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Lecture11a_Basic Gaslift Sec 1 - Principles

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    Gas Lift

    Lecture 11a- Gas Lift, Section 1 - Principles

    Recommended Texts: Handout and

    rt c a t et o s,

    Kermit E. Brown, Volume 2a

    PennWell Publishing Co, Tulsa, OK, 1980

    Akim Kabir

    Senior LecturerDepartment of Petroleum Engineering

    Curtin University of Technology

    Slide 1Section 1 - PrinciplesAug 2008

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    Gas Lift

    y s rt c a t ee e

    Well quit

    Production declines with depletion of reservoirenergy

    Water cut increases Maximize production from naturally flowing wells

    Note that this is different from gas injection for pressure maintenance

    Injection of gas or water into reservoir to maintain reservoirpressure

    Improve recovery

    Slide 2Section 1 - Principles

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    Gas Lift

    Pi

    Qi Reservoir Pressure

    ,

    artificial lift

    is required to

    a er u

    WC1restore or

    increase

    pro uct onProductionProduction

    time t1

    Slide 3Section 1 - Principles

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    Gas Lift

    Gas lifting

    Continuous

    Chamber lift

    Plun er lift?

    Plunger Lift

    Rod um in

    Electrical Submersible pumping

    Progressive Cavity pumping

    Slide 4Section 1 - Principles

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    Gas Lift

    Continuous

    Intermittent

    A Continuous

    Gas Lift System

    Low Pressure gas

    FTHPProduced Fluids + Lift Gas

    Separator

    High Pressure Gas

    CHP

    as t ompressor

    Liquid

    Slide 5Section 1 - Principles Pwf

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    Gas Lift

    Open Semi-closed Closed

    Slide 6Section 1 - Principles

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    Gas Lift

    Gas

    vaves

    closed All valvesclosed

    Bottom valveopen

    Fluid from formationhas built up above

    Bottom valve opens andslug is propelled toward

    Bottom valve closeswhen slug reaches the

    Slide 7Section 1 - Principles

    the bottom alve. the surface surface

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    Gas Lift

    -Production

    as

    Only bottomvalve is o en All valves

    closed

    Fluid from

    formation has

    All valves

    below the slu

    Valves close

    when slugbuilt up abovethe bottom

    open as slugmoves toward surface

    reaches thesurface

    Slide 8Section 1 - Principles

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    Gas Lift

    The injected gas aerates the fluid column and reduces

    the density of the fluid

    e ens y o e co umn re uce , o om o e

    pressure gets lower and less reservoir pressure is

    re uired to ush the l i uid to surface.

    In other words the hydrostatic back pressure to thereservoir is reduced and the reservoir pressure can

    overcome this reduced pressure and initiates the well to

    flow.

    Slide 9Section 1 - Principles

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    Gas Lift

    GL 'ed Dua l Com p le t ion - An Examp le

    MIN I.D.STATUSSHORT STRING

    DEPTH

    Loca t i on :Wel l : XX

    Wel lhead : MCEVOY DUAL (REFURBISHED)

    Standard Wel l Type : X3123 7" LINER

    DEPTHLONG STRING

    M IN I.D . S TA TU S

    Compl et ion Date : 1 .1. 2004

    Max. Deviat ion : 43 deg @ 7131 f t

    A ll De p th s in FT. AH.B THF

    BTHF = 44 FT BDF (T6)Tubing : 3 .1/2" x 9.2 # New VAM, L80

    Tubing tails: 2.7/8" x 6.4 #, NSCT, 2.3/8" x 4.6 # NSCT

    f t . f t .

    in

    3.1/2" XXO-NIPPLE

    3 .1 /2 "KBUG

    3.1/2 " KB UG

    3.1/2 " KB UG

    3.1/2 " KB UG

    3.1/2" XXO-NIPPLE 399437

    1066

    1759

    2355

    2856

    BKR-5

    BKR-5

    DK-13 .1 /2 " K BUG4459

    3.1/2" FLOW COUPLING3.1/2" FLOW COUPLING

    2.8132.813

    2.875

    3 .1 /2 " K BUG5857

    2.9102.910

    3 .1 /2 " K BUG

    3.1 /2 " K BUG

    945

    1667

    DK-1

    B K R - 5

    3 .1 /2 " K BUG

    3.1 /2 " K BUG

    2230

    2763

    DK-1

    B K R - 5

    3.1/2" K B UG 4366B K R - 5

    2.875

    3.1/2" KB UG 5764B K R - 5

    3.1/2" KB UG 6549DKO-23 . 1/ 2" K B U G6674

    BKR-5

    BKR-5

    BKR-5

    DKO-2.

