1.7 pressure drop calculations

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    1

    Pressure Drop Calculations

    1.7-1

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    2

    1.7-2

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    3

    1.7-3 For multiple nozzles in

    parallel

    Vn is the same for each nozzleeven if thedn varies!

    This followssince Dp is the sameacross each nozzle.

    t

    nA117.3

    qv

    2

    2

    t

    2

    d

    -5

    bitAC

    q10*8.311p

    10*074.8

    pcv

    4dn D

    &

    Cd = 0.95

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    4

    1.7-4 Hydraulic Horsepower

    of pump putting out 400 gpm at 3,000 psi = ?

    Power, in field units:

    1714

    000,3*400HHP

    1714

    pqHHP

    D

    Hydraulic Horsepower of Pump = 700 hp

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    5

    1.7-5 What is Hydraulic Impact

    Force

    developed by bit?

    If:

    psi169,1p

    lb/gal12

    gal/min400q

    95.0C

    n

    D

    pqc01823.0F dj D

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    6

    1.7-6 Laminar Flow

    Rheological Models

    Newtonian

    Bingham Plastic

    Power-Law (ADE & API)

    Rotational Viscometer

    Laminar Flow in Wellbore

    Fluid Flow in Pipes

    Fluid Flow in Annuli

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    7

    Laminar Flow of Newtonian Fluids

    A

    F

    L

    V

    Experimentally:

    1.7-7

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    8

    1.7-8 Newtonian Fluid Model

    In a Newtonian fluid the shear stress is directly

    proportional to the shear rate (in laminar flow):

    i.e.,

    The constant of proportionality, is the viscosity

    of the fluid and is independent of shear rate.

    sec

    12

    cm

    dyne

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    9

    1.7-9 Newtonian Fluid Model

    Viscosity may be expressed in poise orcentipoise.

    poise0.01centipoise1

    scm

    g

    1cm

    s-dyne

    1poise1 2

    2cmsecdyne

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    10

    1.7-10 Shear Stress vs. Shear Rate for aNewtonian Fluid

    Slope of line

    .

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    11

    1.7-11 Typical Drilling Fluid Vs. Newtonian,

    Bingham and Power Law Fluids

    0

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    12

    1.7-12 Rheological Models

    1. Newtonian Fluid:

    2. Bingham Plastic Fluid:

    viscosityplastic

    pointyield

    p

    y

    What ify 0?

    py

    rateshear

    viscosityabsolute

    stressshear

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    13

    1.7-13Rotating

    Sleeve

    Viscometer

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    14

    1.7-14 Figure 3.6Rotating

    Viscometer Rheometer

    We

    determinerheological

    properties

    of drilling

    fluids inthis device

    Infinite

    parallel

    plates

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    15

    1.7-15 Rheometer

    (Rotational Viscometer)

    Shear Stress = f (Dial Reading)

    Shear Rate = f (Sleeve RPM)

    Shear Stress = f (Shear Rate)

    )(f BOB

    sleeve

    fluid

    RateShearthe(GAMMA),ofvalue

    theondependsStressShearthe),TAU(

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    16

    1.7-16 Example

    A rotational viscometer containing a Bingham plastic

    fluidgives a dial reading of 12 at a rotor speed of 300RPM and a dial reading of 20 at a rotor speed of 600 RPM

    Compute plastic viscosity and yield point

    12-20

    300600p

    cp8p

    600 = 20300 = 12

    See Appendix A

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    17

    1.7-17 Example

    8-12

    p300y

    2

    y ftlbf/1004

    600 = 20300 = 12

    (See Appendix A)

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    18

    1.7-18 Gel Strength

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    19

    1.7-19 Gel Strength

    = shear stress at which fluid movement begins

    The yield strength, extrapolated from the

    300 and 600 RPM readings is not a good

    representation of the gel strength of the fluid

    Gel strength may be measured by turning the

    rotor at a low speed and noting the dial

    reading at which the gel structure is broken

    (usually at 3 RPM)

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    20

    1.7-20 Gel Strength

    In field units,

    In practice, this is often approximated to

    06.1g 2ft100/lbf

    2ft100/lbf

    The gel strength is the maximum dial readingwhen the viscometer is started at 3 rpm.

    g = max,3

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    21

    1.7-21 Velocity Profiles

    (laminar flow)

    Fig. 4-26. Velocity profiles for laminar flow:

    (a) pipe flow and (b) annular flow

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    22

    It looks like concentric rings of fluid

    telescoping down the pipe at different velocities

    3D View of Laminar Flow in a pipe

    - Newtonian Fluid

    1.7-22

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    23

    1.7-23 Table 4.3 - Summary of

    Equations for Rotational Viscometer

    Newtonian Model

    NaN

    300

    Nr

    066.52

    300a

    or

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    24

    1.7-24 Table 4.3 - Summary of Equationsfor Rotational Viscometer

    300

    N

    or

    1pNy 1

    rpm3atmaxg

    Bingham Plastic Model

    300600p )(NN

    300

    or

    12 NN

    12

    p

    p300y

    or

    or

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    25

    1.7-25 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 drill

    collars and the hole wall

    Pressure loss in the annulus between the drill

    pipe and the hole wall

    Hydrostatic pressure difference ( varies)

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    26

    1.7-26 Pressure losses for laminar

    flow.

    2

    500,1 d

    V

    dL

    dP

    2

    12000,1 dd

    V

    dL

    dP

    dd

    V

    dL

    dP yp

    225500,1 2

    122

    12 200000,1 dddd

    V

    dL

    dP yp

    Newtonian Fluid Bingham Plastic Fluid

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    27

    1.7-27 Types of flow

    Laminar

    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

    Turbulent

    1 7 28 Turbulent

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    28

    1.7-28 Turbulent

    Flow - Newtonian

    Fluid

    We often assume that fluid flow is

    turbulent if Nre > 2100

    cp.fluid,ofviscosity

    inI.D.,piped

    ft/svelocity,fluidavg.v

    lbm/galdensity,fluidwhere

    _

    dv928N

    _

    Re

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    Turbulent Flow -

    Newtonian Fluid

    25.1

    25.075.1_

    75.0f

    d1800

    v

    dL

    dp

    Turbulent Flow -

    Bingham Plastic Fluid

    25.1

    25.0

    p

    75.1_75.0

    fd1800

    v

    dL

    dp

    25.112

    25.0

    p

    75.1_75.0

    f

    dd396,1

    v

    dL

    dp

    25.112

    25.0

    75.1_75.0

    f

    dd396,1

    v

    dL

    dp

    In Annulus

    In Pipe

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