8. Logging While Drilling

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    Logging While Drilling

    Sonic Travel Time

    Resistivity and Conductivity

    Eatons Equations (R, C, Dt, dc)

    Natural Gamma Ray

    Other

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    Assignments

    Homework # 5:

    Ch 2, Problems 21-30

    due Friday, June 18

    Read: All of Chapter 2

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    Logging While Drilling

    Any log that infers shale porosity

    can indicate the compaction state ofthe rock,

    and hence any abnormal pressure

    associated with undercompaction.

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    Logging While Drilling

    Most of the published correlations are

    based on sonic and electric log data.

    Density logs can also be used if

    sufficient data are available.

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    Pore Pressure Gradient vs.

    difference between actual and

    normal sonic travel time

    From Hottman and Johnson

    LA Upper TX Gulf Coast

    to tn, sec/ft

    gp,psi

    /ft

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    Matthews and KellyNormal

    to tn, sec/ft

    gp,psi

    /ft

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    Relationships vary from area to

    area and from age to age

    But, the trends are

    the same.

    to tn, sec/ft

    gp,psi/ft

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    Resistivity and Conductivity

    Rock grains, in general, are very poor

    conductors.

    Saline water in the pores conducts

    electricity and this fact forms the basis

    for inferring porosity from bulk R or Cmeasurements.

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    Resistivity and Conductivity

    Under normal compaction, R increases

    with depth.

    Deviation from the normal trend

    suggests abnormal pressure

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    Resistivity and Conductivity

    FR = Ro/Rw FR = formation

    resistivity factor

    Ro = resistivity of water-

    saturated formation

    Rw = resistivity of pore water

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    Porosity,

    m

    RaF/1

    Porosity of water-saturated rock,

    If a = 1, and m = 2, then f = FR-0.5

    So, f = (Ro/Rw)

    -0.5

    Rw in shales cannot be measured directly

    so Rw in a nearby sand is used instead.

    Ro would tend to increase with increasing

    depth under normally pressured

    conditions. See Fig. 2.63.

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    Fig. 2.63 Normal Compaction

    Ro , m

    Depth,

    ft

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    Example 2.20

    Rw estimated fromnearby well.

    Estimate the pore

    pressure at 14,188 ftusing Foster and

    Whalens techinque.

    So, at 14,188 ft,

    FR = 28.24

    034.0

    96.0

    w

    o

    RR

    RF

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    Transition at

    ~11,800

    Using Eatons Gulf

    Coast correlations,

    sob = 0.974 psi/ft or

    13,819 psig at 14,188

    Eq. Depth = 8,720

    sobe = 0.937 psi/ft or

    8,170 psig at 8,720pne = 0.465*8,720

    = 4,055

    pp = ppe + (sob - sobe)= 4,055+(13,816-8,171)

    = 9,703 psig

    = 13.16 ppg

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    Fig. 2.65 -Hottman & Johnsons upperGulf Coast Relationship between

    shale resistivity and pore pressure

    Rn/Ro

    Gp,

    psi/ft

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    Example 2.21

    Matthews andKelly

    Determine the transition

    depth and estimate the

    pore pressure at 11,500

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    Transition is at ~9,600 ft.

    At 11,500 ft:

    Co = 1,920, and

    Cn = 440

    Co/Cn = 1,920 / 440

    = 4.36

    gp = 0.81 psi/ft (Fig 2.66)

    Example 2.21

    Fig. 2.67

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    gp = 0.81 psi/ft

    rp= 15.6 ppg

    pp = 9,315 psig

    Fig. 2.66

    4.36

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    Eatons Equations

    2.1

    2.1

    2.1

    3

    cn

    conobobp

    o

    nnobobp

    n

    onobobp

    o

    nnobobp

    d

    dgggg

    C

    Cgggg

    R

    Rgggg

    t

    tgggg 34.2.Eq

    35.2.Eq

    36.2.Eq

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    Eatons Equations

    These equations differ from the earliercorrelations in that they take into

    consideration the effect a variable

    overburden stress may have on theeffective stress and the pore pressure.

    Probably the most widely used of the

    log-derived methods

    Have been used over 20 years

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    Solution

    Eaton

    From Eq. 2.35,

    gp = gob - (gob - gn)(Ro/Rn)1.2

    gp = 0.920 - (0.920 - 0.465)(0.264)1.2

    gp = 0.827 psi/ft

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    Solution

    Hottman & Johnson

    Rn/Ro = 1/(0.264) = 3.79

    From Fig 2.65, we then get

    gp = 0.894 psi/ft

    Difference = 0.894 0.827 = 0.067 psi/ft

    Answers differ by 770 psi or 1.3 ppg

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    Discussion

    Actual pressure gradient was

    determined to be 0.818 psi/ft!

    In this example the Eaton method camewithin 104 psi or 0.17 ppg equivalent

    mud density of measured values

    This lends some credibility to the Eaton

    method.

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    Discussion

    In older sediments, exponent may be

    lowered to 1.0 for resistivities.

    Service companies may have more

    accurate numbers for exponents.

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    Natural Gamma Ray

    The K40 isotope tends to concentrate in

    shale minerals thereby leading to the

    traditional use of GR to determine theshaliness of a rock stratum.

    It follows that GR intensity may be used

    to infer the porosity in shales of

    consistent minerology

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    Natural Gamma Ray

    Pore pressure prediction using MWD is

    now possible (Fig. 2.68).

    Lower cps (counts per second) may

    indicate higher porosity and perhaps

    abnormal pressure.

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    Pore pressure gradient prediction fromobserved and normal Gamma Ray counts

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    Example 2.23

    From table 2.17,determine the porepressure gradient at11,100 ft usingZoellers correlation.

    Use the first threedata points to

    establish the normaltrend line.

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    Effective Stress Models

    Use data from MWD/LWD

    Rely on the effective-stress principle as the

    basis for empirical or analytical prediction

    Apply log-derived petrophysical parameters

    of the rock to a compaction model to

    quantify effective stress

    Knowing the overburden pressure, the pore

    pressure can then be determined

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    Dr. Choes Kick Simulator

    Take a kick

    Circulate the kick out of the hole

    Plot casing seat pressure vs. time

    Plot surface pressure vs. time

    Plot kick size vs. time

    etc.