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Numerical and Laboratory Analyses of Unconventional

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PETROLEUM ENGINEERING Numerical and Laboratory Study of Gas Flow through Unconventional Reservoir Rocks RPSEA Piceance Basin Tight Gas Research Review Xiaolong Yin, Assistant Professor Petroleum Engineering, Colorado School of Mines April 21 2011
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Page 1: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Numerical and Laboratory Study of Gas Flow through Unconventional Reservoir Rocks

RPSEA Piceance Basin Tight Gas Research Review

Xiaolong Yin, Assistant Professor

Petroleum Engineering, Colorado School of Mines

April 21 2011

Page 2: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Presentation Outline

• Challenges and our research activities

• Our RPSEA project and collaborators

• Preliminary results

• Goals and objectives

RPSEA Piceance Basin Research ReviewApril 21, 2011, Denver, Colorado

Page 3: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Background

• In very tight reservoir rocks, both measurement techniquesand our understanding of the physics are being challenged

• Our group’s research activities focus on pore-scale physics and flow using direct simulation and experiments

• Specifically, we investigate what makes unconventional rocks unconventional– Surface interaction

– Non-continuum slippage

– Heterogeneity in pore structure and rock-fluid interactions

RPSEA Piceance Basin Research ReviewApril 21, 2011, Denver, Colorado

Page 4: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Our RPSEA Project

• RPSEA 09122-29 – 02/2011 – 02/2014– Use nanofluidic chips and single-molecule detection techniques to

visualize fluid flow in nano-sized pores

– Combine core flooding test and SEM imaging to correlate fluid flow in tight rocks to pore structures

– Develop pore-scale numerical models to provide information that cannot be easily obtained from experiments, such as three-dimensional motion of fluids

• Our Team– Missouri University of Science & Technology – B. Bai (core flooding),

Y. Ma (single-molecule detection)

– Colorado School of Mines – X. Yin (pore-scale models), K. Neeves(nanofluidic chips)

RPSEA Piceance Basin Research ReviewApril 21, 2011, Denver, Colorado

Page 5: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Traditional laboratory studies

• Pulse-decay permeability measurement

• Mercury porosimetry

• Linear core flooding

• Ultra-centrifuge

• PVT (CSM)

These equipments allow us to study

•Porosity and permeability•Storage capacity and transport•Multiphase flows and formation damage

A CMS-300 Pulse-Decay Permeameter

RPSEA Piceance Basin Research ReviewApril 21, 2011, Denver, Colorado

Page 6: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Non-traditional laboratory studies

• What makes flow in unconventional reservoir rocks unconventional?– Surface interactions

– Non-continuum slippage

– Heterogeneity in surfaceproperties

– Fractures and cracks

– In-situ stress

– …

Some of these effects can be studied using micro (right) and nano-scale (below) porous media analogs constructed on silicon / polymer chips

Photo courtesy of Keith Neeves

Chemical Engineering

Colorado School of Mines

This list is probably far from complete.

RPSEA Piceance Basin Research ReviewApril 21, 2011, Denver, Colorado

Page 7: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Preliminary results from micro-chip experiments

Data and photo provided by Keith Neeves and Melissa Wu ,

Chemical Engineering, Colorado School of Mines

RPSEA Piceance Basin Research ReviewApril 21, 2011, Denver, Colorado

0.0

0.1

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0.8

1 2 3 4 5

Pe

rme

abili

ty (

Dar

cy)

Experiment LB Simulation

Permeability comparison

Air-water two phase flow test: Left: The geometry is initially saturated with water

Below: Air is injected in the lower left corner forcing water out of the channels

Page 8: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Simulation of micro- and nano-scale flows

• Numerical tools have been and are being developed to study fluid flow with non-continuum effects in nano-sized pores

Representative porous media geometry models

Experimentally measured φ and k and pore structure

Direct numerical simulation models:•Lattice-Boltzmann (for Navier-Stokes)•DSMC (for non-continuum flows – being developed)

Pore structureRelative permeabilityEffect of stressAdsorption / Desorption

RPSEA Piceance Basin Research ReviewApril 21, 2011, Denver, Colorado

Page 9: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Preliminary results from pore-scale modeling

• Porosity-permeability relation is the key to rock typing and understanding geomechanical effects on fluid flow

0.0000

0.0005

0.0010

0.0015

0.0020

0.0025

0.0030

0.00 0.10 0.20 0.30 0.40

ks2

Porosity

Homogeneous Geometry

Heterogeneous Geometry

Ideal, channelized geometry – porosity-permeability shows a strong correlation

More realistic, heterogeneous geometry –porosity-permeability shows large scattering

RPSEA Piceance Basin Research ReviewApril 21, 2011, Denver, Colorado

Page 10: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Preliminary results from pore-scale modeling

• A universal porosity-permeability correlation can be developed by recognizing that the large pores do not contribute to permeability

0.0000

0.0005

0.0010

0.0015

0.0020

0.0025

0.0030

0.00 0.10 0.20 0.30 0.40

ks2

Conductive Porosity

Homogeneous Geometry

Heterogeneous Geometry

• These data are from our scoping studies using 2D geometries

• 3D simulations and experiments are underway

• Such a correlation can be used to determine the geometry of pores from bulk measurement without resorting to image analysis

RPSEA Piceance Basin Research ReviewApril 21, 2011, Denver, Colorado

Page 11: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

0 0.05 0.1 0.15 0.2 0.25 0.3 0.350

0.005

0.01

0.015

0.02

0.025

Porosity

ka

v2

Parallelized, 3D pore-scale simulator

3D Representative Geometries

3D Porosity-Permeability Data

3D Simulator Parallel Speedup

100

101

102

103

10-3

10-2

10-1

100

101

Number of CoresS

imula

tion t

ime

-1 (

s-1

)

Slope = 1

RPSEA Piceance Basin Research ReviewApril 21, 2011, Denver, Colorado

Page 12: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Goals and objectives

Simulations with controlled

geometries and assumed physics Micro- and nano-

fluidic experiments with controlled

geometries and real physics

Core-scale experiments with

real geometries and real physicsIncreasing level of

reality

The combined approach will significantly improve our understanding of fluid flow on nano-scale and unconventional reservoir dynamics

RPSEA Piceance Basin Research ReviewApril 21, 2011, Denver, Colorado

Page 13: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Acknowledgements

• Collaborators– Baojun Bai, Yinfa Ma (MUST)

– Keith Neeves (CSM, ChemE)

– Qinjun Kang (Los Alamos National Lab)

• Students– Feng Xiao (PE)

– Lei Wang (PE)

– Melissa Wu (ChemE)

• Funding– RPSEA

Page 14: Numerical and Laboratory Analyses of Unconventional

P E T R O L E U M E N G I N E E R I N G

Simulated vs. measured permeability

• Simulation of flow through digital cores from CT-scan

– CT and experimental data from Imperial College

– Numerical simulations are done in CSM

A1 BSS C1 F42A S1 S2

Porosity 42.9 19.6 23.3 33 14.1 24.6

Resolution 3.85 5.345 2.85 9.996 8.683 4.956

K (exp) 7,220 1,286 1,102 59,000 1,678 3,898

K (sim) 8,675 1,507 1,192 59,331 2,006 4,076

% error 20.2% 17.2% 8.1% 0.6% 19.6% 4.6%


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