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Contents Contents 1.1. Introduction Introduction
2.2. The Radial F low Equation The Radial F low Equation
3.3. Straight L ine I nf low PerformanceStraight L ine I nf low PerformanceRelationship Relationship
4.4. Vogel I nf low Performance Relationship Vogel I nf low Performance Relationship
5.5.
Other I nf low Performance Relationship Other I nf low Performance Relationship
6.6. Establishing the Well ' s IPR Establishing the Well ' s IPR
7.7. Use of the I nflow PerformanceUse of the I nflow Performance
Relationship Relationship
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1. INTRODUCTION1. INTRODUCTION
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I nflow Performance
The rate at which fluid will flow towards the
wellbore depends upon
The nature of the fluid,
The type of reservoir rock and theDriving force.
This is driving force is not the reservoir
pressure but the difference in pressure betweenthe reservoir and the wellbore, and is called
The Drawdown (PDD
)
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I nflow Performance
The Inflow
Performance
Relationship (IPR)
quantifies the
flow-rate from
a well as a
function of the
drawdown.
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I nflow Performance
2. THE RADIA L2. THE RADIA L
FLOW EQUATION FLOW EQUATION
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I nflow Performance
Consider radial inflow into a well as depicted in
the Figure.
The change in pressure profile and the pressure
at the outer boundary (pe) depend on the initial
and boundary conditions imposed.
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I nflow Performance
Three different f1ow conditions can be
distinguished:
Transient flowSemi Steady State flow
Steady State flow
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I nflow Performance
Transient f low Trans ient f low
This condition is only applicable for a relatively
short period after some pressure disturbance
has been created in the reservoir.
Transient flow conditions are applied to the
analysis of well tests.
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Sem i Steady State f low Sem i Steady State f low
This condition is applicable to reservoir which
has been producing for a sufficient period of
time so that the effect of the outer boundary has
been felt.
It is considered that
the well is surrounded
at its outer boundary
by a solid "brick wall
which prevents flow of
fluids into the radial cell (Figure). re = drainage radiusrw = well bore radius
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I nflow Performance
Steady State f low Steady State f low
This condition applies to a well draining a cell
which has a completely open outer boundary.
It is assumed that, for:
q A constant
production rate,
q Fluid withdrawal
from the cell willbe exactly
balanced by fluid
entry across the open boundary.
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I nflow Performance
This condition is appropriate when pressure is
being maintained in the reservoir due to either:
Ø Natural water influx, orØ The injection of displacing fluid.
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Radial inf low equat ion fo rRadial inf low equat ion for
steady state flow steady state flow
Assuming that the reservoir is homogeneous
in all reservoir parameters, Darcy's law for the
radial flow of a single phase fluid can beexpressed as:
Where: k = Permeability
A = Flow area
! = Viscosity
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More realistically, for a well located in a
reservoir containing other wells, the radius fromwhich liquid is being
drained is known and
is called the
drainage radius r e.
The inflow equation for Steady State flow may
be written;
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The radial flow model is therefore adapted to
express the drawdown in terms of the average
reservoir pressure P.
This value would be obtained if the producing
field was shut in until the pressure in the
reservoir had equalize, and the average
reservoir pressure is found by analyzing
individual well shut-in bottom hole pressures.
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3. STRA IGHT 3. STRA IGHT - - LINELINE
INFLOW PERFORMANCEINFLOW PERFORMANCE
RELATIONSHIP RELATIONSHIP
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When we consider the parameters in the
equation for the Productivity Index the followingcomments can be made:
Ø h, r e and r w are constant.
Ø k, ! and Bo are pressure dependent.
The criteria is the flowing bottom hole pressurewith respect to the phase envelope of the fluidconsidered.
For single phase flow, which occurs when theflowing pressure is above the bubble pointpressure, these parameters can be consideredconstant (independent of pressure).
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I nflow Performance
Under the above conditions the Productivity
Index (J) is constant and is called "PI".
The equation q = PI x Pdd describes a straight
line.
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I nflow Performance
4. VOGEL INFLOW4. VOGEL INFLOW
PERFORMANCEPERFORMANCE
RELATIONSHIPRELATIONSHIP
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When the flowing bottomhole pressure is belowthe bubble point pressure, two phase liquid and
gas flow occurs in the reservoir and the linear
relationship defined above is no longer valid.
When the pressure declines below Pb.
The permeability decrease,
Oil formation volume factor will decrease,The viscosity will increase.
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This type of behavior has been observed in
solution gas drive reservoirs, as depletionprecedes the productivity of a typical welldecrease.
