foams stabilized by in-situ surface activation of...
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FOAMS STABILIZED BY IN-SITU SURFACE
ACTIVATION OF SILICA MICRO-PARTICLES WITH
SURFACTANT
LAM KOK KEONG
UNIVERSITI TEKNOLOGI MALAYSIA
FOAMS STABILIZED BY IN-SITU SURFACE ACTIVATION OF SILICA MICRO-
PARTICLES WITH SURFACTANT
LAM KOK KEONG
A report submitted in partial fulfillment of the
requirements for the award of the degree of
M.Sc. Petroleum Engineering
Faculty of Petroleum and Renewable Energy Engineering
Universiti Teknologi Malaysia
FEBRUARY 2013
iii
DEDICATION
To my beloved Mother and Father
iv
ACKNOWLEGMENT
I would like to take this opportunity to express my gratitude to everyone who has
been assisting me in preparing this master project report during this semester. First and
foremost, I would like thank my supervisor, Prof. Dr. Ahmad Kamal Bin Idris for his
continuous support, advises, motivation, encouragement and invaluable guidance. Not to
forget, I also would like to highly express my gratitude to Prof Hadi, researcher from
Ibnu Sina, for providing one of the main raw chemicals that is CAB-O-SIL M5 Fumed
Silica to support this master project research. Besides that, I would like to appreciate the
help from Dr. Salasiah, Nur Izzatie Hannah and Cassy from the Applied Chemistry
Department for the sharing of knowledge on the surface properties of the silica
molecules with the fluids. I would also like to convey my special appreciation to my
parents for all the mental support and motivation to help me get through the challenges I
faced throughout this master project. My exclusive appreciation is also extended to the
Faculty of Petroleum and Renewable Energy Engineering, Universiti Teknologi
Malaysia for creating a platform of education opportunity. Last but not least, I am very
appreciative for all my friends who provide support directly and indirectly in assisting
me to complete this project.
v
ABSTRACT
Concept of applying gas foam in EOR was first proposed for gas mobility control
to alleviate the challenges of gas flooding and WAG process due to its high viscosity
and low mobility. Like surfactant, colloidal particles can be employed as surface-active
agent to stabilize the foams and can provide better stability due to its irreversible
adsorption to the interface. To get ultra-stable particle stabilized foams/emulsions, the
surface wettability of commercial raw colloidal particles should be modified (surface
activation) from hydrophilic to partially hydrophobic. However, the studies on the in-
situ surface activation for the micro-particles are yet to be widely performed. Therefore,
the in-situ surface activation of unmodified CAB-O-SIL fumed silica micro-particles by
using anionic surfactant such as Sodium dodecyl benzene sulfonate (SDBS) and alpha
olefin sulfonate (AOS) has been studied. Its effects on the foamability and foam stability
of dispersed solution were analyzed. The research methodology involves the
characterization of aqueous foams, measurement of adsorption of particles at the air-
water interface, and measurement of surface tensions. The independent variables are
concentration of anionic surfactants, concentration of silica micro-particles whereas the
dependent variables are foam volume, foam quality, surface tension, and percentage of
particles adsorbed at interface. The results showed that hydrophilic silica micro-particles
can be surface activated by interacting with anionic surfactants resulting to synergistic
effect in foamability and foam stability. The positive charges on the silica micro-
particles interact with negative charges of anionic surfactant to generate electrostatic
interaction. This generates adsorption of surfactant at the particle-water interface making
the particles to be surface active and bubble more stable. SDBS is more efficient anionic
surfactant for the surface activation of silica micro-particles compared to that of AOS.
