest frequency, followed using the conventional wideband dataset for higher frequencies. For low frequencies, the modeling part of the FWI algorithm can use a source wave field that corresponds with the emitted waves recorded by each low frequency source.
    [0063] The FWI algorithm produces an improved velocity model of the Earth, which can be used to improve the velocity model used for conventional seismic imaging 250.
    [0064] The geological interpretation 270 makes use of both the migrated image provided by conventional processing 250, and the velocity model provided by full waveform inversion 260. These two sources of information can complement each other when performing the geological interpretation.
    [0065] Geological interpretation 270 of the data can be performed on the data further processed according to methods well known in the seismic arts. Based on the result of the interpretation (and potentially combining data from other sources such as well logs, gravity, magnetism, etc.), in some cases, the 280 generation prospect and well planning will be performed from according to methods well known to those skilled in the art. Figures 3A and 3B provide additional details on the steps in Figure 2.
    [0066] According to another embodiment, a method of acquiring a narrowband low frequency seismic survey is provided. Freed from the need to generate a wide range of frequencies, a specialized narrowband source can produce useful data at lower frequencies than was previously possible. In particular, the simplest way to transmit more seismic energy into the ground and thus receive and record higher energy reflected/refracted waves and obtain additional seismic data is simply to signal or scan for longer periods of time. A narrowband low frequency source can emit signals or waves for any suitable time in order to achieve the signal-to-noise ratio.
    [0067] Survey data can be recorded continuously, or as close to continuous as possible. Traditionally the source and receiver locations will normally be recorded in the initial trace records. In the case of continuous data, this information must be kept separately during registration. Any filtering/separation of the signal must be done on the continuous data, before any division of the data into fixed-length traces, as they might be called by some processing algorithms.
    [0068] The frequency ranges of narrowband low frequency sources must be optimized to support the algorithm that will be used to process the data. In particular, if the application is of low frequencies for the inversion of the complete waveform in the frequency domain, only a small number of discrete monochromatic frequencies can be used by the algorithm. This can be achieved by assigning one or more discrete frequencies to each narrowband source. If only one frequency is assigned to a source, it will be considered a monochromatic or monotone source for purposes of the present disclosure. If two or more discrete frequencies are assigned to a source, it can fall between them, or it can produce the frequencies at the same time, or both strategies can be used in combination.
    [0069] The inversion of the complete waveform in the frequency domain of the type that would be suitable for use with the present invention iteratively performs a modeling step followed by an inversion/update step. The conventional intermediate step of correlating recorded data to appear as if they were acquired using an impulsive source tends to be counterproductive in this case. The algorithm conventionally employed in the inversion of the complete waveform in the frequency domain works on standing waves generated by monochromatic sources, not traversing waves generated by an impulsive source. Best results can be obtained when the survey methodology and the algorithm modeling step match as closely as possible. Thus, if the algorithm requires monochromatic fonts, the font(s) in the field must do the same.
    [0070] When it is not practical to correspond with the survey methodology of the processing algorithm, the processing algorithm should be matched with the survey methodology as closely as possible. In particular, it can be difficult to control the precise waveform of the acoustic signal emitted by a low-frequency narrowband source. In that case, the acoustic signal radiated by each low-frequency narrowband source must be measured, and this information used to inform the modeling step of the processing algorithm. In the case of a monochromatic source, it may suffice just to measure the amplitude and phase of the emitted waves.
    [0071] If mobile fonts are used in the field, the processing algorithm modeling step should also model mobile fonts.
    [0072] If the application is, instead of low frequencies for full waveform inversion in the time domain, instead of discrete frequencies a long duration sweep over a narrowband frequency range can be used, by example, a 1.0 to 2.0 Hertz sweep for 40 seconds of time. Again, the acoustic signal radiated by each low-frequency narrowband source must be measured, and this information can be used to inform the modeling step of the processing algorithm.
    [0073] Two or more narrowband low frequency sources that have non-overlapping frequency bands can be triggered simultaneously, unrelated to each other, as their signals can be easily separated by bandpass filtering. In particular, different sources can each have their own trigger grid and program optimized for the sampling requirements for that frequency range.
    [0074] If the goal is to create a velocity model, a small number of low frequencies may suffice and higher frequencies (eg from a conventional/broadband survey) cannot be used. In this case, a narrowband low-frequency survey can be usefully performed without a high-frequency wideband survey follow-up. If higher frequencies that would be better achieved by conventional wideband sources are also desired, narrowband low frequency survey can be designed to increase the bandwidth (frequency range) of conventional seismic survey at the lower end. bandwidth frequency. In this case, the narrowband low frequency survey then complements the conventional survey; this does not replace it. Conventional wideband survey and low frequency narrowband survey can use the same receivers to the extent possible.
