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  • 7/27/2019 Flow Assurance Presentation - Rune Time I

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    Multiphase flow Offshore Subsea Deepwater Long transportation (Near) Arctic

    Scandpower Petroleum Technology

    ro . une . me

    De artment of Petroleum En ineerinUniversity of Stavanger

    Seminar at Aker Solutions, Stavanger May 31st, 2011

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    ut ine an time sc e u e

    8.30 9.15 Flow regimes and impact on phase slippage,fluid concentrations and pressure drop in

    9.25 10.15 Hydrates, wax and asphaltenes

    10.25 -11.00 Multiphase flow influence from interfaces,

    Seminar at Aker Solutions, Stavanger - May31st, 2011

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    Flow re imes and im act on hase sli a e, fluid

    concentrations and pressure drop in pipelines

    GasQG

    LiquidQL

    Stratified liquid and gas is there a flow? How to decide? Some concepts are needed:

    Fluid fractions Flow patterns ( regimes )

    Seminar at Aker Solutions, Stavanger - May31st, 2011

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    QUIZ:

    A simple(st) case of two-phase flow

    Horizontal pipeline

    Equal inflow

    QL = QG

    GasStabilizedinterface ?

    3

    1

    qu

    Any guideline principles?

    4

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    Basic uantities and definitions:- Superficial velocities and fluid fractions

    uGqG

    AGS

    AG

    uL

    qL

    ULS

    qU LLS Mixture velocity :

    qU GGS

    GSLSmix UUU

    LSL Uq Apparent liquid

    L G LS GSq q U U Seminar at Aker Solutions, Stavanger - May31st, 2011

    5

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    Basic uantities and definitions:- True velocities and Slip

    uGqG

    A

    AG

    uL

    qL

    L

    LL

    Aqu

    True (phase) velocities :

    G

    G

    GA

    u

    LGS uuu

    Gu

    p ve oc y :

    and

    NOSLIP condition:

    uL = uG = Umix

    Lu

    Seminar at Aker Solutions, Stavanger - May31st, 2011

    =

    6

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    Basic uantities and definitions:- True liquid fraction versus noslip fraction

    uGqG

    AGS

    AG

    uL

    qL

    ULS

    True real volume fraction

    LSL

    L

    UA

    S = Slip ratioL GLS GSU U

    S

    LSL UqA arentL

    L G LS GSq q U U

    (noslip):Seminar at Aker Solutions, Stavanger - May31st, 2011

    7

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    True fraction noslip fraction (S = 1)as mixture velocity increases

    11

    LSL

    U

    U U

    Flow regime

    S

    ction

    ( Keeping constant

    L SL

    L S G S

    U

    U U

    Segregated flows Mixed flowsLiquid

    fr

    Umix

    0

    Seminar at Aker Solutions, Stavanger - May31st, 2011

    8

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    Flow regimes in horizontal pipesFlow d rect on

    Stratified smoothflow (SS)

    velo

    city

    Stratified wavyflow (SW)

    Lo

    yspeed

    Elongated bubble

    flow (EB)

    ediatevel

    oci

    sing

    flo

    w

    Slug flow (I)

    Inter

    Increa

    Dispersed bubbleflow (DB)

    ighvelocity

    nnu ar wavyflow (A-AW)

    H

    Seminar at Aker Solutions, Stavanger - May31st, 2011

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    ow regime map orizonta pipes

    10Dispersed bubble (DB)

    Elongated Slug flow (I)

    a e an u er 2.5 cm i.d. Pipeair-water flowat atmosphericconditions

    LS

    ms

    u e ow

    (EB/I)

    Annular -annular wavy -

    Mandhane

    Stratified smoothflow (SS)

    Flow direction

    city

    0.1annular mist flow

    Stratified smooth

    Stratifiedwavy

    flow

    Elongated bubbleflow (EB)

    Slug flow (I)

    Stratified wavyflow (SW)

    Lowvelo

    Intermediatevelocity

    0.1 1 10 100

    0.01

    Dispersed bubbleflow (DB)

    Annular (wavy)flow (A-AW)

    I

    Highvelocity

    UGS

    (m/s)

    Seminar at Aker Solutions, Stavanger - May31st, 2011

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    Flow regimes and map vertical pipes

