-
The Linkage of Subsurface Natural Fracture Predictions With Oil
Generation
Estimates -
M. K. Horn
-
Search and Discovery Article #40003 (1999)
*Adapted from a study in Basin History CD, which currently contains 640 worksheet based studies offered by AAPG Data Systems.
ABSTRACT
INTRODUCTION
THE STRESS HISTORY MODEL
THE
HYDROCARBON
GENERATION
MODEL
LINKING THE
HYDROCARBON
GENERATION
MODEL WITH THE OIL
GENERATION
MODEL: COMPUTATION OF FRACTURE OIL
INDEX (FOI)
THE UINTA BASIN AND ALTAMONT BLUEBELL
FIELD
ALTAMONT BLUEBELL RESULTS
COMPARISON OF UINTA RESULTS WITH A
GLOBAL SAMPLE
CONCLUSIONS
FIGURES
APPENDIX I
APPENDIX II
REFERENCES
The Uinta basin of Utah contains oil and gas
in fractured reservoirs. The Altamont-Bluebell field of this
basin is chosen in order to test a concept that could be used to
predict
hydrocarbon
-rich fractured reservoirs in, not only other
parts of the Uinta, but in basins in other parts of the world.
The premise of the concept is to
quantitatively predict the simultaneous occurrence of fracture
formation and
hydrocarbon
generation
. The
advantage of such a prediction is that early emplacement of
hydrocarbons in fractures enhances the probability of the said
fractures remaining open through time; therefore enhancing
reservoir potential. The early emplacement of hydrocarbons in
fractures inhibits post-fracture diagenetic healing. Also, fluid
pressures associated with the hydrocarbons would assist in
maintaining fracture permeability.
Two well-established models are used to a)
predict fracture formation as a function of burial history; and
b) predict
hydrocarbon
generation
also as a function of burial
history. The two models are combined to produce a unique
indicator, called the Fracture Oil Index or FOI. An FOI of less
than -1 is an indicator of
hydrocarbon
-rich fractures. Using
EXCEL spreadsheet formats, the calculated minimum FOI for the
Eocene Green River Formation in the Altamont-Bluebell field is
-58, which occurred 13 Ma at a burial depth of 5.73 km (18,800
ft). The -58 FOI ranks 62 out of 640 in technique-related global studies
carried out in 174 basins (60 studies yielded FOI’s less
than -58).
Natural fractures provide important reservoir targets (Nelson, 1985, Appendix I; Fritz et al, 1985; Chilingar et al, 1972; Hubbert and Willis, 1955; Daniel, 1944). From an oil and gas exploration standpoint, fracture permeability is a prime requisite: the loss of fracture permeability greatly reduces reservoir potential. Permeability can be greatly reduced by diagenetic material filling the width between the walls of fractures (Nelson, 1985, p. 30).
One possibility for keeping fractures open is the injection of hydrocarbons into the fracture space(s) at the time, or immediately after, the formation of the fractures. Hydrocarbons in pore and fracture spaces are known to inhibit post-depositional diagenetic effects such as quartz overgrowth formation.
The challenge, then, becomes the prediction of
the
hydrocarbon
generation
occurring more or less simultaneously,
through geologic time and at a specific locality, with natural
fracture formation.
What we propose is to use the methods of Hunt et
al (1991) to predict oil and gas
generation
potential and to
link this with the Narr and Currie’s (1982) stress analysis
predictor model. The resulting technique, utilizing EXCEL
spreadsheet solutions, breaks down into the following steps for
a specific locality:
1. Digitize and display the burial history of the target site.
2. If more than one burial history is provided at the target site, choose one candidate most probably linked to
hydrocarbon
source.
3. At the 1 km depth on the burial history curve, determine the corresponding geologic age. From the latter value (given as negative Ma for use in calculations), divide the total time to the present into 15 time segments. Read off the burial history curve the corresponding 15 paleo-depths.
4. From the paleo-depths, compute the paleo-temperature at each of the 15 stations. Use the present-day geothermal gradient for this computation if the paleo-temperature from other sources are not available.
5. Using the paleo-temperatures derived from 4 above, compute oil/gas
generation
curves for four activation energies, IIa Fast, IIB Medium Fast, IIC Medium, IID Slow (Hunt et al, 1991) at each of the fifteen stations. Also compute oil/gas
generation
curves at each of the fifteen stations using the Lopatin (1971) method.
