master defense 2011

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COMPARSION OF RELATIVE PERMEABILITY OBTAINED FROM UNSTEADY STATE METHOD WITH THAT OBTAINED FROM A NEW RESISTIVITY MODEL By AHMED IBRAHIM M.Eng Defense 14 th July, 2011

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There is a global acceptance that out of the initial oil in place a maximum of about one third can be recovered by relying on depletion drive energy from the petroleum reservoir. To recover additional resources the depleted energy of the reservoir must be boosted. The usual approach involves water flooding and to maximize recovery under these conditions a sound knowledge of multiphase flow in porous media is required. Relative permeability is a fundamental multiphase flow function that has received immense attention in the petroleum industry. In this regard, a new model of water relative permeability based on resistivity measurement has been developed by Li (2004). He compared his relative permeability data to that obtained using the centrifuge. It was found to show close agreement.This study was conducted with two primary objectives. The first was to compare the new model relative permeability to the widely used unsteady state relative permeability data using a Benchtop Relative Permeameter (BRP 350). The second was to investigate the sensitivity of the new model to brine salinity. The experiment was conducted at ambient conditions with different brine concentrations ranging from 2% to 10%. Results show that the new model predicts relative permeability similar to the Benchtop Relative Permeameter (BRP 350) at lower brine concentration (2%) and at higher brine concentration (4.5% and 10%) close agreement is perceived only at lower water saturations. In addition, the new model has been found not to be sensitive to salinity at lower brine concentration (2% NaCl – 4.5% NaCl) and found to be sensitive at higher brine concentration (10% NaCl).

TRANSCRIPT

Page 1: Master Defense 2011

COMPARSION OF RELATIVE PERMEABILITY OBTAINED FROM UNSTEADY STATE METHOD WITH THAT OBTAINED FROM A NEW RESISTIVITY MODEL

By AHMED IBRAHIM

M.Eng Defense 14th July, 2011

Page 2: Master Defense 2011

OUTLINES

INTRODUCTION

RATIONALE BEHIND ORIGINAL STUDY [KEWEN LI, 2004]

PROJECT OBJECTIVES

THEORETICAL BACKGROUND

EXPERIMENTAL TASK

• MATERIALS USED

• EXPERIMENTAL SET UP

• PROCEDURE

RESULTS

CONCULSIONS

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Page 3: Master Defense 2011

INTRODUCTION

Relative permeability is considered as a dimensionless term. It can be either expressed as percentage or fraction and is usually expressed as the ratio of effective permeability to absolute permeability. Mathematically,

where,

Kr= Relative Permeability

Ke= Effective Permeability [mD or D]

K = Absolute Permeability [mD or D]

Importance of permeability comes in describing the formation as permeable.

3

KK

K er

Page 4: Master Defense 2011

RATIONALE BEHIND ORIGINAL STUDY [KEWEN LI, 2004]

Relative permeability is a dynamic property.

It is hard to measure relative permeability in many cases using direct methods.

The most often used method is JBN [Johnson Bosller Naumann].

Resistivity is easy to measure.

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Page 5: Master Defense 2011

PROJECT OBJECTIVES

The primary objectives of this study were:

1. Measure the relative permeability for an oil/brine system in a sandstone core using the unsteady state method.

2. Measure the resistivity of sandstone cores as a function of saturation.

3. Compare the measured relative permeability with that obtained from a new resistivity model, and

4. Investigate the sensitivity of the new model to brine salinity.

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Page 6: Master Defense 2011

THEORETICAL BACKGROUND

Relative Permeability is an important parameter of multiphase flow in porous media.

The traditional methods of relative permeability measurement depends on Steady State and Unsteady State Methods.

Relative Permeability, Capillary Pressure and Resistivity are the three main fundamental parameters that govern fluid flow in multi phase flow systems.

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Page 7: Master Defense 2011

THEORETICAL BACKGROUND CON’

Some models were developed empirically to calculate relative permeability from capillary pressure data.

It is easier to find a relationship between relative permeability and resistivity.

Kewen Li (2004) developed a new method to calculate relative permeability from resistivity data in consolidated porous media.

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Page 8: Master Defense 2011

THEORETICAL BACKGROUND CON’

His law stated that the wetting phase relative permeability is inversely proportional to the resistivity index of a porous medium. Mathematically,

where,

Krw = Relative Permeability of wetting phase

= Normalized Water Saturation [%]

I =Resistivity Index [Ω/Ω]8

ISK wrw

1"

"

wS

Page 9: Master Defense 2011

THEORETICAL BACKGROUND CON’

and,

• The resistivity index can be defined as:

where,

= Resistivity at specific water saturation [Ω/Ω]

= Resistivity at a water saturation of 100% [Ω/Ω]9

wi

wiww

S

SSS

1

"

o

t

R

RI

tR

oR

Page 10: Master Defense 2011

EXPERIMENTAL TASK

The new equation for relative permeability was tested using water saturation data derived from capillary pressure test.

The aim of this study was to use unsteady state method to obtain water saturation and based on the relationship between saturation and resistivity, resistivity index was calculated using the following equation:

Where,

n = Saturation Exponent and it is equal to 2

The calculated resistivity index was then used to calculate relative permeability.

10

n

w

o

t SR

RI

Page 11: Master Defense 2011

EXPERIMENTAL TASK-MATERIALS USED CON’

The test was carried out on three main fontaineblue sandstones GF 14, GV 25, GV 22 and GV 25 where the wetting phases were Tap water, 2% NaCl, 4.5% NaCl and 10% NaCl, respectively and non-wetting phase was kerosene. The solutions were made using distilled water at ambient conditions.