    Flow regimes - typesFlow regime map

    (small)

    flow

    Slug churnow

    Seminar at Aker Solutions, Stavanger - May31st, 2011

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    Gas concentration profiles

    GGas fraction

    Pipe Up

    Leads to vertical differences: Gas- liquid wetting (evt. water) Asymmetric corrosion (6oclock) Shear stress & Erosion rates Heat transfer rates

    Seminar at Aker Solutions, Stavanger - May31st, 2011

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    Particle slurries in multiphase flow

    D:\BACKUP 2009 - DET ASTRONOMISKE RET 2009\pent Hus 17mars09\Utvalg te high-

    Seminar at Aker Solutions, Stavanger - May31st, 2011

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    Particle slurry regimes - dunes

    Suspended particles in liqud

    Seminar at Aker Solutions, Stavanger - May31st, 2011

    Rabenjafimantsoa and Time ( UIS) - project with Statoil 2000-2005

    14

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    Oil-water-gas flow regime map

    http://www.iceweb.com.au

    /Flow/multiphase_1.htm 15Seminar at AkerSolutions, Stavanger - May31st, 2011

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    Importance of flow regimes

    Much more than just flow appearance:

    Field plan and development Multiphase simulation, pressure and fluid fraction determination Slip ratio and fluid transport rates in long pipelines

    Decisive for quality of multiphase metering

    Flow assurance, safety Process stability and control Pipeline and equipment vibration and fatigue Erosion

    16Seminar at Aker Solutions, Stavanger - May31st, 2011

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    The challenge of calculating

    pressure drop in long traverses

    T e pressure gra ient varies a ong t e pipedue to variation in pipe diameter, inclination

    and mixture density (pressure dependent) outP

    dl

    P P P Pressure at exit:

    in

    ou n

    Sum of pressure drop in all pipe segment

    Challenge in multiphase flow: Thepressureprofile depends on thepressure!

    Seminar at Aker Solutions, Stavanger - May31st, 2011

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    Robust homogeneous pressure drop model

    for two-phase flow

    12000Pressure gradient versus UGS for contant ULSUGS

    x

    6000

    8000

    10000

    dient(Pa/m) Constant Uls= 3m/sConstant Uls= 3m/s

    Total

    ULS

    Friction factor

    2000

    4000

    Pressuregr

    *2

    m mix4 1(Re) U

    2 f

    dp fdx D

    Friction :

    0 5 10 15 20 25 30

    Ugs (m/s)

    m

    h

    dpg sin

    dx

    Hydrostatic:

    mixmix

    dUU

    dxm

    a

    dp

    dx

    Acceleration:EXCEL

    Seminar at Aker Solutions, Stavanger - May31st, 2011

    version18

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    Two-phase pressure drop model Excel version

    UGS Quantity Symbol Value Unit

    LS as ens y rog g m

    Liquid density rol 1000 kg/m 3

    Kinematisk gas viscosity nyg 1,50E-06 m 2/s

    Dynamic gas viscosity myg 1,50E-05 Pa*s

    Liquid viscosity myl 3,00E-03 Pa*s

    Pipe diameter D 1,50E-01 m

    Pipe inclination 20,0 deg 3,49E-01 rad

    Acceleration of gravity g 9,81E+00 m/s^2

    Slipratio S 1,2 ,

    Superficial gas velocity UGS 1,3 m/s

    Mixture velocity Umix 4,8 m/s

    Gas fraction epsg 0,236363636

    Liquid fraction epsl 0,763636364

    Mixture density rom 766 kg/m 3

    Mixture viscosity mym 2,29E-03 Pa*s

    Reynolds number Re 2,40E+05

    Friction factor f 3,86E-03

    2m mixRe U2

    n

    m

    f

    pC

    dx D

    m

    dpg sin

    Frictionpressuredrop dPdx_f 9,08E+02 Pa/mHydrostatic

    pressure

    drop dPdx_h 2,57E+03 Pa/m

    Accelerationalpressuredrop dPdx_a Pa/mTotalpressuredrop dPdx 3,48E+03 Pa/m

    mixmix

    dUUdx

    m

    a

    dpdx

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    The World is Dynamic! need for Measurement

    an ontro

    -does not mean that the individual flowrates (G,L) are constant !

    - Need for multiphase metering for survey and control !

    Separation approachWeatherford

    Mixing approachMPM

    20