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Wellbore Flow Performance
Wellbore Flow Performance
The pressure drop experienced in lifting reservoir
fluids to the surface is one of the main factors affecting
well deliverability.
As much as 80% of the total pressure loss in a flowing
well may occur in lifting the reservoir fluid to the surface
Wellbore flow performance relates to estimating the
pressure-rate relationship in the wellbore as the
reservoir fluids move to the surface through the
tubulars
This flow path may include flow through perforations, a
screen and liner, and packers before entering the
tubing for flow to the surface.
The tubing may contain completion equipment that acts
as flow restrictions such as profile nipples, sliding





Wellbore Flow Performance
 Relationships to estimate this pressure drop in the
wellbore are based on the mechanical energy
equation for flow between two points in a system
as
 Where, α is the kinetic energy correction factor for
the velocity distribution,
 W is the work done by the flowing fluid, and El is the
irreversible energy losses in the system including
the viscous or friction losses.
 For most practical applications, there is no work
done by or on the fluid and the kinetic energy
correction factor is assumed to be one.
Wellbore Flow
Performance
 The total pressure drop is equal to the sum
change in potential energy (elevation),
the
of the
change in
kinetic energy (acceleration), and the energy losses
in the system.
 Considering the differential form for any fluid at
any pipe inclination it becomes
 This fundamental for estimating the pressure drop in
tubulars for single-phase liquid, single-phase vapor,
and multiphase flow
Wellbore Flow Performance
The pressure drop for a particular flow rate can
be estimated and plotted as a function of rate. i.e.
wellhead pressure is fixed and the bottomhole

flowing pressure, pwf , is calculated by determining
the pressure drop.
This approach will yield a wellbore flow
performance curve when the pressure is plotted as
a function of rate as shown in figure below
In the figure the wellhead pressure is held
constant, and the flowing bottomhole pressure is
calculated as a function of rate.
This curve is often called a tubing-performance
curve because it captures the required flowing
bottomhole pressure needed for various rates.



WellboreFlow Performance
Typical tubing performance curve for constant
wellhead pressure
Wellbore Flow Performance
Single-Phase Liquid Flow: Single-phase liquid
is generally of minor interest to the petroleum
engineer, except for the cases of water
supply injection wells.
flow

or
In these cases, above is applicable where the

friction factor, f, is a function of the Reynolds number
and pipe roughness.
The friction factor
the Moody friction
The friction factor
is most commonly estimated from
factor diagram.
is an empirically determined


value that is subject to error because of its
dependence on pipe roughness, which is
affected
by pipe erosion, corrosion, or deposition.
Wellbore Flow Performance
Single-Phase Vapor Flow
Several methods exists for estimating the pressure
drop for single-phase gas flow under static and
flowing conditions.
These methods include the average temperature
and compressibility method and the original and
modified Cullendar and Smith methods.
They require a trial-and-error or iterative
approach to calculate the pressure drop for a
given rate because of the compressible nature of
the gas.
A simplified method for calculating the pressure
drop in gas wells assuming an average
temperature





was presented by Katz et al.
Wellbore Flow
Performance 0.5
 sd5
p 2 es p

2




q  200,000
  in wh 

 


 


g es 1
 TzL f  




g M  

  
 
Valid only for
dry gas
where 𝜀 is
the
absolute pipe roughness ≅ 0.0006in. for most
commercial pipe. f𝑀 is the best-fit equation for the fully
turbulent region of the Moody diagram and is sufficiently
accurate for most engineering calculations.
Wellbore Flow
Performance
 three components of pressure loss in a TPR curve
for a single-phase liquid. a dry gas, and a two-phase
gas/oil mixture.
Wellbore Flow
Performance
 Thus for a given flow rate, wellhead pressure,
and tubing size. there is a particular pressure
distribution along the tubing.
 starting its traverse at the wellhead pressure
and
the
 The
increasing
tubing.
downward toward the intake to
pressure-depth profile is called a pressure
traverse. as shown
.
below.
Wellbore Flow
Performance
Wellbore Flow Performance
Multiphase Flow.
is much more complex than the single-phase flow
problem because there is the simultaneous flow of
both liquid (oil or condensate and water) and vapor
(gas).
The mechanical energy equation is the basis for
methods to estimate the pressure drop under
multiphase flow;
however, the problem is in determining the
appropriate velocity, friction factor, and density to
be used for the multiphase mixture in the calculation.
In addition, the problem is further complicated as
the velocities, fluid properties, and the fraction of
vapor toliquid change as the fluid flows to the surface





