pdf p324 07a (for class) lec mod2 01b poz for abnprs (gonzalez)
TRANSCRIPT
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A New p/z-Gp2 M a t er i a l B a l a n c e f o r A b n o r m a l l y -P r es s u r e d R e s er v o i r s Slide
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A Q u ad r a t ic C u m u l at i v e Pr o d u c t i o n
M o d el f o r t h e M a ter i al B al an c e o f A b n o r m a l l y - P r e s s u r e d G a s R e s e r v o i r s
F.E. Gonzalez, M.S. Thesis Defense
17 October 2003Department of Petroleum Engineering
Texas A&M University
College Station, TX 77843-3116
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Executive Summary "p/z-Gp2" Relation (1/4)
The rigorous relation for the material balance of a drygas reservoir system is given by Fetkovich, et al. as:
)(61551
))((1
ewinjwpg
swpinj WBWBWB
.RWGpG
Giz
ip
iz
ippippecz
p
Eliminating the water influx, water production/injection,and gas injection terms; defining Gp=ce(p )(pi-p) andassuming that Gp
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Simulated Dry Gas Reservoir Case Abnormal Pressure: Volumetric, dry gas reservoir withcf(p) (from Fetkovich).
Note extrapolation to the "apparent" gas-in-place (previous approaches).
Note comparison of data and the new "Quadratic Cumulative Production" model.
Executive Summary "p/z-Gp2" Relation (2/4)
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Anderson L Reservoir Case Abnormal Pressure: South Texas (USA) gas reservoir with abnormal pressure.
Benchmark literature case.
Note performance of the new "Quadratic Cumulative Production" model.
Executive Summary "p/z-Gp2" Relation (3/4)
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Executive Summary
Objectives and RationaleRigorous technique for abnormal pressure analysis.Development of the p/z-Gp
2 modelDerivation from the rigorous material balance.
Validation Field ExamplesCase 1
Dry gas simulation (cf(p) from Fetkovich).
Case 3 Anderson L (South Texas, USA).
Demonstration (MS Excel Anderson L case)Summary
Recommendations for Future Work
Presentation Outline
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Objectives and Rationale
Objectives: Develop a rigorous functional form (i.e., a model) for
the p/zvs.Gpbehavior demonstrated by a typicalabnormally pressured gas reservoir.
Develop a sequence of plotting functions for theanalysis ofp/zGpdata (multiple plots).
Provide an exhaustive validation of this new modelusing field data.
Rationale: The analysis ofp/zGpdata for abnorm-ally pressured gas reservoirs has evolved from empi-rical models and idealized assumptions (e.g., cf(p)=
constant). We would like to establish a rigorous ap-proach one where any approximation is based onthe observation of some characteristic behavior, notsimply a mathematical/graphical convenience.
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Development of the p/z-Gp2 model
Concept: Use the rigorous material balance relation given by
Fetkovich,et al. for the case of a reservoir wherecf(p) is NOT presumed constant.
Use some observed limiting behavior to construct asemi-analytical relation forp/zGpbehavior.
Implementation: Develop and apply a series of data plotting functions
which clearly exhibit unique behavior relative to thep/zGpdata.
Use a "multiplot" approach which is based on the
dynamic updating of the model solution on eachdata plot.
Develop a "dimensionless" type curve approach thatcan be used to validate the model and estimate G.
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p/z-Cumulative Model: (1/3)
The rigorous relation for the material balance of a drygas reservoir system is given by Fetkovich, et al. as:
)(61551
))((1
ewinjwpg
swpinj WBWBWB
.RWGpG
Giz
ip
iz
ippippecz
p
Eliminating the water influx, water production/injection,and gas injection terms, then rearranging gives thefollowing definition:
)])(([where1)1(
// pippecG
G
G
G
zpp
p
p
iizp
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Considering the condition where:
Then we can use a geometric series to represent the Dterm in the governing material balance. The appropriategeometric series is given by:
1 pD G
1)1(3
111
2
x...xxxx/
1)1(1)1(
1
pp
p
GGG
or, for our problem, we have:
2)
1(1 pp
i
i GG
GGz
p
z
p
Substituting this result into the material balance relation,we obtain:
p/z-Cumulative Model: (2/3)
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A more convenient form of the p/z-cumulative model is:
We note that these parameters presume that
is con-stant. Presuming that is linear with Gp, we can derivethe following form:
p/z-Cumulative Model: (3/3)
i
i
z
p
G)
1(
i
i
z
p
G
32)()
1( p
i
ip
i
ip
i
i
i
i Gz
p
G
bG
z
pb
G
aG
z
pa
Gz
p
z
p
pbGa where
Obviously, one of our objectives will be the study of thebehavior of vs.Gp(based on a prescribed value ofG).
2ppii GG
z
p
z
p
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Simulated Dry Gas Reservoir Case A b n o r m al P r es s u r e :A linear trend of vs.Gpis reasonable and should yield an accurate model.
is approximated by a constant value within the trend.
