lecture 04

Upload: last-winter

Post on 12-Oct-2015

17 views

Category:

Documents


0 download

DESCRIPTION

PPT

TRANSCRIPT

  • 5/21/2018 Lecture 04

    1/35

    POROSITY DETERMINATION

    FROM LOGS

    Most slides in this section are modified primarily from NExTPERF Short Course Notes, 1999.

    However, many of the NExT slides appears to have been obtained from other primary

    sources that are not cited. Some slides have a notes section.

  • 5/21/2018 Lecture 04

    2/35

    Well LogSP Resistivity

    OPENHOLE LOG EVALUATION

  • 5/21/2018 Lecture 04

    3/35

    Oil sand

    Gamma

    ray

    Resisitivity Porosity

    Increasingradioactivity

    Increasingresistivity

    Increasingporosity

    Shale

    Shale

    POROSITY DETERMINATION BY LOGGING

  • 5/21/2018 Lecture 04

    4/35

    POROSITY LOG TYPES

    3 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

  • 5/21/2018 Lecture 04

    5/35

    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

  • 5/21/2018 Lecture 04

    6/35

    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)

  • 5/21/2018 Lecture 04

    7/35

    GRAPI0 200

    CALIXIN6 16

    CALIYIN6 16

    RHOBG/C32 3

    DRHOG/C3-0.25 0.25

    4100

    4200

    DENSITY LOG

    Caliper

    Density

    correction

    Gamma ray Density

  • 5/21/2018 Lecture 04

    8/35

    Formation (b)

    Long spacingdetector

    Short spacingdetector

    Mud cake(mc+ hmc)

    Source

  • 5/21/2018 Lecture 04

    9/35

    BULK DENSITY

    fmab 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/ccDolomite 2.87 g/cc

  • 5/21/2018 Lecture 04

    10/35

    POROSITY FROM DENSITY LOG

    Porosity equation

    xohxomff S1S

    fma

    bma

    Fluid density equation

    We usually assume the fluid density (f) is between 1.0 and 1.1. If gas is present, the

    actual 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

    Sxo is the saturation of the flush/zone, decimal

  • 5/21/2018 Lecture 04

    11/35

    DENSITY LOGS

    Working equation (hydrocarbon zone)

    mashshsh

    hcxomfxob

    V1V

    S1S

    b = Recorded parameter (bulk volume)

