pressure drawdown test
TRANSCRIPT
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Assignment No. 01: PCB 3013 Well Test AnalysisLast date for submission : 26Feb., 2015 Max. Marks-05
Q.No.1: What do you know about Linear Discontinuities
(Sealing Faults)? Discuss in detail Draw Down behavior
of a well in the vicinity of a fault.
Q.No.2: State and explain Buildup case and Effect of
Producing time on Pressure Response.
Q.No.3(a): What are the conditions at which fault may bedetected by conducting well test?
(b)Differentiate:
Multiple Fault Systems and Late Transient AnalysisInternal
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PRESSURE DRAWDOWN TEST
A drawdown test is run as follows:
1. The well is shut-in for a period of time longenough to allow the pressure to equalize
throughout the reservoir.2. The pressure measuring equipment is
lowered into the well.
3. The flow is begun at a constant rate and the
bottom-hole pressure is continuouslymeasured.
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The duration of DDT depending upon
objectives & Formation characteristics:
Few hours or several days
Extended DDT (Reservoir Limits) are
primarily run to estimate drainage volume of
Well.
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PRESSURE BEHAVOIR OF A SINGLE
WELL IN AN INFINITE RESERVOIR
The dimensionless pressure at the well
(r D=1) is given by Eq
),(2.141,1
D Di D
n
i
ii t r P Bqkh
t r P
80907.0)ln(21 D D t s P
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s
r c
kt P P
Bq
kh
wt
wf i 280907.00002637.0
ln
2
1
2.141 2
s
r c
k
kh
Bq P P
wt iwf
8686.023.3log6.162
2
in oilfield units:
solving for Pwf ;
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It indicates that a plot of bottom-hole pressure
(also known as the sand-face pressure) Pwf vs.
time, t , should yield a straight line with a slope m
kh
Bqm
6.162
The beginning time of the “semi-log straight line” may be estimated from:
khC st
SSL )000,12000,200(
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SKIN EFFECT
The damaged zone is called the “skin." The main factors responsible for this damage are:
Invasion by drilling fluids
Partial well penetration
Partial completion (productive interval not entirely perforated)
Plugging of perforations
Organic/Inorganic precipitation Improper perforation density or limited perforation
Bacterial growth
Dispersion of clays
Presence of a mud cake and of cement
Presence of a high gas saturation around the wellbore
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The additional pressure drop due to the skin
effect is:
sm skh
Bq P s )(87.0
2.141
or;
w
s
w
s
s
sr
r
kh
Bq
r
r
hk
Bq P ln
2.141ln
2.141
w
s
s
s
r
r
k k h
Bq P ln
112.141
w
s
r
r
sk sk k m s P ln)(87.0
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Semilog plot of a pressure drawdown test indicating
pressure at 1 hr
1200
1300
1400
1500
1600
1700
1800
1900
2000
0.1 1 10 100
P1hr
k h
Bqm
6.1 6 2
Deviation from straight line is due to
wellbore storage and skin effects
P w
f ,
psi
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If the radius, r s, and the permeability, ks, of the skin
zone are known, the skin factor may be estimated
from
sm skh
Bq P s )(87.02.141
w
s
r
r
sk
sk k
m s P ln)(87.0
w
s
s r
r
k
k s ln1
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Thus, if:
(1) ks < k, then s > 0; damaged well
(2) ks > k, then s < 0; stimulated well (fracturing or acidizing)
(3) ks = k, then s = 0; the well is neither damaged nor stimulated.
Hydraulically fractured wells often show values of S rangingfrom -3 to -5. It is not possible to obtain both rs and ks fromEq.
even if k, s, and rw are known. For this, we define an“effective (or apparent) wellbore radius”, rw’, suchthat:
w
s
s r
r
k
k s ln1
w
w
skinr
r
kh
Bq P
'ln
2.141
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Thus;
s r
r w
w
ln'
or;
r r ew w s'
where;
23.3log1513.1
2
1
wt
hr
r c
k
m
Pi P s
where;
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FLOW EFFICIENCY (OR PRODUCTIVITY
RATIO, OR COMPLETION FACTOR)
This parameter measures the degree of producing capability for an
undamaged well.
