Petrophysics in shale gas

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    Petrophysics

    Appraising and DevelopingShale Oil and Gas Reservoirs

    Shale Composition: Petrophysical Perspective

    From Randy Miller, Integrated Reservoir Solutions, Core Lab

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    Shale OGIP Equation

    Where:OGIP = Original gas in place (cubic meters)

    A = Area (square meters)

    h = Shale thickness (meters) m = Matrix porosity (fraction)

    Sg = Gas saturation (fraction)

    Eg = Initial gas expansion factor (scm/rcm)

    Gs = Gas storage capacity, as-received basis (m^3/ton) = Shale density, as-received basis (ton/m^3)

    ]*}**[{* S m GSg Egh AOGIP

    PetrophysicalMeasurements

    from Core

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    Sampling Methodology

    From Core Laboratories

    CoreLabs Analysis Procedure

    From Core Laboratories

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    GRI Reasoning for Using Crushed Samples fo rPorosity Measurements

    From Ted Braun, SPWLA short course, 2011

    Helium was unable to contact all the pore space within an uncrushed sample

    Uncontacted pores are interpreted as grains with zero density

    Result was low porosity and low grain density

    Crushing dramatically increases the surface area to volume ratio resulting in greateraccess to pore space and more representative measurements

    Core porosity needs to be decreased by 0.5-1 porosity unit to correct values to in-situ conditions

    GRI Measurement of Matrix Permeability

    Change in pressurewith time is used tocalculate perm.

    Core chips are assumed to be unfractured (crushing would have broken the corealong fractures) and the measurement is made at surface conditions

    From Ted Braun, SPWLA short course, 2011

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    GRI Measurement o f Phi , So, Sw, Grain Den.

    From Ted Braun, SPWLA short course, 2011

    Water volume is calculated by assuming a water density (salinity)

    Oil volume = (oil weight / assumed oil density) where oil weight = weight loss ofcrushed rock in excess of the water collected in the Dean Stark receiver

    Pore volume = bulk volume grain volume; Porosity = pore volume / bulk volume

    Sw = water volume / pore volume; So = oil volume / pore volume

    Result ing Petrography and Core Data

    EpifluorescencePetrography

    From Randy Miller, Integrated Reservoir Solutions, Core Lab

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    Matrix K vs. Total Porosity by Play

    From Randy Miller, Integrated Reservoir Solutions, Core Lab

    Matrix K vs . Water Saturation by Play

    From Randy Miller, Integrated Reservoir Solutions, Core Lab

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    Distribution of Water and Gas in the Pore Space

    From SPE 131350

    TerraTeks Analysis Procedure

    From SPE 147456

    Retort method

    Differentiates between free and bound fluid volumes basedupon temperature

    Temperature is increased through a series of programmedsteps

    250 degrees F for mobile water

    600 degrees F for mobile oil

    1300 degrees F for clay-bound water and boundhydrocarbons

    Allows reporting of total and effective porosities

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    Table of Shale Core Measurements

    From Terratek

    Reported Porosi ties from Three Different Labs

    From Quinn Passey et al, AAPG Search and Discovery Article 80231

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    Repor ted Permeabiliti es from Three Different Labs

    100 nD

    Service laboratories have developed their own proprietarytechniques and it is difficult to know if the differences in reportedvalues are due to the differences in the data or interpretations

    From Quinn Passey et al, SPE 131350

    Exxons New Approach For

    Measuring Kon shale cores

    (SPE 152257)

    Steady-state app aratusfor measuring permson very tight samples

    Comparison between steady-stateperms from plu gs and pressure decayperms fro m vendors A & B measuredon crush ed samples

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    Mineralogy Comparison by Play

    From Randy Mil ler, Integrated Reservoir Solutions, Core Lab

    Shale Petrophysical Properties by Play

    From Randy Miller, Integrated Reservoir Solutions, Core Lab

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    Comparison of Shale Characteristics

    MONTNEY BARNETT HAYNESVILLE MARCELLUS MUSKWA/OOTLA

    Basin Western Canadian Fort Worth Gulf Coast Appalachian Horn River

    Age Triass ic Miss iss ipp ian Jur assi c Devon ian Devon ian

    Depth, meters 1,500 to 2,400 2,000 to 2,700 3,000 to 4,000 1,500 to 2,400 2,700 to 4,000Reservoir Temperature, C 60 to 80 70 to 90 150 to 175 40 to 65 60 to 80

    Thickness, meters 100 to 300 100 to 150 50 to 100 15 to 75 100 to 180

    Total Porosity, % 4 to 9 3 to 7 6 to 10 5 to 8 3 to 5

    Water Saturation, % 10 to 60 20 to 50 15 to 30 10 to 40 20 to 40

    Sorbed Gas, m 3/mt 0.14 to 0.71 2.0 to 2.8 1.4 to 2.8 1.4 to 4.2 0.85 to 1.70

    Sorbed Gas, % total 5 to 30 40 to 45 25 45 to 55 20 to 40

    TOC, weight % 0.5 to 2.5 3 to 8 3 to 5 5 to 8 2 to 5

    Kerogen Type Type II Type II Type II Type II Type IIVitrinite Reflectance, % Ro 0.3 to 2.5 1.2 to 2.2 1.2 to 2.5 0.9 to 3.5 1.6 to 3.0

