3. pressure loss in the wellbore
TRANSCRIPT
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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