6. At the exact same paleo-time stations, and again using the paleo-temperatures derived from 3 above, compute paleo-stresses using the Narr and Currie (1982) model.
7. In order to link the stress with
hydrocarbon
![]()
generation
, at each of the paleo-time stations, multiply the oil
generation
percent by the minimum horizontal effective stress. Use the "correct" activation energy (see 5 above), or the Lopatin solution, when activation energies are not available. The resulting (arbitrary and relative) index, called FOI, will be negative and large when the potential for oil/gas
generation
occurs more or less simultaneously with natural fracture formation.
The above steps will be carried in the
Altamont-Bluebell field area of the Uinta basin, Utah (Figure 1). Before we present these results,
let’s review the stress history and oil
generation
models
used in this study.
As rocks are buried, overburden weight causes stresses within the rock. Vertical stress can be "translated" into horizontal stresses, which may, in fact become extensional in nature. Extension leads to vertical fracture formation. Among the factors that cause variations in the state of stress within a rock are temperature changes, pore pressure, tectonic loading; and certain rock properties such as Young’s Modulus (rock rigidity) and Poisson’s ratio (used to relate horizontal stress components to vertical stress component) . These multitude of factors have been investigated and quantified by Narr and Curry (1982). Appendix I reviews the Narr and Curry stress history model in terms of stress prediction and related equations, and Figure 2 graphically displays some of their results. We are particularly interested in the minimum horizontal effective stress, sy.
Of interest in the Narr and Curry model is the non-reversabilty of certain processes as a rock goes through its burial - diagenesis - uplift cycle. For example, as rocks are uplifted from their deepest point of burial to shallower depths, rock rigidity cannot become "undone" - the maximum value of Young’s Modulus is imprinted and remains as such as uplift proceeds. These irreversible processes affect the stress burial history.
We have taken the equations of Appendix I and rewritten them in spreadsheet (EXCEL) format. They are then used as described in Step 6 of the introduction.
THE
HYDROCARBON
GENERATION
MODEL
The
hydrocarbon
generation
model used in this
study is that reported by Hunt et al in 1991. In this
model, the time and depth of oil
generation
from petroleum source
rocks containing
type
II kerogens are determined using
time-temperature index (TTI) calculations based on the Arrhenius
equation. Activation energies (E) and frequency factors (A) used
in the Arrhenius equation were obtained from hydrous pyrolysis
experiments.
Activation energies of standard kerogens vary
inversely with their sulfur content (Hunt et al, 1991).
The
kerogen
with the highest sulfur content has the lowest E
value and is the fastest in generating oil, whereas the
kerogen
with the lowest sulfur content has the highest E value and is the
slowest in generating oil. Hunt et al (1991) designated
kerogens as types IIA, B, C, and D on the basis of decreasing
sulfur content and corresponding increasing time-temperature
requirements for generating oil.
In our scheme, we use the E and A values in order
to compute and construct EXCEL worksheet graphs that define oil
generation
as a function of geologic time. The results are
reported within the range zero to 100 percent. Computed values
greater that 100 percent are assumed to be in the thermal gas
generation
range. We display five oil
generation
curves (on one
plot); Four of the five curves represent types IIA, B, C, and D;
the fifth curve represents the Lopatin (1971) solution. We use
Hunt et al’s (1991) equations 3 and 4 (shown as
equations 2 and 3 in Appendix II of this study). Figure 3 is an example display of our oil
generation
EXCEL solution.
The constants used in order to solve the equations of Appendix II are:
">(FREQUENCY FACTOR, 1/m.y.)IIA |
IIB |
IIC |
IID |
|||||
FAST |
M. FAST |
MEDIUM |
SLOW |
|||||
| S (ORG), %: | 1.1E+01 |
9.0E+00 |
7.4E+00 |
5.4E+00 |
(ORGANIC SULFUR) | |||
| E: | 1.4E+02 |
1.8E+02 |
2.0E+02 |
2.2E+02 |
(ACTIVATION ENERGY, kJ/mol)1 | |||
| A: | 7.0E+20 |
4.2E+23 |
1.5E+25 |
5.7E+26 |
(FREQUENCY FACTOR, 1/m.y.) | |||
| R: | 8.3E-03 |
|||||||
| R: | 8.3E-03 |
8.3E-03 |
8.3E-03 |
8.3E-03 |
(GAS CONSTANT) | |||
1. Divide by 4.184 to convert to Kcal/mol
Although
type
II kerogens are the major oil
generators in the world and were used to construct the
hydrocarbon
generation
model, we also use, in lieu of more
sophisticated data, the model for
Type
I kerogens. This, as will
be seen, pertains to the Uinta basin.