vi
ABSTRAK
Konsep yang menggunakan buih gas dalam EOR diperkenalkan bagi kawalan
pergerakan gas supaya dapat mengatasi masalah yang dihadapi dalam pembajiran gas
dan proses WAG. Zarah koloid boleh digunakan sebagai ejen pengaktifan permukaan
untuk menstabilkan buih dan boleh memberikan kestabilian buih yang lebih baik. Ini
adalah disebabkan penjerapan zarah yang sehala di antara permukaan air dan udara. Bagi
mendapatkan ultra stabil buih/emulsi yang dihasilkan oleh zarah-zarah, kebolehbasahan
permukaan zarah koloid yang didapati dalam pasaran mesti diubah daripada hidrofilik
kepada separuh hidrofobik. Namun Demikian, kajian tentang pengaktifan permukaan
secara in-situ bagi miko-zarah belum dijalankan secara luas. Oleh itu, kajian tentang
permukaan “CAB-O-SIL fumed silica” yang diaktifkan secara in-situ dengan surfactant
anionik seperti “Sodium dodecyl benzene sulfonate” (SDBS) and “alpha olefin sulfonate”
(AOS) dijalankan. Kesan-kesannya dalam keboleh-buihan dan kestabilan buih juga
dikaji. The metodologi kajian sains melibatkan pencirian buih-buih, pengiraan peratusan
penjerapan zarah di antara permukaan air-udara, pengiraan ketegangan permukaan.
Pembolehubah bebas dalan kajian ini ialah kepekatan surfactant anionik, kepekatan
silica mikro-zarah. Pembolehubah tak bebas ialah isipadu buih, kualiti buih, ketegangan
permukaan, dan peratusan zarah yang terjerap antara permukaan air-udara. Keputusan
menunjukkan bahawa silika mikro-zarah yang hidrofilik boleh diaktifkan permukaannya
dengan menginteraksikan dengan surfactant anionik dan menyebabkan kesan sinergistik
dalam keboleh-buihan dan kestabilan buih. Caj positif di permukaan silika mikro-zarah
berinteraksi dengan caj negatif surfactant anionik dan menjanakan elektostatic interaksi.
Interaksi ini menyebabhan penjerapan surfactant di permukaan antara air-udara dan juga
mengaktifkan permukaan zarah dan menghasilkan buih yang lebih stabil. SDBS
vii
dibuktikan bahawa lebih effektif sebagai ajen pengakitfan permukaan bagi silika
surfactant mikro-zarah daripada AOS.
viii
TABLE OF CONTENTS
CHAPTER TITLE PAGE
DECLARATION ii
DEDICATION iii
ACKNOWLEGMENT iv
ABSTRACT v
ABSTRAK vi
TABLE OF CONTENTS viii
LIST OF TABLES xii
LIST OF FIGURES xiv
LIST OF ABBREVIATION xvii
LIST OF SYMBOLS xviii
LIST OF APPENDICES xx
1 INTRODUCTION 1
1.1 Background of Study 1
1.2 Problem Statement 4
1.3 Objectives 5
1.4 Scope of Work 6
2 LITERATURE REVIEW 7
2.1 Gas Flooding 7
2.2 Mobility Control in Gas Flooding 8
2.3 Foams 9
2.3.1 Foam Classification 10
ix
2.3.1.1 Bulk Foam 10
2.3.1.2 Foam in a Porous Media 12
2.3.2 Foam Properties 14
2.3.2.1 Foam Quality 15
2.3.2.2 Foam Texture 17
2.3.2.3 Foam Rheology 18
2.3.3 Mechanisms of Foam Generation 19
2.3.3.1 Snap-off 19
2.3.3.2 Lamella Division 21
2.3.3.3 Leave Behind 22
2.3.4 Mechanisms of Foam Destruction 24
2.3.4.1 In Absence of Oil 24
2.3.4.2 In Presence of Oil 25
2.3.5 Fluid Mobility with Foam 25
2.3.5.1 Gas Mobility with Foam 25
2.3.5.2 Liquid Mobility with Foam 26
2.3.6 Foam Stability 27
2.3.6.1 Film Drainage 27
2.3.6.2 Gas Diffusion 29