A physical definition of is elusive Gp=ce(p )(pi-p) implies that has units of1/volume, which suggests is a scaling variable forG.
-GpPerformance (Case 1) (1/2)
a. Case 1: Simulated Performance Case Plot of
versusGp(requires an estimate of gas-in-
place). Note the apparent linear trend of the
data. Recall that Gp=ce(pp-p).
b. Case 1: Simulated Performance Case Plot of
p/zversus Gp. The constant and linear trends
match well with the data essentially a con-
firmation ofb o t h models.
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Anderson L Reservoir Case Abnormal Pressure: Field data will exhibit some scatter, method is relatively tolerant of data scatter.
Constant approximation is based on the "best fit" of several data functions.
The linear approximation for is reasonable (should favor later data).
-GpPerformance (Case 3) (2/2)
a. Case 3: Anderson L Reservoir Case (South
Texas, USA) Plot of versusGp(requires an
estimate of gas-in-place). Some data scatter
exists, but a linear trend is evident (recall that
Gp=ce(p)(pi-p)).
b. Case 3: Anderson L Reservoir Case (South
Texas, USA) Plot ofp/zversus Gp. Both
models are in strong agreement.
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Validation of the p/z-Gp2 model: Orientation
Methodology: All analyses are "dynamically" linked in a spread-
sheet program (MS Excel). Therefore, all analysesare consistent should note that some functions/plots perform better than others b u t t h e m o d el r e s u l t s a r e t h e s am e f o r e v e r y a n al y s i s p l o t .
Validation: Illustrative Analyses p/z-Gp
2 plotting functions based on the proposedmaterial balance model.
-Gpperformance plots used to calibrate analysis.
Gan analysis presumes 2-straight line trends on a
p/z-Gpplot for an abnormally pressured reservoir. pD-Gp Dtype curve approach usep/z-Gp
2 materialbalance model to develop type curve solution thisapproach is most useful for data validation.
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p/z-Gp2 Plotting Functions: Case 1 (1/5)
a. b. c. ppp
p
GdGzpG
Gvs.)/(
0
1
pp
GzpG
vs.)/(1
d. e.ppp
p
GdGzpG
Gvs.
2 )/(
0
1
ppp
p
GdGzpG
Gzp vs.)/(
0
1)/( f. pp
p
pp
GdGzpG
Gzp
Gvs.)/(
0
1)/(
1
pG
z
p
iz
ipzp vs.)/(
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-GpPlotting Functions: Case 1 (2/5)
a. Case 1: Simulated Performance Case Plot of
ce(p)(pi-p) versus Gp(requires estimate ofG).
b. Case 1: Simulated Performance Case Plot of
1/ce(p)(pi-p) versus Gp(requires estimate ofG).
c. Case 1: Simulated Performance Case Plot of
versusGp(requires estimate ofG).
d. Case 1: Simulated Performance Case Plot of
versusGp/G(requires estimate ofG).
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Simulated Dry Gas Reservoir Case A b n o r m al P r es s u r e : Summary p/zGpplot for =constant and =linear cases.
Good comparison of trends, =linear trend appears slightly conservative as itemerges from data trend but both solutions appear to yield same Gestimate.
-GpPlotting Functions: Case 1 (3/5)
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Gan-Blasingame Analysis (2001): Case 1 (4/5)
a. Case 1: Simulated Performance Case Gan Plot 1
ce(p)(pi-p) versus (p/z)/(pi/zi) (requires est. ofG).
b. Case 1: Simulated Performance Case Gan Plot 2
(p/z)/(pi/zi) versus (Gp/G) (requires est. ofG).
c. Case 1: Simulated Performance Case Gan Plot 3
(p/z) versus Gp(results plot).
Gan-Blasingame Analysis:Approach considers the "match"
of the ce(p)(pi-p) (p/z)/(pi/zi)data and "type curves."
Assumes that b o t h abnormaland normal pressurep/ztrendsexist.
Straight-line extrapolation of the"normal"p/ztrend used forG.
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pD-Gp DType Curve Approach: Case 1 (5/5)
a. pD-GpDType curve solution based on the p/z-Gp2
model. pD= [(pi/zi)-(p/z)]/(pi/zi) andGpD=Gp/G
both pDandpDifunctions are plotted.
b. Case 1: Simulated Performance Case Type
curve analysis of (p/z)-Gpdata, this case is
"force matched" to the same results as all of the
other plotting functions.
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p/z-Gp2 Plotting Fcns: Case 3 (Anderson L) (1/5)
a. b. c. ppp
p
GdGzpG
Gvs.)/(
0
1
pp
GzpG
vs.)/(1
d. e.ppp
p
GdGzpG
Gvs.