    [0075] If low-frequency narrowband sources operate at lower frequencies than conventional wideband sources generate, then conventional wideband and narrowband low-frequency surveys can be performed without considering the other. As used herein, "low frequency" can refer to a frequency or range of frequencies less than about 6-8 Hz. As such, low frequency sources are sources that are capable of emitting seismic energy at a usable amplitude at frequencies below about 6-8Hz. In addition, “low frequency narrowband seismic survey” can refer to surveys that use narrowband low frequency sources.
    [0076] If a single narrowband source operates at a frequency that is within the range of an impulsive wideband source, then the wideband source can be located in proximity to the narrowband source, and the timing of the source wideband pulsed signal synchronized with the operating narrowband source such that the phase of the corresponding frequency component of the wideband source corresponds as closely as possible to the phase of the narrowband source. In this way, interference from broadband sources will not cause harm, but will serve as an additional useful source of low frequency energy.
    [0077] The harmonic waves of narrowband sources can overlap the frequencies of waves produced by conventional wideband sources. In this case, the timing of the triggers in the conventional survey and the narrowband emissions in the low-frequency survey should be chosen such that the conventional triggers avoid overlapping the taper at the beginning or end of any narrowband scan. Any interference must then consist of a very simple repeating signal that can be easily predicted and removed, in a way that is analogous to the way that 50 or 60 Hz hum AC is currently removed from Earth data.
    [0078] Some additional considerations apply specifically to an Earth modality. Ground sources, such as vibrators, are operated at fixed locations, so sources cannot operate continuously. Each suitable or optimal low frequency for the processing algorithm will likely be obtained by generating an adapted monochromatic or narrowband vibrator sweep at a source density adapted for that frequency range. Very long scans obviously take longer, but they can still be practically used because far fewer origin points are used to properly sample the Earth at low frequencies (and this advantage is leveraged because it applies to both the X and Y directions).
    [0079] Monochromatic sources, like impulsive sources, will generate undesirable surface waves ("ground roll") in the earth. For monochromatic fonts these cannot usually be completely removed by muting, due to, among other reasons, the extended signature of the fonts. Thus, they can be removed by spatial filtering. This sets a minimum source and/or receiver group and/or matrix spacing to avoid aliasing (frequency skewing) of surface waves.
    [0080] Some additional considerations apply specifically to a marine modality. Marine sources are usually towed behind a seismic acquisition vessel. Each font can be towed to its optimum depth to take full advantage of Ghost surface anti-notch. To achieve the maximum signal-to-noise ratio, sources can operate continuously, and data can be recorded continuously.
    [0081] To generate data for the sources at the desired locations, the data from a time window centered on the time the source was at the desired location will typically be windowed and a bottleneck such as an applied raised cosine bottleneck to minimize any edge effects due to windowing time, preferably using the same window length and taper that are computationally used in the modeling step of the inversion algorithm. The inversion algorithm's modeling step should also model data from a motion rather than a stationary source so that it better represents the true record geometry. Note that this processing sequence requires only a trivial modification of the time and frequency domain FWI algorithms discussed above.
    [0082] One or more of the low frequency sources may also boost or otherwise alternate between two or more frequencies. Sources can also periodically adjust the amplitude of the emitted waves below zero amplitude and cease sounding and then increase the amplitude either back to its maximum amplitude at the same frequency as before or at a different frequency as needed. to the next “trigger point.” Each source will likely follow its own scheme as needed to optimally provide adequate sampling and total emitted energy over its frequency range. There is no specific reason why the “trigger points” at different frequencies should coincide, although in some modalities they might coincide.
    [0083] A wideband seismic source should be understood as one that is designed to produce usable seismic energy over a relatively wide frequency range (more than 2 octaves). For example, a typical conventional seismic source in current use can emit effective amounts of energy over a frequency in the range of about 5 to about 80 Hz (ie, about 4 octaves). Thus, a conventional seismic survey would be a “broadband” survey for the purposes of this disclosure.