    X67043.1/2" X-NIPPLE (CAMCO)2.750

    6737 9.5/8" RDH PACK ER (40-47#)

    67732.7/8" CMD SSDCLOSED

    V67 01 3.1/2 " C MD -S SD

    68092.7/8" XN-NOGO NIPPLECHAM FERED BTM (CAM CO)

    NO PLUG

    2.313

    2.205

    2.750

    3 .1/2 " LOCKABL E COLLET 6737

    67473.1/2" x 2.7/8 X-OVER2.441

    2.900

    2.900

    TOP OF T IE BACK PKR 6913

    NO PLUGCLOSE

    CLOSED7977 3.1/2" CM D-SSD 2.750

    8013 3.1/2" x 2.3/8" X-OVER 1.901

    8275

    8277

    8074

    8080

    8095

    8161

    8162

    36 - Q1.0 - 8180 - 9196, 8214 - 8216

    36 - Q1.5 - 8244 - 8246, 8254 - 8258, 8264 - 8274

    SBS (4 " NU8RD)

    4" WWS TELL TALE

    3.250

    3.423

    OTIS 7 " WD 4 .5 " x 4 .0 "

    4 " GPE

    4 .1/2 " BLA NK CASING

    4.5" LT C x 4 " NU8RD XO

    4" WWS

    4.000

    4.000

    3.875

    3.423

    3.423

    8267 2.3/8" TBG SEAL ASSY 1.901

    9.5 /8" CSG SHOE 7212

    8285

    8291

    OTIS 7 " WD 4 .5 " x 4 .0 "

    SB E

    4.000

    3.250

    + 15 SEAL UNITS SIZE:3.25"

    2 .3 /8 " LOC TB G SEALAS SY + 1 5 S EA L UN ITS

    I : "

    1.901

    OTIS 7" WD 4.5" x 4.0"

    4 " GPE

    4 .1/2 " BLA NK CASING

    4.5" LT C x 4 " NU8RD XO

    4" WWS

    4.000

    4.000

    3.875

    3.423

    3.423

    10489

    10485

    10509

    10572

    10573OPEN2.3/8" XD-SSD 1.875

    10683

    10653

    SBS (4 " NU8RD)

    4" WWS TELL TALE

    SB E

    I " " "

    3.250

    3.423

    3.000

    10676

    10678

    10685

    36 - S8.3/8.4 - 10588 - 10672

    I : .

    2.3/8" XN-NOGO BXP

    2.3/8" x 6 ' PERF. PUP

    2.3/8" W/LINE RE-ENTRY

    GUIDE + DROP-OFFBULLNOSE

    10753

    10756

    10764

    2.3/8" X-NIPPLE

    PXN PLUG

    10717X 1.875

    I . .. 106 7

    36 - S9.3 - 10757 - 10772

    36 - S10.1 - 10793 - 10822

    4" GPE

    4 .1/2 " BLA NK CASING

    4.5" LT C x 4 " NU8RD XO

    4" WWS

    4.000

    3.875

    3.423

    3.423

    10693

    10708

    10741

    10742

    SBS (4 " NU8RD)

    4" WWS TELL TALE

    BULL NOSE ASSY

    3.250

    3.423

    3.403

    10824

    10826

    10833

    1.791

    1.901

    1.901

    Slide 10Section 1 - Principles

    10891LANDING COLLAR

    7" CSG SHOE

    Designed BY :

    DATE : 09 /08 /01 (MARLINE)

    CHECKED: 10 /05 /01 (ESMERALDA)

