 Click to view presentation in PDF format.
  
Click to view presentation in PDF format.
 
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                             |   
         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). Return
      to top.
       |