2.3.6.3 Disjoining Pressure 30
2.3.6.4 Oil Effect 31
2.3.6.5 Surfactant Concentration 32
2.3.6.6 Salinity 32
2.3.6.7 Temperature 33
2.4 Surfactant – Foaming Agent 33
2.5 Solid Particle-Stabilized Emulsions/Foams 34
2.6 Mechanism of Surface Activation 36
2.6.1 Homogeneous Surface Coating 37
2.6.2 Janus Particles 37
2.6.3 In-Situ Surface Activation 38
2.7 Anionic Surfactant and in-situ Surface Activation 38
x
2.8 Chapter Summary 39
3 METHODOLOGY 40
3.1 Equipment 40
3.1.1 KRÜSS: Tensiometer EasyDyne 41
3.1.2 Orbital Shaker 42
3.2 Material 43
3.2.1 CAB-O-SIL M-5 Fumed Silicas 43
3.2.2 Sodium Dodecyl Benzene Sulfonate (SDBS) 44
3.2.3 Alpha Olefin Sulfonate (AOS) 44
3.2.4 De-ionized Water (DI water) 45
3.3 Methods 45
3.3.1 Characteridfzation of Aqueous Foams 46
3.3.2 Measurement of Accumulation of Silica Micro-
particles at the Air-Water Interface
48
3.3.3 Measurement of Surface Tension 48
3.4 Chapter Summary 49
4 RESULTS AND DISCUSSIONS 50
4.1 Characterization of Aqueous Foams 50
4.1.1 Foamability and Foam Stability 50
4.1.1.1 SDBS & Silica Micro-particles 51
4.1.1.2 AOS & Silica Micro-particles 56
4.1.2 Synergistic Effects on Foamability and Foam
Stability
60
4.1.3 Foam Quality 65
4.2 Measurement of Accumulation of Silica Micro-particles
at the Air-Water Interface
67
4.3 Measurement of Surface Tension 69
4.4 Chapter Summary 71
xi
5 CONCLUSIONS AND RECOMMENDATIONS 72
5.1 Conclusions 72
5.2 Recommendations 74
REFERENCES 75
APPENDIX A - E 82 - 103
xii
LIST OF TABLES
TABLE NO. TITLE PAGE
2.1 Foam Quality (Friedmann and Jensen, 1986) 17
4.1 Effects of concentration of silica micro-particles on the Copt
(Sf) and maximum Sf
65
4.2 Effects of concentration of silica micro-particles on the Copt
(Sfs) and maximum Sfs
65
4.3 Minimum concentration of surfactant SDBS and AOS to get
stable foam at different concentration of silica micro-particles
67
A.1 Foam volume generated at various concentration of surfactant
SDBS with 0 ppm and 5,000 ppm silica micro-particles.
83
A.2 Foam volume generated at various concentration of surfactant
SDBS with 10,000 ppm and 20,000 ppm silica micro-
particles.
84
A.3 Foam volume generated at various concentration of surfactant
AOS with 0 ppm and 5,000 ppm silica micro-particles.
85
A.4 Foam volume generated at various concentration of surfactant
AOS with 10,000 ppm and 20,000 ppm silica micro-particles.
86
B.1 Synergistic effect on foamability of surfactant SDBS and
AOS at the presence of 5,000 ppm micro-particles.
88
B.2 Synergistic effect on foamability of surfactant SDBS and 89
xiii
AOS at the presence of 10,000 ppm micro-particles.
B.3 Synergistic effect on foamability of surfactant SDBS and
AOS at the presence of 20,000 ppm micro-particles.
90
B.4 Synergistic effect on foam stability of surfactant SDBS and
AOS at the presence of 5,000 ppm micro-particles.
91
B.5 Synergistic effect on foam stability of surfactant SDBS and
AOS at the presence of 10,000 ppm micro-particles.
92
B.6 Synergistic effect on foam stability of surfactant SDBS and
AOS at the presence of 20,000 ppm micro-particles.
