4. Wellbore Hydraulics, Pressure Drop Calculations

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    PETE 661Drilling Engineering

    Lesson 4

    Wellbore Hydraulics,

    Pressure Drop Calculations

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    Wellbore Hydraulics

    Hydrostatics

    Buoyancy

    Pipe Tension vs. Depth Effect of Mud Pressure Laminar and Turbulent Flow

    Pressure Drop alculations Bingham Plastic Model

    API Power-Law Model

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    Assignments:

    READ: ADE Ch 4

    HW !": On the Web. - AxialTension

    Due 09-20-04

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    )DD(052.0pp 1ii

    n

    1i

    i0 =

    +=

    Fig. 4-3.

    A Complex

    Liquid

    Column

    D!"#.!p

    pD!"#.!p !

    =

    +=

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    5Fig. 4-4. Viewing the Well as a Manometer (U-

    PPUMP= ?

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    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

    psig266,1pa =

    D!"#.!p =

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    Buoyancy Force = weight of fluid displaced$%rchimedes& #"! B'

    Figure 4-9. Hydrauli !ores ating on a

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    Effectie !"uoyed# $eight

    = sf

    e ())

    Buo!n" F!"#or

    $!lid %or ! &olid 'od or !n open-ended pipe(

    sf

    f

    be

    )

    *)

    +*)

    F))

    =

    == )e, buoyed wei-ht) , wei-ht in air

    Fb, buoyancy force

    + , volume of body

    f, fluid densitys, body density

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    )

    E%ample

    For steel,

    immersed in md,

    t!e "o#an$# %a$tor is&

    -allbm.s 565='-allbm.$ f 015=

    //(.!".0"

    !.("((

    s

    f =

    =

    A drillstring weighs &''(''' l"s in air)

    Buoyed weight = &''(''' * ')++& = ++(&'' l"s

    $, 12! lbmft3'

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    Axi!l For"e& in +rillring

    F"= "it weight

    F&, F& are pressure forces

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    imple E%ample - Empty $ell"ore

    Drillpipe wei-ht , (2." lbfft (!&!!! ft

    4D , ".!!! in

    5D , 1.#/0 in

    ( )## 5D4D1

    %

    =

    % , ".#0" in#

    ) , (2." lbfft 6 (!&!!! ft , (2"&!!! lbf

    A.IAL /E0I10( l"f

    2EP/3(

    ft

    ' l"f &45(''' l"f

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    E%ample - &5 l"6gal Mud in $ell"ore

    Drillpipe wei-ht , (2." lbfft (!&!!! ft

    4D , ".!!! in

    5D , 1.#/0 in

    ( )## 5D4D1

    %

    =

    % , ".#0" in#

    ) , (2"&!!! * 1(&(!! , ("3&2!! lbf

    A.IAL /E0I10( l"f

    2EP/3

    (ft

    ' (2"&!!! lbf

    Pressure at bottom , !.!"# 6 (" 6 (!&!!! , /&7!! psiF , P 6 %

    , /&7!! 6 ".#0"

    , 1(&(!! lbf

    &57(4''- 8&(&''

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    A%ial /ension in 2rill tring

    E%ample % drill strin- consists of

    (!&!!! ftof (2." 8ftdrillpipe and

    0!! ftof (1/ 8ftdrill collarssuspended off bottom in ("8-almud

    $Fb, bit wei-ht , !'.

    )hat is the a9ial tension in the

    drillstrin- as a function of depth:

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    E%ample

    Pressure at top of collars

    , !.!"# $("' (!&!!! , /&7!! psi

    Pressure at bottom of collars, !.!"# $("' (!&0!! , 7 psi

    9ross-sectional area of pipe(

    #

    #

    #

    3( in/3."

    ft

    in(116

    ftlb12!

    ftlb".(2% ==

    A&

    1)4**,

    6**,

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    ross*sectional area of collars&

    22 in2.'31'''90

    1'7 ==

    2

    1

    5377352'3 in...

