09 Drilling Hydraulics Hydrostatics

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    1

    PETE 411

    Well Drill ing

    Lesson 9

    Drilling Hydraulics- Hydrostatics

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    2

    Drilling Hydraulics - Hydrostatics

    Hydrostatic Pressure in Liquid Columns

    Hydrostatic Pressure in Gas Columns

    Hydrostatic Pressure in Complex Columns

    Forces on Submerged Body

    Effective (buoyed) Weight of Submerged

    Body

    Axial Tension in Drill String A = FA/A

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    3

    Read:

    Applied Drilling Engineering, Ch.4

    (Drilling Hydraulics) to p. 125

    HW #4

    ADE #1.18, 1.19, 1.24

    Due Monday, Sept 23, 2002

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    4

    Drilling Hydraulics Applications

    Calculation of subsurface hydrostatic

    pressures that may tend to burst orcollapse well tubulars or fracture exposedformations

    Several aspects of blowout prevention

    Displacement of cement slurries andresulting stresses in the drillstring

    WHY?

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    5

    Drilling Hydraulics Applications

    contd

    Bit nozzle size selection for optimum

    hydraulics

    Surge or swab pressures due to vertical

    pipe movement

    Carrying capacity of drilling fluids

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    6Fig. 4-2. The Well Fluid System

    Well Control ppore < pmud < pfrac

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    9

    Incompressible Fluids

    Integrating,

    dDFdp vw=

    0vw pDFp +=

    ]0Dwhenpp[ 0 ==

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    10

    Incompressible Fluids

    In field units, 33.8*144

    4.62 =vwF

    33.8*433.0 =

    052.0=vwF

    1 x 1 x 1

    cube

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    Incompressible fluids

    If p0 = 0 (usually the case except during

    well control or cementingprocedures)

    then,

    0pD052.0p +=

    ft}lbm/gal,{psig,052.0 Dp =

    D052.0

    p=

    p0

    p

    D

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    12

    Compressible

    Fluids

    dDFdp vw=dD052.0dp =

    (1)

    from (3)

    (3)

    (2)

    But, TRMmZTRnZpV ==

    TZ3.80

    pM

    ZRT

    pM

    V

    m=== (4)

    p = pressure of gas, psia

    V = gas volume, gal

    Z = gas deviation factorn = moles of gas

    R = universal gas constant = 80.3

    T = temperature, R

    = density, lbm/gal

    M = gas molecular wt.m = mass of gas

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    Compressible Fluids

    p = pressure of gas, psia

    V = gas volume, gal

    Z = gas deviation factor

    n = moles of gas

    R = universal gas constant,

    = 80.3

    T = temperature,oR

    = density, lbm/gal

    M = gas molecular wt.

    m = mass of gas, lbm

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    14

    Compressible Fluids

    =D

    D

    p

    p 00

    dD

    TZ1544

    M

    p

    dp

    dD

    TZ80.3

    Mp052.0dp =

    From Eqs. (2) and (4):

    D

    D

    p

    p 00[D]

    TZ1544

    M]p[ln =

    Integrating,

    ]

    TZ1544

    )DD(M[exppp 00

    =

    Assumptions?

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    16

    Example (i)

    (i) What is pressure at 10,000 ft?

    ]TZ1544

    )D-M(D[exppp 00000,10 =

    psia1188])140460)(1(1544

    0)-16(10,000[exp1000 =

    +=

    ]

    TZ1544

    )DD(M[exppp 00

    =

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    17

    Example contd

    gallbm331.0

    600*1*3.8016*1000

    TZ3.80pM

    0 ===

    (ii) What is density at surface?

    gal

    lbm

    395.0600*1*3.80

    16*1188

    TZ3.80

    pM000,10 ===

    (iii) What is density at 10,000 ft?

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    18

    Example

    (iv) What is psurf if p10,000 = 8,000 psia?

    ?p surf =

    ]TZ1544

    )DD(M[exppp 00

    =

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    19

    )DD(052.0pp 1ii

    n

    1i

    i0

    =

    +=

    Fig. 4-3.A Complex

    Liquid

    Column

    Dp

    pDp

    =

    +=

    052.0

    052.00

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    20Fig. 4-4. Viewing the Well as a Manometer

    Pa = ?

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    21

    Figure 4.4

    })000,10(0.9)000,1(7.16

    )700,1(7.12)300(5.8)000,7(5.10{052.00

    +

    +++=ppa

    psig00 =p

    psig266,1p a =

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    22

    Buoyancy Force = weight of fluid

    displaced (Archimedes, 250 BC)

    Figure 4-9. Hydraulic forces acting on a foreign body

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    Example

    For steel,

    immersed in mud,

    the buoyancy factor is:

    gal/lbm5.65s =

    )/0.15( gallbmf =

    7710565

    01511 .

    .

    .

    s

    f =

    =

    A drillstring weighs 100,000 lbs in air.

    Buoyed weight = 100,000 * 0.771 = 77,100 lbs

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    Axial Forces in Drillstring

    Fb = bit weight

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    Simple Example - Empty Wellbore

    Drillpipe weight = 19.5 lbf/ft 10,000 ft

    OD = 5.000 in

    ID = 4.276 in

    ( )22 IDOD4

    A =

    A = 5.265 in2

    W = 19.5 lbf/ft * 10,000 ft = 195,000 lbf

    AXIAL TENSION, lbf

    DEP

    TH,

    ft

    0 lbf 195,000 lbf

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    29b221212dpdp

    b2121T

    FAp)AA(pWxw

    FFFWWF}above(c){:PipeDrillAt

    ++=

    ++=

    Anywhere in the Drill Pipe:

    Axial Tension = Wts. - Pressure Forces - Bit Wt.

    FT

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    30

    Axial Tension in Drill String

    Example

    A drill string consists of 10,000 ft of19.5 #/ft drillpipe and 600 ft of 147 #/ft

    drill collars suspended off bottom in

    15#/gal mud (Fb = bit weight = 0).

    What is the axial tension in thedrillstring as a function of depth?

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    Example

    Pressure at top of collars = 0.052 (15) 10,000

    = 7,800 psi

    Pressure at bottom of collars = 0.052 (15) 10,600

    = 8,268 psi

    Cross-sectional area of pipe,

    2

    2

    2

    31in73.5

    ftin144*

    ft/lb490ft/lb5.19A ==

    A1

    10,000

    10,600

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    Example

    Cross-sectional area of collars,

    2

    2 in2.43144*

    490

    147A ==

    2

    12 in5.3773.52.43AAareaalDifferenti ===

    A2

    A1

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    Example

    1. At 10,600 ft. (bottom of drill collars)

    Compressive force = pA

    = 357,200 lbf

    [ axial tension = - 357,200 lbf]

    2

    2 in2.43*in

    lbf268,8=

    4

    32

    1

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    Example

    2. At 10,000 ft+ (top of collars)

    FT = W2 - F2 - Fb

    = 147 lbm/ft * 600 ft - 357,200

    = 88,200 - 357,200

    = -269,000 lbf

    4

    32

    1

    Fb = FBIT= 0

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    37Fig. 4-11. Axial tensions as a function of depth for Example 4.9

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    38

    Example - Summary

    1. At 10,600 ft FT = -357,200 lbf[compression]

    2. At 10,000 + ft FT = -269,000 lbf[compression]

    3. At 10,000 - ft FT = +23,500 lbf[tension]

    4. At Surface FT = +218,500 lbf[tension]