Wellbore Flow
Performance
Considering curve above, in multiphase mixtures there
with

is general trend of increasing pressure gradient
depth and the procedures of calculating the pressure
traverse of multiphase mixtures are complex
Thus , numerous correlations based on field and

experimental observations, which take the form of
either generalized pressure versus distance curves,
equation
s
called gradient curves or empirical pipe flow
are used
Multiphase pipeflow correlations can be classified as

(i) gradient curves
(ii) homogeneous mixture correlations
(iii) flow regime correlations
Wellbore Flow
Performance
drawback of the correlations based on experimental

data is that application to producing wells is limited to
and ftuid
the conditions of rate, geometry, gas/oil ratio,
properties used in the experimental study
Gradient curves

 Main parameters in vertical multiphase pipe flow are
pipe diameter, oil rate, and gas/liquid ratio
Other parameters that might have an effect on

pressure gradient
viscosity. densities
include liquid surface tension.
(oil, gas and water gravities),
flowing
cut.
temperature, gas/liquid solubility, and water
Note: gradient
formed in the
curves
tubing
do not apply if an emulsion

Wellbore Flow
Performance
Sample gradient curves
Sample gradient curves
Example 1
 A well is to be produced into a high-pressure,
gas-gathering line requiring a minimum
wellhead pressure of about 850 psia. Available
tubing has 2.063in. nominal diameter and
1.751 in. inner diameter. Other relevant data
for the well include:
vertical length of tubing 8280 .
depth to mid perforations 8500ft
0.75 (air
150°F
0.78
gas gravity =1)
average
average
tubing temperature
gas Z-factor
pipe roughness 0.0006in.
Solution
Example 2
A certain well is under production at
a
depth of about

5000 ft. The oil is relatively heavy and contains little
solution gas, thereby requiring gas lift to produce. The
tubing is 3.5-in. nominal diameter and preliminary
calculations indicate that 1000scf/ STB gas can be
injected at an economical cost. Added to the
200scf/STB solution gas, this gives a total of
1200scf/STB total GOR. Consider production at an oil
rate of 200STB/D. Assuming that the gas is injected at
the bottom of the tubing.
(i) Determine the required tubing intake pressure if the
wellhead is fixed at 500psia
(ii) Determine the available wellhead pressure when
tubing intake pressure (located near the wellbore) is
2000 psia.
Solution
Wellbore Flow
Performance
 Note, from the gradient curve
The vertical axis represents distance traveled
1)
vertically from a given point where the pressure
is known
𝑑𝑝
The gradient decreases with increasing
2)
𝑑
𝐻
gas/liquid ratio (GLR) until a minimum gradient
𝑑𝑝
is reached. Thereafter the trend reverses and
𝑑
𝐻
increases with increasing gas/liquid ratio
For convenience, the high-Gl.R gradient curves
avoid
3)
are shifted down on the depth scale to
intersection with lower-GLR curves
Wellbore Flow
Performance
4) If production is water-free, then gas/liquid ratio,
GLR equals gas/oil ratio (GOR), but if water/oil
ratio, (WOR) is reported, then the relation
between GLR and GOR is
 Construct the tubing performance of an oil well producing
through tubing with a given diameter and length at a
specific gas/liquid ratio
on Figure below
and wellhead pressure is as shown
WellboreFlow Performance
Construct TPR
by gradient
curve
Example 3
 Given a well which produces
from
the Bromide
sand at a depth of 8000 ft. Solution gas/oil ratio
is 600scf/STB. Use of 3.5-in. nominal tubing is
suggested by the production engineer, who
claims there will be a need for gas life after
only one to two years of production. Construct
the present tubing performance curve, assuming
a wellhead pressure of 200 psia.
Lecture08.pptx for oil and gas engineering students in universities
Solution
Tubing Performance
Lecture08.pptx for oil and gas engineering students in universities
NATURAL FLOW
Based on only a few pieces of data, it is possible
tubing