    %%areaalDifferenti #

    ===

    A:

    A1E%ample ; cont

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    (. %t (!&0!! ft.$bottom of drill collars'

    ompressive force , p %

    , 3"/!! lbf

    ; a9ial tension , * 3"/!! lbf ee %ppendi9 %'

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    :el ;#reng#

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    :el ;#reng#

    s!ear stress at !i$! %lid moement "egins

    +!e #ield strengt!, etrapolated %rom t!e 300

    and 600 :readings is not a good representation o%

    t!e gel strengt! o% t!e %lid

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    :el ;#reng#

    n %ield nits,

    5n practice& this is often appro9imated to

    06.1g=2%t100/l"%

    2%t100/l"%

    +!e gel strengt! is t!e maimmdial reading!en t!e is$ometer is started at 3 rpm.

    g= m!x/3

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    $elo"i# ro%ile&

    l!min!r %lo

    Fig) 8-:>) @elocity profiles for laminar flow

    !a# pipe flow and !"# annular flow

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    It looGs liGe concentric rings of fluid

    telescoping down the pipe at different elocitiesH

    72 @iew of Laminar Flow in a pipe

    - 0ewtonian Fluid

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    !'le 4.3 - ;umm!r o% 9qu!#ion& %or

    o#!#ion!l $i&"ome#er

    0e#oni!n odel

    a

    3!!=

    r

    !00."#

    =

    3!!a =

    or

    !'le 4 3 ;umm!r o% 9qu!#ion& %or

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    !'le 4.3 - ;umm!r o% 9qu!#ion& %or

    o#!#ion!l $i&"ome#er

    300

    or

    1p# 1

    =

    rpm3atmag

    =

    Bing!m l!i" odel

    300600p = )(300

    or

    12

    12

    p =

    p300# =

    or

    or

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    4)

    9x!mple 4.22

    >ompte t!e %ri$tional pressre loss %or a 7? 5?

    annls, 10,000 %tlong, sing t!e slot %lo

    representation in t!e annls. +!e %lo rate is 80

    gal/min. +!e is$osit# is 15 $p. ssme t!e %lopattern is laminar.

    +H 5H &H6

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    9x!mple 4.22

    +!e aerage elo$it# in t!e annls,

    )52.''8(7

    80

    )d2.''8(d

    @

    222

    1

    2

    2

    A

    =

    =

    %t/s1.362A

    =

    ( ) 212

    A

    %

    dd1000

    B

    dC

    dp

    =

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    9x!mple 4.22

    ( )51.0750psi51

    )57(1000

    )000,10()362.1()15(D

    dC

    dpp

    2%

    ==

    ==

    fp

    ( )#(#

    H

    f

    dd(!!!

    vI

    dL

    dp

    =

    / l P P

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    /otal Pump Pressure

    Pressure loss in surf) euipmentPressure loss in drill pipe

    Pressure loss in drill collars

    Pressure drop across the "it no??lesPressure loss in the annulus "etween the drill

    collars and the hole wall

    Pressure loss in the annulus "etween the drill

    pipe and the hole wall

    3ydrostatic pressure difference !aries#

    / f fl

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    /ypes of flow

    L!min!r

    Fig. '30. Caminar and tr"lent %lo patterns in a $ir$lar pipe& (a) laminar

    %lo, (") transition "eteen laminar and tr"lent %lo and ($) tr"lent %lo

    ur'ulen#

    ' l # Fl

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    ur'ulen# Flo -

    0e#oni!n Fluid

    -e o%ten assme t!at %lid %lo is

    #ur'ulen# i% 0re < 21**

    $p.%lid,o%is$osit#B

    in.D.,piped%t/selo$it#,%lidag.

    l"m/galdensit#,%lidE!ere

    A

    ===

    =

    B

    dE928

    A

    e =

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    /ur"ulent Flow -

    0ewtonian Fluid

    #".(

    #".!

    /".(/".!

    f

    d(7!!

    v

    dL

    dp =

    /ur"ulent Flow -

    Bingham Plastic Fluid

    #".(

    #".!

    p

    /".(/".!

    f

    d(7!!

    v

    dL

    dp =

    ( ) #".((#

    #".!

    p

    /".(/".!

    f

    dd320&(

    v

    dL

    dp

    =

    ( ) #".((#

    #".!

    /".(/".!

    f

    dd320&(

    v

    dL

    dp

    =

    In Annulus

    In Pipe

    %P5 P L M d l

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    %P5 Power Law Model

    $onsisten$# inden %lo "e!aior inde

    SHEARSTRESS

    psi

    = K n

    SHEAR RATE, , sec-10

    API P &72

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    @otatin- >leeve +iscometer

    @I91ME/E

    PM

    3(!!

    3!!

    0!!

    $@PM 6 (./!3'

    3EA A/E

    sec -&

    ".(((/!.3

    "((

    (!##

    B1B

    LEE@E

    A00ULU

    2ILL

    /I0J

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    Pressure Drop alculations

    E%amplealculate the pump pressure in thewellbore shown on the ne9t pa-e& usin- the %P5

    method.

