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    42 Oilfield Review

    New Dimensions in LandSeismic Technology

    Malik Ait-MessaoudMohamed-Zerrouk BoulegrounAziza GribiRachid KasmiMahieddine TouamiSonatrach

    Algiers, Algeria

    Boff AndersonPeter Van BaarenWesternGeco

    Dubai, UAE

    Adel El-Emam

    Ghassan RachedKuwait Oil CompanyKuwait

    Andreas LaakeStephen PickeringWesternGeco

    Gatwick, England

    Nick MoldoveanuWesternGeco

    Houston, Texas, USA

    Ali zbek

    Cambridge, England

    For help in preparation of this article, thanks to Mark Daly,Jean-Michel Pascal Gehenn, Will Grace, Dominic Lowdenand Tony McGlue, Gatwick, England; Mark Egan andNorm Pedersen, Houston, Texas; Zied Ben Hamad, Lagos,Nigeria; Mahmoud Korba, Algiers, Algeria; and AndrewSmart, Kuwait.

    DSI (Dipole Shear Sonic Imager), Q-Borehole andVSI (Versatile Seismic Imager) are marks of Schlumberger.Omega2, Q-Land, Q-Marine, VIVID and Well-Driven Seismicare marks of WesternGeco.

    Advanced seismic acquisition and processing technology has come onshore.

    A high-fidelity, high-resolution, integrated single-sensor system is now available

    for use on land. This technology marks a significant step forward for exploration,

    field development and production.

    Seismic technology has achieved amazing featsin exploration and production activities in the

    past few decades. The advance to three-

    dimensional (3D) seismic acquisition and

    imaging of the subsurface, introduced in the

    1980s, was perhaps the most important step.1

    Another was development of four-dimensional

    (4D), or time-lapse, seismic data to monitor how

    reservoir properties such as fluids, temperature

    and pressure change during the productive life of

    a field.2 Introduction of multicomponent seismic

    data acquisition with the recording of shear wave

    signals, in addition to compressional wave data,

    provided a tool for rock characterization andidentification of pore-fluid types.3

    With the worlds ever-growing demand for oil

    and gas, the emphasis in the oil and gas industry

    has shifted to exploring deeper, more complex

    reservoirs and to enhancing production from

    existing assets. Field life can be extended by

    delineating bypassed oil and gas and by placing

    production and injection wells optimally. The

    proactive monitoring of reservoir fluid

    behaviorsaturation and pressureover time,

    allows remedial actions to be implemented

    before production is affected.

    For all these applications, the geophysicist,

    geologist and reservoir engineer require reliable

    and repeatable data of exceptional resolution

    that can be fine-tuned to a specific reservoir

    objective. Exceptional data resolution means

    having data with increased frequency bandwidth

    and low coherent and noncoherent noise, while

    preserving signal fidelity.4

    For decades, the battle between signal andnoise has driven the seismic industry to seek

    ways to suppress noise and to enhance signal.

    The signal is a true representation of the actual

    reflection that corresponds to changes in rock

    characteristics such as lithology, porosity and

    subsurface structure. Both noise, which can be

    coherent or noncoherent, and absorption of higher

    frequencies by the Earth obscure the true nature

    of the signal.

    This article examines a new, integrated single-

    sensor acquisition and processing system that

    delivers measurements that were previously

    unobtainable with conventional recording ofseismic data. Examples from producing assets in

    Kuwait and Algeria illustrate the superior quality

    of these data in terms of signal fidelity and

    frequency bandwidth in comparison with data

    acquired with conventional methods.

    Challenges in Conventional Land Acquisition

    Single-sensor seismic recording has been

    available since the early days of seismic

    exploration. The principle is simple. An impulse

    source such as dynamite or a controlled-

    frequency source such as a vibrating plate on a

    truck sends acoustic energy into the Earth.5 This

    energy propagates in many different directions.

    Downward traveling energy reflects and refracts

    when it encounters boundaries between two

    materials with different acoustic properties.

    Sensors or geophones placed on the surface

    measure the reflected acoustic energy,

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    Autumn 2005 43

    converting it into an electrical signal that is

    displayed as a seismic trace.6

    A complication in land acquisition is that,unlike marine data, a seismic line is rarely shot

    in a straight line because of the presence of

    natural and man-made obstructions such as

    lakes, buildings and roads. More importantly,

    variation in ground elevation causes sound waves

    to reach the recording geophones with different

    traveltimes. The Earths near-surface layer may

    also vary greatly in composition, from softalluvial sediments to hard rocks. This means that

    the velocity of sound waves transmitted through

    this surface layer may be highly variable. Static

    correctionsa bulk time shift applied to a

    seismic traceare typically used in seismic

    processing to compensate for these differences

    in the elevations of sources and receivers and

    near-surface velocity variations.7

    Another major problem in land acquisition i

    that land sources typically generate energy tha

    travels horizontally near the surface, also known

    as airwaves and ground-roll noise. Conventiona

    sensor arrays comprising strings of geophones

    1. Beckett C, Brooks T, Parker G, Bjoroy R, Pajot D, Taylor P,Deitz D, Flaten T, Jaarvik LJ, Jack I, Nunn K, Strudley Aand Walker R: Reducing 3D Seismic Turnaround,Oilfield Review7, no. 1 (January 1995): 2337.

    2. Aronsen HA, Osdal B, Dahl T, Eiken O, Goto R,Khazanehdari J, Pickering S and Smith P: Time Will Tell:New Insights from Time-Lapse Seismic Data, OilfieldReview 16, no. 2 (Summer 2004): 615.