to calculate and plot both inflow and
performance relations
For the typical case when the tubing shoe (inlet)

reaches
pressur
e
the perforation depth, wellbore flowing
and tubing intake pressure are
considered at the same depth
When at a specific rate these two pressures are
flo
w

equal. the
is stable
flow system is in equilibrium and
The intersection of the IPR and TPR curves

determines the rate of stable flow that can be
expected from the particular well
NATURAL FLOW
The intersection of the IPR and TPR curves determines the
rate of stable flow that can
well.
be expected from the particular
NATURAL FLOW
At points where IPR flow equals to TPR , the equilibrium

rate
flow
and pressure constitute what is called the natural
point and the equilibrium rate is called the
natural flow rate
There may be two points of intersection for multiphase

mixtures., one represents a stable flow condition and
the other an unstable one.
The stable point of natural flow is to the right

 Mathematically, the stable point of natural flow exists
when the two performance relations intersect with
slopes (i.e., derivatives) of opposite sign.
If the two curves have slopes of similar sign at the
in rate

point of intersection, then only a small change
will cause the system to change its state of equilibrium,
either
point
killing the well or moving it toward the stable
of natural flow
NATURAL FLOW
Natural flow rate and pressure usually change with

reservoir depletion, depending on the variation in IPR
and TPR resulting from changes in reservoir pressure
and flow characteristics.
The change of natural flow is usually toward a lower

rate if all well parameters remain unchanged.
To offset the natural decline in rate, it is possible to

change equipment or operating criteria to maintain the
desired rate of production.
Lowering the wellhead pressure by choke manipulation

or lowering of separator pressure are simplest
and
most common of the adjustments made by the
operator.
Artificial lift or treating wells by stimulation are other

alternatives for maintaining a desired rate of production
(these are more complicated and costly).
NATURAL FLOW
Changing Wellhead Pressure
Decreasing wellhead pressure by increasing choke

opening will usually shift the TPR curve downward
to a lower intake pressure (increasing the rate of
natural flow)
If = atmospheric condition, the well will
P𝑤ℎ

produce at
Increasing
its maximum flow rate.
pressure will
shift
the wellhead the

TPR curve upward (decreasing flow rate)
If the wellhead pressure is increased beyond a

certain point, then the well will stop producing
because the required
available pressure
pressure exceeds the
NATURAL FLOW
Effect of wellhead pressure on natural flow
NATURAL FLOW
Changing Gas/Liquid Ratio
The effect of a changing gas/liquid ratio is not

as straightforward as for the case of changing
wellhead pressure.
It has different effects on the two components of

pressure loss in
Increasing GLR
tubing-friction and hydrostatic.
lightens the mixture density

and therefore reduces the pressure loss due to
hydrostatic forces.
On other hand, larger quantities of gas usually