    Pressure Gradient, kg/cm 2/m 0.09 to 0.15 0.10 to 0.13 0.18 to 0.21 0.09 to 0.16 0.12 to 0.14

    IP, 10 3m 3/d 50 to 150 30 to 170 140 to 550+ 55 to 170 140 to 280

    OGIP, 109

    m3

    /km2

    0.1 to 3.0 0.5 to 2.2 1.6 to 2.7 0.3 to 1.6 2.0 to 3.5Well Spacing, km 2 0.32 0.1 to 0.4 0.32 to 0.65 0.32 to 0.65 0.16 to 0.65

    Recovery Factor, % 20 to 30 20 to 50 30 20 to 40 20 to 30

    EUR, 10 6m 3 per well 150 to 270 60 to 140 130 to 240 100 to 150 110 to 170

    DeterminingTotal OrganicCarbon from

    Logs

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    How Organic Matter and Uranium are Related

    OxidizingZone

    As t he ano xic zon e expands , organicmatter settles through the oxidizing zonemore rapidly, and therefore more organic

    matter accumulates

    Organic matter is oxidized resulting inproducts (C, N, P) that are recycled bylive organisms

    OxidizingZone

    U+6 (soluble) is reduced to U +4

    (insoluble) when it comes in contactwith organic matter

    U +6U+6

    U+6

    U +4 U+4

    U +6U+6

    More U +4 precipitates as the anoxic zoneexpands and more organic matter is

    preserved

    U +4 U +4U +6

    U +4 U +4

    U +6

    U +4

    Modified from Nick Harris, Source Rocks 101 Short Course

    Relationship between Uranium and TOC

    From Luning and Kolonic, 2003

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    Relationship Between TOC and GR Logs

    Higher TOCvalues equate tohigh GR valuesdue to the affectsof uranium

    However, not allorganic mattercontains uraniumand a spectral GRmay be needed if

    Th or K arepresent

    >15%TOC

    > 600 API

    Modified from Nick Harris, Source Rocks 101 Short Course

    Identifying Organic-rich Shales from GR and RHOB

    Bulk Density

    G R

    Organic-richShales

    Nuttal et al, AAPGSearch and Discovery

    Art icl e 40171

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    Delta Log R Technique

    Organic-poor shales = rock matrix + water Immature organic-rich shales = rock matrix + water +

    solid organic matter

    Mature organic-rich shales = rock matrix + water + solidorganic matter + hydrocarbons

    As a result, compared to organic-poor shales Immature organic-rich shales have higher apparent porosity (due

    to low-density, low-velocity kerogen)

    Mature organic-rich shales have higher apparent porosity andhigher resistivity (as water is displaced by generatedhydrocarbons)

    Delta Log R Technique

    Set the scale so that 50microseconds/foot = 1 resistivitycycle

    Adjust the scales so that in ashale, the sonic and resistivitylogs overlap

    Elsewhere, the sonic log will plotto the left of the resistivity log

    The gap between the two curvesis proportional to the TOC

    The resistivity and sonic valueshere are the baseline values

    From Passey et al, 1990

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    Delta Log R TechniqueThe follow ing expressio n (after Passey et. al.) describes the separationof baselined resistivity and porosity lo g curves;

    Where is curve separation

    R is the measured formation resistivityRns is the resistivity of organic-poor shalesP is the porosity log readingPns is the porosity log reading in organic-poor shalesK is a scale factor dependent on porosity log measurement units

    K = -0.02 for sonic, 2.5 for density, and -0.04 for neutron logs

    TOC is calculated using

    Where TOC is total organic carbon in weight percent

    LOM is the level of organic maturityThe equation above predicts zero TOC where there is no curve separation (baselinecondit ions). In practice, however, all shales have some organic carbon content, so it isnecessary to add 0.2 to 1.6 percent to p redicted TOC. The baseline TOC content of shalesis usually determined from laboratory measurements or using local knowledge.

    From Henderson Petrophysics (www.hendersonpetrophysics.com)

    Delta Log R Technique

    Also need to estimate the Level of Organic Metamorphism (LOM) Approximately equal to Ro * 10 at lower LOM values For higher LOM values: If Ro = 1.1, LOM = 11; If Ro = 1.5, LOM = 12; If Ro =

    1.8, LOM = 13; If Ro = 2.1, LOM = 14; If Ro = 2.3, LOM = 15; If Ro = 2.5, LOM= 16; If Ro = 2.8, LOM = 17; If Ro = 3.3, LOM = 18; If Ro = 3.9, LOM = 19

    From Passey et al, 1990

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    Delta Log R Technique

    Comparison to TOC and S2 dataFrom Passey et al, 1990

    ResolvingFractures with

    Logs

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    Fracture Variations by Layer, Outcrop

    Photo From the Austin Chalk, San Antonio

    From WL Taylor and JV Grant, From Carbonate Deformation: Outcrop Analogs for FracturedReservoirs, 2004, Field trip associated with AAPG Annual Conv.