    3. Barkved O, Bartman B, Compani B, Gaiser J, Van Dok R,Johns T, Kristiansen P, Probert T and Thompson M:The Many Facets of Multicomponent Seismic Data,Oilfield Review16, no. 2 (Summer 2004): 4256.

    4. Coherent noise is unwanted seismic energy that showsconsistent phase from one seismic trace to another. Thismay consist of waves that travel through the air at verylow velocities such as airwaves or air blast, and groundroll that travels through the top of the surface layer, alsoknown as the weathering layer. The energy trapped

    HardDisk/Processing

    Conventional Data Q-Land Data

    FieldTape

    DigitalGroupForming

    a common-midpoint (CMP) gather. The number of tracessummed or stacked is called a fold. For instance, in24-fold data, every stacked trace represents the averageof 24 traces. In the case of dipping beds, there is nocommon depth point shared by multiple sources andreceivers, so dip-moveout (DMO) processing becomesnecessary to reduce smearing or inappropriate mixing of

    data. For more on seismic recording: Farmer P, Gray S,Whitmore D, Hodgkiss G, Pieprzak A, Ratcliff D andWhitcombe D: Structural Imaging: Toward a SharperSubsurface View, Oilfield Review5, no. 1 (January1993): 2841.

    Ashton CP, Bacon B, Mann A, Moldoveanu N,Dplant C, Ireson D, Sinclair T and Redekop G:3D Seismic Survey Design, Oilfield Review6, no. 2(April 1994): 1932.

    7. Ongkiehong L and Askin HJ: Towards the UniversalSeismic Acquisition Technique, First Break6, no. 2(1988): 4663.

    within a layer, also known as multiples, is another formof coherent energy. Noncoherent energy is typicallynonseismic-generated noise, such as noise from wind,moving vehicles, overhead power line or high-voltagepickup, gas flares and water injection plants.

    5. A vibrator source sends a controlled-frequency sweepinto the Earth. The recorded data are then convolvedwith the original sweep to produce a usable signal.

    6. Each trace consists of one recording corresponding to asingle source-receiver pair. In practice, traces from onesource are simultaneously recorded at several receivers.Then, sources and receivers are moved along the surveyline and another set of recordings is made. When aseismic wave travels from a source to a reflector andthen back to the receiver, the elapsed time is the two-way traveltime. The common depth point (CDP) is thehalfway point of the path; it is situated vertically belowthe common midpoint. Sorting of traces by collectingtraces that have the same subsurface midpoint is called

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    are based on the assumption that the upward

    traveling energy, or the reflected wave, arrives at

    the array essentially vertically and simultaneously,

    while the surface-wave noise arrives mainly

    horizontally and sequentially. To cancel this

    source-generated noise, spatially distributed

    receiver groupsarraysare summed.8 Ideally,

    this process results in an attenuation of the noise

    and an improvement of the signal.

    However, there are problems associated with

    conventional arrays. In reality, the sensor array is

    often not located on flat and homogeneous

    ground, so local changes in elevation and surface

    geology lead to fluctuations in the signal arrival

    time (left). These fluctuations are called intra-

    array perturbations. The hard-wired sensor array

    instantaneously sums all traces, and in the case

    of intra-array perturbations, this would lead to a

    partial cancellation of signal. The resulting

    output trace would then be at a lower frequency

    than each of the input signals, and the amplitude

    would be smaller than the sum of the individual

    amplitudes, a phenomenon known as thearray effect.

    Aliasing is a well-known problem that arises

    when the sampling rate of a signal is inadequate

    to capture the higher frequencies in the signal.9

    Not only is the information contained in higher

    frequencies lost, it is incorrectly represented

    (below left). Aliasing is a consideration for

    spatial sampling too, not just temporal sampling.

    Ground roll typically contains many different

    wavelengthsrelated to the distance between

    successive peaks in a waveformthat are

    shorter than the typical group interval or the

    distance between receiver array centers ofgravity in a conventional survey. Due to

    undersampling of ground-roll energy, this energy

    is aliased and passed on to the signal bandwidth,

    causing ambiguity between signal and noise.

    44 Oilfield Review

    > Conventional acquisition onshore. Seismic energy recorded at the receiversarrives at different times because of elevation differences and near-surfacevelocity variations (top). In conventional acquisition, strings of geophoneshard-wired together average the individual sensor measurements and deliverone output trace, whose location is denoted by the center of gravity of thearray, indicated by the red dot (bottom). The resulting output trace has agenerally lower frequency than each of the input signals, and the amplitude issmaller than the sum of the individual amplitudes, a phenomenon known asthe array effect.

    Receiver array length: 45.76 m

    7

    m

    2.08 m 4.16 m

    Seismicsource Receiver array

    Geophone

    > Aliasing effect. Sampling at a frequency lower than the highest frequencypresent in the signal (red curve) results in insufficient samples to capture allthe peaks and troughs present in the data. Not only will inadequate samplingmiss the information on higher frequencies but the signal will be incorrectlydefined (blue curve).

    t

    samplingrate

    Undersampled seismic signalProperly sampled seismic signal

    8. Newman P and Mahoney JT: PatternsWith a Pinch ofSalt, Geophysical Prospecting21, no. 2 (1973): 197219.

    9. Aliasing is the ambiguity that arises because ofinsufficient sampling. It occurs when the signal issampled less than twice the cycle. The highestfrequency defined by a sampling interval is termed theNyquist frequency and is equal to inverse of 2t, wheret is the sampling interval. Frequencies higher than theNyquist frequency will be folded back or wrappedback. This condition can be observed in video or motion

    pictures: the spoke wheels on horse-drawn wagonssometimes appear to be turning backward instead offorward. Aliasing can be avoided by a finer spatialsampling that is at least twice the Nyquist frequency ofthe waveform.