93
C.1 Foam quality for SDBS at the presence of silica micro-
particles with concentration of 0 ppm, 5,000 ppm, 10,000 ppm
and 20,000 ppm
95
C.2 Foam quality for AOS at the presence of silica micro-particles
with concentration of 0 ppm, 5,000 ppm, 10,000 ppm and
20,000 ppm
96
D.1 Calculation steps for the percentage of particles adsorbed at
the air-water interface for surfactant SDBS
98
D.2 Calculation steps for the percentage of particles adsorbed at
the air-water interface for surfactant AOS
99
E.1 Raw data obtained from the KRÜSS Tensiometer EasyDyne
for surfactant SDBS without and with silica micro-particles.
101
E.2 Raw data obtained from the KRÜSS Tensiometer EasyDyne
for surfactant AOS without and with silica micro-particles.
102
xiv
LIST OF FIGURES
FIGURE NO. TITLE PAGE
2.1 An Illustration of the Typical Foam System (Schramm, 1994) 10
2.2 A Schematic Illustration of the Surfactant Molecules Adsorbed on
the Surface Creating the Lamella (Shen, 2006)
11
2.3 The Curve of Disjoining Pressure vs Lamella Thickness (Shen,
2006)
12
2.4 Schematic Illustration of Continuous and Discontinuous Gas Flow
in Porous Media in the Presence of Foam (Tanzil, 2001)
14
2.5 A Curve of Relationship between the Foam Quality and Foam
Viscosity (Bullen et al., 1975)
16
2.6 Snap-off mechanism of bubble generation mechanically (Kovscek
and Radke 1994). (a) Gas enters the pore throat that is filled with
liquid. (b) liquid film swells at the pore throat. (c) the snap off
repeated continually
20
2.7 Lamella division mechanisms (a) lamella stretches at a splitting
point (b) two lamellae form (Kovscek and Radke 1994)
22
2.8 Schematic of lamellae creation by Leave-Behind Method. Rock
grains are represented in lined circles, liquid in gray color, and gas
in white color (Kovscek and Radke 1994)
23
2.9 Pressure difference between the foam lamella surface (Schramm,
1994)
29
2.10 (Upper) Schematic diagram of position of particles at fluid-water 36
xv
FIGURE NO. TITLE PAGE
interface for a contact angle Ɵ < 90˚ (left), Ɵ ~ 90˚ (center), and
Ɵ > 90˚ (right). (Lower) Corresponding emulsion morphology o/w
emulsions are favored (Ɵ < 90˚; left), and w/o are expected (Ɵ >
90˚; right) (Binks, 2002)
3.1 KRÜSS Tensiometer EasyDyne 41
3.2 Orbital shaker 42
4.1 Foam volume of SDBS solutions at different concentration without
silica micro-particles
52
4.2 Foam volume of SDBS solutions at different concentration with
5,000 ppm silica micro-particles
52
4.3 Foam volume of SDBS solutions at different concentration with
10,000 ppm silica micro-particles
53
4.4 Foam volume of SDBS solutions at different concentration with
20,000 ppm silica micro-particles
53
4.5 Comparisons of Foam volume of SDBS solutions at different
concentration with and without 5,000 ppm silica micro-particles
54
4.6 Comparisons of Foam volume of SDBS solutions at different
concentration with and without 10,000 ppm silica micro-particles
55
4.7 Comparisons of Foam volume of SDBS solutions at different
concentration with and without 20,000 ppm silica micro-particles
55
4.8 Foam volume of AOS solutions at different concentration without
silica micro-particles
56
4.9 Foam volume of AOS solutions at different concentration with
5,000 ppm silica micro-particles
57
4.10 Foam volume of AOS solutions at different concentration with
10,000 ppm silica micro-particles
57
4.11 Foam volume of AOS solutions at different concentration with
20,000 ppm silica micro-particles
58
xvi
FIGURE NO. TITLE PAGE
4.12 Comparisons of Foam volume of AOS solutions at different
concentration with and without 5,000 ppm silica micro-particles
59
4.13 Comparisons of Foam volume of AOS solutions at different
concentration with and without 10,000 ppm silica micro-particles
59
4.14 Comparisons of Foam volume of AOS solutions at different
concentration with and without 20,000 ppm silica micro-particles
60
4.15 Effects of Surfactant concentration with 5,000 ppm silica micro-
particles on foamability (Sf)
61
4.16 . Effects of Surfactant concentration with 5,000 ppm silica micro-
