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  • 7/31/2019 QAB2054 Intro Rx Physics [Compatibility Mode]

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    Seismic InterpretationSeismic InterpretationQAB 2054QAB 2054

    SeismicSeismic Spectral AttributesSpectral Attributes

    GeoscienceGeoscience and Petroleumand PetroleumEngineering DepartmentEngineering Department

    6th6th October 2010October 2010

    o Seismic attributes in perspective

    Outline of lecture:-

    o Seismic stratigraphic analysis

    o Seismic wave propagation

    o Seismic spectral analysis

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    attributes

    o Application of specdecom attributes

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    Outcomesof

    the

    lecture:

    Knowledgeof seismicwavespectrums

    Awareofspectralanalysisprocedures

    Describeapplicationofspecdecom in

    seismic interpretationjob

    Inter retation skill in seismic

    stratigraphic domains

    SeismicAttributesarespecificmeasuresofgeometric,kinematic,dynamic,and

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    Measuresof:

    Reflectoramplitudeandtime,energybetweenformationtopandbottom(reflectors),reflectordipandazimuth,illumination,coherence,amplitudeversusoffsetandspectraldecomposition

    egenera a r u escanre a e rec y os ra grap cdeposition(depositionalfacies),tectonicdeformation,and

    reservoirproperties

    ATTRIBUTE CLASSIFICATION

    GEOMETRIC SPECTRAL AVO

    . DIP / AZIMUTH . INSTANTANEOUS(Amp, freq, phase)

    Acoustic Impedance

    Elastic Im edance

    .

    . COHERENCY

    WAVEFORM CLASS

    . SPEC. DECOMP

    Intercept

    Gradient

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    - Surve and Positionin- Seismic Survey Design

    GEOPHYSICAL EXPERTISE

    GEOPHYSICAL CLASSIFICATIONGEOPHYSICAL CLASSIFICATION

    GEOPHYSICS

    SEISMOLOGY - Seismic Data Acquisition- Seismic Data Processing

    - OBC 4 C / Shear Seismic

    SEISMICINTERPRETATION

    3D Visualisation

    Volume Interpretation

    Exploration Success Through

    Innovative Solutions

    QUATITATIVEGEOPHYSICS

    - AVO & Rock Physics- Seismic Inversion

    - Structural Modeling & Imaging- Seismic Attribute Analysis- Time Lapse Seismic

    GEOMORPHOLOGY

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    Erosional Truncation Top Lap Concordance

    Seismic Attributes should able toHel the identification of these

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    On lap Down lap

    Geological fealures.

    Dip / Azimuth Coherency

    Instantaneous Attribute

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    SEISMIC STRATIGRAPHY

    Classify the Seismic Section into Geological Units based on

    Frequency

    Continuity

    Frequency ContinuityAmplitude

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    L

    M

    H

    L

    M

    H

    L

    M

    H

    Seismic Waves Surface Waves

    Body Waves

    10

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    1. P-wavesParticle motion parallel to wave propagation

    wavedirection

    11

    2. S-wavesParticle motion perpendicular to wave propagation

    Seismic Wave PropagationSeismic Wave PropagationAn impulsive force like a blast from dynamite source or Air gun creates a seismicAn impulsive force like a blast from dynamite source or Air gun creates a seismicwave that propagates in the earth . Waves can travel inside the earths body or onwave that propagates in the earth . Waves can travel inside the earths body or onthe surface of the earththe surface of the earth

    v yv y ::There are two types of waves : Body waves like P Longitudinal waves and S: ShearThere are two types of waves : Body waves like P Longitudinal waves and S: Shearwaves .Surface waves are called Rayleigh and Love waves. In contrast to bodywaves .Surface waves are called Rayleigh and Love waves. In contrast to bodywaves ( in seismic band ) surface waves arewaves ( in seismic band ) surface waves are attenuativeattenuative and dispersive.and dispersive.

    BODY WAVE : P & SBODY WAVE : P & S

    Particle motion in P waves is in the same direction as the wave, . P waves areParticle motion in P waves is in the same direction as the wave, . P waves arecaused rimaril b chan e in volume . P wave velocit de end hence on Bulkcaused rimaril b chan e in volume . P wave velocit de end hence on Bulk

    12

    modulus Kmodulus K Longitudinal P wave (Compressional & Refraction)

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    TRANSVERSE OR SHEAR WAVE

    Shear Wave on the other hand are created due to

    13

    .

    motion is perpendicular to the direction of propagation

    of wave.