    10. El-Emam A, Moore I and Shabrawi A: Interbed MultiplePrediction and Attenuation: Case History from Kuwait,presented at the 2005 SEG International Exposition and75th Annual Meeting, Houston, (November 611, 2005).

    11. Roden R and Latimer R: An IntroductionRockGeophysics/AVO,The Leading Edge22, no. 10(October 2003): 987.

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    Tests of varying array lengths have shown the

    degradation in signal quality caused by

    increasing the array size (right). For longer

    offset receiver arrays, the arrival time of the

    signal can vary significantly at either end of the

    array, smearing the higher frequencies when

    summed within the group. Therefore, just as

    adequate temporal sampling of the recorded

    trace is needed to successfully record a given

    frequency, a sufficiently small group interval is

    required to record a particular spatial frequency.

    A problem common to all seismic acquisition

    is energy trapped between subsurface layers,

    known as interbed multiples, caused by a strong

    velocity contrast between layers. This occurs

    when the energy from the source reflects more

    than once in its travel path. Interbed multiples

    are analogous to a bouncing ball trapped between

    two layers, which continues to bounce until it

    loses its energy. Borehole seismic data, which are

    acquired when sources are placed on the surface

    and receivers are anchored in a borehole, help

    identify the interfaces that generate theseinterbed multiples. Recent developments in data-

    driven methods and the use of vertical seismic

    profile (VSP) data to guide surface-seismic

    multiple attenuation, such as Interbed Multiple

    Prediction (IMP), seem promising.10

    The quality of the raw seismic dataset is

    fundamental to achieving superior frequency

    resolution and high signal-to-noise ratio.

    Amplitude and phase preservation of the input

    signals is critical in all facets of stratigraphic

    interpretation, including prestack seismic

    inversion, amplitude variation with offset (AVO)

    and amplitude variation with angle (AVA)interpretation. An analysis of the variation in

    reflection amplitudes with source-geophone

    distance or offset gives some valuable insights

    into reservoir properties such as lithology,

    porosity and pore fluid.11

    Because land data often exhibit poor signal-to

    noise ratios arising from irregular geometries and

    noise contamination, a fundamental change in

    acquisition and processing methods was required.> Signal degradation with an increase in array size. A point-source, point-receiver test was carriedout with single sensors spaced 2 m [6.6 ft] apart and a single vibrator source. A 16-m [53-ft] arraywas formed by summing groups of nine consecutive geophones and assigning the summed signalto a channel placed in the center of gravity of the array (bottom). The group interval is the distance

    between consecutive channels. Similarly, a 32-m [105-ft] array was formed by summing groups of17 consecutive geophones. By using 2-m sensor spacing, wave types were recorded without aliasing(top left). As the sensors were grouped into arrays of increasing length of 16 m ( top middle) and32 m (top right), first the airwave, then the ground roll and finally the first breaks became aliased,manifested as cross-banded signal areas in the shot domain. Aliasing also manifests as a wrap-aroundof the noise energy in the frequency-wavenumber domain, not shown here. (Data courtesy of Shell.)

    0.0

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    Channel 3Channel 2Channel 1

    Group interval

    Reflectedwaves

    Airw

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    A Change in Acquisition Philosophy

    In the early 1990s, WesternGeco began extensive

    research on compressional wave (P-wave)

    sensitivity that led to a fundamental change in

    acquisition philosophy. Experiments conducted

    on synthetic signals revealed the effects of

    source and receiver statics, recording electronics

    specifications, source phase distortion and

    receiver sensitivity on P-waves (below).

    Excluding coherent source-generated noise,

    ambient noise and source frequency sweep, the

    dominant effects on the signal-to-noise ratio are

    due to perturbations that could not be corrected

    for within an analog array. Factors such as source

    and receiver statics, coupling of the geophone to

    the ground, geophone position and tilt, source

    positioning, and amplitude and phase distortion

    in the sources were more important than

    hardware changes in the geophone or the

    recording system itself. A small error of 1 ms in

    receiver statics results in the introduction of

    -29 dB of noise relative to the signal. Such static

    errors are commonly found within a conventionalanalog receiver group.

    Knowledge gained from these experiments

    was used to design and build the Q-Land single-

    sensor land seismic system to reduce the effects

    of these perturbations while addressing the issue

    of coherent noise removal such as ground roll. A

    receiver spacing that is half (or less) of the

    ground-roll wavelength would be adequate to

    sample ground-roll noise without aliasing. Just as

    temporal aliasing arises from insufficient

    sampling in time, a large receiver interval leads

    to spatial aliasing.

    The new Q-Land system digitizes each sensor

    at the recording location (next page, top). To

    achieve this fine spatial sampling, the recording

    system requires a massive increase in the

    number of live channels. A live channel means

    that the receivers are connected to record

    simultaneously. Compared with a typical high

    channel-count conventional system, which may

    have 4,000 to 5,000 channels that record live, the

    new point-receiver acquisition system has 20,000

    or more live channels. The Q-Land system is the

    first to implement an integrated point-receiveracquisition and processing methodology.