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Page 12: Master Defense 2011

EXPERIMENTAL TASK-EXPERIMENTAL SET UP CON’

Two instruments were used in this study:

• Electrical Properties System Atmospheric.

• Benchtop Relative Permeameter BRP 350.

• Cydar® Simulator.

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Page 13: Master Defense 2011

EXPERIMENTAL TASK- PROCEDURE CON’

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Page 14: Master Defense 2011

RESULTS

SAMPLE SALINITY (NaCl)

ɸ (%) Ka (mD) Ro (Ω.m) ConfiningPressure (psi)

Back Pressure (psi)

GF 14 3.6*10-3 6.77 6.66 39,504,269 759.7 205.8

GV 25 2 7.08 6.51 60 737.7 259.8

GV 22 4.5 6.41 5.44 35.290 691.3 230.7

GV 25 10 6.32 3.86 16.524 738.6 190.9

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Page 15: Master Defense 2011

RESULTS-MONOPHASIC PERMEABILITY CON’

GV 25 2% NaCl

GV 22 4.5% NaCl

R² = 0.999

0

20

40

60

80

100

120

140

160

0 1 2 3 4 5 6

Del

ta P

[p

si]

Flow Rate [cm3/min]

GV 25 Monophasic Permeability

R² = 0.999

020406080

100120140160180200

0 1 2 3 4 5 6

Del

ta P

[p

si]

Flow Rate [cm3/min]

GV 22 Monophasic Permeability

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Page 16: Master Defense 2011

RESULTS-MONOPHASIC PERMEABILITY CON’

GV 25 10% NaCl R² = 0.998

0

50

100

150

200

250

300

0 1 2 3 4 5 6

Del

ta P

[p

si]

Flow Rate [cm3/min]

GV 25 Monophasic Permeability

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Page 17: Master Defense 2011

RESULTS-COMPARSION OF RELATIVE PERMEABILITY CON’

GV 22 2% NaCl

GV 25 4.5% NaCl

0

0.2

0.4

0.6

0.8

1

0 0.2 0.4 0.6 0.8 1

Rel

ativ

e P

erm

eab

ilit

y

Water Saturation [%]

Comparsion GV 25

Krw BRP 350

Krw resis

Krw Corey

0

0.2

0.4

0.6

0.8

1

0 0.2 0.4 0.6 0.8 1

Rel

ativ

e P

erm

eab

ilit

y

Water Saturation [%]

Comparison GV 22

Krw BRP 350

Krw resis

Krw corey's 17

Page 18: Master Defense 2011

RESULTS-COMPARSION OF RELATIVE PERMEABILITY CON’

GV 25 10% NaCl

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

0 0.2 0.4 0.6 0.8 1

Rel

ativ

e P

erm

eab

ilit

y

Water Saturation [%]

Comparsion GV 25

Krw BRP

Krw resis

Krw Corey

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Page 19: Master Defense 2011

RESULTS-RELATIVE PERMEABILITY CURVES CON’

GV 25 2% NaCl

GV 22 4.5% NaCl

0

0.2

0.4

0.6

0.8

1

0 0.2 0.4 0.6 0.8 1

Rel

ativ

e P

erm

eab

ilit

y

Water Saturation [%]

Relative Permeability Curve GV 25

Krw

Kro

0

0.2

0.4

0.6

0.8

1

0 0.2 0.4 0.6 0.8 1

Rel

ativ

e P

erm

eab

ilit

y

Water Saturation [%]

Relative Permeability Curve GV 22

Krw

Kro19

Page 20: Master Defense 2011

RESULTS-RELATIVE PERMEABILITY CURVES CON’

GV 25 10% NaCl

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

0 0.2 0.4 0.6 0.8 1

Rel

ativ

e P

erm

eab

ilit

y

Water Saturation [%]

Relative Permeability Curve GV 25

Krw

Kro

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Page 21: Master Defense 2011

RESULTS-PRODUCED WATER VOLUME VERSUS TIME CON’

GV 25 2% NaCl GV 22 4.5% NaCl21

Page 22: Master Defense 2011

RESULTS-PRODUCED WATER VOLUME VERSUS TIME CON’

GV 25 10% NaCl

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Page 23: Master Defense 2011

RESULTS-DIFFERENTIAL PRESSURE VERSUS TIME CON’

GV 25 2% NaCl GV 22 4.5% NaCl

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Page 24: Master Defense 2011

RESULTS-DIFFERENTIAL PRESSURE VERSUS TIME CON’

GV 25 10% NaCl

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Page 25: Master Defense 2011

RESULTS-SENSITIVITY CON’

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

0 0.2 0.4 0.6 0.8 1

Rel

ativ

e P

erm

eab

ilit

y

Water Saturation [%]

Sensitivity of brine Salinity

Krw resis 2%

Krw resis 4.5%

Krw resis 10%

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Page 26: Master Defense 2011

CONCULSIONS

The new model is found to calculate relative permeability in close agreement with that obtained from Benchtop Relative Permeameter BRP 350 at higher and lower water saturations.

The wetting phase relative permeability inferred from the resistivity data are close to those calculated from the Benchtop Relative Permeameter for a concentration of 2% NaCl.

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Page 27: Master Defense 2011

CONCULSIONS CON’

At higher brine concentrations (4.5% &10% NaCl) close agreement is observe only at lower and higher water saturations and a deviation between these saturations.

The new model has been found not to be sensitive to salinity variation for the range of brine concentration investigated in this study (2% NaCl - 10% NaCl).

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