    Sxomf = Mud filtrate component

    (1 - Sxo) hc = Hydrocarbon component

    Vshsh = Shale component

    1 - - Vsh = Matrix component

  • 5/21/2018 Lecture 04

    12/35

    DENSITY LOGS

    If minimal shale, Vsh

    0

    If hcmff, then

    b

    = f

    - (1 - ) ma

    fma

    bmad

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

    3

    b = Bulk density from log measurement, g/cm3

    f = Density of fluid in rock pores, g/cm3

    hc = Density of hydrocarbons in rock pores, g/cm3

    mf = Density of mud filtrate, g/cm3

    sh = Density of shale, g/cm3

    Vsh = Volume of shale, fraction

    Sxo = Mud filtrate saturation in zone invaded by mud filtrate, fraction

  • 5/21/2018 Lecture 04

    13/35

    GRC0 150

    SPCMV

    -160

    40

    ACAL

    6

    16

    ILDC0.2 200

    SNC0.2

    200

    MLLCF

    0.2

    200

    RHOC1.95 2.95

    CNLLC0.45

    -0.15

    DTus/f150 50

    001) BONANZA 1

    10700

    10800

    10900

    BULK DENSITY LOG

    Bulk Density

    Log

    RHOC

    1.95 2.95

  • 5/21/2018 Lecture 04

    14/35

    NEUTRON LOG

    Logging tool emits high energy

    neutrons into formation

    Neutrons collide with nuclei of

    formations atoms

    Neutrons lose energy (velocity) witheach collision

  • 5/21/2018 Lecture 04

    15/35

    NEUTRON LOG

    The most energy is lost when colliding

    with a hydrogen atom nucleus

    Neutrons are slowed sufficiently to be

    captured by nuclei

    Capturing nuclei become excited andemit gamma rays

  • 5/21/2018 Lecture 04

    16/35

    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

  • 5/21/2018 Lecture 04

    17/35

    NEUTRON LOG

    Theoretical equation

    Nmashshsh

    NhcxoNmfxoN

    V1V

    S1S

    N = Recorded parameter

    Sxo Nmf = Mud filtrate portion

    (1 - Sxo) Nhc= Hydrocarbon portion

    VshNsh = Shale portion

    (1 - - Vsh) Nhc = Matrix portion where = True

    porosity 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

    Sxo = Mud filtrate saturation in zone invaded

    by mud filtrate, fraction

  • 5/21/2018 Lecture 04

    18/35

    GRC0 150

    SPCMV

    -160

    40

    ACAL

    6

    16

    ILDC0.2 200

    SNC0.2

    200

    MLLCF

    0.2

    200

    RHOC1.95 2.95

    CNLLC0.45

    -0.15

    DTus/f150 50

    001) BONANZA 1

    10700

    10800

    10900

    POROSITY FROM NEUTRON LOG

    Neutron

    Log

    CNLLC

    0.45 -0.15

  • 5/21/2018 Lecture 04

    19/35

    Upper

    transmitter

    Lower

    transmitter

    R1R2

    R3R4

    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

  • 5/21/2018 Lecture 04

    20/35

    sec

    50

    T0E2

    E1E3

    Mud waves

    Rayleigh

    waves

    Compressional

    waves

  • 5/21/2018 Lecture 04

    21/35

    Lithology Typical Matrix Travel

    Time, tma, sec/ftSandstone 55.5Limestone 47.5Dolomite 43.5

    Anydridte 50.0Salt 66.7

    COMMON LITHOLOGY MATRIX

    TRAVEL TIMES USED

  • 5/21/2018 Lecture 04

    22/35

    ACOUSTIC (SONIC) LOG

    Working equation

    mashshsh

    hcxomfxoL

    tV1tV

    tS1tSt

    tL = Recorded parameter, travel time read from log

    Sxotmf= Mud filtrate portion

    (1 - Sxo) thc = Hydrocarbon portion

    Vshtsh = Shale portion

    (1 - - Vsh) tma = Matrix portion

  • 5/21/2018 Lecture 04

    23/35

    ACOUSTIC (SONIC) LOG

    If Vsh

    = 0 and if hydrocarbon is liquid

    (i.e. tmftf), 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

  • 5/21/2018 Lecture 04

    24/35

    DT

    USFT140 40

    SPHI

    %30 10

    4100

    4200

    GR

    API0 200

    CALIX

    IN6 16

    ACOUSTIC (SONIC) LOG

    Sonic travel time

    Sonic

    porosity

    Caliper

    Gamma

    Ray

  • 5/21/2018 Lecture 04

    25/35

    SONIC LOG

    The response can be written as follows:

    fmalog 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

  • 5/21/2018 Lecture 04

    26/35

    GRC0 150

    SPCMV

    -160

    40

    ACAL

    6

    16

    ILDC0.2 200

    SNC0.2

    200

    MLLCF

    0.2

    200

    RHOC1.95 2.95

    CNLLC0.45

    -0.15

    DTus/f150 50

    001) BONANZA 1

    10700

    10800

    10900

    SONIC LOG

    Sonic

    Log

    DT

    150 50us/f

  • 5/21/2018 Lecture 04

    27/35

    EXAMPLE

    Calculating Rock Porosity

    Using an Acoustic Log

    Calculate the porosity for the following intervals. The measured travel times from the

    log 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 is

    saturated with water having a tf= 189.0 sec/ft.

  • 5/21/2018 Lecture 04

    28/35

    GRC0 150

    SPCMV

    -160

    40

    ACAL

    6

    16

    ILDC0.2 200

    SNC0.2

    200

    MLLCF

    0.2

    200

    RHOC1.95 2.95

    CNLLC0.45

    -0.15

    DTus/f150 50

    001) BONANZA 1

    10700

    10800

    10900

    SPHIss

    45

    -15

    EXAMPLE SOLUTION SONIC LOG

    SPHI

  • 5/21/2018 Lecture 04

    29/35

    FACTORS AFFECTING SONIC

    LOG RESPONSE

    Unconsolidated formations

    Naturally fractured formations

    Hydrocarbons (especially gas)

    Rugose salt sections

  • 5/21/2018 Lecture 04

    30/35

    RESPONSES OF POROSITY LOGS

    The three porosity logs:

    Respond differently to different matrixcompositions

    Respond differently to presence of gas orlight oils

    Combinations of logs can:

    Imply composition of matrix Indicate the type of hydrocarbon in pores

  • 5/21/2018 Lecture 04

    31/35

    GAS EFFECT

    Density - is too high

    Neutron - is too low

    Sonic - is not significantlyaffected by gas

  • 5/21/2018 Lecture 04

    32/35

    ESTIMATING POROSITY FROM

    WELL LOGS

    Openhole logging tools are the most common method

    of determining porosity:

    Less expensive than coring and may be less

    risk of sticking the tool in the hole

    Coring may not be practical in unconsolidatedformations or in formations with high secondary

    porosity such as vugs or natural fractures.

    If porosity measurements are very important, both

    coring and logging programs may be conducted so

    the log-based porosity calculations can be used to

    calibrated to the core-based porosity measurements.

  • 5/21/2018 Lecture 04

    33/35

    Influence Of Clay-Mineral DistributionOn Effective Porosity

    Dispersed ClayPore-filling

    Pore-lining

    Pore-bridging

    Clay Lamination

    Structural Clay(Rock Fragments,

    Rip-Up Clasts,Clay-Replaced Grains)

    e

    e

    e

    ClayMinerals

    Detrital QuartzGrains

    e

    e

  • 5/21/2018 Lecture 04

    34/35

    FlowUnits

    Gamma RayLog

    PetrophysicalData

    PoreTypes

    LithofaciesCore

    1

    2

    3

    4

    5

    CorePlugs

    CapillaryPressure

    vs k

    GEOLOGICAL AND PETROPHYSICALDATA USED TO DEFINE FLOW UNITS

    Schematic Reservoir Layering Profile

  • 5/21/2018 Lecture 04

    35/35

    Schematic Reservoir Layering Profile

    in a Carbonate Reservoir

    Baffles/barriers

    3150

    SA -97ASA -251

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

    SA -346SA -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