Tuesday 21 May 2013 - Keynote - Charles Fairhurst

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    Fractures and Fracturing

    a presentation

    by

    Charles Fairhurst*

    to

    The International Conference for Effective and Sustainable

    Hydraulic Fracturing

    20-22 May 2013,

    The Hilton Brisbane, Australia.

    *Senior Consultant, Itasca Consulting Group, Inc. Minneapolis, USA.

    Professor Emeritus, University of Minnesota. Minneapolis.

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    Purposes of Hydraulic Fracturing

    to enhance connectivity between existing fractures

    for improved

    fluid flow

    conditioning

    -where natural fracturing is not sufficient

    (e.g. Caving of longwall goaf ;block caving in mines).

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    Kirsch (1898)Circle

    Inglis (1913)

    Ellipse

    Griffith (1921). Stress is highly concentrated at tip of

    degenerate ellipse very thin crack or flaw.

    Tensile Strength of Solid should be about

    E/3. Actual strength is three orders lower.

    Inter-atomic Force-Separation Relationship

    Stress Concentrations around

    holes in Isotropic Continuum

    Fracture Mechanics

    Linearly Elastic Fracture Mechanics (LEFM)

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    Theorem of Minimum Potential Energy.

    The stable equilibrium state of a system is that for whichthe potential energy

    of the system is a minimum.

    The equilibrium position, if equilibrium is possible,must be one in which

    rupture of the solid has occurred, if the system can pass from the unbroken to

    the brokencondition by a process involving acontinuous decrease of potential

    energy.

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    P = W +U + S +K ( + )

    Changes in

    P = Potential Energy of System.W = Potential Energy of Applied Forces

    U = Strain Energy

    S = Surface Energy

    K = Kinetic Energy

    F =Frictional Energy etc.

    Crack accelerates, decelerates, goes

    around or through grains seekingMinimum Potential Energy path.

    Potential Energy Changes during

    Crack Propagation throughHeterogeneous Solid under Tension Crack may stop, but rock strength may

    decrease with time - and crack may extend.

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    Crack Propagation from Internally Pressurized Hole in a Glass Plate

    Porter and Fairhurst (1970) - after Mindlin (1939)

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    Hydraulic Fracturing (1949)Unlike previous discussion, fracture extension is by fluid injection

    In an impermeable medium, the viscous energy dissipation associated with driving fluid through the fracture

    (Reynolds , Poiseuille laws) competes with the energy required to break the solid material.In a permeable medium, fluid leak-off further complicates the mechanics of crack propagation.

    Fracturing of the rock at the crack tip is governed by LEFM i.e. the asymptotic form

    w = K1s

    1/2

    ,

    w is crack aperture, and s is distance from the crack tip.

    Where viscous flow dominates, the coupling between the fluid flow and solid deformation leads

    to the asymptotic formw =K2s

    2/3

    K1, K2 are constants.

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    Scaling

    The discovery of scaling laws very often allows an increase,

    sometimes even a drastic change, in the understanding of not only asingle phenomenon but a wide branch of science.

    G.I.Barenblatt. Scaling [Cambridge Univ.Press (2003)]

    Important attribute of classical analyses is that solution is given in

    terms of dimensionless groups.

    ..

    Previous analyses assumed that the medium was a

    homogeneous continuum.

    Will now consider rock mass.

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    Rock in situ is probably the most complex material encountered in any

    engineering discipline.

    Pre-loaded by tectonic and gravitational loads for many millions of years,

    transected with fractures and a variety of planar discontinuities, etc., the

    mechanical behavior can only be determined directly in the field.

    .

    Mining evolved empirical rules over many, many years; well aware of

    complexity

    - technology going beyond limits of experience - into uncharted territory.

    -direct 3D access to subsurface. (shared with Civil Engineering)

    - little R&D investment in rock mechanics in past 2~ 3 decades.

    Petroleum- (150 year history) - direct 1D access only; some rules ;

    - intensive R&D - results proprietary.

    Other subsurface engineering developments -Enhanced Geothermal,Carbon Sequestration; Drill Cuttings Injection; Tight Shales, etc.?

    - Relatively little experience

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    Importance of Pre-existing Fracture Networks

    Enhanced Geothermal Systems - Fenton Hills, New Mexico, 1970

    .idea that hydraulic pressure causes competent rock to rupture and

    create a disc-shaped fracture was refuted by the seismic evidence.

    Instead, it came to be understood that

    hydraulic stimulation leads to the opening of existing

    natural joints

    that have been sealed by secondary mineralization.

    Over the years additional evidence has been generated to show that the

    joints oriented roughly orthogonal to the direction of the least principal

    stress open first, but additional joints open as the hydraulic pressure is

    increased

    (Duchane and Brown GHC Bulletin Dec. 2002 p.15 GHC (Geo-Heat Center)

    http://geoheat.oit.edu/
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    Increasingfluidpressure

    Hydraulic Fracturing may be preceded by Slip on JointsIn a Permeable Jointed Rock.