    Fracture Variations by Layer, FMI Log

    Image from a vertical well inthe Barnett Shale illustratesthe relationship betweenmechanical bed thickness andfracture height and length

    The joints terminate at bedboundaries (blue arrows)which separate strata ofdifferent rock mechanicalproperties

    Fracture height and length is,therefore, a function of bedthickness and fracture attitude

    From C. Stamm et al, Barnett Shale, NewLWD sensor technology, SPWLA, 2007

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    Petrophysical AnalysisExample

    Visual Log Assessment GR log

    Higher values indicate higher TOC (hot shales >150 API units)

    Resistivity log Higher resistivity values indicate greater hydrocarbon presence

    Density log Lower values ( 8 pu (limestone matrix)

    Neutron log

    High neutron response (>35 pu) indicative of clays or coals

    Geochemical log Presence of pyrite (associated with higher TOC) Low clay content is a good indicator of brittleness

    From R. Salter and R. Lewis, Schlumberger

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    Recommended Logging Suite

    Spectral GR Induction or Laterolog

    Density with PE curve

    Neutron

    Acoustic scanning tool

    Image log

    Geochemical logging tool Such as the Elemental

    Capture Spectroscopy tool(ECS) for mineralogy,kerogen, matrix density

    From Erik Rylander, Schlumberger

    Generic Petrophys ical Approach for Shale Gas

    Computational process Determine the mineralogy (including kerogen)

    Compute TOC from kerogen (function of kerogen type andmaturity)

    Compute sorbed gas using Langmuir isotherms for samples withvariable TOC values

    Determine effective porosity and Sw; compute free gas

    Convert free gas into scf/ton and add to adsorbed gas to obtaintotal gas

    Key outputs Gas saturation, porosity, hydrocarbons in place per unit

    Can apply reservoir and pay cutoffs if desired

    From Erik Rylander, Schlumberger

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    Mineralogy and TOC

    Need to combine thegeochemical log outputwith knowledge of whichcomponents are present inthe shale (from X-raydiffraction and petrography)

    Typically these are calcite,quartz, pyrite, illite,kaolinite, kerogen, andporosity

    Kerogen is then convertedto TOC

    From Keith Bartenhagen, Schlumberger

    Conversion of Kerogen to TOC

    Kerogen contains carbonand other elements

    As kerogen matures,carbon content increases

    Need to assume a value forK based on thermalmaturity

    Type I II IIIDiagnesis 1.25 1.34 1.48End of Catagenesis 1.20 1.19 1.18

    Maturity Constants

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    Free Gas Calculation

    Need to calculateporosity and Sw valuesfrom the logs thatmatch core-derivedvalues

    May have to changeparameters along thewell to get a match

    Need to know claycontent, matrix density,

    Rw, and electricalproperties

    From Keith Bartenhagen, Schlumberger

    Void Space Correction

    Accounts for the volume of measuredfree space occupied by the sorbed gas

    Shale A shows a decrease of 14.2% offree gas and 11.6% of total gas

    Shale B shows a decrease of 30.2% offree gas and 17.1% of total gas

    From Ray Ambrose et al, SPE 131772

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    Convers ion of Free Gas to SCF/ton

    From R. Salter and R. Lewis, Schlumberger

    Total Gas Log

    K. Bartenhagen,Schlumberger

    80

    200

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    Net Reservoir and Pay Flags

    Net Reservoir >2% Gas-filled porosity

    Pay>4 pu effective porosity2% TOC>100 nanodarcies permeability

    From R. Salter and R. Lewis, Schlumberger

    Technique will likely underestimate the total moveablegas, but can be used to identify wells with the highest productivity/EUR and help explain why they are so good

    A Rigorous Petrophysical Workflow

    1. Load, quality assure, and edit log and core data2. Shift the cores to the log depths3. Apply environmental corrections, if necessary4. Determine if there are sufficient core samples5. Set parameter values based on available logs & cores6. Compute TOC from logs and cores7. Compute fluid density8. Compute average inorganic matrix density and TOC density9. Compute total porosity corrected for the volume of kerogen10. Convert TOC (weight percent) to bulk volu me of kerogen

    11. Recalculate apparent matrix values for the presence of kerogen12. Compute Sw and bulk volume gas (gas-filled porosi ty)13. Compute free, sorbed and total gas14. Compute gas-in-place15. Compute lithologic volumes

    From Log-Core Calibrated Shale Gas Evaluation Procedures, a Weatherford document

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    Summary

    Petrophysics is critical for Estimating production potential

    Selecting completion intervals and designs

    Identifying poor performers

    Quantifying non-shale reservoirs, stimulation barriers, and water-bearing intervals

    Keys to successful evaluation include Gathering sufficient, high-quality data

    Calibrating the logs to other data

    Innovations that will allow us to better quantify gas storage andflow capacity