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Bode Omoboya 16 th May, 2013 1 Introduction Bakken Shale Case Study Barnett Shale Case Study Other Forward Modeling Projects

Field and Physical Modeling Study of the Bakken Formation

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Page 1: Field and Physical Modeling Study of the Bakken Formation

Bode Omoboya

16th May, 2013

1

Introduction

Bakken Shale Case Study

Barnett Shale Case Study

Other Forward Modeling Projects

Page 2: Field and Physical Modeling Study of the Bakken Formation

VTI Anisotropy

Isotropic or HTI

Anisotropy

Due Open

Vertical

Fractures

VTI Anisotropy

Geologic Age Upper Devonian

/Lower Miss

Lithology

(Middle Member)

Sandstone

/Siltstone

/Dolomite

Total Area (sq mi) 200000

Total Gas (tcf) 945

Producable Gas (tcf) 20

Depth (feet) 10000

Thickness (feet) 150

Pressure (psi) 5600

Porosity (%) 5

Matrix Permeability

(nD)

10000

Pressure Gradient

(psi/ft)

0.5

Clay Content (Middle

Member %)

5

Average Horz Well

Cost ($M)

5.5

Most oil in the Bakken

petroleum system resides in

open fractures in the Middle

Member (Pitman et al, 2001). Source: USGS 2

Page 3: Field and Physical Modeling Study of the Bakken Formation

MD= 9100 ft

MD= 9250 ft

3 Well: NELSON

Upper Shale

Middle Member

Lower Shale

Core Image from NDIC

Page 4: Field and Physical Modeling Study of the Bakken Formation

𝐼𝐺𝑅 =𝐺𝑅𝑙𝑜𝑔 − 𝐺𝑅𝑚𝑖𝑛

𝐺𝑅𝑚𝑎𝑥 − 𝐺𝑅𝑚𝑖𝑛

1000 ft. Interval 40% – 60% Vsh

200 ft. Interval 80% Vsh

𝑉𝑠ℎ =𝐼𝐺𝑅

3 − 2𝐼𝐺𝑅

Steiber, 1970

4 Data Courtesy of Hess Corporation

Page 5: Field and Physical Modeling Study of the Bakken Formation

X/D=1 4500ft (offset)

V=3000ft/s V=16000ft/s

t=700 ms

t=1800 ms X= 0 ft X= 15000 ft

5

C11 C33

C44

C66

C13

e g d

343 227 54 106 107 0.255 0.481 -0.051

𝞰 from Core = 0.341 𝞰 from Seismic ≈ 0.32 Jones and Wang, 1981

Page 6: Field and Physical Modeling Study of the Bakken Formation

Physical modeling of anisotropic domains: Ultrasonic imaging of laser-etched fractures in glass (Geophysics, 2013 ) Robert. R. Stewart Nikolay Dyaur Bode Omoboya J.J.S de Figueiredo Mark Willis Samik Sil

Before Post-stack Migration

After Post-stack Migration

Model C1

6

Page 7: Field and Physical Modeling Study of the Bakken Formation

Minimum Offset 400m

Maximum Offset 2000m

CMP Interval 20m

Depth of Model 800m ( TWT to end of model = 350ms)

Average Velocity of Model 5800m/s

Dominant Frequency/

Wavelength

120 Hz / 50m

Model C3

Model C10

Model C9 “BAKKEN MODEL”

Schematic of NMO eta scan

experiments on glass models 7

Page 8: Field and Physical Modeling Study of the Bakken Formation

Model C3

Max 𝞰 = 0.0

Blank Model

Model C10

Max 𝞰 = 0.23

VTI Model

Model C9 Azimuth 0

Max 𝞰 = 0.14

VTI+HTI+VTI

Model C9 Azimuth 45

Max 𝞰 = 0.08

VTI+HTI+VTI

Model C9 Azimuth 90

Max 𝞰 = -0.06

VTI+HTI+VTI

-0.1

-0.05

0

0.05

0.1

0.15

0.2

0.25

0 2 4 6

Max 𝞰

𝞰

Model C3

Blank Model

Model C10

VTI Model

Model C9

Azimuth 0

Model C9

Azimuth 45

Model C9

Azimuth 90

8

𝞰= -0.3 𝞰= 0.3 𝞰= -0.3 𝞰= 0.3

t = 350 ms

t = 350 ms

t = 350 ms

t = 350 ms

t = 350 ms

Page 9: Field and Physical Modeling Study of the Bakken Formation

N-S structural cross section through the Newark Field in the Fort Worth Basin. Modified after Burna and Smosna, 2011

