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E-raamat: Wetting and Spreading Dynamics, Second Edition

(Loughborough University, Leicestershire, UK), (Instituto PluriDisciplinar, Madrid, Spain)
  • Formaat: 494 pages
  • Sari: Surfactant Science
  • Ilmumisaeg: 02-Jul-2019
  • Kirjastus: CRC Press
  • Keel: eng
  • ISBN-13: 9780429013744
  • Formaat - PDF+DRM
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Wetting and Spreading Dynamics explains how surface forces acting at the three-phase contact line determine equilibrium, hysteresis contact angles, and other equilibrium and kinetics features of liquids when in contact with solids or with other immiscible liquids. It examines the interaction of surface forces, capillary forces, and properties of the transition zone between the bulk liquid and solid substrate.

Significantly revised and updated, the Second Edition features new chapters that cover spreading of non-Newtonian liquids over porous substrates, hysteresis of contact angles on smooth homogeneous substrates, equilibrium and hysteresis contact angles on deformable substrates, and kinetics of simultaneous spreading and evaporation.

Drawing together theory and experimental data while presenting over 150 figures to illustrate the concepts, Wetting and Spreading Dynamics, Second Edition is a valuable resource written for both newcomers and experienced researchers.
Preface to the First Edition xiii
Acknowledgments xv
Preface to the Second Edition xvii
Acknowledgments xix
About the Authors xxi
1 Surface Forces and Equilibrium of Liquids on Solid Substrates 1(24)
Introduction
1(1)
1.1 Wetting and Neumann-Young's Equation
2(6)
1.2 Surface Forces and Derjaguin's Pressure
8(9)
Components of the Derjaguin's Pressure
10(7)
Molecular or Dispersion Component
10(2)
Electrical Double Layers
12(1)
Electrokinetic Phenomena
13(1)
The Electrostatic Component of the Derjaguin's Pressure
13(2)
Structural Component of the Derjaguin's Pressure
15(2)
1.3 Static Hysteresis of Contact Angle
17(5)
Static Hysteresis of Contact Angles from the Microscopic Point of View: Surface Forces
20(2)
Reference
22(3)
2 Equilibrium Wetting Phenomena 25(100)
Introduction
25(1)
2.1 Thin Liquid Films on Flat Solid Substrates
25(7)
Equilibrium Droplets on the Solid Substrate under Oversaturation (Pe < 0)
29(1)
Flat Films at the Equilibrium with Menisci (Pe > 0)
30(2)
2.2 Non-flat Equilibrium Liquid Shapes on Flat Solid Surfaces
32(10)
General Consideration
33(3)
Microdrops: The Case Where Pe > 0 (The Case of Under-Saturation)
36(1)
Microscopic Quasi-equilibrium Periodic Films
37(4)
Microgcopic Equilibrium Depressions on β-Films
41(1)
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
42(11)
Equilibrium of Liquid in a Flat Capillary: Partial Wetting Case
43(1)
Meniscus in a Flat Capillary
44(3)
Meniscus in a Flat Capillary: Profile of the Transition Zone
47(1)
Partial Wetting: Macroscopic Liquid Drops
48(3)
Profile of the Transition Zone in the Case of Droplets
51(21)
Axisymmetric Drops
52(1)
Meniscus in a Cylindrical Capillary
53(1)
Appendix 1
53(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
54(5)
2.5 Thickness of Equilibrium Wetting Films on Rough Solid Substrates
59(7)
2.6 Equilibrium Films on Locally Heterogeneous Surfaces: Hydrophilic Surface with Hydrophobic Inclusions
66(6)
2.7 Equilibrium of Droplets on a Deformable Substrate: Influence of the Derjaguin's Pressure
72(13)
Introduction
73(1)
Derjaguin's Pressure and Deformation of Soft Substrates
73(2)
Mathematical Model and Derivation
75(3)
Spherical Region: h - hS > t1
78(1)
Transitional Region: h - hS less or equal to t1
78(4)
Equilibrium Contact Angle
82(1)
Jacobi's Condition
83(2)