increases pressure losses due to friction.
NATURAL FLOW
Effect of gas/liquid ratio on natural flow
NATURAL FLOW
 Note, increase GLR pays only to a certain point, higher
GLRs does not offset the additional costs of
increasing the injected gas compared with
incremental of oil produced
Changing Tubing Diameter.
 The effect of tubing diameter on natural flow is
similar to the effect of gas/liquid ratio
 Increasing diameter increases the rate of natural
flow until a critical diameter is reached, after which
rate will decrease
 Thus Natural flow is the primary criterion used to
choose tubing size.
include
 Other criteria price, availability, mechanical
considerations, and future production characteristics
NATURAL FLOW
Effect of tubing diameter on natural
NATURAL FLOW
Changing Inflow Performance
 Deteriorating inflow performance is the natural
result of reservoir depletion
 average
absence
reservoir pressure decreases in the
of artificial pressure maintenance
drive.
or a
strong natural water
 Gas and water injection can be used to arrest
the decline in IPR caused by depletion.
 Additional reductions
result from
in inflow performance may
(i) damage near the wellbore related to drilling and
completion operations
(ii) reduced drainage area due to infill drilling
NATURAL FLOW
(iii) reduced permeability due to two-phase flow,
compaction or fines migration,
(iv) increased viscosity due to gas liberation from
reservoir oil, or
(v) transient effects usually associated with low-
permeability formations.
 Note: For most flowing wells the actual
difference
in
elevation between mid perforations and the tubing
shoe is only about 30 feet, or the length of one
joint of tubing.
 In other situations, the tubing shoe is substantially
above the perforations and wellbore flowing
pressure does not equal tubing intake pressure.
NATURAL FLOW
Effect of changing inflow performance on natural flow
NATURAL FLOW
Effect of a pump on well performance.
NATURAL FLOW
(i) Now, to correct for the distance between the
tubing intake and mid perforations, the
separation
extension
interval should be considered as an
of the tubing
 And an additional pressure drop along the interval
is added to the pressure drop in the tubing and
the composite is used to develop the tubing
performance relation, the pressure drops is given as
NATURAL FLOW
(ii) An alternative to adjusting the TPR curve for
depth
level
separation is to transfer the IPR up to the
of the tubing shoe.
 The resulting performance curve will be called
the pseudo-IPR (or shifted IPR)
 However, the use of this method is generally not
recommended except for special applications such
as solving downhole pump
NATURAL FLOW
Depth adjustment by
(a) adjusting the tubing
performance curve
and
(b) shifting the inflow
performance curve.
Example 4
Assume a well 1 (W1) as discussed in example 3

has been tested at a rate of 202 STB/D during a
three-day period. Stabilized wellbore flowing
pressure measured 3243 psia. Another wells say W2
and W3 were previously tested with a multirate
sequence, which indicated the exponent in the IPR
equation (Fetkovich] ranges from 0. 77 to 0.81. if a
value of 0.8 is assumed to apply to W1 well. Average
reservoir pressure is 4000 psia.
Determine the rate of natural flow, assuming the

tubing performance calculations in example 3
apply (i.e., = 200psia, GLR = 600scf/STB, and
𝑃𝑤h
8000ft of tubing having a 3.5-in. nominal diameter).
Example
Table (a) and (b) shows production
and tubing performance data
respectively,
1) Plot gas rate versus the
difference of average reservoir
pressure squared and intake
5 Multirate Data
flowing pressure squared on the
log-log plot and determine the
point of natural flow for this
well.
2) Plot the gas IPR and
the tubing performance
curves on Cartesian
coordinates. Once again
determine point of natural
flow.
Tubing Perfonnance Relation
the
3) Discuss the advantages of a log-log plot of
the well performance curves over a
Cartesian plot.
Examples 6
Production from the Davis No. 5 (Examples 3 and

4) suddenly dropped after five years of
production. By running a special tubing gauge tool, it
was determined that the tubing had collapsed at 6537
ft. During a workover job to replace the tubing. it was
discovered that the casing had also collapsed at the
same depth. The collapsed casing interval has been
reamed out to full bore and has been milled out
1
throughout the
the
pay zone. A 2-in. liner
6000
has been
5
set inside damaged casing from to 8000 ft.
The well has been completed with 3.5-in. tubing which
was run only to 5950 as shown in Fig. below. A
7
changeover to 2 8-in. to run the tubing inside the liner
up to the perforations depth was considered too costly
and unnecessary.
following
A test the workover

indicated an average reservoir
pressure of 2000 psi a and a
gas/oil ratio of 2500 scf/STB. In
addition, a flowing pressure
gradient in the 5.5-in. liner was
measured as 𝐺f = 0.26psi/ft. During
the test a rate of 320 STB/D was
recorded, with a stabilized flowing
bottomhole pressure of 842 psia.
Assuming exponent n equals
equation.
0.8

in the backpressure
predict the natural flow of the well
with 200psia wellhead pressure.