    Hydro-Shearing

    Hydraulic

    Fracturing

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    Fracture

    representation

    3D Discrete

    Fracture Network

    (DFN)

    Intact rock

    representation

    (including brittlefracture)

    Synthetic Rock Mass (SRM)

    Bondedparticle

    assemblyintersected

    withfractures(SRM)

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    13

    The consequence is that each element appears to bephysically isolatedfrom its neighbors during one time step;

    Thus

    Explicit Finite Difference Method - The Calculation Cycle.(Results of each cycle can be superimposed to form a movie of evolution of deformation)

    Forces are fixed

    duringthis

    calculation

    Strain rates are

    fixed duringthis

    calculation

    (forallmass-points)

    (forallelements)

    All Itasca codes use an explicitsolution method that marches on in time

    (even for static problems). Cundall, 1970.

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    Observed Path of Hydraulic Fracture as revealed by Mine-Back

    Courtesy Jeffrey et al; CSIRO

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    Response to Complexity and Lack of Understanding in Engineering.

    1. Develop empirical rules based on experience.

    2. Develop theory to refine and improve practice.

    Industrial Revolution later development of Continuum Mechanics.Rock Mechanics in Mining and Civil Engineering. (3D access to rock mass)

    Petroleum - 1D access (borehole) greater research emphasis (proprietary)

    Limits to Empiricism

    requires practical experience;

    applicable only within bounds of available experience.

    Proposed applications of Hydraulic Fracturing to situations where

    Little prior experience.

    No time to develop empirical rules.

    Enhanced Numerical Modeling and Observational Tools are Available.

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    Numerical Experiments.

    Rock mechanics models fall into the class of data-limited problems;

    one seldom knows enough about a rock mass to model it unambigously.

    The purpose of modelling data-limited problems is to gain understanding

    and to explore potential trade offs and alternatives, rather than to make

    absolute predictions

    A model is an aid to thought, rather than a substitute for thinking.

    plan the modelling exercise in the same way as you would plan a laboratoryexperiment.

    (Starfield and Cundall, 1988)

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    Major Challenge

    is to define

    realistic

    Discrete Fracture Networks (DFNs)

    especially for borehole access situations.

    Progress!

    Do DFN characteristics depend significantly on rock

    formations e.g. crystalline; sedimentary?

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    Fracture Imaging

    Schlumberger

    P

    P

    P

    P P

    S

    S

    P

    Imaging of reflected waves (PtPand StS) when the tool is above or

    below the fracture.

    Imaging with mode conversions(PtS and StP) when the fracture is

    between the transmitter and

    receiver.

    Waves return to the tool based on

    the geometry of the event relative

    to the tool:

    Up-dip reflector imaged when the

    tool is above the fracture

    Down-dip reflector imaged when

    the tool is below the fracture

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    Horizontal well with open fractures away from the wellbore

    Schlumberger

    24

    00

    -20

    20

    -40

    F

    eet

    X000 X100 X200 X300 X400 X500

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    Summary #

    Reflections from monopole receivers have been

    used to successfully image structure and fractures

    Depth of investigation can vary greatly, but can

    beas much as 140 ft on each side of theborehole.

    Bridges the resolution gap between wireline and

    seismic data.

    Complementary data from Stoneley mobility,

    Anisotropy, Rock properties and potentially

    Radial Profiling can be acquired in the same

    pass.

    0.1 1.0 10 100

    0.1

    1.0

    10

    100

    Range [m]

    Resolution[m]

    ultra-

    sonic

    sonic

    2D seismic

    3D seismicVSP

    (3D)Deep

    Acoustic

    Imaging

    The Acoustic Gap

    0.1 1.0 10 100 1000

    100

    10

    1

    0.1

    10

    D.Grael et al*; Borehole Acoustic Reflection Survey (BARS) from Modern, Dipole Acoustic Logs for High-Resolution

    Seismic-Based Fracture Illumination and Imaging SPWLA (Soc. Petrophysicists and Well Logging Analysts),

    53rd

    Annual Logging Symposium, June 16-20, 2012 Cartagena , Columbia .

    *D. Grae, G. A. Ugueto C., J. A. Roberts, H. Yamamoto, T. Oliver and G. Martine

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    (a)Micro

    Seismic

    Indication

    of

    Upward

    Migration

    of

    Fluidalong Fault during HydraulicFracturing

    (b)NumericalExplanationof

    UpwardMigration.

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    In Situ Stress and Critically Stressed Sub-Surface

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    In-Situ Stress State

    1. Magnitude and Orientation affected by undetected fractures/faults

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    Observed variability of normal stress across a thrust fault at the URL, Pinawa,Canada.

    Local In situ Stresses Affected by Local Variations on Faults

    How do In situ Stresses Change with Rock Type;

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    Limestone

    H > V> h

    Argillite(indurated clay)

    H = V = h

    Limestone

    V > H > h

    In

    Situ

    Stresses

    Change

    with

    Rock

    Type

    (Underground

    Research

    Laboratory,

    Bure.

    France)

    How do In situ Stresses Change with Rock Type;

    Relevance to Tight Gas Shales ?