    /he releant rotational iscometer readingsare as follows

    @3 , 3 $at 3 @PM'

    @(!!, #! $at (!! @PM'

    @3!!, 32 $at 3!! @PM'

    @0!!, 0" $at 0!! @PM'

    P DP

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    PPUMP , P2P = P29

    = PBI/ 01KKLE

    = P296A00 = P2P6A00

    = P32

    # , #7! -almin

    , (#." lb-al

    Pressure Drop

    alculations

    P"UM"

    P D 5 D ill Pi 12 = 8 5 in

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    6*

    Power-Law 9onstant $n%:

    Pressure Drop 5n Drill Pipe

    Fluid 9onsistency Inde% $&%:

    Aerage BulG @elocity in Pipe $'%:

    12 = 8)5 in

    I2 = 7)+ in

    L = &&(8'' ft

    /3/.!32

    0"lo-3#.3

    @

    @lo-3#.3n

    3!!

    0!! =

    =

    =

    2737.0

    600 se$017.2022,1

    6511.5

    022,1

    11.5

    cm

    dyneRK

    n

    n ===

    sec

    ft!!.7

    /7.3

    #7!61!7.!

    D

    J1!7.!+

    ## ===

    P D 5 D ill Pi #$ % 4 &

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    Effectie @iscosity in Pipe $ e%:

    Pressure Drop 5n Drill Pipe

    eynolds 0um"er in Pipe $(Re%:

    #$ % 4.&in'$ % .*

    in+ % ,,4!t

    n(n

    en1

    (n3

    D

    +20K(!!

    +

    =

    cP"3/3/.!61

    (/3/.!63

    /7.3

    7620!(/.#6(!!

    /3/.!(/3/.!

    e =

    +

    =

    0(0&0"3

    ".(#6!!.76/7.362#7+D2#7

    e

    @e ==

    =

    P D 5 D ill Pi #$ % 4 &

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    ()*E: (Re+ ,-.., soFriction Factor in Pipe $/%:

    Pressure Drop 5n Drill Pipe #$ % 4.&in '$ %.* in

    + % ,,4!t

    /o

    b

    @eaf =

    !/"2.!"!

    23.3/3/.!lo-

    "!

    23.3nlo-

    a =+

    =

    +

    =

    #02!.!/

    /3/.!lo-/".(

    /

    nlo-/".(b =

    =

    =

    !!/(#0.!0(0&0

    !/"2.!

    af

    #02!.!b

    @e

    ===

    P D 5 D ill Pi #$ % 4.&

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    Friction Pressure Jradient $dP0dL%:

    Pressure Drop 5n Drill Pipe #$ % 4.&in '$ %.* in

    + % ,,4!t

    Friction Pressure 2rop in 2rill Pipe:

    1!!&((6!"73/.!LdL

    dP

    P =

    =

    "d0% 11&

    0si

    ft

    psi!"73/.!

    /7.367(.#"

    ".(#676!!/(#0.!

    D7(.#"

    +f

    dL

    dP ##

    ==

    =

    P D 5 D ill ll #$ % 1.&

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    Power-Law 9onstant $n%:

    Pressure Drop 5n Drill ollars

    Fluid 9onsistency Inde% $&%:

    Aerage BulG @elocity inside 2rill 9ollars $'%:

    #$ % 1.&in '$ %2.& in

    + % 1!t/3/.!

    32

    0"lo-3#.3

    @

    @lo-3#.3n

    3!!

    0!! =

    =

    =

    #

    n

    /3/.!n

    0!!

    cm

    secdyne!(/.#

    !##&(

    0"6((."

    !##&(

    @((."K ===

    sec

    ft#7.(7

    ".#

    #7!61!7.!

    D

    J1!7.!+

    ## ===

    #$ % 1.&P D 5 D ill ll

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    Effectie @iscosity in 9ollars$ e%:

    eynolds 0um"er in 9ollars $(Re%:

    #$ 1.&in '$ %2.& in

    + % 1!t

    Pressure Drop 5n Drill ollars

    n(n

    en1

    (n3

    D

    +20K(!!

    +

    =

    cP#(.37/3/.!61

    (/3/.!63

    ".#

    #7.(7620!(/.#6(!!

    /3/.!(/3/.!

    e =

    +

    =

    7/!&(3#(.37

    ".(#6#7.(76".#62#7+D2#7

    e

    @e ==

    =

    #$ % 1.&P D 5 D ill ll

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    #$ 1.&in '$ %2.& in

    + % 1!t

    Pressure Drop 5n Drill ollars

    ()*E: (Re+ ,-.., soFriction Factor in 29 $/%: b@eaf =

    /o

    !/"2.!"!

