12 Laminar Flow Slot Flow

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    PETE 411

    Well Drilling

    Lesson 12

    Laminar Flow - Slot Flow

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    Lesson 12 - Laminar Flow - Slot Flow

    4The Slot Flow Approximation4Shear Rate Determination

    4Pressure Drop Calculations

    4Laminar Flow

    4Turbulent Flow4Transition Flow - Critical Velocity

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    Read:

    Applied Drilling Engineering

    Ch.4 to p. 145

    Homework #6

    On the WebDue Friday, October 4, 2002

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    Representing the Circular Annulus as a Slot

    )r(r!WslotofWidth

    )r(rhslotofHeight

    rr!WhslotequivalentofArea

    "2

    "2

    2

    "

    2

    2

    +==

    ==

    ==

    { slot approximation is OK if (d1/d2 > 0.3 }

    Equal

    Area

    and

    Height

    Simpler

    Equations

    -yetaccurate

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    5Free body diagram for fluid element in a narrow slot

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    yW#LdL

    dppyWpF

    ypWF

    f

    22

    "

    ==

    =

    Representing the Annulus as a Slot

    F4 = y +yWL = +ddyy WL

    F3 =WL

    Consider:

    - pressure forces

    - viscous forces

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    Representing the Annulus as a Slot

    state,steadyAt

    F = m aSumming forces along flow:

    F = 0

    F

    "

    F2 + F3

    F4 = 0

    0LW#ydy

    d$$-LW$yW#L

    dL

    dp-p-ypW f =

    ++

    ,gSimplifyin dp f

    dLd

    dy= 0

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    Representing the Annulus as a Slot

    dydv% =

    :integrateandvariablesSeparate

    Model,FluidNewtonianWith

    dp fdL

    ddy

    = 0

    dL

    dpy

    0

    f $$ +=Evaluate 0 at wall where y = 0

    = %$

    But,

    of

    dL

    dpy

    dy

    dv$$ +==

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    Representing the Annulus as a Slot

    += dy$ydL

    dp-dv 0

    f

    00f

    2

    v

    y$

    dL

    dp

    2

    yv +=

    of $

    dL

    dpy

    dy

    dv +=

    0 v0,y when0vSince 0 ===

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    Representing the Annulus as a Slot

    h$-

    dL

    dp

    2

    h-0h,y when0 vSince 0f

    2

    ===

    dL

    dp

    2

    h-$ f0 =

    ( )2f yhydL

    dp

    2

    "v =

    Hence, substituting for v0 and 0 :

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    Representing the Annulus as a Slot

    == vWdyvdAq

    The total flow rate:

    ( )

    =

    h

    0

    2f dyyhydL

    dp

    2

    Wq

    dL

    dp

    "2

    Whq f

    3

    =

    g,Integratin

    "2

    2

    "

    2

    2 rrhand)r(r!Wh ==But

    ( )2f yhydL

    dp

    2

    "v =

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    Representing the Annulus as a Slot

    2

    "2

    2

    "

    2

    2

    f

    )r)(rr(rdL

    dp

    "2

    !

    q =

    )r(r!

    q

    A

    qv

    2"

    22 ==velocity,averageBut

    2

    "2

    _

    f

    )r(r

    v"2

    dL

    dp

    =

    In field units,2

    "2

    _

    f

    )d"000(d

    v

    dL

    dp

    =

    psi/ft, cp., ft/sec, in

    dL

    dp

    12

    Whq f

    3

    =

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    Example 4.22

    Compute the frictional pressure loss for a 7 x

    5 annulus, 10,000 ft long, using the slot flowrepresentation in the annulus. The flow rate

    is 80 gal/min. The viscosity is 15 cp.

    Assume the flow pattern is laminar.

    7 5 1

    6

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    Example 4.22

    The average velocity in the

    annulus,

    )52.448(7

    80

    )d2.448(d

    qv

    222

    "

    2

    2

    _

    =

    =

    ft/s".362v_

    =

    ( )2"2

    _

    f

    dd"000

    v

    dL

    dp

    =

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    Example 4.22

    A somewhat more accurate answer, using an

    exact equation for a circular annulus, results

    in a value of 50.9792 psi.

    Difference = 0.0958 psi i.e., within 0.2%

    ( )5".0750psi5"

    )57("000

    )000,"0()362."()"5(

    DdL

    dp

    #p 2f

    ==

    ==

    fp

    ( )2

    "2

    _

    f

    dd"000

    v

    dL

    dp

    =

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    Determination of Shear Rate...(why?)

    If shear rate in well is known:

    1. Fluid can be evaluated in viscometer at

    the proper shear rate.

    2. Newtonian equations can sometimes

    give good accuracy even if fluid isnon-Newtonian.

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    Determination of Shear Rate

    The maximum value of shear rate will

    occur at the pipe walls.