2 )/(
0
1
ppp
p
GdGzpG
Gzp vs.)/(
0
1)/( f. pp
p
pp
GdGzpG
Gzp
Gvs.)/(
0
1)/(
1
pGz
p
iz
ipzp vs.)/(
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-GpPlotting Functions: Case 3 (2/5)
a. Case 3: Anderson L (South Texas) Plot of
ce(p)(pi-p) versus Gp(requires estimate ofG).
b. Case 3: Anderson L (South Texas) Plot of
1/ce(p)(pi-p) versus Gp(requires estimate ofG).
c. Case 3: Anderson L (South Texas) Plot of
versusGp(requires estimate ofG).
d. Case 3: Anderson L (South Texas) Plot of
versusGp/G(requires estimate ofG).
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Case 3 Anderson L Reservoir (South Texas (USA)) Summary p/zGpplot for =constant and =linear cases.
Good comparison of trends, =constant and =linear cases in good agreement.
Data trend is very consistent.
-GpPlotting Functions: Case 3 (3/5)
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Gan-Blasingame Analysis (2001): Case 3 (4/5)
a. Case 3: Anderson L Reservoir Gan Plot 1 ce(p)(pi-p)
versus (p/z)/(pi/zi) (requires est. ofG).
b. Case 3: Anderson L Reservoir Gan Plot 2 (p/z)/(pi/zi)
versus (Gp/G) (requires est. ofG).
c. Case 3: Anderson L Reservoir Gan Plot 3 (p/z)
versusGp(results plot).
Gan-Blasingame Analysis:We note an e x c e l l en t "match" of
thece(p)(pi-p) (p/z)/(pi/zi) dataand the "type curves."
Both the abnormal and normalpressurep/ztrends appear ac-curate and consistent.
Straight-line extrapolation of the"normal"p/ztrend used forG.
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pD-Gp DType Curve Approach: Case 3 (5/5)
Case 3 Anderson L Reservoir (South Texas (USA)) pD-Gp Dtype curve solution matched using field data.
Note the "tail" in thepDtrend for small values ofGp D(common field data event).
"Force matched" to the same results as each of the other plotting functions.
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Case 3 Anderson L (South Texas (USA))Literature standard case.
A 3-well reservoir, delimited by faults.
Good quality data.
Evidence of overpressure from static pressure tests.
Analysis: (Implemented using MS Excel)p/z-Gp
2 plotting functions.
-Gpperformance plots.
Gan analysis (2-straight line trends on a p/z-Gpplot).
pD-Gp Dtype curve approach.
Example Analysis Using MS Excel: Case 3
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Summary: (1/3)
Developed a new p/z-Gp2 material balance model for
the analysis of abnormally pressured gas reservoirs:
The -function is presumed (based on graphical
comparisons) to be either constant, or approximatelylinear with Gp. For the =constant case, we have:
where:
2)
1(1 pp
i
i GG
GGz
p
z
p ))((
1pippec
Gp
2pp
i
i GGz
p
z
p
i
i
z
p
G)
1(
i
i
z
p
G
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Base relation: p/z-Gp2 form of the gas material balance
a. P l o t t i n g F u n c t i o n 1:(quadratic)
b. P l o t t i n g F u n c t i o n 2:(linear)
c. P l o t t i n g F u n c t i o n 3:(quadratic)
ppp
pGdGzp
G
Gvs.)/(
0
1
pp
GzpG
vs.)/(1
pG
z
p
iz
ipzp vs.)/(
pp
p
p
GdGzpG
G
vs.2
)/(
0
1
ppp
p
GdGzpG
Gzp vs.)/(
0
1)/(
ppp
pp
GdGzpG
Gzp
Gvs.)/(
0
1)/(
1
2ppii GG
zp
zp
ii
zp
G)1(
ii
zp
G
d. P l o t t i n g F u n c t i o n 4 :(linear)
e. P l o t t i n g F u n c t i o n 5 :(quadratic)
f.P l o t t i n g F u n c t i o n 6:(linear)
Summary: (2/3)
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The plotting functions developed in this work havebeen validated as tools for the analysis reservoirperformance data from abnormally pressured gasreservoirs. Although the straight-line functions (PF2,PF4, and PF6) could be used independently, but werecommend a combined/simultaneous analysis.
The
-Gpplots are useful for checking data con-sistency and for guiding the selection of the -value.These plots represent a vivid and dynamic visualbalance of all of the other analyses.
The Gan analysis sequence is also useful for orient-
ing the overall analysis
particularly the ce(p)(pi-p)versus (p/z)/(pi/zi) plot.
ThepD-Gp Dtype curve is useful for orientationparticularly for estimating the or (D) value.
Summary: (3/3)
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Recommendations for Future Work:
Consider the extension of this methodology forcases of external drive energy (e.g., water influx, gasinjection, etc.).
Continue the validation of this approach by applyingthe methodology to additional field cases.
Implementation into a stand alone software.
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A Q u ad r a t ic C u m u l at i v e Pr o d u c t i o n
M o d el f o r t h e M a ter i al B al an c e o f A b n o r m a l l y - P r e s s u r e d G a s R e s e r v o i r s
F.E. Gonzalez, M.S. Thesis Defense
17 October 2003Department of Petroleum Engineering
Texas A&M University
College Station, TX 77843-3116