Wetting and Spreading Dynamics
Saved in:
| Main Author | |
|---|---|
| Other Authors | |
| Format | Electronic eBook |
| Language | English |
| Published |
Boca Raton, FL :
CRC Press,
2019.
|
| Edition | Second edition. |
| Series | Surfactant science series.
|
| Subjects | |
| Online Access | Full text |
| ISBN | 9780429013737 0429013736 9780429506246 0429506244 9780429013744 0429013744 9780429013720 0429013728 9781138584075 113858407X |
| Physical Description | 1 online resource |
Cover
Table of Contents:
- Cover
- Half Title
- Title Page
- Copyright Page
- Table of Contents
- Preface to the First Edition
- Acknowledgments
- Preface to the Second Edition
- Acknowledgments
- About the Authors
- 1: Surface Forces and Equilibrium of Liquids on Solid Substrates
- Introduction
- 1.1 Wetting and Neumann-Young's Equation
- 1.2 Surface Forces and Derjaguin's Pressure
- Components of the Derjaguin's Pressure
- Molecular or Dispersion Component
- Electrical Double Layers
- Electrokinetic Phenomena
- The Electrostatic Component of the Derjaguin's Pressure
- Structural Component of the Derjaguin's Pressure
- 1.3 Static Hysteresis of Contact Angle
- Static Hysteresis of Contact Angles from the Microscopic Point of View: Surface Forces
- References
- 2: Equilibrium Wetting Phenomena
- Introduction
- 2.1 Thin Liquid Films on Flat Solid Substrates
- Equilibrium Droplets on the Solid Substrate under Oversaturation (Pe <
- 0)
- Flat Films at the Equilibrium with Menisci (Pe >
- 0)
- 2.2 Non-flat Equilibrium Liquid Shapes on Flat Solid Surfaces
- General Consideration
- Microdrops: The Case Where Pe >
- 0 (The Case of Under-Saturation)
- Microscopic Quasi-equilibrium Periodic Films
- Microscopic Equilibrium Depressions on ß-Films
- 2.3 Equilibrium Contact Angle of Menisci and Drops: Liquid Shape in the Transition Zone from the Bulk Liquid to the Flat Films in Front
- Equilibrium of Liquid in a Flat Capillary: Partial Wetting Case
- Meniscus in a Flat Capillary
- Meniscus in a Flat Capillary: Profile of the Transition Zone
- Partial Wetting: Macroscopic Liquid Drops
- Profile of the Transition Zone in the Case of Droplets
- Axisymmetric Drops
- Meniscus in a Cylindrical Capillary
- Appendix 1
- 2.4 Profile of the Transition Zone between a Wetting Film and the Meniscus of the Bulk Liquid in the Case of Complete Wetting.
- 2.5 Thickness of Equilibrium Wetting Films on Rough Solid Substrates
- 2.6 Equilibrium Films on Locally Heterogeneous Surfaces: Hydrophilic Surface with Hydrophobic Inclusions
- 2.7 Equilibrium of Droplets on a Deformable Substrate: Influence of the Derjaguin's Pressure
- Introduction
- Derjaguin's Pressure and Deformation of Soft Substrates
- Mathematical Model and Derivation
- Spherical Region: h−hs>
- t1
- Transitional Region: h
- hs = t1
- Equilibrium Contact Angle
- Jacobi's Condition
- 2.8 Deformation of Fluid Particles in the Contact Zone
- Two Identical Cylindrical Drops/Bubbles
- Interaction of Cylindrical Droplets of Different Radii
- Shape of a Liquid Interlayer between Interacting Droplets: Critical Radius
- 2.9 Liquid Profiles on Curved Interfaces, Effective Derjaguin's Pressure. Equilibrium Contact Angles of Droplets on Outer/Inner Cylindrical Surfaces and Menisci inside Cylindrical Capillaries
- Liquid Profiles on Curved Surface: Derivation of Governing Equations
- Equilibrium Contact Angle of a Droplet on an Outer Surface of Cylindrical Capillaries
- Equilibrium Contact Angle of a Meniscus inside Cylindrical Capillaries
- Derjaguin's Pressure of Uniform Films in Cylindrical Capillaries
- 2.10 Line Tension
- The Comparison with the Experimental Data and Discussion
- 2.11 Capillary Interaction between Solid Bodies
- Appendix 2
- References
- 3: Hysteresis of Contact Angles Based on Derjaguin's Pressure
- Introduction
- 3.1 Hysteresis of Contact Angle of a Meniscus inside a Capillary with Smooth Homogeneous Non-deformable Walls
- The Derjaguin's Pressure Components
- The Derjaguin's Pressure and Wetting Phenomena
- Hysteresis of Contact Angle in Capillaries
- Calculation Procedure
- Conclusions
- 3.2 Hysteresis of Contact Angle of Sessile Droplets on Non-deformable Substrates
- Introduction.