)0(
s J
J FE
ideal
actual
wf
actual P P
q J
skinwf
ideal P P P
q J
wf
skinwf
P P
P P P
FE
where;
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In presence of steady state or a new well .
If FE < 1 = damaged well
If FE > 1 = stimulated well
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DAMAGE RATIO AND DAMAGE FACTOR
Both damage ratio and damage factor reflect wellbore
conditions
The damage ratio is defined as the inverse of
flow efficiency and
The damage factor results by subtracting theflow efficiency from unity.
skinwf
wf
p p P
p P
FE DR
1
wf
skin
P P
P FE DF
1If DF > 0; damaged well
If DF < 0; improved or stimulated wellInternal
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WELLBORE STORAGE
Wellbore storage or afterflow is the continued
influx from a formation into the wellbore after
the well is shut-in.
During short-time production, dimensionlesspressure is directly proportional to
dimensionless time:
D
Dwf i
ct P P
Bqkh
2.141
C hr c
C wt
D 2
89359.0
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Parameter C in Eq. is the wellbore storage
coefficient given in bbl/psi, and may be
estimated from completion data.
a) For a completely fluid-filled wellbore (injectionwell), i.e. compressive wellbore storage, the
expected value of C is given by:
where c is the compressibility of the fluid in the
wellbore, and Vw is the total wellbore volume in
bbl.
wcV C
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For a wellbore with a rising (pumping well)
or falling liquid level, i.e. non-compressive
wellbore storage:
Thus, wellbore storage and skin effect
determine the time required to reach thesemi-log straight line of a drawdown plot.
This time may be estimated from:
)/)(144/( c
u
g g V C
D D Cst )5.360( Internal
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Substituting Eq. for dimensionless time
22
89359.0)5.360(
0002637.0
wt wt hr hc s
r c
kt
kh
C st SSL
)5.360(66.3388
D
DSSL
C
t
kh
C t
66.3388or;
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After plugging the dimensionless parameters
tD and CD, it yields:
This equation is extremely useful in well testdesign. Thus, if one log cycle of straight line
is desired, the test should be run for a period
of time T:
C kh
st SSL
)12000200000(
SSLt T 10
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The drawdown stabilization time and the drainage
radius during the test can be determine by:
The maximum pressure response occurs at tmax
which is defined a
and for any producing time, tp, the radius of
investigation is given by:
k
Act t s
43560380
t
sd
c
t k r
029.0
k
r ct t
2
max
948
t
p
inv c
t k
r 0325.0Internal
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The time at which the pseudosteady state period
takes place is given by:
For any producing time, tp, Eq. can be expressed as:
t
p
invc
t k r
0325.0
k
r ct et pss
2948
Eq is appropriate for square geometries.
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For circular systems, the appropriate relationship is
The wellbore storage coefficient may be estimatedfrom a plot of P vs. time on a log-log graph paper.
The slope of such a curve is one during the period
dominated by wellbore storage effect. Any point i on this straight line portion may be used to
find C, or:
k
r ct et pss
21190
i
i
p
t qBC
24Internal
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For a drawdown test, the time is simply theflowing time and P = Pi - Pwf, thus:
C calculated from Eqs. should be similar
If they are not, it could be an indicator ofwhether the liquid level is falling or rising.
Other reasons for this difference might beeither high gas-oil ratio at the wellbore orhighly stimulated well, among others.
wf i
P P
t qBC
24
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RESERVOIR LIMIT TEST
This is a drawdown test run long enough for
the purpose of estimating the drainage
volume of the well.
This test uses the pseudo-steady stateportion of the plot of Pwf vs. flowing time.
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k
r ct
et
0 0 0 2 6 3 7.0
2
k
r ct et
0 0 0 8 8.0
2
P
,
ps
i
wf
Time, hrs
Region I Region II Region III
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Region I in Fig. corresponds to the portion of
the test responsible to analysis by transient
methods.