    SEISMIC REFLECTION PROCESS IN EXPLORATION

    Fig 1(b)

    The physical process of reflection is illustrated above for one reflector in (a) and severalsuccessive reflector in depth in ( b), There are commonly several layers beneath the earth'ssurface that contribute reflections to a single seismogram. The unique advantage of seismicreflection data is that it permits mapping of many horizon or layers with each shot.

    Fig 1(a)

    14Multi-channel recordings for seismic reflection

    Figure 2 indicates the arrivals that recorded on a multi-channel seismograph. Note that the subsurfacecoverage is exactly one-half of the surface distanceacross the geophone spread. The subsurface samplinginterval is one-half of the distance between geophones

    on the surface

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    Vertical (Temporal) Resolution Limits

    Full Wavelength

    Resolved Layer

    Half Wavelength

    Resolved Layer

    Quarter Wavelength

    Unresolved Layer

    (Detected)Single Reflection

    No Layer

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    Physical Factors Affecting Seismic Wave Propagation

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    Convolutional Model

    + =Time

    *

    Source Input Earth Noise Seismic traces

    SEI SMI C TRACE

    0- +

    High Frequency10 60 Hz (Cycles/sec)

    Polarity (Hard)(Soft)

    Amplitude (-)

    (Reservoir)

    0 Phase

    90 Phase

    ase

    Wavelength= v /= 3000/30

    Resolution = 25 m

    = 100 m

    Low Frequency6 35 Hz

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    Wave l e t shape

    Poss ib le Se ism ic Sign at ur es

    cous c mpe ance

    Reflectivity

    Time Dip

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    Curvature

    time

    0

    functionoffrequencyforthecomponentsofawavetrainorwavelet

    Fourieranalysisinvolvefindingfrequency

    Fouriertransformisconversionoftimefunctionintofrequencydomainrepresentationandviceversa

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    Decompositionofmeasuredsignalsintospectralour er componen s oa enua e ow requency

    groundrole(culturalnoise),andhighfrequencyrandomnoise.

    Spectraldecompositionisalsoknownasshortwindowdiscretetransforms

    ses x engt ana ys sw n ow ora requenc es,allowingustocomparewhichfrequencycomponentismoredominantinageologicformation

    Interpretersareconcernwithwhatfrequencytuningoccurs

    DiscreteFouriertransformdecomposethedataintos nuso a componen ssepara e y1 o2 z or nerfeaturesofinterest,otherwiseweneedonly todecomposedataat10Hzintervalsforbandlimitedseismicdataof100mswindow

    Spectralcomponentimageswithhigherlateral

    amplitudedataprovided.

    Appropriateforformationbasedattributessuchastuningthicknessandmappingstratigraphic variability.

    (Marfut,2006,SEGDISNo.9)

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    20 Hz

    50HZ

    20ms

    Concept of Spectral analysis

    20 ms

    FREQ.

    50 MS

    DBFREQ.

    TUNNINGShale

    Amp

    THIN

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    THICKNESS (MS)

    THIN BED TUNNING & RESPONSE

    50 ms

    THICK

    WELL A WELL B

    SPECTRAL ANALYSIS SPECDECOMP

    55HzLowFrequency

    HighFrequency

    24

    FREQUENCY

    35Hz

    Courtesy Petrofac

    Two wells show different facies. Well A is high frequency. B low frequency.Well A peaks at 55hz and B at 35hz Specdecomp Spectral analysis ( extreme right )

    reveals the channel. Thinner beds respond to high frequency.

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    NUMERICAL GEOLOGICAL MODELLING

    VALLEY

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    TRANSFER

    FUNCTION

    CHANNEL

    CHANNEL MODELLING

    Wavelet Classif ication (Seismic-Facies)

    Classify seismic trace shapes intoseismic facies within an interval(constant or variable thickness)

    B100CL 5to25ms 12 class B80-B100cl, 12 classes

    us ng eura e wor ec no ogy

    26Channel signatur e

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    Specif ic Examples of Seismic At t ribut es Maps

    Channel paths

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    Rms amplit ude Wavelet class specdecomp

    ThankyouFORYOURATTENTION