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Optimized Recovery from Unconventional Reservoirs: How Nanophysics, the Micro-Crack Debate, and Complex Fracture Geometry Impact Operations

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  • Optimized Recovery from Unconventional Reservoirs: How Nanophysics, the Micro-Crack Debate, and Complex Fracture Geometry Impact Operations

  • Salt Lake City | Bratislava | Calgary | Houston | Jammu | London | Sydney

    ~120 EGI Staff & Affiliated Scientists

  • Large

    Small

    Fast

    Slow

    Rasoul Sorkhabi | Global Systems

    Michal Nemčok | Orogenic Systems

    Lansing Taylor | Prospect- to Seismic-scale Structure

    John McLennan | Reservoir Geomechanics

    Ian Walton | Well-bore Geomechanics

    Milind Deo | Pore to Nano-scale Engineering

    2 New Books

  • • Near Wellbore

    • Well-to-Well

    • Field Development

    150 ft

    1000 ft

    miles

    Ne

    t p

    rese

    nt

    valu

    e

    Completion Technology

    Ne

    t p

    rese

    nt

    valu

    e

    Pressure Maintenance

    Ne

    t p

    rese

    nt

    valu

    e

    Spacing / Geometry

    Optimized Recovery from Unconventional Reservoirs

  • Liquids from Shales

    Milind Deo, Ph.D.Professor and ChairChemical Engineering

    Palash Panja, Ph.D.Post-Doctoral ResearcherEnergy & Geoscience Institute

    • Probability density functions (PDFs)• Obtained using Monte Carlo simulations

    kmRsiℓfpiCfdRs/dppwfng

  • Oil Recovery from Shales1 yr 10 yrs 20 yrs Economic Rate

    5 bbl/d/fracture

    *Xf Km Km Km

    Km *Xf *Xf Rsi

    Rsi Rsi Rsi *Xf

    Pi dRs/dp dRs/dp Pi

    dRs/dp Pi Pi Cf

    *Pwf ng Cf dRs/dp

    ng Cf *Pwf *Pwf

    Cf *Pwf ng ng

    Symbol Property

    Km Matrix perm

    Xf Hydraulic Fracture spacing

    Rsi Initial dissolvedgas oil ratio

    dRs/dp Slope of dissolved GOR

    Pi Initial pressure

    ng Gas rel. perm exponent

    Cf Compressibility

    Pwf Producing BHP Only 2 of the variables are operationally

    controllable parameters

    Most important

    Least important

    Ranking

  • Bryony Richards, Ph.D.Senior PetrologistEnergy & Geoscience Institute

  • • Pressure – 15,000 psi• Temperature 300oF• High-resolution Volume and

    Pressure Measurements

    Absolute permeability

    1 Day, 200 nD 14 days, 5 nD

    Relative permeability

    Shale Interrogator

  • Manas Pathak, Ph.D.Energy & Geoscience Institute

  • rockporerock

    Micro

    rockporerock

    Nano

    Surface Interaction

    At the Nano-scale, permeability is not a rock property but also depends on fluid-rock interaction

  • rockporerock

    Nano

    rockporerock

    Nano

    RestrictionMolecular Dynamics

    Dro

    p b

    elo

    w b

    ub

    ble

    po

    int

    Bubble point is suppressed in nano-pores

  • Shale Gas Production Analysis

    Cumulative production and production rate

    where depends on:– Pressures (bhfp, pore or reservoir pressure)– Reservoir quality/ GIP (permeability, porosity)– Gas properties (viscosity, compressibility, equation of state)– Productive fracture surface area

    t

    CqtCQ

    p

    p 21,

    pC

    0

    0.2

    0.4

    0.6

    0.8

    1

    1.2

    1.4

    1.6

    1.8

    0 2 4 6

    pro

    du

    ctio

    nra

    te (

    bsc

    /ye

    arf)

    time (years)

    0

    200000

    400000

    600000

    800000

    1000000

    1200000

    0 1 2 3

    cu

    mu

    lati

    ve p

    rod

    uc

    tio

    n (

    ms

    cf)

    sqrt(time) years^0.5

    Ian Walton, Ph.D.Research ScientistEnergy & Geoscience Institute

    Gas Production Model

  • • Measure the production coefficient• Estimate pressures, porosity etc• Infer productive fracture surface area

    Productive fracture surface area in the Barnett: 1-5 MM sq ft.

    0

    1

    2

    3

    4

    5

    6

    7

    8

    9

    10

    0 100 200 300 400 500

    Su

    rfac

    e a

    rea

    (MM

    sq

    ft)

    matrix permeability (nD)

    Typical Productive Fracture Surface For Barnett Wells

    poor producer

    average producer

    good producer

    Estimate of Productive Fracture Surface Area

  • Example15 transverse hydraulic fracs each 200 ft high and 500 ft across

    Frac surface area = 2*15*200*500 sq ft= 3 MM sq ft

    Mass balance

    • Frac fluid: Frac surface area ~ 100 MM sq ft

    • Proppant: Propped frac surface area ~ 1-5 MM sq ft

    Estimate of Created Fracture Surface Area

  • • Gas is produced from the volume defined by extent of primary fracture network

    • Most of the fracture fluid resides in the large secondary fracture network and is eventually imbibed into the matrix

    Large scale slickwater fracturing is very inefficient: thevolume of the productive fractures represents only asmall percentage of the volume of the fluid pumped.