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    Gas Lift

    INJECTION GAS

    No gas injection; Well is Dead

    PRESSURE (PSI)500 10000

    Dummy

    Fluid Level

    500

    CASING PRESSURE

    Dummy 1000 TUBING PRESSURE

    Valve 1

    Valve 2

    EPTH(

    FTT

    VD)

    1500

    2000

    Valve 3

    Orifice 2500

    3000

    Pr

    Slide 12Section 1 - Principles SIBH

    P

    =

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    Gas Lift

    FTHPProduced Fluids + Lift Gas

    as ys em

    Low Pressure gas

    bubbling up

    the well,

    lightening the

    fluid column in

    Gaslift Compressor

    High Pressure Gas

    t e we

    CHP

    Separator

    Liquid

    Lift gas injectedat the deepest

    mandrel

    Slide 13Section 1 - Principles

    Pwf

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    Gas Lift

    PRESSURE (PSI)500 10000

    Well Flowing

    INJECTION GAS Dummy

    Fluid Level

    500

    CASING

    Press

    TUBING

    Press.

    Dummy 1000

    Valve 1

    Valve 2

    1500

    2000

    Valve 3

    Orifice 2500

    3000

    Slide 14Section 1 - PrinciplesPr

    Pwf

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    Gas Lift

    A Well Bein Gas Lifted

    PRESSURE (PSI)

    0

    500 10000

    Well Flowing

    INJECTION GASDummy

    Fluid Level

    500

    CASING

    Press

    TUBING

    CASING PRESSURE

    Dummy 1000

    .

    Valve 2

    1500

    2000

    a ve

    Orifice 2500

    3000

    3500

    Slide 15Section 1 - PrinciplesPr

    Pwf

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    Gas Lift

    To enable the well that wil l not flow naturally

    to produce o ncrease pro uc on ra es n na ura ow ng

    wells

    To remove or unload fluids from gas wells.

    Slide 16Section 1 - Principles

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    Gas Lift

    us ave a source o gas

    Imported gas from other fields may result in start up

    problems Possible high installation cost

    Top sides modif ications to existing platforms

    Bottomhole pressure can not be reduced too much,since backpressure of two phase flow up the tubing has

    .

    Significant effort required to operate effectively

    Can be too forgiving Quite inefficient (energy)

    Slide 18Section 1 - Principles

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    Gas Lift

    -

    Continuous f low is similar to natural flow and isachieved b controllin the in ection of as into thefluid column to cause aeration from the point ofinjection

    Advantages: Takes full advantage of the gas energy available at the

    surface

    g er pro uc on vo ume

    Equipment can be centralized Valves can either be wireline or tubing retrieved

    Disadvantages:

    Must have a continuous source of gas. a es o e a ove p or e c en ng. Bottom hole producing pressure increases both with

    depths and volume

    Slide 20Section 1 - Principles

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    Gas Lift

    - Intermittent flow is by injecting gas of suff icient volume and

    surface, this usually require high gas rate to reduce the liquidfallback. The liquid to surface is in slug or piston form.

    Advantages: Can obtain lower producing bottom hole pressure than

    continuous flow and at low rates.

    Suitable for well with production below 150 bpd (low P.I wells)

    Can remedy wax deposition in tubing for waxy crude

    Disadvantages: Limited in volume.

    Causes surge on surface equipment. Equipment must be designed to handle the surge.

    Cause interruption to other flowing wells in the productionsystem

    Slide 21Section 1 - Principles

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    Gas Lift

    or ow ro uc on e s, n erm en ow gas s abetter Choice.

    BFPD)

    - -

    2-7/8 TUBING - 200 TO 300 BFPD 3-1/2 TUBING - 300 TO 400 BFPD

    3 Main Categories - Intermittent gas lift

    - Chamber lift - Plunger lift ? (can be used without gaslift as well)

    Slide 22Section 1 - Principles

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    Gas Lift

    Injecting gas into the well reduces weight of the fluid

    column and conse uentl reducin the flowin bottom holeProduced Fluid + Lift Gas

    pressure. (Optimal product ion)

    1900

    Optimal injection

    point

    1600

    1500

    Q1 =2000 b/d

    Inj. Gas = 1mscf/d

    w

    Qliq500 2000 2200

    Non Optimal lift ing

    w = ps g

    Q1 =2200 b/d

    Inj. Gas = 2mscf/d

    At high draw-down i.e. high gas in ject ion rate:

    1) Non-darcy flow in IPR

    2) Causes increase in the frict ional losses in the tubing

    Slide 23Section 1 - Principles

    thus offsetting the reduction of weight in the fluid

    column.