    For circular pipe, at the pipe wall,

    dL

    dp

    2

    r

    $

    fw

    w =from (Eq. 4.5")

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    Determination of Shear Rate

    From Eq. 4.54b,

    (at the wall)

    w

    _

    w

    2

    w

    _

    ww

    2

    w

    _

    f

    r

    v4$

    r

    v8*

    2

    r$

    r

    v8

    dL

    dp

    =

    =

    =

    dL

    dp

    2

    r$ fww =

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    Determination of Shear Rate (why?)

    Using the Newtonian Model,

    Changing to field units,

    w

    _

    w

    _

    w

    r

    v4

    r

    v4*

    "

    $% ===

    dv96%

    _

    =

    (circular pipe)

    sec-", ft/sec, in

    w

    _

    wr

    v4$ =

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    Annulus:

    From the slot flow approximation,

    dL

    dp

    2

    )rr(

    dL

    dp

    2

    h f"2fw

    ==

    But, Eq. 4.60 c

    2

    "2

    _

    )(

    "2

    rr

    v

    dL

    dp f

    =

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    Shear Rate in Annulus

    "2

    _

    2

    "2

    _

    "2 6

    )(

    "2

    2

    )(

    rr

    v

    rr

    vrrw

    =

    =

    "2

    _

    "2

    _

    w

    rr

    v6

    rr

    v6"

    =

    ==

    In field units:(annulus)

    "2

    _

    dd

    v"44

    =

    Where, ft/secinisv_

    inchesinaredandd 2"

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    Power - Law: Example 4.24

    A cement slurry has a flow behavior index of

    0.3 and a consistency index of 9,400 eq. cp.

    The slurry is being pumped in an 8.097 * 4.5 -inch annulus at 200 gal/min.

    (i) Assuming the flow pattern is laminar,

    compute the frictional pressure

    loss per 1,000 ft of annulus.

    (ii) What is the shear rate at the wall?

    n = 0.3

    K = 9,400

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    Example 4.24

    )d2.448(d

    qvvel.,Avg.(i)

    2

    "

    2

    2

    _

    =

    s/ft803."v_

    =

    ( )22_

    5.4097.8448.2

    200

    v =

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    Example 4.24

    n

    n"

    "2

    _n

    f

    0.0208n

    "2

    )d"44,000(d

    vK

    dL

    dp,Press.Drop

    +

    = +

    0.3

    ".3

    0.3

    f

    0.0208

    0.3"2

    4.5)097"44,000(8.

    3)9,400(".80

    dL

    dp

    +

    =

    ftpsi/1,00077.9psi/ft0779.0

    dL

    dp========

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    Example 4.24 contd

    (ii) Shear rate at pipe wall,

    ( )

    +

    =

    n

    "2

    dd

    v48%

    "2

    _

    w

    +

    =

    0.3

    "2

    4.58.097

    ".803*48% w

    "

    w s"28%

    = = 75 RPM

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    Total Pump Pressure

    Pressure loss in surf. equipment

    Pressure loss in drill pipe

    Pressure loss in drill collars

    Pressure drop across the bit nozzles

    Pressure loss in the annulus between the drillcollars and the hole wall

    Pressure loss in the annulus between the drillpipe and the hole wall

    Hydrostatic pressure difference ( varies)

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    Total Pump Pressure

    )#P(PPPPPPP HYDDPADCABDCDPSCPUMP ++++++=

    PUMP

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    Types of Flow

    Laminar Flow

    Flow pattern is linear (no radial flow)

    Velocity at wall is ZERO

    Produces minimal hole erosion

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    Types of Flow - Laminar

    Mud properties strongly affect

    pressure losses

    Is preferred flow type for annulus

    (in vertical wells)

    Laminar flow is sometimes referred toas sheet flow, or layered flow:

    * As the flow velocity increases, the flow type

    changes from laminar to turbulent.

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    Types of Flow

    Turbulent Flow

    Flow pattern is random (flow in all directions)

    Tends to produce hole erosion

    Results in higher pressure losses

    (takes more energy)

    Provides excellent hole cleaningbut

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    Types of flow

    Mud properties have little effect on pressure losses

    Is the usual flow type inside the drill pipe and collars

    Thin laminar boundary layer at the wall

    Turbulent flow, contd

    Fig. 4-30. Laminar and turbulent flow patterns in a circular pipe: (a) laminar

    flow, (b) transition between laminar and turbulent flow and (c) turbulent flow

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    Turbulent Flow - Newtonian Fluid

    The onset of turbulence in pipe flow is

    characterized by the dimensionlessgroup known as the Reynolds number

    dvN

    _

    Re =

    dv&928N

    _

    Re =

    In field units,

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    Turbulent Flow -

    Newtonian Fluid

    We often assume that fluid flow is

    turbulent if Nre > 2,100

    cp.fluid,ofviscosity

    inI.D.,piped

    ft/svelocity,fluidavg.v

    lbm/galdensity,fluid&where

    _

    =

    =

    =

    =

    dv&928N

    _

    Re =