Geologic Age Mississipian

Lithology Dense Organic

rich shale

Water Saturation

((clay-bound)

20-30%

Gas Saturation 70-80%

Depth (feet) 4000 - 5000

Thickness (feet) 5-1000 ft

Pressure (psi) 5600

Porosity (%) 5

Natural fractures 100 to 120 deg

Natural fractures More common in

limestone

interbeds

Artificial fractures Oriented in the

direction of

minimal stress

Page 10: Field and Physical Modeling Study of the Bakken Formation

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Well X Well Y

Data Courtesy of Marathon Oil

Page 11: Field and Physical Modeling Study of the Bakken Formation

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Page 12: Field and Physical Modeling Study of the Bakken Formation

t = 0s

t = 1.5s

Page 13: Field and Physical Modeling Study of the Bakken Formation

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t = 0s

t = 1.5s

h = -0.2

h = 0.2

Page 14: Field and Physical Modeling Study of the Bakken Formation

Well Y

Page 15: Field and Physical Modeling Study of the Bakken Formation

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t = 0.55ms

t = 0.85ms

Base Marble Falls

Top Barnett

Top Ellenberger

Page 16: Field and Physical Modeling Study of the Bakken Formation

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t = 0.55ms

t = 0.85ms

Base Marble Falls

Top Barnett

Top Ellenberger

Page 17: Field and Physical Modeling Study of the Bakken Formation

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t = 0.55ms

t = 0.85ms

Base Marble Falls

Top Barnett

Top Ellenberger

Page 18: Field and Physical Modeling Study of the Bakken Formation

Constituent Materials: • Resin • Plexiglass (polycarbonate) • Copper tubes

Experimental study of the influence of fluids on seismic azimuthal anisotropy. (Geophysical Prospecting, 2013, submitted, under review) Bode Omoboya Emrah Pacal J.J.S de Figueiredo Nikolay Dyaur Robert. R. Stewart

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Page 19: Field and Physical Modeling Study of the Bakken Formation

19

Vs

(Z)

m/s

Page 20: Field and Physical Modeling Study of the Bakken Formation

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0

5

10

C11 C33 C33 C44 C55

Sti

ffn

ess

C

oe

ffic

ien

t (G

Pa

)

Water Saturated

Laboratory Measured

Gassmann Predicted

0

5

10

C11 C33 C33 C44 C55

Sti

ffn

ess

Co

eff

icie

nt

(Gp

a)

Glycerin Saturated

Laboratory Measured

Gassmann Predicted

C11 C33 C13 C44 C55

C11 C33 C13 C44 C55

Page 21: Field and Physical Modeling Study of the Bakken Formation

Model M2 Crack Density = 4.5 %

Model M3 Crack Density = 4.0 %

Model M1 Reference Model

Hudson, 1981

ɛ = 𝑁𝜋𝑟2ℎ

𝑉

Shear wave anisotropy from aligned inclusions: ultrasonic frequency dependence of velocity and attenuation (Geophysical Journal International, 2013) J.J.S de Figueiredo Nikolay Dyaur Bode Omoboya Robert. R. Stewart 21

Page 22: Field and Physical Modeling Study of the Bakken Formation

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Page 23: Field and Physical Modeling Study of the Bakken Formation

ϒ =1

2

𝑉𝑠12

𝑉𝑠22 − 1

Type equation here.

Thomsen, 1986

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Page 24: Field and Physical Modeling Study of the Bakken Formation

Dr. Steve Peterson – Marathon Oil

Michelle Simon – Hess Corporation

Dr. Edip Baysal – Paradigm

Schlumberger (For VISTA Processing Software)

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