3. pressure loss in the wellbore

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    Pressure Loss in the Wellbore

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    Lecture Outcomes

     At the end of this lecture, students should be able to:

    • Identify the major components of pressure losses in the

    wellbore

    • Explain the origin and applicability of common industry

    multiphase flow correlations

    • Define slip and liquid holdup

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    Introduction

    • !or the "ast majority of wells, the major part of

    pressure loss in the production system is the

    wellbore

    • #articular care must be therefore be ta$en to

    understand and model this pressure drop

    correctly%

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    Introduction

    • #ressure loss in the wellbore may also be called

    &outflow' or tubing performance or "ertical lift

    performance ()*#+

    • It is used in conjunction with pressure drop in

    the reser"oir  or &inflow' performance relationship

    (I#+ for well performance prediction (flowrates

    and pressures+

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    Introduction

    Note that it may be incorporated into reservoir models as vertical lift

     performance (VLP) curves or tubing hydraulic tables

    !igure -: I# and )*# cur"es

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    Wellbore Fluid Fundamentals

    • !low up the wellbore can be laminar or turbulent, single or multiphase,

    "ertical or inclined

    • .ultiphase flow is complex and cannot be described completely by

    equations

    • .odels rely on correlations to allow calculation of pressure loss

    • /he dominant component is hydrostatic head (gra"ity pressure loss+ 

    • /he secondary component is resistance to flow (friction pressure loss+

    • /he minor component is $inetic energy change (acceleration pressure

    loss+

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    Wellbore Fluid Fundamentals

    !igure 0: A schematic of a wellbore

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    1oted that the top and the bottom of the wellbore are often called &nodes':

    • /he top nodes is the depth of the wellhead (where the pressure is termed

    well head or tubing pressure 2 #wh or 34# or /4#+

    • /he bottom node is the depth of the reser"oir (or well face+, usually chosen

    as top perforations or top open hole (2 #wf+%

    • #wf stands for pressure at the well face and not flowing pressure (at 5ero

    flow, #wf 2 static reser"oir pressure, #+% /his is usually chosen as the

    solution node for well performance prediction (i%e% inflow and outflowintersection+

    Wellbore Fluid Fundamentals

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    6uidelines for magnitudes of these pressure components

    are as follows:

    • !or oils, acceleration term is usually negligible andgra"ity term is a minimum of 789 of the total

    • !or low 6 oils (or high water cut wells+, gas "olumes

    are small and the gra"ity term is typically ;

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    Gravity Term

    !or most wells, this is dominant pressure loss component and

    therefore is must be calculated correctly%

    ?alculation of the gra"ity term requires:

    • determination of oil, water and gas densities at element (#a" , /a"+

    • calculation of phase "olumes and areas at element (#a" , /a"+• calculation of mixture density at element (#a" , /a"+

    where:

     @mix 2 lbBcuftC 4/)D 2 ft /)DC

     #gra"ity 2 psiC

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    • /he abo"e calculation assumes that the liquid and gas phases areflowing at the same "elocity in the wellbore%

    • In reality the gas phase will mo"e faster due to buoyancy forces,

    gi"ing rise to a slip velocity :

    • slip "elocity 2 gas "elocity liquid "elocity

    • /he consequence of slip is a change in the areas of each phase(the effecti"e liquid area increases+%

    • /he slipcorrected liquid area is termed liquid holdup (4*+:

    Gravity Term

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    • /he correction from 9* to 4* by accounting for slip is determined by

    multiphase flow correlations

    • 1ote that the noslip density represents the minimum # gra"ity case

    and is a useful diagnostic

    • Flip is determined by finding the "elocities of each phase which is

    dependent on flow distribution

    • Determination of slip is highly complex and depends on a number of

    parameters

    • /hese parameters are often grouped together in the form of flow regime

    maps

    Gravity Term

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    Exercise

    ?onsider two cases of the same amount of gas (089+ distributed

    differently in the liquid phase

     

    • In which case would the slip be highest and why?

    • hich fluid parameter is most influential in determining thedistribution?

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    Multiphase FlowCorrelations

    Most oil wellswould be inbubble fowtowards the

    bottom o the

    wellbore andmove to slug

    fow towards themiddle and top o

    the wellbore.Slug fow is

    usually thedominant fow

    regime.