    23.3/3/.!lo-

    "!

    23.3nlo-

    a =

    +

    =

    +

    =

    #02!.!/

    /3/.!lo-/".(

    /

    nlo-/".(b =

    =

    =

    !!"71!.!7/!&(3

    !/"2.!

    af

    #02!.!b

    @e

    ===

    #$ % 1.&P D 5 D ill ll

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    Friction Pressure Jradient $dP0dL%:

    Friction Pressure 2rop in 2rill 9ollars:

    #$ 1.&in '$ %2.& in

    + % 1!t

    Pressure Drop 5n Drill ollars

    ft

    psi3/7!.!

    ".#67(.#"

    ".(#6#7.(76!!"71!.!

    D7(.#"

    +f

    dL

    dP ##

    ==

    =

    0!!63/7!.!LdL

    dPP

    =

    =

    "d% 22

    0si

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    Pressure Drop across oles

    $3,% ,, 2nds

    (in) $32% ,,

    2nds (in) $3%

    ,2 2nds (in)

    ( )#####

    (#((((

    #7!6".(#6("0P

    ++=

    "3oles% ,21

    0si

    ( )##3###

    (

    #

    DDD

    J("0P

    ++

    =

    Pressure Drop

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    6)

    Pressure Drop

    in DH4LE

    %nnulus

    $H#+5 % *.&in#$$6 % 1.&

    in

    + % 1

    Q = 280 gal/min

    = 12.5 lb/gal*.&in

    $ % * &Pressure Drop

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    Power-Law 9onstant $n%:

    Fluid 9onsistency Inde% $&%:

    Aerage BulG @elocity in 29631LE Annulus $'%:

    $H#+5 % *.&

    in#$$6 % 1.&

    in+ %1 !t

    Pressure Drop

    in DH4LE %nnulus

    "1(3.!3

    #!lo-0"/.!

    @

    @lo-0"/.!n

    3

    (!! =

    =

    =

    #

    n

    "1(3.!n

    (!!

    cm

    secdyne330.0

    #.(/!

    #!6((."

    #.(/!

    @((."K ===

    sec

    ft7!7.3

    ".0".7

    #7!61!7.!

    DD

    J1!7.!+

    ###

    (

    #

    #

    =

    =

    =

    $ % * &

    Pressure Drop

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    Effectie @iscosity in Annulus $ e%:

    eynolds 0um"er in Annulus $(Re%:

    $H#+5 % *.&

    in#$$6 % 1.&

    in+ %1 !t

    cP#!."""1(3.!63

    ("1(3.!6#

    ".0".7

    7!7.36(11330.06(!!

    "1(3.!("1(3.!

    e =

    +

    =

    ( ) ( )0!!&(

    #!.""

    ".(#67!7.36".0".72#7+DD2#7

    e

    (#

    @e =

    =

    =

    n(n

    (#

    en3

    (n#

    DD

    +(11K(!!

    +

    =

    Pressure Drop

    in DH4LE %nnulus

    $ # % *.&

    Pressure Drop

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    /o

    $H#+5 % *.&

    in#$$6 % 1.&

    in+ %1 !t

    ()*E: (Re1 ,-..Friction Factor in Annulus $/%:

    !("!!.!0!!&(

    #1

    #1f

    @e

    ===

    ( ) ( ) ftpsi

    !"#00.!".0".77(.#"

    ".(#67!7.36!("!!.!

    DD7(.#"

    +f

    dL

    dP #

    (#

    #

    =

    =

    =

    0!!6!"#00.!LdLdPP ==

    "d7hole% ,.1

    0si

    Pressure Drop

    in DH4LE %nnulus

    Pressure 2rop

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    q = 280 gal/min

    = 12.5 lb/gal

    Pressure 2rop

    in 2P631LE Annulus

    $H#+5 % *.& in

    #$$" % 4.& in

    + %,,4 !t

    Pressure 2rop $H#+5 % *.& in

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    Power-Law 9onstant $n%:

    Fluid 9onsistency Inde% $&%:

    Aerage BulG @elocity in Annulus $'a%:

    Pressure 2rop

    in 2P631LE Annulus

    H#+5

    #$$" % 4.& in

    + %,,4 !t

    "1(3.!3

    #!lo-0"/.!