    The same concept is applicable to the seismic

    sources. The source array can be replaced by

    point sources. In addition, to prevent aliasing in

    the common midpoint domain, the source

    interval should be small, ideally equal to the

    receiver interval. The new point-source, point-

    receiver recording technique replaces the

    conventional method of using sensor and source

    arrays to attenuate noise and to improve signal-

    to-noise ratio.12 Recording seismic data through

    point receivers rather than analog receiver

    arrays has several potential advantages,

    including better static solutions, velocity

    estimation, amplitude preservation, bandwidth

    retention and noise attenuation.

    This point-source, point-receiver methodology

    increases data volume by more than an order of

    magnitude. Advances in data transmission and

    computing power have enabled the development

    and deployment of this cost-effective, high

    channel-count recording system.

    A New Integrated Acquisitionand Processing System

    The new Q-Land system is a 20,000 live-channel

    seismic acquisition and processing technology.

    The typical sampling rate for the system is 2 ms.

    However, the Q-Land system can record with

    30,000 live channels when the sample rate is

    changed to 4 ms. Digital recording of the

    incoming wavefield at densely spaced receiver

    positions ensures that the recorded signal

    and noise are properly sampled and are

    therefore unaliased.

    In Q-Land acquisition geometry, one source

    line and one receiver line that are orthogonal toeach other form a cross-spread. These are then

    repeated spatially within the acquisition area.

    Each source-receiver pair generates a trace that

    corresponds to a subsurface midpoint. If the

    midpoints corresponding to all source-receiver

    pairs are binned, with a bin size equal to half the

    receiver by half the source interval, every bin will

    be one midpoint corresponding to single-fold

    coverage. Thus, the cross-spreads provide single-

    fold subsets of the continuous wavefield, sampled

    finely enough to prevent aliasing of the coherent

    noise, through which a cross-spread volume is

    generated (next page, bottom).

    46 Oilfield Review

    > P-wave sensitivity chart for land acquisition. Experiments were conducted on synthetic signals tounderstand the effect of perturbations such as source and receiver statics, recording electronics,source phase distortion, and receiver sensitivity. The chart shows that hardware changes in thereceiver or the recording system have low signal error, as compared with other factors that cause asignificantly higher signal error. The ability to correct for these higher order perturbations allows forthe preservation of signal fidelity and bandwidth within the seismic data.

    Distortion

    Gain tolerance

    Synchronization

    0 -10 -20 -30 -40 -50

    Signal error in dB

    Signal error, %, 95% confidence interval

    Perturbation

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    100 31.6 10 3.16 1 0.32 0.1 0.03 0.01 0.003

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    Statics

    12. Ongkiehong and Askin, reference 7.

    13. Christie P, Nichols D, zbek A, Curtis T, Larsen L,Strudley A, Davis R and Svendsen M: Raising theStandards of Seismic Data Quality, Oilfield Review13,no. 2 (Summer 2001): 1631.

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    Sophisticated algorithms are then applied in

    a processing technique called digital group

    forming (DGF). DGF comprises three main steps.

    The first is correction to each geophone for intra-

    array perturbations such as amplitude, elevation

    differences and near-surface velocity variations.

    After the geophone outputs are grouped, the

    result is a signal with a frequency bandwidth

    similar to that of the individual traces and an

    amplitude almost equal to the sum of the

    individual amplitudes. This step is similar to the

    one applied in the Q-Marine single-sensor

    marine seismic system.13

    > A three-dimensional (3D) display of the cross-spread volume. A cross-spread configuration is achieved by deploying receivers along a line in onedirection and placing sources along an orthogonal line (right). Each source-receiver pair generates information from a subsurface point that, for a flatsurface, is located at the midpoint between source and receiver (gray area). In this example of cross-spread configuration, with receiver sampling at 5 m[16 ft] and source sampling at 20 m [66 ft], the subsurface coverage is single fold. A 3D view of the cross-spread volume shows that the ground-roll noiseis confined within a conical shape volume, making its removal or attenuation by 3D filters in the frequency-wavenumber domain more effective (left).

    ReceiverlineSourcelin

    e

    Time

    Sourceline

    Receiver line

    Area ofcommonmidpointcoverage

    > The Q-Land acquisition and processing system. A line ofreceivers is laid out perpendicular to a line of sources andevery source point is recorded by every receiver point. Theexample shows 10 receiver lines that are 200 m [656 ft] apart,with 1,824 point receivers per receiver line that result in18,240 live receivers (top). In digital group forming using theOmega2 software processing system, the seismic traces fromindividual geophones have perturbation corrections made toeach geophone (bottom). Data-adaptive filters are thenapplied over a number of traces to suppress coherent noise.An output trace from a number of sensors can then be pro-duced at the desired spatial sampling.

    Sou

    rceline

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    Sensors

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    The second step applies data-adaptive filters

    for noise suppression. Noise attenuation can

    include, but is not limited to, coherent and

    ambient-noise attenuation, high-voltage power

    line pickup cancellation, and airwave and flare-

    noise attenuation. There are different ways to

    attenuate noise using digital filtering techniques.

    However, the design of optimal 3D digital filters

    is important to realize the potential of point-

    receiver recording.