Under these conditions,
a plot of flowing bottomhole pressure againstproduction rate resultsin a curved, rather than
a straight line and thereis a progressivedeterioration in the inflowperformance relationships as the reservoir isdepleted.
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I nflow Performance
The inflow performance relationships shown in
the previous Figure may be redefined as nodimensional IPR's.
This is done by
expressing the bottomhole flowing pressure
as a fraction of the
maximum shut-in
pressure, and the
relevant flow rate as
a fraction of the maximum production rate for
that curve, at very similar throughout most of
the producing life of the reservoir.
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It is shown that non-dimensional IPR's apply tomany different reservoirs.
Exceptions are wells with:
qLarge positive skins,
q High viscosity crudes, and
q Very high rate producers.
Because of the similar nature of the non-
dimensional IPR's, it is possible to group theminto one representative curve which closely
approximates them all.
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The curve giving the best fit to the non-dimensional IPR's shown above is called the
reference IPR curve, or the Vogel IPR.
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The equation of the reference curve is:
If q/q max is plotted against pWf / p, the referencecurve will result.
Having established the maximum possible flow
rate and the reservoir pressure, plotting q
against pwf will give the actual inflow
performance relationship for a particular well.
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For comparison to the Vogel IPR, therelationship for a straight line (PI) IPR would
be;
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5. OTHER INFLOW5. OTHER INFLOW
PERFORMANCEPERFORMANCE
RELATIONSHIPS RELATIONSHIPS
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5.1 IPR or reservoirs with static pressures5.1 IPR or reservoirs with static pressures
above bubble point pressureabove bubble point pressure
5.2 Gas Well5.2 Gas Well IPR's IPR's
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5.1 IPR or reservoirs w ith s tat ic p ressu res5.1 IPR or reservoirs w ith s tat ic p ressu resabove bubble point pressure above bubble point pressure
The IPR's described in the previous sections
dealt with either above or below bubble pointconditions.
It is more realistic to define an IPR which is valid
for both conditions.
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Above Pb the IPR will respond linear and whenthe Pwf is below Pb a curved IPR will occur.
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The solution for Pwf < Pb is then:
Where J* is the Productivity Index for the
straight line part of the IPR.
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5.2 Gas Well5.2 Gas Well IPR's IPR's
The IPR's described in the previous sections are
applicable to oil wells only.
In gas wells, fluid velocity around the well bore
is much higher than that found in oil wells.
Due to this high velocity, turbulent flow will
occur resulting in an additional pressure drop.
In addition the gas viscosity and
compressibility are highly dependent on
pressure and temperature.
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The resulting non-linear IPR of gas wells is
often expressed as:
Where Q = the pressure drop due to laminar
(Darcy) flow and
bQ2 = the pressure drop due to inertial
turbulent (non-Darcy) flow.
The constants a, and b can be derived from
known reservoir and gas properties.
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6. ESTABLISHING6. ESTABLISHING
THE WELL'S IPR THE WELL'S IPR
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The inflow performance
relationship for a given
well has to be
established by
a well test.
In theory, oneproduction rate with
corresponding bottom
hole pressure and the
shut-in pressure willdefine the inflow
performance
relationship.
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In practice a number of flow rates may be taken
to confirm the well performance.
If a sample of formation fluid is taken and
analyzed to establish the bubble point pressure,
it will be possible to decide whether to use the
straight line, the Vogel or the Vogel / Glass
inflow performance relation hit.
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During well testing, it should not be necessaryto draw the well bore pressure down very low in
order to establish the maximum inflow potential
of the well, the IPR may be used to establish
this value.
In the case that the formations being tested are
friable, unconsolidated sands, it is unwise to
apply a high drawdown for a fear of collapsingthe formation and getting no test data at all.
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7. USE OF THE INFLOW7. USE OF THE INFLOW
PERFORMANCEPERFORMANCERELATIONSHIP RELATIONSHIP
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The inflow performance relationship is useful asa tool to monitor well performance and predict
the stimulation and artificial lift to requirements
of a number of wells.
The IPR for a well must be known in order to
size the well tubular correctly.
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Based on interpolation between wells, if the
initial IPR for a well is lower than expected in aparticular part of the reservoir, it may then be
suspected that the formation has been badly
damaged during the drilling and completion
phase.
Mapping the IPR's across the field may highlight
this situation.
When well bore damage is confirmed by a build-
up survey the well may require stimulation.
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Even with stimulation, the inflow performance
of a well will decline with falling reservoirpressure.
Plotting this decline
will indicateapproximately when
the wells will have to
be artificially lifted in
order to maintain therequired off take rate
from the field.