    @

    @lo-0"/.!n

    3

    (!! =

    =

    =

    #

    n

    "1(3.!n

    (!!

    cm

    secdyne330.0

    #.(/!

    #!6((."

    #.(/!

    @((."K ===

    sec

    ft(2/.#

    ".1".7

    #7!61!7.!

    DD

    J1!7.!+

    ###

    (

    #

    #

    =

    =

    =

    Pressure 2rop

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    Effectie @iscosity in Annulus $ e%:

    eynolds 0um"er in Annulus $(Re%:

    p

    in 2P631LE Annulus

    n(n

    (#

    en3

    (n#

    DD

    +(11K(!!

    +

    =

    cP01.2/"1(3.!63

    ("1(3.!6#

    ".1".7

    (2/.#6(11330.06(!!

    "1(3.!("1(3.!

    e =

    +

    =

    ( ) ( )!11&(

    01.2/

    ".(#6(2/.#6".1".72#7+DD2#7

    e

    (#

    @e =

    =

    =

    Pressure 2rop

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    /o 0si

    Pressure 2rop

    in 2P631LE Annulus

    ()*E: (Re1 ,-..Friction Factor in Annulus $/%:

    !##22.!!11&(

    #1

    #1f

    @e

    ===

    ( ) ( ) ftpsi

    !(313.!".1".77(.#"

    ".(#6(2/.#6!##22.!

    DD7(.#"

    +f

    dL

    dP #

    (#

    #

    =

    =

    =

    1!!&((6!(313.!LdLdPP ==

    "d07hole% ,&.2 0si

    P 2 9 l

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    Pressure 2rop 9alcs)

    - UMMA -

    PPUMP , P2P = P29 = PBI/ 01KKLE

    = P296A00 = P2P6A00 = P32

    PPUMP , 00" = ##/ = (&!#0

    = 3# = ("3 = !

    PPUMP = &(4& &5 = :(&'7 psi

    P"UM" = P$/ + P33 + PH8$

    :(&'7 psi

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    PPUMP = &(4& &5

    = :(&'7 psi

    PH8$, !

    P"UM" = P$/ + P33 + PH8$

    P$/ = P$" + P$6 + P:'T 3#;;+5/

    , 00" = ##/ = (&!#0 , (&2(7

    psiP33= P$6733 + P$"733

    , 3# = ("3 , (7"

    P

    ='

    NFrictionN Pressures

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    7)

    !

    "!!

    (&!!!

    (&"!!

    #&!!!

    #&"!!

    ! "&!!! (!&!!! ("&!!! #!&!!! #"&!!!

    9umulatie 2istance from -tandpipe( ft

    N

    FrictionNPressure(psi

    2ILLPIPE

    2ILL 91LLA

    BI/ 01KKLE

    A00ULU

    3ydrostatic Pressures in the $ell"ore

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    8*

    y

    !(&!!!

    #&!!!

    3&!!!

    1&!!!

    "&!!!

    0&!!!

    /&!!!

    7&!!!

    2&!!!

    ! "&!!! (!&!!! ("&!!! #!&!!! #"&!!!

    9umulatie 2istance from -tandpipe( ft

    3

    ydrostaticPre

    ssure(psi

    B3P

    2ILL/I0J A00ULU

    Pressures in the $ell"ore

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    !(&!!!

    #&!!!

    3&!!!

    1&!!!"&!!!

    0&!!!

    /&!!!

    7&!!!2&!!!

    (!&!!!

    ! "&!!! (!&!!! ("&!!! #!&!!! #"&!!!

    9umulatie 2istance from -tandpipe( ft

    Pressure

    s(psi

    /A/I9

    9I9ULA/I0J

    $ell"ore Pressure Profile

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    !

    #&!!!

    1&!!!

    0&!!!

    7&!!!

    (!&!!!

    (#&!!!

    (1&!!!

    ! #&!!! 1&!!! 0&!!! 7&!!! (!&!!!

    Pressure( psi

    2ept

    h(

    f

    2ILL/I0J

    A00ULU

    $>tatic'

    BI/

    Pipe Flow Laminar

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    Pipe Flow * Laminar

    5n the above e9ample the flow down thedrillpipe was turbulent.

    Gnder conditions of very hi-h viscosity&

    the flow may very well be laminar.

    ()*E: i/ (Re1 ,-.., then

    Friction Factor in Pipe $/%:

    @e

    (0f =

    D7(.#"

    +f

    dL

    dP #

    =

    Then and

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    84

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    vfdpH

    #

    n = 1.*