porosity determination

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    POROSITY DETERMINATIONFROM LOGS

    Most slides in this section are modified primarily from NExT PERF Short Course Notes, 1999.However, many of the NExT slides appears to have been obtained from other primarysources that are not cited. Some slides have a notes section.

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    Well LogSP Resistivity

    OPENHOLE LOG EVALUATION

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    Oil sand

    Gammaray

    Resisitivity Porosity

    Increasingradioactivity Increasingresistivity Increasingporosity

    Shale

    Shale

    POROSITY DETERMINATION BY LOGGING

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    POROSITY LOG TYPES3 Main Log Types

    Bulk density

    Sonic (acoustic) Compensated neutron

    These logs do not measures porosity directly. To

    accurately calculate porosity, the analyst mustknow:Formation lithology Fluid in pores of sampled reservoir volume

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    DENSITY LOGS Uses radioactive source to generate

    gamma rays

    Gamma ray collides with electrons information, losing energy Detector measures intensity of back-

    scattered gamma rays, which is relatedto electron density of the formation Electron density is a measure of bulk

    density

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    DENSITY LOGS

    Bulk density, b, is dependent upon:

    Lithology Porosity

    Density and saturation of fluids in pores

    Saturation is fraction of pore volumeoccupied by a particular fluid (intensive)

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    GR API 0 200

    CALIX IN 6 16

    CALIY IN 6 16

    RHOB G/C3 2 3

    DRHO G/C3 -0.25 0.25

    4100

    4200

    DENSITY LOG

    Caliper

    Density

    correction

    Gamma ray Density

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    Formation ( b)

    Long spacingdetector

    Short spacingdetector

    Mud cake( mc + h mc )

    Source

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    BULK DENSITY

    f mab 1Matrix Fluids in

    flushed zoneMeasures electron density of a formationStrong function of formation bulk density

    Matrix bulk density varies with lithology

    Sandstone 2.65 g/cc

    Limestone 2.71 g/cc Dolomite 2.87 g/cc

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    POROSITY FROM DENSITY LOG

    Porosity equation

    xohxomf f S1S

    f ma

    bma

    Fluid density equation

    We usually assume the fluid density ( f ) is between 1.0 and 1.1. If gas is present, theactual f will be < 1.0 and the calculated porosity will be too high.

    mf is the mud filtrate density, g/cc

    h is the hydrocarbon density, g/cc

    S xo is the saturation of the flush/zone, decimal

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    DENSITY LOGS

    Working equation (hydrocarbon zone)

    mashshsh

    hcxomf xob

    V1V

    S1S

    b = Recorded parameter (bulk volume)

    S xo mf = Mud filtrate component

    (1 - S xo) hc = Hydrocarbon component Vsh sh = Shale component

    1 - - V sh = Matrix component

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    DENSITY LOGS If minimal shale, V

    sh 0

    If hc mf f , then

    b

    = f - (1 - )

    ma

    f ma

    bmad

    d = Porosity from density log, fractionma = Density of formation matrix, g/cm 3

    b = Bulk density from log measurement, g/cm 3

    f = Density of fluid in rock pores, g/cm 3

    hc = Density of hydrocarbons in rock pores, g/cm 3

    mf = Density of mud filtrate, g/cm 3

    sh = Density of shale, g/cm 3

    Vsh = Volume of shale, fractionSxo = Mud filtrate saturation in zone invaded by mud filtrate, fraction

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    GRC 0 150

    SPC MV -160 40

    ACAL 6 16

    ILDC 0.2 200

    SNC 0.2 200

    MLLCF 0.2 200

    RHOC 1.95 2.95

    CNLLC 0.45 -0.15

    DT us/f 150 50

    001) BONANZA 1

    10700

    10800

    10900

    BULK DENSITY LOG

    Bulk DensityLog

    RHOC1.95 2.95

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    NEUTRON LOG

    Logging tool emits high energyneutrons into formation

    Neutrons collide with nuclei offormations atoms

    Neutrons lose energy (velocity) witheach collision

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    NEUTRON LOG

    The most energy is lost when collidingwith a hydrogen atom nucleus

    Neutrons are slowed sufficiently to becaptured by nuclei

    Capturing nuclei become excited andemit gamma rays

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    NEUTRON LOG Depending on type of logging tool either gammarays or non-captured neutrons are recorded

    Log records porosity based on neutronscaptured by formation

    If hydrogen is in pore space, porosity is relatedto the ratio of neutrons emitted to those countedas captured

    Neutron log reports porosity, calibratedassuming calcite matrix and fresh water in pores,if these assumptions are invalid we must correctthe neutron porosity value

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    NEUTRON LOG

    Theoretical equation

    Nmashshsh

    NhcxoNmf xoN

    V1V

    S1S

    N = Recorded parameter

    S xo Nmf = Mud filtrate portion

    (1 - S xo) Nhc = Hydrocarbon portion

    Vsh Nsh = Shale portion

    (1 - - V sh ) Nhc = Matrix portion where = Trueporosity of rock

    N = Porosity from neutron log measurement, fraction

    Nma = Porosity of matrix fraction

    Nhc = Porosity of formation saturated with

    hydrocarbon fluid, fraction

    Nmf = Porosity saturated with mud filtrate, fraction

    Vsh = Volume of shale, fraction

    S xo = Mud filtrate saturation in zone invadedby mud filtrate, fraction

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    GRC 0 150

    SPC MV -160 40 ACAL

    6 16

    ILDC 0.2 200

    SNC 0.2 200 MLLCF

    0.2 200

    RHOC 1.95 2.95

    CNLLC 0.45 -0.15

    DT us/f 150 50

    001) BONANZA 1

    10700

    10800

    10900

    POROSITY FROM NEUTRON LOG

    NeutronLog

    CNLLC0.45 -0.15

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    Uppertransmitter

    Lower

    transmitter

    R1 R2

    R3 R4

    ACOUSTIC (SONIC) LOG

    Tool usually consists ofone sound transmitter(above) and two receivers(below)