LINKING THE
HYDROCARBON
GENERATION
MODEL WITH THE OIL
GENERATION
MODEL: COMPUTATION OF
FRACTURE OIL INDEX (FOI)
Fracture Oil Index (FOI) is defined as the
product of minimum horizontal effective stress sy and oil
generation
percent
(Horn, 1995). An FOI of less than -1.0 is an indicator of
hydrocarbon
fracture potential. In our EXCEL solution, the
calculation is made 15 times, at each of the previously described
time stations on the burial history curve.
THE UINTA BASIN AND ALTAMONT-BLUEBELL FIELD
Typical of foredeep basins world-wide, the Uinta basin of Utah (Figure 1) is asymmetrical, with the basin depocenter lying close to the northern buttressed end of the basin. Depths reach 20,000 ft (6095 m) in the basin depocenter.
Uinta basin was created by the indentation of the Colorado Plateau into the North American craton during the Laramide plate movements (Harthill and Bates, 1996). Postdepositional shift of the structural axis of the basin in late Tertiary time produced a regional updip pinchout of northerly derived sandstones into a lacustrine "oil-shale" sequence (Lucas and Drexler, 1976). Fracture directions are N15°-50°W. At the Altamont-Bluebell field,VSP surveys defined N35°W as the open fracture direction (Harthill and Bates, 1996).
In the Uinta basin, the term oil shale
refers to fine-grained rock that contains a large amount of
organic material. (Sweeney et al, 1987). Strata of the
Green River Formation were formed in a lacustrine environment
that began in the middle to late Paleocene and reached maximum
extent in middle Eocene time. Varves that can be traced over
kilometers contain organic and inorganic matter deposited in
yearly cycles. The organic material is mostly amorphous
kerogen
derived from the lipid fraction of lake algae and from
terrestrial spores and pollen (Yen, 1976). This
kerogen
is a
classic example of a
Type
I
kerogen
in the classification scheme
of Tissot and Welte (1978).
Altamont Bluebell reservoirs occur on the gently dipping southern limb of the Uinta basin. Production occurs in the Eocene Green River - Wasatch section and Paleocene Flagstaff Limestone between depths of 7,875 and 16,735 ft (2,400 and 5,100 m). The producing interval is up to 2,300 ft (700 m) thick. Reservoir rocks are predominantly low-porosity, fine-grained sandstone, siltstone, and carbonate. The reservoir is substantially overpressured; the ratio of fluid pressure to overburden weight locally exceeds values of 0.8, and values in excess of 0.6 occur over an area greater than 772 mi2 (2,000 km2) (Lucas and Drexler, 1976, Narr and Currie 1982). Structural closure plays no part in entrapment of hydrocarbons at Altamont-Bluebell; regional dip provides the setting for updip porosity pinchouts. Fractures in the reservoirs of essential for commercial flow rates. The reservoirs are essentially self-sourcing (Figure 4) with migration paths dependent upon fracture clusters. Initial well productivities were at flow rates up to 5,000 bbl/day with gas/oil ratios ranging from 1,500 cu ft/bbl (4,250 m3/bbl) in the updip part of the field to 500 cu ft/bbl (1,415 m3/bbl) downdip. Reservoir drive mechanism is liquid expansion-solution gas (Lucas and Drexler, 1964). In 1955 Carter No. 2 Bluebell Unit discovered gas (5.37 million cu ft/day) in sandstone in the Green River Formation (Osmond et al, 1968).
We shall now repeat the seven steps presented in the introduction, applied directly to the Shell 1-11B4 Brotherson well, Altamont-Bluebell field, Utah.
1. Digitize and display the burial history of the target site.
Figure 5 represents the EXCEL-graphed burial history, derived from a scanned image of Figure 11 of Sweeney et al (1987). The burial history represents the Shell 1-11B4 Brotherson well.
2. If more than one burial history is provided at the target site, choose the candidate most probably linked to
hydrocarbon
source.
The Eocene burial history curve is chosen.