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Lecture08.pptx for oil and gas engineering students in universities

  • 2. Wellbore Flow Performance The pressure drop experienced in lifting reservoir fluids to the surface is one of the main factors affecting well deliverability. As much as 80% of the total pressure loss in a flowing well may occur in lifting the reservoir fluid to the surface Wellbore flow performance relates to estimating the pressure-rate relationship in the wellbore as the reservoir fluids move to the surface through the tubulars This flow path may include flow through perforations, a screen and liner, and packers before entering the tubing for flow to the surface. The tubing may contain completion equipment that acts as flow restrictions such as profile nipples, sliding     
  • 3. Wellbore Flow Performance  Relationships to estimate this pressure drop in the wellbore are based on the mechanical energy equation for flow between two points in a system as  Where, α is the kinetic energy correction factor for the velocity distribution,  W is the work done by the flowing fluid, and El is the irreversible energy losses in the system including the viscous or friction losses.  For most practical applications, there is no work done by or on the fluid and the kinetic energy correction factor is assumed to be one.
  • 4. Wellbore Flow Performance  The total pressure drop is equal to the sum change in potential energy (elevation), the of the change in kinetic energy (acceleration), and the energy losses in the system.  Considering the differential form for any fluid at any pipe inclination it becomes  This fundamental for estimating the pressure drop in tubulars for single-phase liquid, single-phase vapor, and multiphase flow
  • 5. Wellbore Flow Performance The pressure drop for a particular flow rate can be estimated and plotted as a function of rate. i.e. wellhead pressure is fixed and the bottomhole  flowing pressure, pwf , is calculated by determining the pressure drop. This approach will yield a wellbore flow performance curve when the pressure is plotted as a function of rate as shown in figure below In the figure the wellhead pressure is held constant, and the flowing bottomhole pressure is calculated as a function of rate. This curve is often called a tubing-performance curve because it captures the required flowing bottomhole pressure needed for various rates.   
  • 6. WellboreFlow Performance Typical tubing performance curve for constant wellhead pressure
  • 7. Wellbore Flow Performance Single-Phase Liquid Flow: Single-phase liquid is generally of minor interest to the petroleum engineer, except for the cases of water supply injection wells. flow  or In these cases, above is applicable where the  friction factor, f, is a function of the Reynolds number and pipe roughness. The friction factor the Moody friction The friction factor is most commonly estimated from factor diagram. is an empirically determined   value that is subject to error because of its dependence on pipe roughness, which is affected by pipe erosion, corrosion, or deposition.
  • 8. Wellbore Flow Performance Single-Phase Vapor Flow Several methods exists for estimating the pressure drop for single-phase gas flow under static and flowing conditions. These methods include the average temperature and compressibility method and the original and modified Cullendar and Smith methods. They require a trial-and-error or iterative approach to calculate the pressure drop for a given rate because of the compressible nature of the gas. A simplified method for calculating the pressure drop in gas wells assuming an average temperature      was presented by Katz et al.
  • 9. Wellbore Flow Performance 0.5  sd5 p 2 es p  2     q  200,000   in wh           g es 1  TzL f       g M         Valid only for dry gas where 𝜀 is the absolute pipe roughness ≅ 0.0006in. for most commercial pipe. f𝑀 is the best-fit equation for the fully turbulent region of the Moody diagram and is sufficiently accurate for most engineering calculations.
  • 10. Wellbore Flow Performance  three components of pressure loss in a TPR curve for a single-phase liquid. a dry gas, and a two-phase gas/oil mixture.