    An ideal filter would pass all the desired

    frequencies in the pass band with no distortion,

    and completely reject all frequencies outside the

    range of interest, called the stop band. The ideal

    spatial anti-alias filter response would also be

    azimuthally isotropic, that is the array response

    would be the same for energy arriving from all

    angles. There are two problems associated with

    anti-alias filter performance for conventional

    data acquisition: imperfect rejection of

    azimuthally varying levels of noise in the stop

    band and an imperfect flat response in the pass

    band (below). The Q-Land technique of forming

    an orthogonal acquisition geometry into cross-

    spreads is well suited to the application of three-

    dimensional anti-alias filters. A filtering

    technique based on the APOCS method

    alternating projections onto convex setsis an

    effective approach that works optimally on cross-

    spread geometry.14

    48 Oilfield Review

    14. A well-known mathematical technique, APOCS is aniterative technique that derives filter parameters toremove coherent noise. The algorithm, working in 3Dspace, switches constantly between sample domainwith time on one axis and x and y on the other twoaxesand frequency transform domainwithfrequency on one axis and wavenumber in x and y

    directions, kx and ky, on the other two. Wavenumber isthe inverse of wavelength and represents the frequencyof the wave in space. For more on APOCS: zbek A,Hoteit L and Dumitru G: 3-D Filter Design on aHexagonal Grid for Point-Receiver Land Acquisition,EAGE Research Workshop, Advances in SeismicAcquisition Technology, Rhodes, Greece,September 2023, 2004.

    Quigley J: An Integrated 3D Acquisition and ProcessingTechnique Using Point Sources and Point Receivers,Expanded Abstracts, 2004 SEG International Expositionand 74th Annual Meeting, Denver, (October 1015, 2004):1720.

    17. A zero-offset VSP is acquired when a seismic sourceis placed on the surface close to the wellhead andreceivers are positioned at different depths in aborehole. In a walkaway VSP, an array of receiverscollects data for multiple source positions located alonga line that extends from the wellhead. For more on VSPand walkaway VSPs: Arroyo JL, Breton P, Dijkerman H,

    Dingwall S, Guerra R, Hope R, Hornby B, Williams M,Jimenez RR, Lastennet T, Tulett J, Leaney S, Lim T,Menkiti H, Puech J-C, Tcherkashnev S, Burg TT andVerliac M: Superior Seismic Data from the Borehole,Oilfield Review15, no. 1 (Spring 2003): 223.

    15. Shabrawi A, Smart A, Anderson B, Rached G andEl-Emam A: How Single-Sensor Seismic ImprovedImage of Kuwaits Minagish Field, First Break23, no. 2(February 2005): 6369.

    16. The Q-Borehole system optimizes all aspects of boreholeseismic services, from job planning through dataacquisition, processing and interpretation. Well logs,VSP and surface-seismic data are combined to build aproperty model of vertical velocities, frequencyattenuation factors, anisotropy related to verticalvariations in interval velocities and the multipleswavefield. The model is then used for enhancedsurface-seismic processing and calibration in theWell-Driven Seismic process.

    > Three-dimensional spatial anti-alias filter response. The problem of unwanted noise contaminating the signal bandwidth area is illustrated. The spatialanti-alias filter response displays amplitude on the vertical axis, and wavenumbers along the two horizontal axes, kx and ky, in x and y directions. The color

    represents the magnitude in dB. An efficient filter would pass the signal that is at around k=0, and stop or reject any noise for all other directions for k 0.For a conventional 16-m receiver array, noise leaks into the signal from almost all azimuths ( left). In contrast, for point-receiver data, the anti-alias filterusing the APOCS filter design technique shows the effectiveness of the filter in rejecting noise ( right).

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    Autumn 2005 49

    The last step is spatial resampling of the

    output data according to the desired group

    interval. Analog arrays, once laid out in the field,

    have almost no flexibility to adjust the output-

    sampling interval, whereas with digital group

    forming, any output sampling is possible down to

    the granularity of the individual sensors.

    While data from conventional arrays may

    provide reasonable results for structural

    interpretation, detailed reservoir analysis using

    seismic inversion or AVO techniques is limited to

    a narrow frequency band because of aliased

    noise wrapping back in the frequency range of

    interest (below right). With such reduced

    bandwidth, AVO and inversion are unlikely to

    produce meaningful results. The densely spaced

    point receivers employed by Q-Land methodology

    provide alias-free data, and hence, a more

    complete bandwidth for AVO interpretation.

    In complex geological settings where conven-

    tional array data are unable to deliver the

    required results, single-sensor data provide

    significant improvement in signal fidelity andfrequency bandwidth. This improvement enables

    interpretation of subtle stratigraphic features

    and increased vertical and lateral resolution of

    the seismic response as demonstrated in the

    following two examples from Kuwait and Algeria.

    Pioneering New Technologies in Kuwait

    The Minagish field in southwestern Kuwait was

    selected for a Q-Land pilot study in 2004, to

    address several development and exploration

    objectives. One goal was to provide a detailed

    image of multiple reservoir intervals within the

    Cretaceous for fluid-front monitoring.Discovered in 1959, the Minagish field is one

    of the countrys main producers, with production

    primarily from carbonate rocks, including the

    Minagish oolites. A waterflood program resulted

    in water influx overriding oil in layers with

    high permeabilities.

    A previous 3D seismic survey in 1996, with

    source and receiver arrays of 50-m [165-ft]

    spacing, provided poor imaging of deeper

    prospects and limited the vertical and lateral

    resolution at principal reservoir zones.

