taller ejercicio 1 dd
TRANSCRIPT
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1. Problem No 1.
A new well, in a small bounded reservoir, North
of Hobbs, New Mexico, was produced at a constant
rate of 360 STB/D.
The initial pressure throughout the reservoir priorto the flow test was 4620 psia.
Part 1. Conventional Techniques
A) Skin Effect1. Calculate reservoir transmissibility and
permeability.
2. Compute the skin factor.3. Calculate flow efficiency, damage ratio and
damage factor. Is the wellbore damaged or
stimulated? Why?
4. Calculate the radial distance of the skin, ifthe formation permeability from lab.measurements is expected to be affected 410
percent by the skin. Compare with theapparent radius, rw.
5. What is the flow rate without the skineffect?
B) Wellbore Storage6. Find the wellbore storage coefficient.7. Estimate the starting time of the semilog
straight line.
C) System Geometry8. Calculate the drainage volume and drainage
area (in acres) of this well.
9. Find the shape factor of this drainage area.10.Determine the system geometry.11.Estimate the drawdown stabilization time.12.Compute the radius of drainage created
during this drawdown test.
Table 1.1. Drawdown Test Data for Problem No. 1
t
[hrs]
Pwf
[psia]
t
[hrs]]
Pwf
[psia]
0 4,620 4.000 4,360
0.020 4,588 7.000 4,325
0.030 4,576 10.000 4,300
0.044 4,552 20.000 4,256
0.060 4,528 30.000 4,230
0.100 4,505 50.000 4,195
0.200 4,486 70.000 4,172
0.400 4,478 80.000 4,160
0.700 4,450 90.000 4,150
1.000 4,435 100.000 4,140
2.000 4,400 125.000 4,120
3.000 4,380
Solution
1. Conventional Techniques
Skin effect
Using data given on Table 1.1, Pwf vs. time isgraphed on Cartesian (Fig. 1.1) and semi log (Fig
1.2). Cartesian plot shows clearly the pseudo stable
state of flow characterized by a straight line
Because the infinite active line is before PSS, thestraight line in semilog is plotted avoiding the PSS.
4000
4100
4200
4300
4400
4500
4600
4700
0 10 20 30 40 50 60 70 80 90 100 110 120 130 140
Time (hours)
Pwf(Psia)
Pint=4245
m*=1
Fig. 1.1 Cartesian plot Pwf vs. time
4000
4100
4200
4300
4400
4500
4600
4700
0.01 0.1 1 10 100 1000
Time(hours)
Pwf(Psia)
m=140
P1hr=4440
Fig. 1.2 Semilog plot Pwf vs. time
From figure 1.2
cyclepsiam /1402
44404160
Permeability is computed from
mh
qk
6.162 (1.1)
mdk 56.538*140
84.0*22.1*360*6.162
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[Homework Number 1] Dora Restrepo 2
Transmissibility
cp
ftmdkh *10.510
84.0
8*56.53
Skin factor is computed from
23.3log1513.1
2
1
wt
hri
rc
k
m
pps
(1.2)p1hris read from Fig. 1.2 on the infinite acting line.
P1h = 4440 psia. Then,
23.3
29.0*10*42*84.0*10.0
56.53log
140
444046201513.1
25s
16.3s
Eq. 1.3 allows find psvalue:
skh
qps
2.141 (1.3)
psips 6.383)16.3(*8*56.53
22.1*84.0*3602.141
Flow efficiency, damage radio and damage factor
are estimated from:
wf
swf
pp
pppFE
(1.4)
Pwf is the last value of pressure at the end of thetest and average pressure will be considered equal
to pi, which implies the assumption that the well is
new or steady state.
%17777.141204620
)3.383(41204620
FE
FEDR
1 (1.5)
%5757.077.1
1DR
FEDF 1 (1.6)
%7777.077.11 DF
These values show that the area next to the wellbore
is stimulated because S < 0, FE > 1, DR < 1, and
DF < 0. According to Tiab (2004) this value of s isinto the range for hydraulically fractured wells (-3
to -5)
Radial distance of the skin:
w
s
s r
r
k
kS ln1
(1.7)
In terms of rs:
1
* sk
k
S
ws err (1.8)
ks = 4.10*k from laboratory measurement
expectations. So, ks= 219.6 md
Then,
fters 8.18*29.01
6.219
56.53
16.3
Apparent radius:
s
ww err ' (1.9)
fterw 8.6*29.0')16..3(
The flow rate without effect skin is calculated using
the next set of equations:
ideal
actual
J
JFE (1.9)
In terms of Jideal:
FE
JJ actual
ideal (1.10)
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and,
skinwf
idealppp
qJ
(1.11)
Finding Jactual:
wf
actualpp
qJ
(1.12)
72.041204620
360
actualJ
Substituting this value on Eq. 1.10,
4.077.1
72.0
idealJ
Using Eq. 1.4 and leaving Eq. 1.11 in terms of q:
FE
qq actual
s 0 (1.13)
DSTBqs /20377.1
3600
Wellbore Storage
Wellbore storage coefficient is estimate using Eq.
1.14 and taking (t/p)i data from Fig. 1.3 at any
convenient point on the unit slope.
10
100
1000
0.01 0.1 1 10 100 1000
Time (hours)
P, t*P'
(t*p')i =70 psia
(p)i
ti = 0.042
TSSL = 4 hr
pr = 390 psia
tr = 30 hr
trpi = 64 hr
Fig. 1.3. Pressure derivative.
ip
tqC
24
(1.14)
psia
bblC 01.0
70
043.0
24
22.1*360
Reading tSSL (starting time of semilog straight
line) from Fig. 1.3; tSSL = 4 hr. Using Eq 1.15 we
find for tSSL:
Ckh
stSSL
/
)*000,12000,200( (1.15)
hrtSSL 6.401.084.0/8*56.53
)]16.3(*000,12000,200[
System geometry
From Fig. 1.1, pressure at the intercept is 4245
psia, and m*is calculated as the slope of the straight
line:
12
12*
tt
ppm
(1.16)
19080
41504160* m
But m* in terms of A is:
Ahc
qm
t
23395.0* (1.17)
Then,
hmc
qA
t )(
23395.0
*
(1.18)
2
536.941,295
8*.)1(*10*1042.0
22.1*360*23395.0ftA
AcresA 79.6
AhV (1.19)309.753,2368*36.941,295*10.0 ftV
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Shape factor
mpp
A
hr
em
mC
)(303.2
*
int1
456.5 ( 1.20)
8.301
140456.5 140)42454454(303.2
eCA
System geometry
pssDA tm
mt
*
1833.0 (1.21)
Where tpss is the starting time of pseudosteady
state flow, and is obtained from Fig. 1.1. tpss= 42hours. Then,
055.042)140(
)1(1833.0
DAt
With CA= 30.8 and tDA= 0.055, the reservoir hasthe next geometry with less than 1% error for tDA:
Where the shape is taken fromAppendix D, page 265 (Pressure
Transient Testing):
CA = 30.8828
tDA= 0.05
Drawdown stabilization time
k
Act ts
)43560(380
(1.22)
1.7856.53
)79.6*43560(10*42*10.0*84.0380
5
st
12. Radius of drainage created during the test
t
s
dc
ktr
029.0 (1.23)
1.30810*42*10.0*84.0
1.78*89.50029.0
5
dr