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Colloid and Surface Chemistry is a subject of immense importance and implications both to our everyday life and numerous industrial sectors, ranging from coatings and materials to medicine and biotechnology.
How do detergents really clean? (Why can't we just use water?) Why is milk "milky"? Why do we use eggs so often for making sauces? Can we deliver drugs in better and controlled ways? Coating industries wish to manufacture improved coatings e.g. for providing corrosion resistance, which are also environmentally friendly i.e. less based on organic solvents and if possible exclusively on water. Food companies want to develop healthy, tasty but also long-lasting food products which appeal to the environmental authorities and the consumer. Detergent and enzyme companies are working to develop improved formulations which clean more persistent stains, at lower temperatures and amounts, to the benefit of both the environment and our pocket. Cosmetics is also big business! Creams, lotions and other personal care products are really just complex emulsions.
All of the above can be explained by the principles and methods of colloid and surface chemistry. A course on this topic is truly valuable to chemists, chemical engineers, biologists, material and food scientists and many more.
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Seitenzahl: 858
Veröffentlichungsjahr: 2016
Cover
Title Page
Preface
References
Useful Constants
Symbols and Some Basic Abbreviations
About the Companion Web Site
1 Introduction to Colloid and Surface Chemistry
1.1 What are the colloids and interfaces? Why are they important? Why do we study them together?
1.2 Applications
1.3 Three ways of classifying the colloids
1.4 How to prepare colloid systems
1.5 Key properties of colloids
1.6 Concluding remarks
Appendix 1.1
Problems
References
2 Intermolecular and Interparticle Forces
2.1 Introduction – Why and which forces are of importance in colloid and surface chemistry?
2.2 Two important long-range forces between molecules
2.3 The van der Waals forces
2.4 Concluding remarks
Appendix 2.1 A note on the uniqueness of the water molecule and some of the recent debates on water structure and peculiar properties
References for the Appendix 2.1
Problems
References
3 Surface and Interfacial Tensions – Principles and Estimation Methods
3.1 Introduction
3.2 Concept of surface tension – applications
3.3 Interfacial tensions, work of adhesion and spreading
3.4 Measurement and estimation methods for surface tensions
3.5 Measurement and estimation methods for interfacial tensions
3.6 Summary
Appendix 3.1 Hansen solubility parameters (HSP) for selected solvents
Appendix 3.2 The “ϕ” parameter of the Girifalco–Good equation (Equation 3.16) for liquid–liquid interfaces. Data from Girifalco and Good (1957, 1960)
Problems
References
4 Fundamental Equations in Colloid and Surface Science
4.1 Introduction
4.2 The Young equation of contact angle
4.3 Young–Laplace equation for the pressure difference across a curved surface
4.4 Kelvin equation for the vapour pressure,
P
, of a droplet (curved surface) over the “ordinary” vapour pressure
P
sat
for a flat surface
4.5 The Gibbs adsorption equation
4.6 Applications of the Gibbs equation (adsorption, monolayers, molecular weight of proteins)
4.7 Monolayers
4.8 Conclusions
Appendix 4.1 Derivation of the Young–Laplace equation
Appendix 4.2 Derivation of the Kelvin equation
Appendix 4.3 Derivation of the Gibbs adsorption equation
Problems
References
5 Surfactants and Self-assembly. Detergents and Cleaning
5.1 Introduction to surfactants – basic properties, self-assembly and critical packing parameter (CPP)
5.2 Micelles and critical micelle concentration (CMC)
5.3 Micellization – theories and key parameters
5.4 Surfactants and cleaning (detergency)
5.5 Other applications of surfactants
5.6 Concluding remarks
Appendix 5.1 Useful relationships from geometry
Appendix 5.2 The Hydrophilic–Lipophilic Balance (HLB)
Problems
References
6 Wetting and Adhesion
6.1 Introduction
6.2 Wetting and adhesion via the Zisman plot and theories for interfacial tensions
6.3 Adhesion theories
6.4 Practical adhesion: forces, work of adhesion, problems and protection
6.5 Concluding remarks
Problems
References
7 Adsorption in Colloid and Surface Science – A Universal Concept
7.1 Introduction – universality of adsorption – overview
7.2 Adsorption theories, two-dimensional equations of state and surface tension–concentration trends: a clear relationship
7.3 Adsorption of gases on solids
7.4 Adsorption from solution
7.5 Adsorption of surfactants and polymers
7.6 Concluding remarks
Problems
References
8 Characterization Methods of Colloids – Part I
8.1 Introduction – importance of kinetic properties
8.2 Brownian motion
8.3 Sedimentation and creaming (Stokes and Einstein equations)
8.4 Kinetic properties via the ultracentrifuge
8.5 Osmosis and osmotic pressure
8.6 Rheology of colloidal dispersions
8.7 Concluding remarks
Problems
References
9 Characterization Methods of Colloids – Part II
9.1 Introduction
9.2 Optical microscopy
9.3 Electron microscopy
9.4 Atomic force microscopy
9.5 Light scattering
9.6 Spectroscopy
9.7 Concluding remarks