3. At the 1 km depth on the burial history curve for the candidate source, determine the corresponding geologic age. From the latter value, divide the total time to the present into 15 time segments. Read from the burial history curve the corresponding paleo-depths. Note that for purposes of calculation, time values are given in -Ma.
TIME |
TIME |
DEPTH |
DEPTH |
START |
FINISH |
START |
FINISH |
Ma |
Ma |
Km |
Km |
-50.0 |
-47.0 |
-1.01 |
-1.45 |
-47.0 |
-43.0 |
-1.45 |
-2.64 |
-43.0 |
-40.0 |
-2.64 |
-3.83 |
-40.0 |
-37.0 |
-3.83 |
-4.48 |
-37.0 |
-33.0 |
-4.48 |
-5.11 |
-33.0 |
-30.0 |
-5.11 |
-5.70 |
-30.0 |
-27.0 |
-5.70 |
-5.73 |
-27.0 |
-23.0 |
-5.73 |
-5.73 |
-23.0 |
-20.0 |
-5.73 |
-5.73 |
-20.0 |
-17.0 |
-5.73 |
-5.73 |
-17.0 |
-13.0 |
-5.73 |
-5.73 |
-13.0 |
-10.0 |
-5.73 |
-5.68 |
-10.0 |
-7.0 |
-5.68 |
-5.13 |
-7.0 |
-3.0 |
-5.13 |
-4.40 |
-3.0 |
0.0 |
-4.40 |
-3.83 |
4. From the paleo-depths, compute the paleo-temperature at each of the 15 stations. Detailed analysis of temperature data by Chapman et al (1984) provides an estimate of 25°C/km for the present-day geothermal gradient in the Uinta basin. Sweeney et al (1987) assumed that the geothermal gradient from the Tertiary to the present has been constant, and they ignored localized effects on thermal gradient by factors such as overpressuring, lithologic variation, and hydrothermal circulation. A value of 10°C is chosen for the long-term average surface temperature.
TIME |
TIME |
DEPTH |
DEPTH |
TEMP |
TEMP. |
START |
FINISH |
START |
FINISH |
START |
FINISH |
Ma |
Ma |
Km |
Km |
C |
C |
-50 |
-47 |
-1.01 |
-1.45 |
35 |
46 |
-47 |
-43 |
-1.45 |
-2.64 |
46 |
76 |
-43 |
-40 |
-2.64 |
-3.83 |
76 |
106 |
-40 |
-37 |
-3.83 |
-4.48 |
106 |
122 |
-37 |
-33 |
-4.48 |
-5.11 |
122 |
138 |
-33 |
-30 |
-5.11 |
-5.70 |
138 |
153 |
-30 |
-27 |
-5.70 |
-5.73 |
153 |
153 |
-27 |
-23 |
-5.73 |
-5.73 |
153 |
153 |
-23 |
-20 |
-5.73 |
-5.73 |
153 |
153 |
-20 |
-17 |
-5.73 |
-5.73 |
153 |
153 |
-17 |
-13 |
-5.73 |
-5.73 |
153 |
153 |
-13 |
-10 |
-5.73 |
-5.68 |
153 |
152 |
-10 |
-7 |
-5.68 |
-5.13 |
152 |
138 |
-7 |
-3 |
-5.13 |
-4.40 |
138 |
120 |
-3 |
0 |
-4.40 |
-3.83 |
120 |
106 |
5. Using the paleo-temperatures derived from 4 above, compute oil/gas
generation
curves for four activation energies, IIa Fast, IIB Medium Fast, IIC Medium, IID Slow (Hunt et al, 1991) at each of the fifteen stations. Also compute oil/gas
generation
curves at each of the fifteen stations using the Lopatin (1971) method.