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    Flow Regime Map

    • !low regime maps use combinations of dimensionless groups for

    the gas and liquid phases% /hese are plotted on the x and y axes

    respecti"ely and the intersection determines the flow regime%

    • /he boundaries between the flow regimes are found experimentally%

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    Flow Regime Map

    Note the primary fluid parameters of importance are liquid density

    and gas-liquid interfacial tension.

    #ractical implications of these grouped parameters are:

    -% 4igh interfacial tension fluids (biodegraded oils+ will support large

    bubble si5es ( slug flow+∴

    0% *ow interfacial tension fluids ("olatile oils+ cannot support large

    bubbles ( mist flow+∴

    G% /he correct determination of gasliquid interfacial tension is criticalH

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    Selection For Flow Correlations

    •  Applying the appropriate holdup correlation depends on flow regime

    detection and the emphasis of the experimental wor$ performed in

    deri"ing the correlation%

    • 6eneral comments on the origin and applicability of common

    industry correlations are as follows:

    Fancher-Brown (!"#$ %o-slip correlation. &ood as a diagnosticsince this give the minimum possiblegravity pressure loss

    &ri'th-allis (!"$ Bubble fow correlation. )dopted by

    *agedorn-Brown and others todetermine bubble-slug fow boundary

    +uns and ,os (!"$ omprehensive wor including fowregime map and derivation o holdupcorrelations or each. Best in mist fow

    regime

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    Selection For Flow Correlations

    4agedornrown(original -;>J+ ?ombined the results of 6riffith3allis, 4agedornrown and Duns and os with "elocity determinedboundaries% ?an gi"e discontinuities%

    eggs and rill(-;JG+

    ?orrelation deri"ed for hori5ontal flow and thenmodified for angle for de"iated wells% 6ood for pipelinesbut usually o"erpredicts for wells%

    ontinue..

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    Selection For Flow Correlations

    • Fince most oil wells are in slug flow (with some bubble flow towards

    the bottom of the wellbore+, 4agedornrown (modified+ would be

    the best choice% .ost commercially de"eloped correlations for oil

    wells use 4agedornrown as the basis%

    •!ancher rown is a no slip correlation and is a useful diagnosticsince it will predict the minimum #wf (slip will increase #wf+% If a

    measured gauge pressure in the wellbore is less than !ancher

    rown then a data measurement or #)/ problem exists%

    • eggs K rill is good for surface flowlines and pipelines but is not

    recommended for oil wells, de"iated or otherwise%

    • Duns and os is recommended for wet gas or gascondensate wells

    that are dominant in mist flow% /he 6ray correlation, not mentioned

    abo"e, is appropriate for dry gas wells%

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    Friction Term

    • /he main dependencies of frictional pressure loss are mixture"elocity (or flowrate+, pipe diameter and "iscosity% It is "ery sensiti"e 

    to gas "olumes since this directly affects "elocities%

    • 1ote that it is in"ersely proportional to diameter to the fifth power%

    • /he equation for friction pressure loss (per unit length+ is as follows:

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    Friction Term

    • !riction factor (f+ is correlated to !eynolds number (e+ and tubing

    roughness (L+ from the .oody Diagram (de"eloped for single phase

    flow+%

     

    • 1ote that for laminar flow (e M 0888+, the friction factor 2 >=Be

    • /ubing roughness (granularity of the tubing inside wall+ is onlyrele"ant in turbulent flow% In laminar flow, roughness has no effect%

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    Friction Term

    /ypical "alues of roughness (L+ are as follows:

    • Ftainless steel B -G9 ?r 8%8888> in

    • .ild steel 8%888> in

    • ?orroded tubingBcast iron 8%8- in

    • "or turbulent conditions in multiphase flow , the frictional loss term is

    influenced by slip%

    • )arious authors ha"e modified the friction term for bubble, slug and

    mist flow%•  A twophase eynolds number is used accounting for gas and liquid

    "iscosities%

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    Acceleration Term

    • /his results from $inetic energy losses due to the rate of change of "elocity%

    • It is usually only significant at the top of the wellbore with low flowing

    pressures and large gas "olumes%

    • 6enerally this is negligible for most oil wells%

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    uestion !!

    Than" #ou