    [0084] On the other hand, a narrowband seismic source should be understood as being one that does not cover a wide frequency range, for example, two octaves or less. For example, at frequencies around 1 Hz, 2 octaves would cover a frequency range of 1-4 Hz. A narrowband source may be so named because its frequency range with usable energy is much smaller than for a typical wideband source, for example, at a frequency in the range of 1 to about 4 Hz, or 1 to about 2 Hz (one eighth) etc. However, a narrowband source may be one where only a limited number of narrow frequency bands are output by the source. For example, a source rich in harmonics that produces very narrow bands centered around 2, 4, 8, 16, 32 and 64 Hz, but with very little energy at frequencies in between, would be considered a narrow band source. Thus, a narrowband seismic source can emit a wave with a discrete low frequency that falls within a narrow frequency band of 2 +/- 0.1 Hz, along with its harmonics, which are also narrowband, so that the cumulative bandwidth of the low frequency wave and its harmonics is narrow (for example, less than a few Hz). For purposes of the present disclosure the term "narrowband source" shall be interpreted to mean at least the types of seismic sources listed above, whether such source(s) is disposed on land or in an environment marine and whether tunable, customizable, modifiable or not (for example, a non-tunable narrowband source may be one that has been specifically designed and constructed for the purposes of emitting a particular narrow seismic signal). A “narrowband seismic survey” will be a seismic survey that has been carried out using one or more narrowband sources.
    [0085] It should be noted that, although the present disclosure has spoken of "almost monochromatic", "monochromatic", "single frequency" and/or "discrete frequency" acoustic sources, these terms should be interpreted to include multiple cases where the source emits substantially at a single frequency, regardless of harmonics. Furthermore, when a seismic survey is described as being “monochromatic” this term is to be understood to mean that a survey was collected in which the source(s) operated at one or a plurality of distinct frequencies. Thus, a narrowband source includes a discrete frequency source as a special case.
    [0086] It should further be noted that although the present invention has been discussed primarily in terms of frequency domain full waveform inversion, the present disclosure would be similarly applicable for the time domain version of the present method processing. The relationship between frequency and time in seismic data is well known, and those skilled in the art will recognize that conversion between these domains is routinely performed.
    [0087] As mentioned above, in some cases, seismic signals from the narrowband survey can be combined with data from a conventional seismic survey at the same or a nearby location to produce an advanced survey that has the bandwidth wider than would be possible with a conventional survey alone. This combination can be done in several ways. For example, it is well known to those skilled in the art how to combine seismic traces (or lines, volumes, etc.) from two different conventional seismic surveys into a single survey. Whenever the trigger and receiver locations are coincident (or nearly coincident), simple stacking (together addition) of the corresponding traces can be used, eventually with amplitude balancing or trace weighting and being used to make the amplitudes in different traces comparable. In other cases, frequency domain balancing before summation can be useful. In cases where the receiving sites differ, interpolation and/or extrapolation can be used to create datasets that can be more easily combined. These are some of the many ways in which two seismic traces with different amplitudes and frequency content and potentially acquired at slightly different locations can be combined. Those of ordinary skill in the art will readily be able to devise other approaches.
    [0088] Furthermore, in some cases, the narrowband survey will have utility that is separate and distanced from any wideband seismic survey. For example, in some embodiments, a plurality of monochromatic sources will be used to collect a narrowband survey. This set of narrowband seismic data will then be subjected to an FWI algorithm that, in some modalities, operates frequency by frequency to calculate an inverse. The resulting inversion can then be used later in seismic prospecting.
    [0089] In the previous discussion, the language was expressed in terms of operations performed on conventional seismic data. However, it is understood by those skilled in the art that the invention described herein can be applied to advantage in other areas of the subject matter, and used to locate subsurface minerals other than hydrocarbons. By way of example only, the same approach described here could be used to process and/or analyze multi-component seismic data, shear wave data, mode converted data, well-crossed survey data, VSP data, shape sonic records waveform, controlled source data or other electromagnetic data (CSEM, t-CSEM, etc.), or model-based digital simulations of any of the above. Furthermore, the methods claimed hereinafter can be applied to mathematically transformed versions of those same data traces, including, for example, filtered data traces etc. In summary, the process disclosed here can potentially be applied to a wide variety of geophysical time series types, but can be applied to a set of spatially related time series.
    [0090] Although the device of the invention has been described and illustrated herein by reference to certain preferred embodiments in relation to the accompanying drawings, various additional changes and modifications, in addition to those indicated or suggested herein, may be made thereto by those skilled in the art. in the technique, without departing from the spirit of the inventive concept, the scope of which must be determined by the following Claims.
