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    ,PT. PERTAMINA (PERSERO)PT. PERTAMINA (PERSERO) -- UPSTREAMUPSTREAM TECHNOLOGY CENTER (TECHNOLOGY CENTER ( UUTC )TC )

    Presented in Joint Convention HAGI-IAGIMakassar, September 26th-29th 2011

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    AgendaBackground

    Theoryandmethod

    SurfacegeologyconditionDataprocessing

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Background Thequalityoflandseismicdatamostlyinfluencedbynearsurface

    geologicalconditions,asinareaswithaweatheredlayervarieslaterally,

    theoutcropsof limestoneorareaswithahighelevationvariation

    Theeffectofnearsurfaceismainlyonseismicdataprocessing,in

    .

    Inaccuraciesinstaticcorrectionwillnotgivetheoptimalresultofseismic

    dataprocessingwhichisshownintheseismicsection.

    Variousstaticcorrectionmethodhasbeenformulatedanddevelopedfrom

    uphole/elevation,refractionthroughtomographymethod.

    Thispaperwillbediscussesregardingtheuseofrefractiontomography

    methods forgeologyandvelocitymodelbuildingwhichwillthenbeused

    .

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Theory

    and

    methodRefractiontomographyisamethodtoobtainthevelocity

    distribution

    model

    of

    head

    wave

    travel

    time

    (first

    break)

    (Shearer,1999)

    2approaches:

    1. Nearsurfacemodelconsistingoflocallyflatlayers(onthescaleo t eo setrange .F rstarr va sareassume to et eonseto

    headwavespropagatingalongtherefractinginterfacesbetween

    theselayers

    2. Modelwithaverticalvelocitygradient.Firstarrivalsare

    assumedtobetheonsetofdiving(turning)waves.

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Theory

    and

    method

    headwaverefractionmodel (Osypov 2001)

    Timeisassumedtocomefromthewavefront propagatesalongtheplaneof

    refractionbetweenthetwola ers

    Kinematicparametersofthewavefront isassumedtobelinearandtheinitial

    wavetraveltimearegroupedintolayersofdelaytimesandrefractorvelocity.

    assumptionsonthecriticalanglerefractorlayer

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Theory

    and

    method

    Divingwaverefractionmodel (Osypov 2001)

    Thekinematicparameterofdivingwavearenonlinear.

    Wavepropagationmediumismodeledasamountofcellsthatarepassedbythe

    rays.

    Timetraveldifferencesbetweencalculated andobservedareconvertedtobe

    slownessintoeverycell

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Theory

    and

    method

    (a)Traveltimecurveasfunctionofoffsetx

    (b)TransformationTraveltimecurveinto pdomain

    (c)TransformationTraveltimecurveintoxpdomain

    (Osypov 2001)

    (d)Velocitycurvevs depthzasaresultfrom(a)usescurvetransformationestimation(b)or

    (c)byHerglotzWiechert approachJoint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Parameter

    of

    2D seismicShot point interval : 50 meter

    Receiver point interval : 25 meter

    Channel : 240 channels

    Tail : 60 channels / lineShooting template : Symetric Split Spread (120120)

    Source : explosive

    Source depth : 20 30 m

    Fold coverage : 6000 %

    Low/High Cut Filter : out/125 Hz

    Charge size : 25 Kg

    Receiver : Geop one SM24GS32CT

    Geophone string : 18 geophone perstring

    Sampling rate : 2 (two) milisecond

    Record length : 6 second

    Near o set : 12,5 meterFar offset : 2.987,5 meter

    Tape format : SEGD IBM3490 Catridge

    Polarity : Normal polarity (SEG standard)

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Data

    of

    2D seismic

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Near

    surface

    geology

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Near

    surface

    geology

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Data processing

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Data processing: first

    break

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Static

    correction:

    refraction

    method

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Staticcorrection:refractiontomographymethod

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Refraction

    tomography:

    2

    layers

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Refraction

    tomography:

    3

    layers

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Seismicsection

    Staticcorrection:refraction

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Seismicsection

    Staticcorrection:refraction+residualstatic

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Seismicsection

    Staticcorrection:refractiontomography2layers

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    Seismicsection

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

    Staticcorrection:refractiontomography3layers

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    Seismicsection

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

    Staticcorrection:refractiontomography2layers+residual

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    Conclusions

    Accuratefirstbreakpicksisneededforgeologicalandvelocity

    modelbuildingbyrefractiontomography, whichareusedfor

    staticcorrectioncalculation.

    Theamountoflayersthatareusedforcalculationwillinfluence

    thegeologyandvelocitymodelquality.

    n sresearc ,re rac on omograp ys a ccorrec onme o

    givesbetterstaticcorrectionthanconventionalrefractionmethod.

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011

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    ThankyoutoDirektorat Jendral Migas forallowing

    Matindok 2Dseismicdatatobeusedforthisresearch

    Joint Convention HAGI-IAGI Makassar, September 26th-29th 2011