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Delineation of
a Diagenetic Trap Using P-Wave and Converted-Wave Seismic Data in the Miocene
McLure Shale, San Joaquin Basin, California*
By
Robert Kidney1, John Arestad2, Anne Grau1,
and Robert Sterling1
Search and Discovery Article #20012 (2003)
*Adapted from an oral presentation at the AAPG’s annual convention, 2003, Salt
Lake City, Utah, May, 2003. A companion article, entitled
“Success!
Using Seismic Attributes and Horizontal Drilling to Delineate and Exploit a Diagenetic Trap, Monterey Shale, San Joaquin Valley, California,” is
Search and Discovery Article #20011 (2003).
1EOG Resources, Inc, Denver, CO
([email protected])
2ExplorTech, Littleton, CO
Abstract
North Shafter and
Rose oil fields, located in California’s San Joaquin Basin, produce hydrocarbons
from a subtle stratigraphic trap within the Miocene Monterey Formation. The
trap-reservoir system was created during the burial process of a thick
diatomaceous shale sequence that forms various diagenetic facies. Integration of
well and 2-D p-wave seismic data shows that a significant amplitude anomaly is
present over both the reservoir (quartz) and seal (Opal-CT) facies, making
delineation of the updip edge problematic. The porosity of the Opal-CT and
reservoir quartz facies ranges from 50% to 24%.
From petrophysical analysis and seismic modeling the following conclusions can
be drawn. The Opal-CT and hydrocarbon-saturated quartz have nearly the same
acoustic impedance. The Opal-CT is low density while the hydrocarbon-saturated
quartz is low velocity. The presence of gas-saturated oil in the quartz reduces
the interval velocity in a manner similar to the Gassmann effect in high
porosity sandstones. The down-dip wet quartz interval is not associated with a
seismic amplitude anomaly since its impedance is similar to the bounding shales.
Finally, converted-wave data, which primarily images lithology rather than
fluids, can be used to delineate the low density Opal-CT from the higher density
quartz.
Based on the above
conclusions, 2-D converted-wave data were acquired to complement the p-wave
data. From these data sets the regional Opal-CT to quartz phase transformation
boundary was mapped and a matrix of amplitude signatures versus facies was
constructed. This work then formed the basis for mapping the hydrocarbon
saturated quartz facies.
uAbstract
uFigures
captions
uRock
properties & seismic attributes
uDiscrimination
of lithology & fluid type
uSeismic
anomaly
uAbstract
uFigures
captions
uRock
properties & seismic attributes
uDiscrimination
of lithology & fluid type
uSeismic
anomaly
uAbstract
uFigures
captions
uRock
properties & seismic attributes
uDiscrimination
of lithology & fluid type
uSeismic
anomaly
uAbstract
uFigures
captions
uRock
properties & seismic attributes
uDiscrimination
of lithology & fluid type
uSeismic
anomaly
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Figure
2. Cross plotting density vs. sonic identifies pay on wells logs--but
not on seismic.
Typical values in oil reservoir are 150
msec/ft
(sonic) and 2.00 gm/cc (density).
Figure
3. Tie of seismic attributes to rock properties. Seismic anomaly
reflects change in fluid content and change in mineralogy.
Figure
4. Gassmann effect (reduction of interval velocity in quartz section
with
gas-saturated oil), shown by P-wave/S-wave plot.
Figure
5. P- and S- wave seismic modeling, with Gassman effect in the P-wave
model, which shows both mineralogical and fluid effects, while only the
mineralogical changes are shown in the S-wave model.
Figure
6. P- and C- wave seismic program developed for Rose / North Shafter
development.
Figure
7. Seismic lithology discrimination: Lower interval, North Shafter
Field, with P-wave seismic showing Gassman effect and C-wave seismic
showing the change in mineralogy.
Figure
8. Seismic lithology discrimination: Lower interval, North Shafter
Field. Both P-wave and C-wave show only the change in mineralogy.
Figure
9. Regional
conversion in lower interval of opal CT to quartz on P-wave and C-wave
seismic profiles. The two lines are from North Shafter Field and the
northern boundary of North Shafter Field.
Figure
11. Seismic profile, illustrating that an amplitude map necessarily is a
composite of both upper and lower intervals.
Figure
12. Seismic profiles (top profile from Rose Field and lower profile from
North Shafter Field), demonstrating that amplitudes downdip from the
regional are the anomalies.
(Figures
1,
2,
3,
4 and 5)
An
integrated study of the Miocene Monterey Formation in the San Joaquin
Basin resulted in discovery of oil in its McLure Member and in the
subsequent development of North Shafter and Rose oil fields (Figure
1). Integration of density vs. sonic data from well logs with
2-D (P-wave) seismic data does not delineate the reservoir from the
updip seal. The two corresponding reservoir and trap facies
(hydrocarbon-bearing quartz and Opal-CT, respectively) have essentially
the same impedance (velocity x density). On the other hand, the
impedance of the downdip, water-bearing quartz stratigraphic section is
similar to that of the bounding shales.
(Figures
5,
6,
7,
8,
9 and 10)
Planning of a seismic program (Figure
6) subsequent to seismic modeling (Figure
5) of P- and S- wave data focused on discriminating lithology
and fluid type, given the following:
Opal-CT stratigraphic section is low-density.
Hydrocarbon-saturated, quartz section has low velocity.
C(converted)-wave data images lithology rather than fluids.
Data from the seismic program shows that the gas-saturated
oil in the quartz section in both an upper and a lower interval reduces
the interval velocity in a similar fashion to the Gassmann effect in
sandstones with high porosity (Figures
4
and 5). There is no seismic
anomaly associated with the water-bearing quartz section in both
intervals. Converted-wave data delineates the Opal-CT section (with low
density) from the quartz section (with higher density).
In
effect, the P-wave data define the downdip water-bearing interval, and
the converted-wave data defines the updip diagenetic seal formed by the
Opal-CT interval (Figures
7,
8,
9, and 10).
The region
in between these two areas is the hydrocarbon-bearing reservoir
interval.
(Figures
1,
11, and
12)
Amplitude anomalies of the upper interval and the lower interval are
downdip from the regional (Figures
11 and
12). The seismic-anomaly map (Figure 1) presents a composite of
both intervals (Figure 12).
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