    Characterizing fracture density and orientation,

    necessary to optimally place horizontal wells and

    maximize production, was also a problem. Noise

    arising from gas flares and water injection plants,

    coupled with seismic-generated noise such as air

    blast, ground roll and multiples, caused extreme

    distortions in the seismic data.

    In addition, the Minagish field posed an

    unusual operational hazard. The area was strewn

    with unexploded cluster bombs and mines from

    earlier military activity.

    A detailed understanding of the internal

    reservoir structure was essential for a planned

    water injection scheme to work. Forward seismic

    modeling using rock properties from core

    samples and logs has shown that a 5 to 95%

    change in water saturation could result in a 5%

    difference in acoustic impedancea product of

    velocity and density of the rock. However, a

    previous 4D study in 1998 shows the inability to

    detect these small changes due to the

    background noise level in conventional seismic

    data. Some of the limiting factors were frequency

    resolution, inferior noise attenuation and a low

    signal-to-noise ratio. To allow monitoring of

    minute changes in reservoir behavior, it was

    obvious that a step change in acquisition

    methodology was necessary to reduce noncoherent

    signal and coherent noise.

    Four tightly grouped vibrators in a rectangle

    of 12.5 m [41 ft] by 5 m [16.4 ft] vibrated in

    synchrony at 60% of their peak force capability o

    80,000 lbf [356 kN]. Driving at less than peak

    force provided a low distortion in the seismic

    source. The vibrators were set as close a

    possible to resemble a point source while

    maximizing energy input into the Earth. The

    Q-Land system recorded 14,904 channels at a

    2-ms sampling rate.15 Perturbation correction

    were made to each receiver and each source

    prior to summation in the DGF process.

    In addition, a Q-Borehole integrated borehole

    seismic study was planned at the inception of the

    Q-Land pilot program.16 A zero-offset VSP and

    two walkaway VSPs recorded the data around the

    center of the survey area.17 The integration o

    surface seismic and borehole geophysical data

    was vital to ensure that all steps in the

    processing sequence, from digital group forming

    through to the final migrated stack, were

    optimally calibrated utilizing some of the latest

    > Impact of aliasing on frequency bandwidth. A test conducted with a 16-m receiver array displaysaliasing of ground roll and airwave because of the wrap-around effect seen in the frequency-wavenumber (fk) domain (left). The airwave (solid black line) is completely aliased. However, the

    ground-roll noise (dashed black line) is folded back into the signal frequency band above thefrequency where the dashed lines intersect. The signal, which is expected to dominate the centralarea of the fk plot as k approaches zero, becomes contaminated. This means that data-adaptivespatial filtering can no longer remove the coherent noise without damage to the signal. The usablefrequency bandwidth for AVO processing, for example, is substantially reduced for conventional arraydata because aliasing distorts the higher frequencies in both amplitude and phase. In contrast to thispoint-receiver data clearly show an unaliased response that permits processing of the entire usefulfrequency range without coherent noise contamination (right). (Data courtesy of Shell.)

    U s a b l e b a n d w i d t h

    -200 -100 0

    Wavenumber, 1/km

    Point Sensors at 2 m

    100 200

    Usable

    bandwidth

    60

    50

    40

    30

    20

    10

    0

    -30 -20 -10 10 200

    Wavenumber, 1/km

    30

    Frequency,

    Hz

    60

    50

    40

    30

    20

    10

    0

    Frequency,

    Hz

    Aliasednoise

    16-m Array

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    developments in the Well-Driven Seismic

    process.18 Restoration of true amplitude

    and phase, effective multiple suppression

    and compensation for frequency absorption

    with depth provided superior imaging and

    resolution (above).

    The zero-offset VSPs at two control wells, an

    injector and a producer, resolved seven intra-

    reservoir zones. Conventional seismic data, with

    a frequency bandwidth of 10 to 45 Hz, showed

    only three of these events, which led to a flawed

    interpretation that there were no obstructionsbetween the two wells and injected fluids could

    flow freely between two wells. The Q-Land

    volume imaged the same seven intrareservoir

    zones seen on the VSPs. The enhanced resolution

    from Q-Land data, with a frequency bandwidth of

    6 to 70 Hz, enabled the seismic interpreters to

    map stratigraphic features. Also identified were

    tar mats at the injector well that act as baffles

    and inhibit fluid movement. In addition, minor

    faults and deeper gas targets obscured by

    interbed multiples energy were now imaged.19

    Encouraged by the results of this Q-Land pilot

    study, the operator is in the process of planning a

    full-field survey using the Q-Land system. Plans

    to reevaluate pore pressure and fracture

    characterization incorporating the new Q-Land

    data are also under consideration.

    The Seismic Challenge in Algeria

    An oil field in Algeria, known to be one of the

    most seismically challenging fields in the world,

    was selected for a Q-land study. Since the

    discovery of this field in the 1950s, many wellshave been drilled. Oil and gas production is

    mainly from Cambro-Ordovician fluviomarine,

    clastic reservoirs. Despite the large number of

    wells drilled, abrupt changes in lithology and

    fault compartmentalization have made full-field

    reservoir characterization from well data alone

    difficult. Few seismic surveys have been

    attempted in the past because of a poor seismic

    response and failure to image the reservoir

    zones. As a result, reservoir zones were identified

    from petrophysical and pressure data. In

    addition, a weak correlation between well

    log and core permeability indicated that

    the permeability could be strongly influenced

    by fractures.

    There are several geophysical and geological

    challenges. The main producing reservoir, a

    braided-channel fluvial system, has a highly

    heterogeneous distribution of sand and shale.