  • 11. Wellbore Flow Performance  Thus for a given flow rate, wellhead pressure, and tubing size. there is a particular pressure distribution along the tubing.  starting its traverse at the wellhead pressure and the  The increasing tubing. downward toward the intake to pressure-depth profile is called a pressure traverse. as shown . below.
  • 13. Wellbore Flow Performance Multiphase Flow. is much more complex than the single-phase flow problem because there is the simultaneous flow of both liquid (oil or condensate and water) and vapor (gas). The mechanical energy equation is the basis for methods to estimate the pressure drop under multiphase flow; however, the problem is in determining the appropriate velocity, friction factor, and density to be used for the multiphase mixture in the calculation. In addition, the problem is further complicated as the velocities, fluid properties, and the fraction of vapor toliquid change as the fluid flows to the surface     
  • 14. Wellbore Flow Performance Considering curve above, in multiphase mixtures there with  is general trend of increasing pressure gradient depth and the procedures of calculating the pressure traverse of multiphase mixtures are complex Thus , numerous correlations based on field and  experimental observations, which take the form of either generalized pressure versus distance curves, equation s called gradient curves or empirical pipe flow are used Multiphase pipeflow correlations can be classified as  (i) gradient curves (ii) homogeneous mixture correlations (iii) flow regime correlations
  • 15. Wellbore Flow Performance drawback of the correlations based on experimental  data is that application to producing wells is limited to and ftuid the conditions of rate, geometry, gas/oil ratio, properties used in the experimental study Gradient curves   Main parameters in vertical multiphase pipe flow are pipe diameter, oil rate, and gas/liquid ratio Other parameters that might have an effect on  pressure gradient viscosity. densities include liquid surface tension. (oil, gas and water gravities), flowing cut. temperature, gas/liquid solubility, and water Note: gradient formed in the curves tubing do not apply if an emulsion 
  • 18. Example 1  A well is to be produced into a high-pressure, gas-gathering line requiring a minimum wellhead pressure of about 850 psia. Available tubing has 2.063in. nominal diameter and 1.751 in. inner diameter. Other relevant data for the well include: vertical length of tubing 8280 . depth to mid perforations 8500ft 0.75 (air 150°F 0.78 gas gravity =1) average average tubing temperature gas Z-factor pipe roughness 0.0006in.
  • 20. Example 2 A certain well is under production at a depth of about  5000 ft. The oil is relatively heavy and contains little solution gas, thereby requiring gas lift to produce. The tubing is 3.5-in. nominal diameter and preliminary calculations indicate that 1000scf/ STB gas can be injected at an economical cost. Added to the 200scf/STB solution gas, this gives a total of 1200scf/STB total GOR. Consider production at an oil rate of 200STB/D. Assuming that the gas is injected at the bottom of the tubing. (i) Determine the required tubing intake pressure if the wellhead is fixed at 500psia (ii) Determine the available wellhead pressure when tubing intake pressure (located near the wellbore) is 2000 psia.
  • 22. Wellbore Flow Performance  Note, from the gradient curve The vertical axis represents distance traveled 1) vertically from a given point where the pressure is known 𝑑𝑝 The gradient decreases with increasing 2) 𝑑 𝐻 gas/liquid ratio (GLR) until a minimum gradient 𝑑𝑝 is reached. Thereafter the trend reverses and 𝑑 𝐻 increases with increasing gas/liquid ratio For convenience, the high-Gl.R gradient curves avoid 3) are shifted down on the depth scale to intersection with lower-GLR curves
  • 23. Wellbore Flow Performance 4) If production is water-free, then gas/liquid ratio, GLR equals gas/oil ratio (GOR), but if water/oil ratio, (WOR) is reported, then the relation between GLR and GOR is  Construct the tubing performance of an oil well producing through tubing with a given diameter and length at a specific gas/liquid ratio on Figure below and wellhead pressure is as shown
  • 25. Example 3  Given a well which produces from the Bromide sand at a depth of 8000 ft. Solution gas/oil ratio is 600scf/STB. Use of 3.5-in. nominal tubing is suggested by the production engineer, who claims there will be a need for gas life after only one to two years of production. Construct the present tubing performance curve, assuming a wellhead pressure of 200 psia.