Region II in the same plot is referred to latetransient method
Region III, semi-steady state behavior, is the
reservoir limit test itself which is governed by:
Aw
DA DC r
At P
2458.2ln
2
1ln
2
12
2
where the area, A, is given in ft2Internal
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Substituting
A
r t
C
kt t w D
A
DA
20002637.0
s P P kh
Bq P wf i D
2.141
s
C r
A
kh
Bq P t
Ahc
qB P
Aw
i
t
D 22458.2
lnln6.7023395.0
2
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This equation is of the general form y = mx + b.
Thus, during pseudo-steady state, a Cartesian plot of Pwf vs. t
should be a straight line.
The slope and intercept of such a straight line are:
0
500
1000
1500
2000
2500
0 20 40 60 80 100
Pint
Slope=m
t, hr
P w
f ,
psi
*
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The slope m* in Fig. may be used to calculate thevolume of the reservoir portion being drained by the
test well (drainage volume in ft3):
The Dietz shape factor, C A, may be estimated from:
Ahc
qBm
t
23395.0*
s
C r
A
kh
Bq P P
Aw
i 22458.2
lnln6.70
2int
*
23395.0
mc
qB Ah
t
m P P
A
hr
em
mC
int130 3.2
*456.5
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The shape factor is used to determine the reservoir
configuration (circle, rectangle, hexagon, etc.) as follows:
From table 1 find a value of CA which corresponds most
closely to the value calculated from Eq.
Calculate the dimensionless time at start of pseudo-steadystate period
Compare (tDA)pss obtained from following Eq. with the “Exact
for (tDA)pss > ” column of the table 1. If (tDA)pss the value
obtained from this column, then the shape corresponding to
the “most closely” value of C A is the most likely configuration
of the system. Mattews, Brons and Hazebroek first studied
shape factors for several drainage geometries.
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Table 1. Shape factors for various single-well drainage areas
C A
31.62
31.6
27.6
27.1
21.9
30.8828
12.9851
4.5132
3.3351
21.8369
10.8374
4.5141
2.0769
3.1573
0.1
0.1
0.2
0.2
0.4
0.1
0.7
0.6
0.7
0.3
0.4
1.5
1.7
0.4
0.06
0.06
0.07
0.07
0.12
0.05
0.25
0.30
0.25
0.15
0.15
0.50
0.5
0.15
Less than1 % error
for tDA >
0.1
0.1
0.09
0.09
0.08
0.09
0.03
0.025
0.01
0.025
0.025
0.06
0.02
0.005
Use infinite system solutions with less than
1 % error for tDA >
1
1
0.098 0.9 0.6 0.015
Exact for
for tDA >
60°
1
1/3
43
1
1
1
1
1
1
1
Bounded
reservoirs
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C A
0.5813
0.1109
5.379
2.6896
0.2318
2.3606
2.6541
2.0348
1.9986
1.662
1.3127
0.7887
19.1
25.0
2.0
3.0
0.8
0.8
4.0
1.0
0.175
0.175
0.175
0.175
0.175
0.175
--
--
0.6
0.6
0.3
0.3
2.0
0.4
0.08
0.09
0.09
0.09
0.09
0.09
--
--
Less than1 % error
for tDA >
0.02
0.005
0.01
0.01
0.03
0.025
Cannot use
Cannot use
Cannot use
Cannot use
Cannot use
Cannot use
--
--
Use infinite system solutions with less th
1 % error for tDA >
1
2
1
2
1
4
1
4
1
4
1
5
Vertical-Fractured
reservoirs
1
1
xf/xe=0.1
1
1
xf/xe=0.2
1
1
xf/xe=0.3
1
1
xf/xe=0.5
1
1
xf/xe=0.7
1
1
xf/xe=1.0
Water-Drive reservoirs
Unknown Drive mechanism
0.1155 4.0 2.0 0.011
4
Use (Xe/Xf) in place of A/rw
for fractured reservoirs
2 2
Exact for
for tDA >
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