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AV Direct Method for Determining Organic Shale Potential from Porosity and Resistivity Logs to Identify Possible Resource Plays* Thomas Bowman 1 Search and Discovery Article #110128 (2010) Posted June 14, 2010 *Adapted from oral presentation at session, Genesis of Shale Gas--Physicochemical and Geochemical Constraints Affecting Methane Adsorption and Desorption, at AAPG Annual Convention, New Orleans, LA, April 11-14, 2010 1 Mantle Oil & Gas, LLC ([email protected]) Abstract Today many geoscientists are faced with identifying possible resource plays throughout the world. Determination of potential organic content of the shale sections is one of the first estimations that is often made, and time and again there is a lack of information readily and inexpensively available to make these preliminary estimates. As Passey (AAPG, 1990) and others have shown, there are several methods that can be used to determine the organic content by interpretation of various electric logs. One such method, referred to as the Δ log R technique, used for identifying and calculating total organic carbon in organic-rich rocks can be quickly estimated by the improvement of cross-plotting sonic logs (DT) and log (natural logarithm) of resistivity data and determining the shale line that can then be used to calculate a pseudo-sonic log that is then displayed over the existing sonic logs to determine the organic shale potential for a zone in an individual well. In water- saturated, organic-lean rocks, the two curves parallel each other and allow the shale calculation line to be determined. However, in either hydrocarbon reservoir rocks or organic-rich shale sections a separation between the curves occur. Using the gamma-ray curve, reservoir intervals can be identified and eliminated from the analysis. The separation in organic-rich intervals results from two effects: the porosity curve responds to the presence of low-density, low-velocity kerogen, and the resistivity curve responds to the formation fluid. In mature source rocks the magnitude of the resistivity increases because of the presence of generated hydrocarbons. By cross-plotting multiple wells this technique can provide relative information for an area or entire shale section. This method requires little more than a simple cross-plot and log calculation mathematics to provide a geoscientist sufficient data to easily and quickly determine potential organic shale sections. Across an area, these log cross-plot displays support the correlation and mapping of organic-rich shale sections and allow the geoscientist to quickly determine high graded areas of focus for further study. This method allows organic richness to be assessed in a wide variety of lithologies and maturities using common well logs and has been applied to many of the North American shale plays, such as the Barnett, Woodford, Eagle Ford and Marcellus shales. Copyright © AAPG. Serial rights given by author. For all other rights contact author directly.

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Page 1: source rock from logs AAPG.pdf

AVDirect Method for Determining Organic Shale Potential from Porosity and Resistivity Logs to Identify Possible

Resource Plays*

Thomas Bowman1

Search and Discovery Article #110128 (2010)

Posted June 14, 2010 *Adapted from oral presentation at session, Genesis of Shale Gas--Physicochemical and Geochemical Constraints Affecting Methane Adsorption and Desorption, at AAPG Annual Convention, New Orleans, LA, April 11-14, 2010 1Mantle Oil & Gas, LLC ([email protected])

Abstract

Today many geoscientists are faced with identifying possible resource plays throughout the world. Determination of potential organic content of the shale sections is one of the first estimations that is often made, and time and again there is a lack of information readily and inexpensively available to make these preliminary estimates. As Passey (AAPG, 1990) and others have shown, there are several methods that can be used to determine the organic content by interpretation of various electric logs. One such method, referred to as the Δ log R technique, used for identifying and calculating total organic carbon in organic-rich rocks can be quickly estimated by the improvement of cross-plotting sonic logs (DT) and log (natural logarithm) of resistivity data and determining the shale line that can then be used to calculate a pseudo-sonic log that is then displayed over the existing sonic logs to determine the organic shale potential for a zone in an individual well. In water-saturated, organic-lean rocks, the two curves parallel each other and allow the shale calculation line to be determined. However, in either hydrocarbon reservoir rocks or organic-rich shale sections a separation between the curves occur. Using the gamma-ray curve, reservoir intervals can be identified and eliminated from the analysis. The separation in organic-rich intervals results from two effects: the porosity curve responds to the presence of low-density, low-velocity kerogen, and the resistivity curve responds to the formation fluid. In mature source rocks the magnitude of the resistivity increases because of the presence of generated hydrocarbons. By cross-plotting multiple wells this technique can provide relative information for an area or entire shale section. This method requires little more than a simple cross-plot and log calculation mathematics to provide a geoscientist sufficient data to easily and quickly determine potential organic shale sections. Across an area, these log cross-plot displays support the correlation and mapping of organic-rich shale sections and allow the geoscientist to quickly determine high graded areas of focus for further study. This method allows organic richness to be assessed in a wide variety of lithologies and maturities using common well logs and has been applied to many of the North American shale plays, such as the Barnett, Woodford, Eagle Ford and Marcellus shales.