  • 29. NATURAL FLOW Based on only a few pieces of data, it is possible tubing  to calculate and plot both inflow and performance relations For the typical case when the tubing shoe (inlet)  reaches pressur e the perforation depth, wellbore flowing and tubing intake pressure are considered at the same depth When at a specific rate these two pressures are flo w  equal. the is stable flow system is in equilibrium and The intersection of the IPR and TPR curves  determines the rate of stable flow that can be expected from the particular well
  • 30. NATURAL FLOW The intersection of the IPR and TPR curves determines the rate of stable flow that can well. be expected from the particular
  • 31. NATURAL FLOW At points where IPR flow equals to TPR , the equilibrium  rate flow and pressure constitute what is called the natural point and the equilibrium rate is called the natural flow rate There may be two points of intersection for multiphase  mixtures., one represents a stable flow condition and the other an unstable one. The stable point of natural flow is to the right   Mathematically, the stable point of natural flow exists when the two performance relations intersect with slopes (i.e., derivatives) of opposite sign. If the two curves have slopes of similar sign at the in rate  point of intersection, then only a small change will cause the system to change its state of equilibrium, either point killing the well or moving it toward the stable of natural flow
  • 32. NATURAL FLOW Natural flow rate and pressure usually change with  reservoir depletion, depending on the variation in IPR and TPR resulting from changes in reservoir pressure and flow characteristics. The change of natural flow is usually toward a lower  rate if all well parameters remain unchanged. To offset the natural decline in rate, it is possible to  change equipment or operating criteria to maintain the desired rate of production. Lowering the wellhead pressure by choke manipulation  or lowering of separator pressure are simplest and most common of the adjustments made by the operator. Artificial lift or treating wells by stimulation are other  alternatives for maintaining a desired rate of production (these are more complicated and costly).
  • 33. NATURAL FLOW Changing Wellhead Pressure Decreasing wellhead pressure by increasing choke  opening will usually shift the TPR curve downward to a lower intake pressure (increasing the rate of natural flow) If = atmospheric condition, the well will P𝑤ℎ  produce at Increasing its maximum flow rate. pressure will shift the wellhead the  TPR curve upward (decreasing flow rate) If the wellhead pressure is increased beyond a  certain point, then the well will stop producing because the required available pressure pressure exceeds the
  • 34. NATURAL FLOW Effect of wellhead pressure on natural flow
  • 35. NATURAL FLOW Changing Gas/Liquid Ratio The effect of a changing gas/liquid ratio is not  as straightforward as for the case of changing wellhead pressure. It has different effects on the two components of  pressure loss in Increasing GLR tubing-friction and hydrostatic. lightens the mixture density  and therefore reduces the pressure loss due to hydrostatic forces. On other hand, larger quantities of gas usually  increases pressure losses due to friction.
  • 36. NATURAL FLOW Effect of gas/liquid ratio on natural flow
  • 37. NATURAL FLOW  Note, increase GLR pays only to a certain point, higher GLRs does not offset the additional costs of increasing the injected gas compared with incremental of oil produced Changing Tubing Diameter.  The effect of tubing diameter on natural flow is similar to the effect of gas/liquid ratio  Increasing diameter increases the rate of natural flow until a critical diameter is reached, after which rate will decrease  Thus Natural flow is the primary criterion used to choose tubing size. include  Other criteria price, availability, mechanical considerations, and future production characteristics
  • 38. NATURAL FLOW Effect of tubing diameter on natural