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    Aseismic slip induced by forced fluid flow as detected by P-wave tomogrqphy

    (Soultz-sous-Frets, France) Cornet et al; 2012

    (a) The injection program (black curve is flow rate; blue curve is well-head pressure; horizontal axis is time in

    days;

    (b) 3D view of the seismic cloud with respect to the GPK2 borehole. Vertical axis is depth and horizontal axes

    are distances respectively toward the north and toward the east; and

    (c) Horizontal projections corresponding to the yellow horizontal plane. The vertical green plane is shown as

    line AB in the plots of part c. P-wave velocity tomography for sets 2,3 and 4 are indicated respectively by

    orange, yellow and green colors in the injection program. The vertical axis corresponds to North.

    20%Drop

    in

    Vp.

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    Vp 6.4km/s=1.00

    Vp 5.1km/s=0.80

    Aseismic Deformation

    20%dropinPwavevelocityinregion

    ~500moutsideseismiccloud.

    2.0E+07

    d

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    0

    5

    10

    15

    20

    25

    0 2 4 6 8 10

    BoreholePressure(MPa)

    Total

    Time

    (days)

    0.0E+00

    2.0E+06

    4.0E+06

    6.0E+06

    8.0E+06

    1.0E+07

    1.2E+07

    1.4E+07

    1.6E+07

    1.8E+07

    0 250 500 750

    Pressure(Pa)

    Distance(m)

    2days

    6days

    7days

    8days

    9days

    10days

    0.0E+00

    2.0E+06

    4.0E+06

    6.0E+06

    8.0E+06

    1.0E+07

    1.2E+07

    1.4E+07

    1.6E+07

    1.8E+07

    2.0E+07

    0 250 500 750

    Pressure(Pa)

    Distance(m)

    2days

    6days

    7days

    8days

    9days

    10days

    =104 mD

    Fluid Flow into Far -Field

    continues

    after Borehole Depressurization.

    =250mD

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    9

    Why Doesnt Microseismicity Correlate

    With Production?

    The Total Rock Volume

    Affected by

    Microseismicity

    Accounts for Less

    Than 1% of Gas

    Production in First 6

    Months

    IngrainInc

    Micro-permeabe gas shales.

    Courtesy Prof.A.Nur

    Stones

    have

    begun

    to

    speak,

    because

    an

    ear

    is

    there

    to

    hear

    them.

    ..

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    g p ,Cloos,ConversationswiththeEarth(1954),4

    Fracture

    Network

    Engineering.

    Synthetic

    Rock

    Mass

    and

    Synthetic

    Seismicity

    Modelsarecomparedwithobservedmicroseismic signalsforrealtime controlof

    fracturenetworkdevelopment. (EnhancedGeothermalSystems.)

    Microseismicity predicted

    and

    observed.

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    Rock Conditioning

    In situ Rock Weakening /Size Reduction

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    Pre-Splitting (Atlas Copco)

    Plexiglas after Detonation of Explosive in Hole

    (Persson et al; (1970) ISRM Congress, Betgrade (1970)

    Rock Conditioning - Hydraulic (Gas) Fracturing

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    C l i

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    Conclusions.Hydraulic Fracturing applications increasingly important for extraction of resources and

    injection /disposal of waste products.

    Pre-existing fracture systems have dominant effect on hydra-frac development and related

    stimulation procedures.

    Rock Fracture Mechanics is potentially as broad as classical Fracture Mechanics.

    Rock mass embraces wide variety of constitutive behaviors; rock is not critically

    stressed everywhere in crust; concept can be very misleading.

    Micro-seismic detection systems are essential but do not identify full response of system to

    stimulation additional geophysical tools needed.

    Datalimited nature of Earth Resource Engineering problems gives added importance

    to analysis and modeling.

    Numerical experiments (scalable) can be major aid to practical advance but will require

    planning/co-ordination to allow sound Mechanics-Informed practical decisions.

    Fracture Network Engineering is sound goal, but requires considerable additional

    development.

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    Thank you

    - to the organizers of Hydraulic Fracturing 2013

    for the invitation to participate in the Conference

    and to present this Lecture;

    - to the audience for your attention.

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    Back - up Slides

    D/R = 0.1 D/R = 0.2Potential for core damage during

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    0

    0

    0.2

    2 4

    0.4

    0.6

    D/R = 1D/R = 2

    t

    t

    tt

    t

    o

    o

    oo

    o

    /

    /

    / /

    /0.00

    0.50

    0.25

    t o/

    0.00

    0.50

    0.25

    t o/

    0.0

    1.0

    0.5

    t o/

    0.0

    1.0

    0.5

    Maximum

    Maximum Maximum

    Maximum

    = 0.05

    = 0.5 = 1.0

    = 0.1

    Core Depth / Core Radius, D/R

    t

    o

    /

    Max.tensilestressincore

    Far-fieldstress

    ,

    D

    R

    g gcoring operation

    Numericalresults

    Best fit curve

    Let

    Let

    n

    m

    =

    =

    =

    =

    t

    ti

    c

    c

    c

    o

    o

    o

    tensile strength

    induced tension in core

    compressive strength

    in-situ horizontal stress

    [n ~ 0.1]

    [m ~ 0.5]

    Then core damage occurs if

    >

    >

    n/m

    0.2i.e.,

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