    Sound is generated,travels through formation

    Elapsed time betweensound wave at receiver 1

    vs receiver 2 is dependentupon density of mediumthrough which the soundtraveled

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    sec50

    T0 E2

    E1 E3

    Mud wavesRayleigh

    wavesCompressional

    waves

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    Lithology Typical Matrix Travel

    Time, tma , sec/ftSandstone 55.5Limestone 47.5Dolomite 43.5Anydridte 50.0Salt 66.7

    COMMON LITHOLOGY MATRIX

    TRAVEL TIMES USED

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    ACOUSTIC (SONIC) LOG

    Working equation

    mashshsh

    hcxomf xoL

    tV1tV

    tS1tSt

    tL = Recorded parameter, travel time read from log

    S xo tmf = Mud filtrate portion

    (1 - S xo) thc = Hydrocarbon portion

    Vsh tsh = Shale portion

    (1 - - V sh ) tma = Matrix portion

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    ACOUSTIC (SONIC) LOG If V

    sh = 0 and if hydrocarbon is liquid

    (i.e. tmf tf ), then

    tL = tf + (1 - ) tma

    or

    maf

    maLs

    tt

    tt

    s = Porosity calculated from sonic log reading, fraction

    tL = Travel time reading from log, microseconds/ft

    tma = Travel time in matrix, microseconds/ft

    tf = Travel time in fluid, microseconds/ ft

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    DT

    USFT 140 40

    SPHI % 30 10

    4100

    4200

    GR API 0 200

    CALIX IN 6 16

    ACOUSTIC (SONIC) LOG

    Sonic travel time

    Sonicporosity

    Caliper

    GammaRay

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    SONIC LOG

    The response can be written as follows:

    f malog t1tt

    maf

    ma

    tt

    tt

    log

    tlog = log reading, sec/ft

    tma = the matrix travel time, sec/ft

    tf = the fluid travel time, sec/ft

    = porosity

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    GRC 0 150

    SPC MV -160 40 ACAL

    6 16

    ILDC 0.2 200

    SNC 0.2 200 MLLCF

    0.2 200

    RHOC 1.95 2.95

    CNLLC 0.45 -0.15

    DT us/f 150 50

    001) BONANZA 1

    10700

    10800

    10900

    SONIC LOG

    Sonic

    Log

    DT150 50us/f

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    EXAMPLE

    Calculating Rock PorosityUsing an Acoustic Log

    Calculate the porosity for the following intervals. The measured travel times from thelog are summarized in the following table.

    At depth of 10,820, accoustic log reads travel time of 65 s/ft.

    Calculate porosity. Does this value agree with density and neutronlogs?

    Assume a matrix travel time, tm = 51.6 sec/ft. In addition, assume the formation issaturated with water having a tf = 189.0 sec/ft.

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    GRC 0 150

    SPC MV -160 40 ACAL

    6 16

    ILDC 0.2 200

    SNC 0.2 200 MLLCF

    0.2 200

    RHOC 1.95 2.95

    CNLLC 0.45 -0.15

    DT us/f 150 50

    001) BONANZA 1

    10700

    10800

    10900

    SPHI ss 45 -15

    EXAMPLE SOLUTION SONIC LOG

    SPHI

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    FACTORS AFFECTING SONIC

    LOG RESPONSE

    Unconsolidated formations

    Naturally fractured formations

    Hydrocarbons (especially gas)

    Rugose salt sections

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    RESPONSES OF POROSITY LOGS

    The three porosity logs: Respond differently to different matrix

    compositions Respond differently to presence of gas or

    light oils

    Combinations of logs can : Imply composition of matrix Indicate the type of hydrocarbon in pores

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    GAS EFFECT

    Density - is too high

    Neutron - is too low Sonic - is not significantly

    affected by gas

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    ESTIMATING POROSITY FROMWELL LOGS

    Openhole logging tools are the most common methodof determining porosity:

    Less expensive than coring and may be lessrisk of sticking the tool in the hole

    Coring may not be practical in unconsolidatedformations or in formations with high secondaryporosity such as vugs or natural fractures.

    If porosity measurements are very important, bothcoring and logging programs may be conducted sothe log-based porosity calculations can be used tocalibrated to the core-based porosity measurements .

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    Influence Of Clay-Mineral DistributionOn Effective Porosity

    Dispersed Clay Pore-filling Pore-lining Pore-bridging

    Clay Lamination

    Structural Clay (Rock Fragments,

    Rip-Up Clasts, Clay-Replaced Grains)

    e

    e

    e

    Clay Minerals

    Detrital Quartz Grains

    e

    e

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    FlowUnitsGamma RayLogPetrophysicalDataPoreTypesLithofaciesCore

    1

    2

    3

    4

    5

    CorePlugsCapillary Pressure vs k

    GEOLOGICAL AND PETROPHYSICALDATA USED TO DEFINE FLOW UNITS

    S h ti R i L i P fil

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    Schematic Reservoir Layering Profilein a Carbonate Reservoir

    Baffles/barriers

    3150

    SA -97A SA -251

    SA -356 SA -71 SA -344 SA -371 SA -348

    SA -346 SA -37

    3200

    3250

    3300

    3350

    3100

    3150

    3250

    3300

    3250

    3150

    3200

    3100

    3150

    3200

    3250

    3200

    3250

    3250

    3350

    3300

    3150

    3200

    3250

    3300

    3100

    3200

    3250

    3300

    3350

    3150

    3200

    3250

    Flow unit