Copyright © AAPG. Serial rights given by author. For all other rights contact author directly.

Page 2: source rock from logs AAPG.pdf

Meissner, F.F., 1978, Petroleum geology of the Bakken Formation, Williston Basin, North Dakota and Montana in Montana Geological Society, The Economic geology of the Williston Basin; Montana, North Dakota, South Dakota, Saskatchewan, Manitoba, p. 207-227. Meyer, B.L., and M.H. Nederlof, 1984, Identification of source rocks on wireline logs by density/resistivity and sonic transit/resistivity crossplots: AAPG Bulletin, v. 68, p. 121-129. Nixon, R.P., 1973, Oil Source Beds in Cretaceous Mowry Shale of Northwestern Interior United States: AAPG Bulletin, v. 57/1, p. 136-157. Passey, Q.R., S. Creaney, J.B. Kulla, F.J. Moretti, and J.D. Stroud, 1990, A practical model for organic richness from porosity and resistivity logs: AAPG Bulletin, v. 74, p. 1777-1794. Philippi, G. T., 1968, Essentials of the petroleum formation process are organic source material and a subsurface temperature controlled chemical reaction mechanism, in Advances in organic geochemistry: Oxford, Pergamon Press, p. 25-46. Schmoker, J.W., 1981, Determination of organic-matter content of Appalachian Devonian shales from gamma-ray logs: AAPG Bulletin, v. 65/7, p. 1285-1298.

References

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Theme VIII: Genesis of Shale Gas – Physicochemical and Geochemical Constraints Affecting Methane Adsorption and Desorption

Direct Method for Determining Organic Shale Potential from Porosity and Resistivity Logs to

Identify Possible Resource PlaysT. Bowman

Mantle Oil & Gas, LLC

AAPGAnnual Convention & Exhibition

New Orleans, April 2010

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• Theory – determine where potential TOC is located using a

relatively simple calculation method.

• Methods – Modified ΔlogR Technique using Cross Plots

• Examples – Various US shale plays

• Conclusion – Observed information

AAPGAnnual Convention & ExhibitionNew Orleans, April 2010

Outline

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• Passey, Q. R., S. Creaney, J. B. Kulla, F. J. Moretti

and J. D. Stroud, 1990, A practical model for organic richness from porosity and resistivity logs: AAPG Bulletin, V. 74, P 1777-1794.

• Meyer, B. L., and M. H. Nederlof, 1984, Identification of source rocks on wireline logs by density/resistivity and sonic transit/resistivity crossplots: AAPG Bulletin, V. 68, P 121-129.

Methods - References

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MATRIXW

AT

ER

NON-SOURCE

SOLID Φ

MATRIX

WA

TE

R

IMMATURE SOURCE

SOLID Φ

ORGANIC MATTER

MATRIX

WA

TE

R

MATURE SOURCE

SOLID Φ

ORGANIC MATTER

Mature Source Rocks – As a Source Rock Matures, a portion ofthe solid organic matter is transformed to liquid or gaseoushydrocarbons which move into the pore space, displacing theformation water.*

*After Philippi (1968), Nixon (1973) and Meissner (1978)

Source Rock Composition

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• Source Rocks - shales and lime-mudstones containingsignificant amounts of organic matter.