- Equilibrium Contact Angle and Derjaguin's Pressure for Sessile Droplets
- Static Hysteresis of the Contact Angle of Sessile Droplets on Smooth Homogeneous Substrates
- Expressions for the Advancing Contact Angle
- Expressions for the Receding Contact Angle
- Conclusions
- 3.3 Hysteresis of Contact Angle of Sessile Droplets on Deformable Substrates
- Introduction
- Equilibrium Contact Angle of Droplet on Deformable Substrates and the Surface Forces Action: A Simplified Model Adopted in this Section
- Theory and Model for Hysteresis of Contact Angle on a Deformable Substrate
- Results and Discussions
- Conclusions
- Appendix: Advancing Contact Angle
- References
- 4: Kinetics of Wetting
- Introduction
- 4.1 Spreading of Nonvolatile Liquid Drops over Flat Solid Substrates: Qualitative Analysis
- Capillary Regime of Spreading
- Gravitational Spreading as a Continuation of the Capillary Spreading Regime
- Similarity Solution
- Spreading of Very Thin Droplets
- 4.2 Spreading of Nonvolatile Liquid Drops over Dry Surfaces: Influence of Surface Forces
- n = 2 Case
- n = 3 Case
- Comparison with Experiments
- Conclusions
- Appendix 1
- Appendix 2
- Appendix 3
- Appendix 4
- 4.3 Spreading of Drops over a Surface Covered with a Thin Layer of the Same Liquid
- 4.4 Quasi-Steady-State Approach in the Kinetics of Spreading
- 4.5 Dynamic Advancing Contact Angle and the Form of the Moving Meniscus in Flat Capillaries in the Case of Complete Wetting
- Appendix 5
- Asymptotic Behavior of Solution of y d y y 3 3 = -1 at y . 8
- 4.6 Motion of Long Drops in Thin Capillaries in the Case of Complete Wetting
- Appendix 6
- 4.7 Liquid Film Coating of a Moving Thin Cylindrical Fiber
- Statement of the Problem
- Derivation of the Equation for the Liquid-Liquid Interface Profile
- Equilibrium Configuration.
- Matching of Asymptotic Solutions in Zones I and II
- Equilibrium Case (Ca = 0)
- Numerical Results
- 4.8 Blow-off Method for Investigating Boundary Viscosity of Volatile Liquids
- Boundary Viscosity
- Theory of the Method
- Experimental Part
- Conclusions
- 4.9 Combined Heat and Mass Transfer in Tapered Capillaries with Bubbles under the Action of a Temperature Gradient
- Cylindrical Capillaries
- Tapered Capillaries
- 4.10 Spreading of Non-Newtonian Liquids over Solid Substrates
- Governing Equation for the Evolution of the Profile of the Spreading Drop
- Gravitational Regime of Spreading
- Capillary Regime of Spreading
- Conclusions
- References
- 5: Spreading over Porous Substrates
- Introduction
- 5.1 Spreading of Liquid Drops over Saturated Porous Layers
- Theory
- Liquid inside the Drop (0 <
- z <
- h(t, r))
- Inside the Porous Layer outside the Drop (- . <
- z <
- 0, L <
- r <
- l)
- Materials and Methods
- Results and Discussion. Experimental Determination of the "Effective Lubrication Coefficient" .
- 5.2 Spreading of Liquid Drops over a Thin Dry Porous Layer: Complete Wetting Case
- Theory
- Inside the Porous Layer outside the Drop (- . <
- z <
- 0, L <
- r <
- l)
- Experimental Part
- Independent Determination of K p p c
- Results and Discussion
- Appendix 1
- 5.3 Spreading of Liquid Drops over Thick Porous Substrates: Complete Wetting Case
- Theory
- Inside the Porous Substrate
- Experimental Part
- Results and Discussion
- Spreading of Silicone Oil Drops of Different Viscosity over Identical Glass Filters
- Spreading of Silicone Oil Drops over Filters with Similar Properties but Made of Different Materials
- Spreading of Silicone Oil Drops with the Same Viscosity (. = 5 P) over Glass Filters with Different Porosity and Average Pore Size
- Conclusions.