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    Gas Lift

    A wells ability to produce fluid

    a reduction in bottom hole pressure i.e.

    theP(Reservoir Bottom Hole)

    Slide 24Section 1 - Principles

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    Gas Lift

    Required Data

    Static Bottom Hole Pressure

    Pressure in the wellbore at the perforations under-

    SBHP, Pr, Ps

    Flowin Bottom Hole Pressure

    Pressure in the wellbore at the perforations with thewell producing at a given rate

    , ,

    Drawdown

    Change in pressure from static to flowing SBHP-FBHP = P

    Fluid Rate

    Slide 25Section 1 - Principles

    e test per orme w e runn ng survey =

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    Gas Lift

    One way to quantify a wells productivity

    is to use a relationship known as:

    production rate and drawdown (rate and

    ressure

    Slide 26Section 1 - Principles

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    Gas Lift

    PI = BLPD / P

    Drawdown

    =

    BLPD = P * PI

    Slide 27Section 1 - Principles

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    Gas Lift

    ne way o p o e ro uc v y s n erms o ro uc v yIndex (PI)

    The PI is a convenient term to compare performance between.

    SBHP

    BHP

    PI is expressed in terms of rate versus drawdown (bpd / psi)Rate

    Slide 28Section 1 - Principles

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    Gas Lift

    RELATIONSHIP

    We have another curve to describe the inflow into the well

    from the formation. This is theinflow curve

    (inflow, .

    P

    B

    Rate

    Slide 29Section 1 - Principles

    G Lift

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    Gas Lift

    RELATIONSHIP

    The inflow curve can be derived using any two points. Normally

    the SBHP is given as one point. e oge curve s one n ow re a ons p:

    Q/Qmax = 1 - 0.2(FBHP/SBHP) - 0.8(FBHP/SBHP)2

    where FBHP and Q are measured data (normally from a surveyand a concurrent welltest).

    H

    P

    SBHP

    B

    Q

    FBHPQmax

    Slide 30Section 1 - Principles

    Rate

    G Lift

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    Gas Lift

    PI is a more simple way to handle inflow.

    IPR is more complex, and more correct than, u requ res e er a a o correc ycalculate

    P

    B PI

    Rate

    Slide 31Section 1 - Principles

    Gas Lift

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    Gas Lift

    we compare e n ow mo e an e ou ow mo eby drawing them on the same graph, we can find the

    expected flow rate and FBHP.

    BH

    P

    FBHP

    Rate This technique is the basis for more complex predictions

    such as the equil ibrium curve and the lift gas performancecurve.

    Slide 32Section 1 - Principles

    Gas Lift

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    Gas Lift

    Inflow: Pwf = Pres dPres dPperf

    Outflow: Pwf = Psep + dPfl + dPtbg

    TGLR3Inflow OutflowTGLR2

    BHP

    TGLR3 > TGLR2 > TGLR1

    Rate

    Slide 33Section 1 - Principles

    Gas Lift

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    Gas Lift

    900)

    n m e as or max mum

    flowrate is desired

    2) Limited Gas or the most

    600

    700

    on(BPD econom ca ra e s es re

    1) Production is fixed

    Water /gas coning

    300400

    rodu

    cti

    Sand production

    Governmentregulations

    321

    0

    100Net

    Gas lift Injection (Mscfd)

    Slide 34Section 1 - Principles

    Gas Lift

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    Gas Lift

    Qinj

    production as we approach maximum point

    700

    800

    900

    BPD) Optimum Injection Point Qliq

    400

    500

    600

    uctio

    n(

    Sub-optimum in jecting points

    100

    200

    300

    N

    etPro

    0

    50 100 200 300 400 500 600 700 800 900 1000

    Gas lift In ection Mscfd

    Slide 35Section 1 - Principles


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