A table of the results for the four activation energies and the Lopatin solution follows:
TIME |
DEPTH |
TEMP. |
% OIL |
% OIL |
% OIL |
% OIL |
% OIL |
FINISH |
FINISH |
FINISH |
IIA |
IIB |
IIC |
IID |
LOPA- |
Ma |
Km |
C |
FAST |
M. FAST |
MEDIUM |
SLOW |
TIN |
-47 |
-1.45 |
46.2 |
0.3 |
0.0 |
0.0 |
0.0 |
0.0 |
-43 |
-2.64 |
76.1 |
20.1 |
0.1 |
0.0 |
0.0 |
0.1 |
-40 |
-3.83 |
105.7 |
100.0 |
6.0 |
0.2 |
0.0 |
0.7 |
-37 |
-4.48 |
121.9 |
100.0 |
70.3 |
4.0 |
0.8 |
5.0 |
-33 |
-5.11 |
137.7 |
100.0 |
100.0 |
47.2 |
13.9 |
20.9 |
-30 |
-5.70 |
152.6 |
100.0 |
100.0 |
98.9 |
71.3 |
47.4 |
-27 |
-5.73 |
153.4 |
100.0 |
100.0 |
100.0 |
98.4 |
83.3 |
-23 |
-5.73 |
153.4 |
100.0 |
100.0 |
100.0 |
100.0 |
96.7 |
-20 |
-5.73 |
153.4 |
100.0 |
100.0 |
100.0 |
100.0 |
99.0 |
-17 |
-5.73 |
153.4 |
100.0 |
100.0 |
100.0 |
100.0 |
99.7 |
-13 |
-5.73 |
153.4 |
100.0 |
100.0 |
100.0 |
100.0 |
99.9 |
-10 |
-5.68 |
152.1 |
100.0 |
100.0 |
100.0 |
100.0 |
100.0 |
-7 |
-5.13 |
138.2 |
100.0 |
100.0 |
100.0 |
100.0 |
100.0 |
-3 |
-4.40 |
119.9 |
100.0 |
100.0 |
100.0 |
100.0 |
100.0 |
0 |
-3.83 |
105.7 |
100.0 |
100.0 |
100.0 |
100.0 |
100.0 |
In the Sweeney et al (1987) kinetic model,
which applies only to Green River Shale, an activation energy of
52.4 kcal/mole (219.24 kJ/mol) was determined. This value
corresponds very closely to the SLOW oil
generation
data (E = 220
kJ/mol).
6. At the exact same paleo-time stations, and again using the paleo-temperatures derived from 4 above, compute paleo-stresses using the Narr and Currie (1982) model.
The factors that enter into a stress history calculation and their minimum and maximum values for the Altamont-Bluebell field are summarized in the following table:
PARAMETER |
MINIMUM |
MAXIMUM |
COMMENTS |
PALEO-DEPTH (KM) |
-1.45 |
-5.73 |
|
YOUNG’S MODULUS, E |
16,913 |
66,905 |
Represents rock rigidity. |
POISSON’S RATIO, n |
0.259 |
0.402 |
Relates vertical stress to horizontal stresses. |
ROCK DENSITY, r |
2.14 |
2.57 |
|
COEFFICIENT OF THERMAL EXPANSION, a |
3.58E-06 |
5.29E-06 |
|
VERTICAL TOTAL STRESS, Sz, MPa |
30 |
145 |
|
FLUID PRESSURE GRADIENT, MPa/m |
0.010 |
0.020 |
Table 1 of Narr and Currie, 1982. Represents overpressured section. |
FLUID PRESSURE, P, MPa |
14.5 |
114.7 |
|
PALEO TEMPERATURE, °C |
35.2 |
153.4 |
|
MAXIMUM HORIZONTAL REGIONAL STRAIN, ex |
1.0E-03 |
1.0E-03 |
|
MINIMUM HORIZONTAL REGIONAL STRAIN, ey |
0.0 |
0.0 |
|
MAXIMUM EFFECTIVE HORIZONTAL STRESS, sx |
-5.20 |
38.22 |
|
MINIMUM EFFECTIVE HORIZONTAL STRESS, sy |
-58.34 |
11.40 |
Used to Calculate Fracture Oil Index. |
7. In order to link the stress with
hydrocarbon
![]()
generation
, at each of the paleo-time stations, multiply the oil
generation
percent by the minimum horizontal effective stress. Use the "correct" activation energy (see 5 above), or the Lopatin solution, when activation energies are not available. The resulting (arbitrary and relative) index, called FOI, will be negative and large when the potential for oil/gas
generation
occurs more or less simultaneously with natural fracture formation.