• Non-Source Rocks - also contain small amounts of organicmatter (< 1 wt. %).

• Organic-rich sediments have a higher resistivity than organic-lean sediments

•Organic-rich rocks - increase in sonic transit time and an increase in resistivity

• Organic-rich rocks can be relatively highly radioactive (higher gamma-ray reading than ordinary shales and limestones) Schmoker, 1981

Hypothesis

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After Passey et al. (1990)

Schematic guide for the interpretation of a wide variety of features observed on Δ log R overlays

Schematic of Δ log R Response

NON SOURCE

IMMATURE SOURCE

RESERVOIR

NON SOURCE

MATURE SOURCE

HIGH Φ RESERVOIR

“COALY”

COALS

NON SOURCE

TIGHT

LOW Φ RESERVOIR

INTERPRETATIONSONIC (---) / RESISTIVITY (-)GR

150 100 50

Δ log R0 1

Δ T (µsec/ft)

Δ log R

WATER

WATER

GAS OR OIL

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Passey Method In Practice

SP-100 40.0

GR0.00 150

ILD(AIT90)0.20 2000

6500

6600

6700

6800

6900

7000

7100

7200

7300

7400

7500

9.625

5.5

-6129 403MBLF

-6504 354BRNT

-5800.00

-5900.00

-6000.00

-6100.00

-6200.00

-6300.00

-6400.00

-6500.00

-6600.00

-6700.00

-6800.00

-5800.000

-5900.000

-6000.000

-6100.000

-6200.000

-6300.000

-6400.000

-6500.000

-6600.000

-6700.000

-6800.000

MINT CREEK 2H424393097700

-5800.00

-5900.00

-6000.00

-6100.00

-6200.00

-6300.00

-6400.00

-6500.00

-6600.00

-6700.00

-6800.00

DT120 20.0

9.625

5.5

-6129 403MBLF

-6504 354BRNT

-5800.00

-5900.00

-6000.00

-6100.00

-6200.00

-6300.00

-6400.00

-6500.00

-6600.00

-6700.00

-6800.00

-5800.000

-5900.000

-6000.000

-6100.000

-6200.000

-6300.000

-6400.000

-6500.000

-6600.000

-6700.000

-6800.000

MINT CREEK 2H424393097700

-5800.00

-5900.00

-6000.00

-6100.00

-6200.00

-6300.00

-6400.00

-6500.00

-6600.00

-6700.00

-6800.00

10 100 90 40

Scale Sonic and Resistivity where 50 µsec/ft equal to 1 decade Resistivity (ohm-m)Δ log R

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Modified Procedure

1. Calculate LogR of all Resistivity logs2. Cross-Plot LogR vs Sonic (DT)*3. Determine low Resistivity Shale line4. Calculate new Sonic (pseudo-sonic

DtR) from Shale line [DtR=b-m*LogR]

5. Overlay pseudo-sonic (DtR) over sonic6. Highlight cross over of pseudo-sonic

with DT7. Interpret Organic shale section

*Use Porosity log in place of DT

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-1 -0.5 0 0.5 1 1.5 2 2.5 3 3.5 4

54

63

72

81

90

99

108

117

126

135

LOGR

DT

Log Data: MINT CREEK(2H), Untitled1: DT vs. LOGR

DT = 100.538828 - 25.1536122*LOGR

Log R

DT

Shale LineDtR=105-25*LogR

Shale Play

Cross Plot AnalysisBarnett Core (Mississippian)

Fort Worth Basin

Carbonates

1 Decade Resistivity

50 µ

sec/

ft

PasseyΔ Log R

Slope

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Conclusions

1. Organic-rich sediments have a higher resistivity than organic-lean sediments

2. Organic-rich rocks - increase in sonic transit time and an increase in resistivity

3. Organic-rich rocks can be relatively highly radioactive (higher gamma-ray reading than ordinary shales and limestones)

4. The ΔLogR cross plot is a quick and easy determination of resource

5. Word of Warning

Page 34: source rock from logs AAPG.pdf

Thank You