    Productive Reservoir Volume

  • Oil Recovery from Shales1 yr 10 yrs 20 yrs Economic Rate

    5 bbl/d/fracture

    *Xf Km Km Km

    Km *Xf *Xf Rsi

    Rsi Rsi Rsi *Xf

    Pi dRs/dp dRs/dp Pi

    dRs/dp Pi Pi Cf

    *Pwf ng Cf dRs/dp

    ng Cf *Pwf *Pwf

    Cf *Pwf ng ng

    Symbol Property

    Km Matrix perm

    Xf Hydraulic Fracture spacing

    Rsi Initial dissolvedgas oil ratio

    dRs/dp Slope of dissolved GOR

    Pi Initial pressure

    ng Gas rel. perm exponent

    Cf Compressibility

    Pwf Producing BHP Only 2 of the variables are operationally

    controllable parameters

    Most important

    Least important

    Ranking

  • Greater penetration, lower fracture density?

    Idealized Conception

    www.halliburton.com

    Lower GRV, higher fracture density?

    Plausible Complexity

    www.drillingcontractor.org

    Interaction with hoop stress

    Interaction with natural fractures

    Interaction with bedding

    Lans Taylor, Ph.D.Research ScientistEnergy & Geoscience Institute

    Large Scale Geologic Controls on Hydraulic Stimulation

    John McLennan, Ph.D.Associate Professor of Chemical EngineeringEnergy & Geoscience Institute

    Mechanical Stratigraphy for Hydraulic Stimulation

  • Does bedding plane slip explain diffuse zones of micro-seismicity during frac jobs?

    Jim Rutledge, SLB Microseismic Services, “The Signature of Shearing Driven by Hydraulic Opening”, HGS Mudrocks Conf. 2015

    Systematic Chaotic

  • North Sea

    Karoo, S. Africa

    Photo: Alan Cooper, www.otago.ac.nz

  • Compressional Crossing

    Process Zone

    Material 1

    Material 2

    Material 1

    Material 2

    σK1 σK1

    σT σT

    Modified from Renshaw & Pollard, 1995

  • Rigid but compressible vs.Flexible but incompressible

    Initial condition

    Vertical loadunconfined

    Vertical loadlateral confinement

    σHflexible > σHrigid

    as Poisson Ratio decreases, Young’s Modulus increases

    Rigid

    Flexible

    Rigid

    Flexible

    Rigid

    Differential Motion

    Con

    stan

    t st

    ress

    Con

    stan

    t st

    rain

  • How is present day stress influenced by basin form and topography?

    Does creep enhance stress heterogeneity?

  • FLEXIBLE

    RIGID

    FLEXIBLE

    RIGID

    FLEXIBLE

    RIGID

    Pressure

    Shale

    Sandstone

    Sandstone

    Sandstone

    Shale

    Shale

    Horizontal Stress Magnitude

    MostCompressive

    LeastCompressive

  • Stratigraphic arrangement matters

    Horizontal Stress Magnitude

    MostCompressive

    LeastCompressive

    FLEXIBLE

    RIGID

    Shale

    Sandstone

    FLEXIBLE

    RIGID

    Shale

    Sandstone

    Sandstone

    Hydraulic Fracture

    FLEXIBLERIGID

    Shale

    Un

    ifo

    rm P

    ress

    ure

    thin sandencasedin shale

    thin shaleencasedin sand

    Co

    arse

    nin

    g u

    pw

    ard

    se

    qu

    en

    ceC

    oarse

    nin

    g u

    pw

    ard se

    qu

    en

    ce

  • Horizontal Stress Magnitude

    MostCompressive

    LeastCompressive

    FLEXIBLE

    RIGID

    Un

    ifo

    rm P

    ress

    ure

    Shale

    Sandstone

    FLEXIBLE

    RIGID

    RIGID

    Shale

    Sandstone

    Sandstone

    Hydraulic Fracture

  • Different placement of horizontal wells will lead to different hydraulic fracture patterns

    Net PressureNet Pressure

  • Finite Element

    Behavior of gradational interfaces

    Direct measurement

    Discrete Element Models

  • Curvature Analysis

    SLB: Dynel2DCourtesy of Laurent Maerten

    1) Input horizon 3) Stress prediction2) Bending model

  • Curvature for Unconventional Targets

    Rigid layers isolated

    Flexible layers isolated

  • Dislocation Analylsis

    (Maerten, et al., AAPG Bull, 2006)

    Fault Locking

    Regional / Counter-regional Faulting

  • 1972 2017

    mailto:[email protected]:[email protected]:[email protected]