particles on foam stability (Sfs)
62
4.17 Effects of Surfactant concentration with 10,000 ppm silica micro-
particles on foamability (Sf)
62
4.18 Effects of Surfactant concentration with 10,000 ppm silica micro-
particles on foam stability (Sfs)
63
4.19 Effects of Surfactant concentration with 20,000 ppm silica micro-
particles on foamability (Sf)
63
4.20 Effects of Surfactant concentration with 20,000 ppm silica micro-
particles on foam stability (Sfs)
64
4.21 Foam quality of foam generated at various surfactant concentration
of SDBS at different concentration of silica micro-particles
66
4.22 Foam quality of foam generated at various surfactant concentration
of AOS at different concentration of silica micro-particles
66
4.23 Fractions of Silica Micro-particles adsorbed at the air-water surface
at different SDBS and AOS concentration
69
4.24 Surface tension of SDBS solutions with and without 20,000 ppm
silica micro-particles
70
4.25 Surface tension of AOS solutions with and without 20,000 ppm
silica micro-particles
71
xvii
LIST OF ABBREVIATIONS
AOS - alpha olefin sulfonate
CMC - Critical Micelle Concentration
CO2 - Carbon dioxide
EOR - Enhanced oil recovery
HLB - Hydrophile-lipophile
OPEC - Organization of petroleum exporting countries
ROS - Residual oil saturation
SDBS - Sodium dodecyl benzene sulfonate
WAG - Water alternate gas flooding
xviii
LIST OF SYMBOLS
Cmin - Minimum concentration of surfactant needed to stabilize the foam
Cmin (Qb) - Minimum surfactant concentration needed to get stable foam based
on the foam quality
Copt (Sf) - Optimum surfactant concentration that contributes to maximum
synergistic effect on foamability
Copt (Sfs) - Optimum surfactant concentration that contributes to maximum
synergistic effect on foam stability
Ɵ - contact angle at the fluid-water interface
PA - Liquid pressure at center lamella
PB - Liquid pressure at Plateau border
PCA - Capillary pressure at center lamella
PCB - Capillary pressure at Plateau border
PG - Pressure in gas- phase
Qb - Foam quality
R - Radius of curvature
R1A - radius of curvature at the lamella center
R1B - radius of curvature at the plateau border
Sf - Synergistic effect on foamability (%)
Sfs - Synergistic effect on foam stability (%)
T - Room Temperature
V0 - Foam volume generated immediately after shaken
V0P+S - Foam volume generated immediately using surfactant with particles
only after shaken
xix
V0S - Foam volume generated immediately using surfactant only after
shaken
V30 - Foam volume after 30 minutes
V30P+S - Foam volume generated using surfactant with particles only after 30
minutes
V30S - Foam volume generated using surfactant only after 30 miniutes
Vg - Gas foam volume
VL - Liquid solution volume
w - Amount of silica micro-particles drained into the beaker
w0 - Amount of silica micro-particles initially added to the dispersion
x (%) - Percentage of silica particles adsorbed at the air-water interface
σ - Interfacial tension
xx
LIST OF APPENDICES
APPENDIX TITLE PAGE
A Results of Characterization of Aqueous Foam
(Foamability and Foam Stability)
85
B Results of Characterization of Aqueous Foam
(Synergistic effects on Foamability and Foam
Stability)
90
C Results of Characterization of Aqueous Foam
(foam quality)
97
D Results of Measurement of Accumulation of
Particles at Air-Water Interface
100
E Results of Measurement of Surface Tensions 103
1
CHAPTER 1
1 INTRODUCTION
1.1 Background of Study
Energy demand increased significantly from 1996 to 2012 reaching 89.6 million
barrels per day. Oil and gas has been the global leading energy generating resources. By
2035, it is expected by OPEC that the energy demand figure is increased to 109.7
million barrels per day. It is due to the growing energy demand from developing
countries. Nowadays, the global oil supply is gradually outpaced by the global oil
demand and it imposes a threat of energy security in the world. On the other hand, it
becomes harder to discover new oil well to substitute the produced reserves (Alvarado
and Manrique, 2010).