  • 39. NATURAL FLOW Changing Inflow Performance  Deteriorating inflow performance is the natural result of reservoir depletion  average absence reservoir pressure decreases in the of artificial pressure maintenance drive. or a strong natural water  Gas and water injection can be used to arrest the decline in IPR caused by depletion.  Additional reductions result from in inflow performance may (i) damage near the wellbore related to drilling and completion operations (ii) reduced drainage area due to infill drilling
  • 40. NATURAL FLOW (iii) reduced permeability due to two-phase flow, compaction or fines migration, (iv) increased viscosity due to gas liberation from reservoir oil, or (v) transient effects usually associated with low- permeability formations.  Note: For most flowing wells the actual difference in elevation between mid perforations and the tubing shoe is only about 30 feet, or the length of one joint of tubing.  In other situations, the tubing shoe is substantially above the perforations and wellbore flowing pressure does not equal tubing intake pressure.
  • 41. NATURAL FLOW Effect of changing inflow performance on natural flow
  • 42. NATURAL FLOW Effect of a pump on well performance.
  • 43. NATURAL FLOW (i) Now, to correct for the distance between the tubing intake and mid perforations, the separation extension interval should be considered as an of the tubing  And an additional pressure drop along the interval is added to the pressure drop in the tubing and the composite is used to develop the tubing performance relation, the pressure drops is given as
  • 44. NATURAL FLOW (ii) An alternative to adjusting the TPR curve for depth level separation is to transfer the IPR up to the of the tubing shoe.  The resulting performance curve will be called the pseudo-IPR (or shifted IPR)  However, the use of this method is generally not recommended except for special applications such as solving downhole pump
  • 45. NATURAL FLOW Depth adjustment by (a) adjusting the tubing performance curve and (b) shifting the inflow performance curve.
  • 46. Example 4 Assume a well 1 (W1) as discussed in example 3  has been tested at a rate of 202 STB/D during a three-day period. Stabilized wellbore flowing pressure measured 3243 psia. Another wells say W2 and W3 were previously tested with a multirate sequence, which indicated the exponent in the IPR equation (Fetkovich] ranges from 0. 77 to 0.81. if a value of 0.8 is assumed to apply to W1 well. Average reservoir pressure is 4000 psia. Determine the rate of natural flow, assuming the  tubing performance calculations in example 3 apply (i.e., = 200psia, GLR = 600scf/STB, and 𝑃𝑤h 8000ft of tubing having a 3.5-in. nominal diameter).
  • 47. Example Table (a) and (b) shows production and tubing performance data respectively, 1) Plot gas rate versus the difference of average reservoir pressure squared and intake 5 Multirate Data flowing pressure squared on the log-log plot and determine the point of natural flow for this well. 2) Plot the gas IPR and the tubing performance curves on Cartesian coordinates. Once again determine point of natural flow. Tubing Perfonnance Relation the 3) Discuss the advantages of a log-log plot of the well performance curves over a Cartesian plot.
  • 48. Examples 6 Production from the Davis No. 5 (Examples 3 and  4) suddenly dropped after five years of production. By running a special tubing gauge tool, it was determined that the tubing had collapsed at 6537 ft. During a workover job to replace the tubing. it was discovered that the casing had also collapsed at the same depth. The collapsed casing interval has been reamed out to full bore and has been milled out 1 throughout the the pay zone. A 2-in. liner 6000 has been 5 set inside damaged casing from to 8000 ft. The well has been completed with 3.5-in. tubing which was run only to 5950 as shown in Fig. below. A 7 changeover to 2 8-in. to run the tubing inside the liner up to the perforations depth was considered too costly and unnecessary.
  • 49. following A test the workover  indicated an average reservoir pressure of 2000 psi a and a gas/oil ratio of 2500 scf/STB. In addition, a flowing pressure gradient in the 5.5-in. liner was measured as 𝐺f = 0.26psi/ft. During the test a rate of 320 STB/D was recorded, with a stabilized flowing bottomhole pressure of 842 psia. Assuming exponent n equals equation. 0.8  in the backpressure predict the natural flow of the well with 200psia wellhead pressure.