Presión Capilar a Partir de Registros

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    1/12/2006

    Capillary Pressure From Logs

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    PredictPredict SwSw distributiondistribution in reservoirin reservoir

    (compare with log data, initialize simulator)(compare with log data, initialize simulator)

    PredictPredict free water levelfree water level

    Predict Rock Type, Quality and Pore geometryPredict Rock Type, Quality and Pore geometry

    Assist in interpretation/calculation ofAssist in interpretation/calculation of relativerelative

    permeabilitypermeability

    CalculateCalculate pore size distributionpore size distribution

    Applications of CapillaryApplications of Capillary

    Pressure DataPressure Data

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    r

    Cos

    Cos

    Capillary pressureCapillary pressure exists whenever twoexists whenever twoimmiscible phases are present in a fineimmiscible phases are present in a fine

    tube, andtube, and is defined as the pressure dropis defined as the pressure drop

    across the curved liquid interfaceacross the curved liquid interface..

    r

    Cos2Pc

    =

    hgPc =

    Capillary pressure in a tube can beCapillary pressure in a tube can becalculated if the fluidcalculated if the fluid interfacial tensioninterfacial tension,,

    rockrock--fluidfluid contact anglecontact angle, and the tube, and the tube

    radiusradius are known.are known. Capillary pressure can also be expressedCapillary pressure can also be expressed

    as a hydrostatic head. It is equal to theas a hydrostatic head. It is equal to the

    product of theproduct of the heightheight of the liquid rise, theof the liquid rise, the

    density differencedensity difference of the two liquids, andof the two liquids, and

    thethe gravitational constant.gravitational constant.

    Pw-PnwPc =

    CAPILLARY PRESSURE THEORYCAPILLARY PRESSURE THEORY

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    0 1Water Saturation

    HeightAboveWaterLevel

    B

    A

    AARockRock--typetype BBRockRock--typetype

    Pore size and d istr ibut ion inf luence the magnitu de of ir reduciblewater and the height of th e transit ion zone. Smaller pores and pore throats mean low er permeabi l i ty and

    high er Sw

    Effect of Pore Geometry

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    As h ydro carbon s accumulate, the largest pores are drained f irst . Smaller po res are drained as the HC co lumn (height or pressure)

    increases

    A

    B

    Effect of Pore Geometry

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    0 100%Sw

    IrreducibleWa

    terSaturation

    Swir

    WellWell

    Top Transition Zone

    Transition Zone

    Free Water Level

    (Pc = 0)

    HC and

    Mobile Water

    Observed HC-WC

    (Pc = Pce)

    HC, water-free

    D

    E

    PT

    H

    Fluid Distribution in a HC

    Reservoir

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    A

    Rock type B

    Rock type A

    B

    Capillary PropertiesCapillary Properties

    Calibrated Log ResponseCalibrated Log Response

    CAPILLARYPRESSURE

    HEIGHTINRESERVOIRABOVEFWL

    0 Sw 1

    Sealing Fault

    A

    A

    B

    FWL

    OWC

    OWC OWC

    Relationship of Reservoir Saturations to:

    Logged Interval

    Rt

    Sw Profile in Wellbore

    Rt = F Rw / Swn

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    0 1

    Sw

    Cap

    illaryPressureorH

    eightAboveFWL

    OWC

    OWC

    OWC

    FWL

    SedimentarySequence

    A B CRock Type

    0 1

    Sw

    Sw from Wireline

    B

    A

    C

    B

    A

    B

    A

    C Sw trace

    Sw Distribution by

    CAPILLARY PRESSURE Model

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    Capillary Pressure Curves from NMR

    - 1

    10 -4 10 -3 10 -2 10 -1 10 0 10 1

    T2 (s)

    Cumulative

    T2

    Distribution

    951211-02

    T2 distributions are normally displayed as incremental porosity

    distributions. Integrating from left to right gives us cumulative porosity

    distributions

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    Capillary Pressure Summary

    Primary Uses

    Determine pore throat size distribution

    Determine vertical wetting phase

    saturation distribution

    Help separate rock types (quality)