Therefore, enhanced oil recovery (EOR) methods are the key techniques applied
to increase the oil recovery from the existing oil reservoirs, and to increase the oil field
production life cycle by mobilizing the remaining trapped oil. Enhanced oil recovery
(EOR) involves the injection of fluids that are not present in the underground reservoir
to mobilize the immobile remaining oil (Lake, 1989). There are several common types
2
of enhanced oil recovery techniques that are chemical flooding, thermal recovery
processes, gas flooding, microbial enhanced oil recovery and vibro-seismic technology.
Gas flooding is one of the most widely applied EOR methods in field
applications. Gas flooding is normally applied on the reservoir that has been water-
flooded. The type of gas injected in this method can be hydrocarbon (light natural gas)
and non-hydrocarbon. The non-hydrocarbon gas can be nitrogen, carbon dioxide, flue
gas, hydrogen sulfide, and others. The fundamental mechanism of gas flooding method
is to increase microscopic sweep efficiency of the oil displacement and reduce the
residual oil saturation (Lake, 1989).
The main issues of the gas flooding are the viscous fingering and gravity
segregation of displacing gas due to frontal instability. To mitigate these problems,
water alternating gas injection (WAG) has been used in several field applications
(Dicharry et al, 1973, Warner, 1977). One of the drawbacks is that the contact between
the resident oil (displaced fluid) and injected gas (displacing fluid) is blocked by the
large quantity of injected water leading to a larger ROS. This water-blocking
phenomenon is more detrimental in water-wet reservoir or the reservoir that has been
water-flooded previously as secondary recovery technique (Stalkup, 1970). Some of the
injected gas (such as CO2) has high solubility in water and it increases the consumption
of that gas making the project less economically feasible.
Concept of applying gas foam for mobility control was first proposed by Bond
and Holbrook (1958). To alleviate the challenges of gas flooding and WAG process,
foam flooding using the injected gas can be the potential solution to it (Fried, 1961;
Kovscek and Radke, 1994; Rossen, 1996; Du et al., 2007; Farajzadeh et al., 2009). It is
very useful applying foams in EOR techniques to improve displacement efficiency
because of its high viscosity and mobility during the displacement across a porous a
3
medium (Green et. al., 1998). Extensive experimental studies were performed on using
surfactant as the foam generation agent to stabilize the foam to reduce the gas mobility
in gas flooding (Kim et al., 2005). However, there are several weaknesses on surfactant-
stabilized foam that are high surfactant retention in porous media, relatively low foam
stability, and degradation of surfactant at reservoir condition (Kim et al., 2004;
Ransohoff et al., 1988; Wang, 1984).
Solid particles can be employed as surface-active agent to stabilize the foams
besides surfactant. Like the surfactant, the solid particles can be adsorbed at the interface
between aqueous and non-aqueous phases, which makes it surface active. The solid-
stabilized foams have been applied in a variety of industries due to its higher adhesion
energy for the particle adsorption at the foam interface. Surfactants and solid particles
have been compared for their ability to stabilize foams/emulsions (Binks et al., 2002,
Horozoy 2008). Furthermore, colloidal particles can provide better stability because
when the colloidal particles are held at the interface, the adsorption can be irreversible
and the particles are not easily desorbed from the interface. Bink and Horozov (2005)
reported that a particle with size of larger than 100 nm could be irreversibly adsorbed on
the interface. Furthermore, Wilson (1980), and Sun and Gao (2002) reported that solid
micro-particles with size of several µm could be employed as the foam stabilizer to
generate stable foam or emulsion dispersion.