    The oil field has also been affected by multiple

    episodes of fault deformation and reactivation,

    resulting in complex fault and fracture patterns

    that are difficult to image. Added to these

    problems, a small velocity and density contrast at

    the top of the reservoir and within the reservoir

    units makes detection of reservoir units difficult.

    In addition, the influence of strong interbedmultiples obscures the signal, and the presence

    of a thick evaporite layer above the reservoir

    causes severe attenuation of higher frequencies,

    resulting in a poor signal-to-noise ratio. All these

    problems lead to a poor tie to wells, making it

    extremely difficult to map the interwell region.

    Typically, the maximum usable frequency

    obtained from the target reservoir has been

    around 35 to 40 Hz. This translates into a

    maximum vertical resolution of 40 m [131 ft].

    However, mapping the reservoir units with any

    degree of confidence requires a vertical

    resolution of less than 20 m and much lower

    noise levels.

    50 Oilfield Review

    18. The Well-Driven Seismic process uses borehole seismicdata for true amplitude and phase recovery, velocityanalysis, multiple attenuation, anisotropic migration andangle-based muting. For more on the Well-DrivenSeismic technique: Morice SP, Anderson J,Boulegroun M and Decombes O: Integrated Boreholeand Surface Seismic: New Technologies for Acquisition,Processing and Reservoir Characterization; HassiMessaoud Field, presented at the 13th SPE Middle EastOil and Gas Show and Conference (MEOS), Bahrain,June 912, 2003.

    19. El-Emam et al, reference 10.

    > Comparison of conventional 3D seismic data and Q-Land data in the Minagish field, Kuwait. The Q-Land data ( right) show a much higher lateral andvertical resolution as compared with conventional seismic data (left). The Minagish target reservoir appears at about 1,500 ms.

    1,400

    1,500

    1,600

    Two-waytraveltime,

    ms

    Conventional 3D Data Q-Land Data

    1,700

    1,800

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    Autumn 2005 51

    A pilot survey with the Q-Land system was

    initiated to address these geophysical and

    geological challenges. Integration of borehole-

    seismic data and surface-seismic data was

    planned at the onset of the project, and the

    acquisition parameters were optimized through

    presurvey planning and testing.

    Q-Land seismic data were acquired over an

    area covering 44 km2 [17 mi2], with a dense grid

    of sensors, equating to a density of 20,000 sensors

    per km2. Borehole geophysical data included

    measurements of zero-offset VSP, a two-

    dimensional (2D) walkaway VSP using the VSI

    Versatile Seismic Imager with 154 geophone

    positions in the borehole, and sonic measure-

    ments using the DSI Dipole Shear Sonic Imager.

    The Q-Borehole seismic system aided in

    Well-Driven Seismic processing.

    The surface-seismic processing results were

    compared with well data at key stages in the

    processing sequence, so that the processing

    parameters were optimized to tie the fina

    seismic data to the wells. The bandwidth

    obtained ranged from 6 Hz to 80 Hz, nearly

    double the previously recorded high-resolution

    2D seismic results. For the first time, the

    frequency resolution obtained from surface

    seismic data matched that obtained from a VSP

    providing an excellent well tie (below).

    > A Q-Land example from Algeria. Exceptional resolution (frequencies above 80 Hz) was obtained with the Q-Land survey (top right), in which the frequencybandwidth has nearly doubled in comparison to a high-resolution 2D survey (top left). In addition, the excellent match between the vertical seismic profile(VSP) data (shown within the red box, bottom) and Q-Land data will permit advanced reservoir characterization studies. (Data courtesy of Sonatrach.)

    High-Resolution 2D Data Q-Land Data

    Two-waytraveltime,

    ms

    X,500

    X,600

    X,700

    X,800

    X,900

    Y,000

    Y,100

    Distance Distance

    VSP

    Distance

    Two-waytraveltime,

    s

    X.4

    X.5

    X.6

    X.7

    X.8

    -25

    -20

    -15

    -10

    -5

    0

    -400 20 40 60

    Frequency, Hz

    Power,dB

    80 100 120

    -35-30

    Signal

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    Seismic amplitude was inverted to compute

    absolute acoustic impedance (AI) volume (above).

    Low AI correlates reasonably well with high-

    porosity sands. At 80-Hz frequency, for an interval

    velocity of about 4,500 m/s [14,765 ft/s], this low AI

    zone equates to a thickness resolution of about

    14 m [46 ft]. This degree of resolution has never

    been achieved in this geological environment.

    To assess the relationship between perme-ability and fault proximity, which is generally

    associated with higher fracture density, several

    seismic attributes were computed.

    Extraction of fractures and faults from the

    seismic data involved several steps. Seismic

    attribute cubes that enhance discontinuities

    in the data, also known as edge-enhancing

    attributes, were computed. The edge-detection

    seismic volumes include variance, dip and

    deviation. The ant-tracking algorithm was then

    applied to the edge-detection cube to highlight

    the discontinuities in the seismic data, and to

    map faults and fractures.20 Distance to fault

    (DTF) attributes were then generated from

    filtered sets of faults from the ant-track cube and

    mapped into the 3D geocellular grid (next page).

    The DTF attribute helps identify zones that

    are highly fractured. A crossplot between

    permeability and DTF confirms the trend: higher

    well log permeability when close to faults. Astrong inverse relationship between core

    permeability and DTF was observed on about 70%

    of wells.