Problems
References
10 Colloid Stability – Part I
10.1 Introduction – key forces and potential energy plots – overview
10.2 van der Waals forces between particles and surfaces – basics
10.3 Estimation of effective Hamaker constants
10.4 vdW forces for different geometries – some examples
10.5 Electrostatic forces: the electric double layer and the origin of surface charge
10.6 Electrical forces: key parameters (Debye length and zeta potential)
10.7 Electrical forces
10.8 Schulze–Hardy rule and the critical coagulation concentration (CCC)
10.9 Concluding remarks on colloid stability, the vdW and electric forces
Appendix 10.1 A note on the terminology of colloid stability
Appendix 10.2 Gouy–Chapman theory of the diffuse electrical double-layer
Problems
References
11 Colloid Stability – Part II
11.1 DLVO theory – a rapid overview
11.2 DLVO theory – effect of various parameters
11.3 DLVO theory – experimental verification and applications
11.4 Kinetics of aggregation
11.5 Concluding remarks
Problems
References
12 Emulsions
12.1 Introduction
12.2 Applications and characterization of emulsions
12.3 Destabilization of emulsions
12.4 Emulsion stability
12.5 Quantitative representation of the steric stabilization
12.6 Emulsion design
12.7 PIT – Phase inversion temperature of emulsion based on non-ionic emulsifiers
12.8 Concluding remarks
Problems
References
13 Foams
13.1 Introduction
13.2 Applications of foams
13.3 Characterization of foams
13.4 Preparation of foams
13.5 Measurements of foam stability
13.6 Destabilization of foams
13.7 Stabilization of foams
13.8 How to avoid and destroy foams
13.9 Rheology of foams
13.10 Concluding remarks
Problems
References
14 Multicomponent Adsorption
14.1 Introduction
14.2 Langmuir theory for multicomponent adsorption
14.3 Thermodynamic (ideal and real) adsorbed solution theories (IAST and RAST)
14.4 Multicomponent potential theory of adsorption (MPTA)
14.5 Discussion. Comparison of models
14.6 Conclusions
Acknowledgments
Appendix 14.1 Proof of Equations 14.10a,b
Problems
References
15 Sixty Years with Theories for Interfacial Tension –
Quo Vadis
?
15.1 Introduction
15.2 Early theories
15.3 van Oss–Good and Neumann theories
15.4 A new theory for estimating interfacial tension using the partial solvation parameters (Panayiotou)
15.5 Conclusions –
Quo Vadis
?
Problems
References
16 Epilogue and Review Problems
Review Problems in Colloid and Surface Chemistry
Index
End User License Agreement
Chapter 01
Table 1.1
Examples of colloidal systems, i.e. one type of compound, e.g. solid particles or liquid droplets, in a medium. Different combinations are possible depending on the phase of the particles (dispersed phase) and the (dispersion) medium they are in. Two gas phases will mix on a molecular level and do not form a colloidal system.
Table A1
Overview of what can be measured and what can be calculated in the area of colloid and surface chemistry
Chapter 02
Table 2.1
Change in standard molar Gibbs energy, enthalpy and entropy (all in kJ mol
–1
) for the transfer of hydrocarbons from pure liquids into water at 25 °C (Prausnitz, Lichtenthaler and de Azevedo, 1999; Gill and Wadso, 1976). Notice the large negative entropy changes due to the hydrophobic effect. In the case of
n
-butane, the entropy decrease amounts to 85% of the Gibbs energy of solubilization, while for other hydrocarbons the entropic contribution is even larger
Table 2.2
Van der Waals interaction (potential) energies between particles/surfaces;
V
A
is the potential energy (in J or J m
–2
for the interaction between two surfaces),
H
is the interparticle/intersurface distance and
R
is the radius (for spherical particles);
A
is the Hamaker constant (see Equations 2.6–2.8 and Hamaker, 1937) and, depending on the application, is evaluated under conditions of either vacuum/air or a dielectric (i.e. a liquid medium, in which case an effective Hamaker constant must be used).
C
is defined in Equation 2.6 and
ρ
is the number density (molecules/volume)
Table 2.3
Comparison of intermolecular forces between two identical molecules. The
C
-values of the van der Waals forces (
) for identical molecules are given at 0 °C; C-values are expressed in 10
–79
J m
6
Table 2.4
Multiple choice questions
Table 2.5
Blend-solvent miscibility
Chapter 03
Table 3.1
Surface tension values for typical liquids and solids (in mN m
–1
)
.
The solid surface tension values are “ideal” (production under vacuum) and will be much lower under normal laboratory conditions or after exposure in air. Except otherwise indicated, the values are at 20–25 °C
Table 3.2
Liquid–liquid interfacial tensions (and liquid surface tensions) for some liquids. All values are given at room temperature (20 °C). Differences in miscibility in, for example, aqueous solutions with hydrocarbons, fluorocarbons or alcohols can be elucidated from the values of the interfacial tensions. The higher the interfacial tensions, the lower the miscibility. For alcohols smaller than butanol, the interfacial tensions with water are zero, as such alcohols are completely miscible in water. Fluorocarbons have among the lowest surface tensions due to their very weak van der Waals forces
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