As pointed out in 5 above, In the Sweeney et
al (1987) kinetic model, which applies only to Green River
Shale, an activation energy of 52.4 kcal/mole (219.24 kJ/mol) was
determined. This value corresponds very closely to the SLOW oil
generation
data (E = 220 kJ/mol). Therefore, IID activation data
are used to calculate the FOI:
TIME |
DEPTH |
TEMP. |
% OIL |
Min. eff. |
|
FINISH |
FINISH |
FINISH |
IID |
horizontal |
FOI |
Ma |
Km |
C |
SLOW |
stress |
% |
-47 |
-1.45 |
46.2 |
0.0 |
10.84 |
0.0 |
-43 |
-2.64 |
76.1 |
0.0 |
11.40 |
0.0 |
-40 |
-3.83 |
105.7 |
0.0 |
4.44 |
0.0 |
-37 |
-4.48 |
121.9 |
0.8 |
-4.45 |
-0.0 |
-33 |
-5.11 |
137.7 |
13.9 |
-15.79 |
-2.2 |
-30 |
-5.70 |
152.6 |
71.3 |
-29.20 |
-20.8 |
-27 |
-5.73 |
153.4 |
98.4 |
-35.39 |
-34.8 |
-23 |
-5.73 |
153.4 |
100.0 |
-41.13 |
-41.1 |
-20 |
-5.73 |
153.4 |
100.0 |
-46.87 |
-46.9 |
-17 |
-5.73 |
153.4 |
100.0 |
-52.60 |
-52.6 |
-13 |
-5.73 |
153.4 |
100.0 |
-58.34 |
-58.3 |
-10 |
-5.68 |
152.1 |
100.0 |
-57.77 |
-57.8 |
-7 |
-5.13 |
138.2 |
100.0 |
-51.64 |
-51.6 |
-3 |
-4.40 |
119.9 |
100.0 |
-43.61 |
-43.6 |
0 |
-3.83 |
105.7 |
100.0 |
-37.44 |
-37.4 |
Figure 6 is a plot of
the FOI. As presented above, a FOI of less than -1.0 is an
indicator of
hydrocarbon
fracture potential. According to this
model, simultaneous and effective oil
generation
and fracture
formation began about 40 Ma at Altamont-Bluebell.
COMPARISON OF UINTA RESULTS WITH A GLOBAL SAMPLE
In terms of a relative comparison of FOI from the Uinta Altamont-Bluebell area with a global sample, Figure 7 represents the frequency distribution from 640 case studies distributed in 174 basins. The Altamont-Bluebell example indicates a minimum FOI of -58.3. In the global sample, there are only 61 studies with a FOI less than that found at Altamont-Bluebell. The basins in which the 60 case studies yielded values of less than -58 are:
ALBERTA
ANADARKO
APPALACHIAN
ARABIAN
BENI
CALTANISETTA
CAMPOS
CHACO
GULF COAST
GULF OF VENEZUELA
ILLINOIS
KURA
LOS ANGELES
MARACAIBO
MIDDLE AMAZON
MINCH
NORTH SEA, NORTH
NORTH SEA, SOUTH
PERMIAN
PICEANCE
PO
RATON
RHONE FAN
RIO GRANDE
SACRAMENTO/SAN JOAQUIN
SAN JORGE
SOUTH ADRIATIC
TARANAKI
TARIM
TRANSYLVANIAN
TRINIDAD-TOBAGO
UCAYALI - HUALLAGA
UINTA
VENTURA/ SANTA BARBARA
VIENNA
WEST SIBERIAN
WESTERN OVERTHRUST / BASIN & RANGE
ZAGROS
ZHUNGEER (JUNGGAR)
1. The fact that the Uinta basin of Utah contains
oil and gas in fractured reservoirs makes it an ideal choice
location to test a concept that could be used to predict
hydrocarbon
-rich fractured reservoirs not only in other parts of
the Uinta but also in basins in other parts of the world.
2. One can quantitatively predict the
simultaneous occurrence of fracture formation and
hydrocarbon
generation
. Such a situation heightens the
probability of the fractures remaining open through time,
therefore enhancing reservoir potential.
3. Two well-established models can be used to a)
predict fracture formation as a function of burial history and b)
predict
hydrocarbon
generation
also as a function of burial
history.
4. The two models can be combined to produce a
unique indicator, called the Fracture Oil Index or FOI. An FOI of
less than -1 is an indicator of
hydrocarbon
-rich fractures.
5. Using EXCEL spreadsheet formats, the calculated minimum FOI for the Eocene Green River Formation in the Altamont-Bluebell field is -58, which occurred 13 Ma at a burial depth of 5.73 km (18,800 ft). The -58 FOI ranks 62 out of 640 in technique-related global studies carried out in 174 basins (60 studies yielded FOI’s less than -58).