However, the raw commercial particles are normally not surface active at most of
the liquid interfaces. For silica particles, they are normally extremely hydrophilic. To get
ultra-stable particle stabilized foams/emulsions, the particle surface must be activated by
the wettability modification. The surface activation can be performed by several
methods: homogeneous surface coating, Janus particles and in-situ surface activation.
Homogeneous surface coating can be done on the silica by having surface silylation to
modify the surface hydrophobicity to be more hydrophobic but it costs highly in
commercial scales. Janus particles is the particles at which part of surface is coated to be
4
hydrophilic and part of the surface is treated to be hydrophobic but there is a limitation
to have large commercial scale of production. In-situ surface activation is the well –
known as an easy wettability modification method, which is to just interact the particles
with amphiphilic compounds. In-situ surface activation can be relatively less
complicated and much cheaper methods to produce the surface-active particles.
Cui et al. (2010) highlighted that the unmodified silica particle can be surface
activated by the anionic surfactant. The anionic surfactant can provide the negative
charges to have electrostatic interaction and form monolayer adsorption of the surfactant
at the particle-water interface. The electrostatic interaction modifies the surface
properties of the particle from hydrophilic to partially hydrophobic forming an ultra-
stable foam or emulsion stabilizer.
1.2 Problem Statement
The implication of foam in mobility control was brought up by Bond and
Holbrook (1958). One of the foaming agents commonly used is surfactant. There were
many extensive research efforts carried out on surfactant-stabilized foams and they
presented several weaknesses that are unstable foam properties, high surfactant retention
in porous media and surfactant degradation at reservoir condition (Kim et al., 2004;
Ransohoff et al., 1988; Wang, 1984). The surfactants of small molecular weight had
been widely researched and applied in the industries; solid particulate stabilizers pique
the interest of researchers in their applications.
5
Bink and Horozov (2005) reported that a particle with size of larger than 100 nm
could be irreversibly adsorbed on the interface. Furthermore, Binks (2005) highlighted
that there are only two examples in which solid micro-particles are used as foam
stabilizers. The functions of micro-particles were reported by Wilson (1980), and Sun
and Gao (2002) to be used as the effective foam stabilizer to generate stable foam or
emulsion dispersion. However, the raw commercial micro-particles are not surface-
active and highly hydrophilic. To obtain ultra-stable particle stabilized foam or emulsion,
the surface properties of the particles must be modified to be partially hydrophobic. Cui
et al. (2010) shows that in-situ surface activation with anionic surfactant can efficiently
increase the foamability and foam stability of the particles. However, the studies on the
in-situ surface activation for the micro-particles are not widely performed.
1.3 Objectives
In this research, anionic surfactants such as Sodium dodecyl benzene sulfonate
(SDBS) and alpha olefin sulfonate (AOS) are used as the in-situ surface activation agent
for unmodified CAB-O-SIL fumed silicas with size range of 0.1 – 0.3 µm. The main
objectives of this study are:
• To investigate the impact of the treated micro-particles on the foamability
and foam stability
• To compare anionic surfactants SDBS and AOS and identify which of it
is more efficient.
6
1.4 Scope of Work
The focus of this study is to examine the behavior of anionic surfactants on the
foamability and foam stability without and with the presence of micro-particles. It is also
to study the in-situ surface activation of the untreated CAB-O-SIL fumed silicas (micro-
particles) by interaction with anionic surfactant, and to assess the impact on the
foamability and foam stability of the aqueous dispersions.
76
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