    权利要求:
    Claims (11)
    [0001]
    1. Method of Seismic Exploration Above Subsurface Region, containing structural or stratigraphic characteristics favorable to the presence, migration or accumulation of hydrocarbons, characterized in that it comprises the steps of: (a) selecting (210) at least one band frequency band low-frequency narrow; (b) providing (210) at least one narrowband seismic source for each of said at least one low frequency narrowband frequency band, each of said selected narrowband seismic sources emitting seismic energy within a corresponding narrowband low frequency range; (c) performing (220) a narrowband seismic survey near the subsurface region using each of said at least one narrowband seismic source, thereby creating a narrowband seismic survey; (d) collect (210, 220) a wideband seismic survey close to said narrowband seismic survey; (e) using (250) seismic data from said narrowband seismic survey and said wideband seismic survey to calculate a full waveform inversion (240, 260), thereby forming an advanced survey; and (f) using (270) at least a portion of said advanced survey to explore hydrocarbons within said subsurface region, wherein the broadband survey is based on frequencies higher than the frequency range of at least a narrowband seismic source.
    [0002]
    2. Above Subsurface Region Seismic Exploration method according to Claim 1, characterized in that at least one of said at least one narrowband seismic source is a monochromatic seismic source.
    [0003]
    The above Subsurface Region Seismic Exploration method according to Claim 1, characterized in that at least one of said at least one narrowband seismic source is a tunable seismic source.
    [0004]
    4. Above Subsurface Region Seismic Exploration Method, according to Claim 1, characterized in that said narrowband seismic survey and said wideband seismic survey are obtained simultaneously.
    [0005]
    A Seismic Exploration Method Above Subsurface Region, according to Claim 1, characterized in that said narrowband frequency range comprises a frequency range less than or equal to two octaves.
    [0006]
    6. Seismic Exploration Method Above Subsurface Region, according to Claim 1, characterized in that it further comprises the steps of: (a) accessing (210) a complete waveform inversion data set obtained according to the steps of: (1) recording at least one wave field emitted from one of said at least one low-frequency narrowband seismic source; (2) select a full waveform inversion algorithm (240, 260); and (3) using (250) said narrowband seismic survey, said wideband seismic survey, said at least one recorded emitted wave field to calculate a complete waveform inversion (240, 260) along of different frequencies according to said selected full waveform inversion algorithm (240, 260), wherein data corresponding to at least one of said different frequencies is obtained from said narrowband seismic survey and data corresponding to at least one of said different frequencies are obtained from said wideband survey and wherein said at least one emitted wave field is used as input to said modeling part of said full waveform inversion algorithm.
    [0007]
    The above Subsurface Region Seismic Exploration method according to Claim 6, characterized in that said complete waveform inversion dataset is a complete waveform inversion dataset in the frequency domain. .
    [0008]
    The above Subsurface Region Seismic Exploration method according to Claim 6, characterized in that said full waveform inversion dataset is a time domain full waveform inversion dataset .
    [0009]
    9. Method of Seismic Exploration Above Subsurface Region, according to Claim 6, characterized in that said narrowband seismic survey and said wideband seismic survey are obtained simultaneously.
    [0010]
    Seismic Exploration Method Above Subsurface Region, according to Claim 6, characterized in that said narrowband frequency range comprises a frequency range less than or equal to two octaves.
    [0011]
    11. Method of Seismic Exploration Above Subsurface Region, according to Claim 6, characterized in that said narrowband frequency range covers a frequency range less than or equal to 8 Hz.
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    同族专利:
    公开号 | 公开日
    EA026043B1|2017-02-28|
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    MX2013006728A|2013-12-06|
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    法律状态:
    2018-12-18| B06F| Objections, documents and/or translations needed after an examination request according [chapter 6.6 patent gazette]|
    2020-02-04| B06U| Preliminary requirement: requests with searches performed by other patent offices: procedure suspended [chapter 6.21 patent gazette]|
    2020-12-08| B07A| Application suspended after technical examination (opinion) [chapter 7.1 patent gazette]|
    2021-06-08| B350| Update of information on the portal [chapter 15.35 patent gazette]|
    2021-07-13| B09A| Decision: intention to grant [chapter 9.1 patent gazette]|
    2021-08-24| B16A| Patent or certificate of addition of invention granted [chapter 16.1 patent gazette]|Free format text: PRAZO DE VALIDADE: 20 (VINTE) ANOS CONTADOS A PARTIR DE 16/12/2011, OBSERVADAS AS CONDICOES LEGAIS. |
    优先权:
    申请号 | 申请日 | 专利标题
    US42396210P| true| 2010-12-16|2010-12-16|
    US61/423,962|2010-12-16|
    PCT/US2011/065616|WO2012083234A2|2010-12-16|2011-12-16|Seismic acquisition using narrowband seismic sources|
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