    However, to answer questions about whether

    those fractures and small-scale faults enhance or

    degrade permeability, grid cells were extracted

    in the vicinity of seismic faults with greater

    length, that is, those that intercept both

    basement and the overlying Hercynian

    unconformity. Seismic acoustic impedance was

    then mapped into these cells to discriminate

    between sealing and draining faults. A high cell-

    average acoustic impedance in the vicinity of a

    fault suggests that the fractures act as flow

    barriers, because the fractures were cemented

    with pyrite or shale. Conversely, a low acoustic

    impedance in the vicinity of a fault suggests a

    higher proportion of open, fluid-filled fractures,

    which have lower density than rock. This may

    suggest that tectonically induced fractures

    enhance draining of hydrocarbon.

    Wells are continually being drilled in this

    area, and additional drilling is planned in 2006

    guided by the interpretation results of the

    Q-Land data.

    Toward Fit-For-Purpose Seismic Data

    The fundamentally improved measurements

    delivered by Q-Land technology radically expand

    the potential of seismic data. With the lower noise

    associated with single-sensor acquisition and

    processing, and the ability to correct for

    perturbations within a group, array design and

    fold are no longer the dominant factors inimproving signal-to-noise ratio. Rather, sensor

    spacing and a requirement to adequately sample

    coherent noise become the main drivers in

    designing the acquisition geometry. Since it is

    now possible to recover a signal more faithfully,

    the vibrator source can also be reevaluated,

    making it possible to record shorter, single

    sweeps of frequency with a better sampling of

    the wavefield.

    These design considerations now offer the

    possibility of acquiring point-source and point-

    receiver exploration surveys with a lower field

    effort, compared with equivalent surveys usingconventional source and receiver arrays. The

    Q-Land surveys acquired to date suggest that the

    use of smaller groups of vibrators can provide

    data that are equal to or better than larger arrays

    of vibrators and geophones. Smaller groups of

    vibrators allow for more efficient operation.

    The Q-Land VIVID imaging services enhance

    the value of seismic data recorded throughout

    the life of a field. In the exploration phase, the

    low-noise Q-Land data make it possible to

    acquire high-quality seismic surveys with wider

    line spacing and lower fold than a survey

    acquired with conventional technology and still

    meet or exceed the imaging expectations. In

    subsequent surveys for appraisal or development,

    it is possible to acquire the data by interleaving

    lines between the previous surveys to build up

    the fold. The data from the original surveys and

    the current survey are processed together using

    52 Oilfield Review

    > Acoustic Impedance (AI) cross section. The Hercynian unconformity forms the top of the reservoirzone (dashed line). The vertical thickness of the low AI interval within the reservoir section indicatesa thickness in the range of 10 to 15 m [33 to 49 ft]. (Data courtesy of Sonatrach.)

    Well AcousticImpedance

    Distance

    Two-waytra

    veltime,s

    Normalizedacousticimpedance

    Low

    High

    Depth

    ,ft

    X.9

    XY,000

    XX,000

    Y.0

    Y.1

    33 to 49 ft

    Reservoirsection

    20. The ant-tracking algorithm delineates discontinuities in aseismic cube and maps faults and fractures. Thealgorithm tracks discontinuities built upon previousknowledge, mimicking the behavior of ants when theyfind the shortest path between their nest and their foodsource. The ants communicate using pheromones, achemical substance that attracts other ants. Therefore,the shortest path to the food source will be marked withmore pheromones than the longest path, so the next antis more likely to choose the shortest route, and so on.The idea is to distribute a large number of theseelectronic ants in a seismic volume. Ants deployed

    along a fault should be able to trace the fault surface forsome distance before being terminated. The algorithmthen automatically extracts the result as a set of fault-patches, a highly detailed mapping of discontinuities.Fault discrimination is based on the size of the fault, itsorientation, and on the amplitude of verticaldisplacement. For more on ant tracking: Pedersen SI,Randen T, Snneland L and Steen : Automatic FaultExtraction Using Artificial Ants, Expanded Abstracts,2002 SEG International Exposition and 72nd AnnualMeeting, Salt Lake City, Utah, USA (October 611, 2002):512515.

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    A t 2005 53

    the required group interval to image the target

    correctly. This is the concept of uncommitted

    seismic data for the life of a field.

    Exploration leads can be pursued during the

    same survey. This results in a lower cumulative

    environmental footprint of the overall seismic

    program, in addition to reduced development

    time. As the data have a high signal-to-noise ratio

    and fidelity, they can be reused at each stage of a

    fields development, ensuring that the explora-

    tion investment is not lost.

    With unsurpassed seismic data quality and a

    versatile approach to acquisition geometry and

    innovations in processing, the Q-Land acquisi

    tion and processing system will have a major

    impact on the life of the field, in exploration

    development and reservoir monitoring. RG

    > Relationship between seismic acoustic impedance and permeability. Seismic acoustic impedance (AI) and distance to fault (DTF)attributes are combined and mapped onto a geocellular volume ( top). A dual filter based on proximity to fault and seismic AI thresholdvalue is applied to the volume. The filtering assumes that fractures that are open and fluid-saturated have lower velocity and density,and therefore lower AI (bottom right). These are discriminated against faults that are cemented, with higher AI caused by silicificationor pyrite filling (bottom left). (Data courtesy of Sonatrach.)

    High Acoustic Impedance Along Faults

    Combined Acoustic Impedance and Distance to Fault Attributes

    Low Acoustic Impedance Along Faults

    Flow barriers

    Fractures enhancing permeability