2.8 Deformation of Fluid Particles in the Contact Zone
85(12)
Two Identical Cylindrical Drops/Bubbles
86(3)
Interaction of Cylindrical Droplets of Different Radii
89(3)
Shape of a Liquid Interlayer between Interacting Droplets: Critical Radius
92(5)
2.9 Liquid Profiles on Curved Interfaces, Effective Derjaguin's Pressure. Equlibrium Contact Angles of Droplets on Outer/Inner Cylindrical Surfaces and Menisci inside Cylindrical Capillaries
97(7)
Liquid Profiles on Curved Surface: Derivation of Governing Equations
98(4)
Equilibrium Contact Angle of a Droplet on an Outer Surface of Cylindrical Capillaries
100(2)
Equilibrium Contact Angle of a Meniscus inside Cylindrical Capillaries
102(1)
Derjaguin's Pressure of Uniform Films in Cylindrical Capillaries
103(1)
2.10 Line Tension
104(10)
The Comparison with the Experimental Data and Discussion
113(1)
2.11 Capillary Interaction between Solid Bodies
114(5)
Appendix 2
119(2)
Reference
121(4)
3 Hysteresis of Contact Angles Based on Derjaguin's Pressure 125(36)
Introduction
125(1)
3.1 Hysteresis of Contact Angle of a Meniscus inside a Capillary with Smooth Homogeneous Non-deformable Walls
125(12)
The Derjaguin's Pressure Components
127(1)
The Derjaguin's Pressure and Wetting Phenomena
128(1)
Hysteresis of Contact Angle in Capillaries
129(5)
Calculation Procedure
134(3)
Conclusions
137(1)
3.2 Hysteresis of Contact Angle of Sessile Droplets on Non-deformable Substrates
137(9)
Introduction
137(2)
Equilibrium Contact Angle and Derjaguin's Pressure for Sessile Droplets
139(2)
Static Hysteresis of the Contact Angle of Sessile Droplets on Smooth Homogeneous Substrates
141(1)
Expressions for the Advancing Contact Angle
142(3)
Expressions for the Receding Contact Angle
145(1)
Conclusions
146(1)
3.3 Hysteresis of Contact Angle of Sessile Droplets on Deformable Substrates
146(9)
Introduction
147(1)
Equilibrium Contact Angle of Droplet on Deformable Substrates and the Surface Forces Action: A Simplified Model Adopted in this Section
147(2)
Theory and Model for Hysteresis of Contact Angle on a Deformable Substrate
149(4)
Results and Discussions
153(2)
Conclusions
155(1)
Appendix: Advancing Contact Angle
155(2)
Reference
157(4)
4 Kinetics of Wetting 161(110)
Introduction
161(7)
4.1 Spreading of Nonvolatile Liquid Drops over Flat Solid Substrates: Qualitative Analysis
168(17)
Capillary Regime of Spreading
172(5)
Gravitational Spreading as a Continuation of the Capillary Spreading Regime
177(1)
Similarity Solution
178(2)
Spreading of Very Thin Droplets
180(5)
4.2 Spreading of Nonvolatile Liquid Drops over Dry Surfaces: Influence of Surface Forces
185(11)
n = 2 Case
191(1)
n = 3 Case
191(3)
Comparison with Experiments
194(2)
Conclusions
196(1)
Appendix 1
196(1)
Appendix 2
197(1)
Appendix 3
198(1)
Appendix 4
199(1)
4.3 Spreading of Drops over a Surface Covered with a Thin Layer of the Same Liquid
200(6)
4.4 Quasi-Steady-State Approach in the Kinetics of Spreading
206(7)
4.5 Dynamic Advancing Contact Angle and the Form of the Moving Meniscus in Flat Capillaries in the Case of Complete Wetting
213(4)
Appendix 5
217(3)
Asymptotic Behavior of Solution of y3 d3y/dx3 = y - 1 at y right arrow infinity
217(3)
4.6 Motion of Long Drops in Thin Capillaries in the Case of Complete Wetting
220(8)
Appendix 6
228(3)
4.7 Liquid Film Coating of a Moving Thin Cylindrical Fiber
231(7)
Statement of the Problem
232(1)
Derivation of the Equation for the Liquid-Liquid Interface Profile
232(2)
Equilibrium Configuration
234(1)
Matching of Asymptotic Solutions in Zones I and II
234(2)
Equilibrium Case (Ca = 0)
236(1)
Numerical Results
237(1)
4.8 Blow-off Method for Investigating Boundary Viscosity of Volatile Liquids
238(14)
Boundary Viscosity
238(1)
Theory of the Method
239(12)
Experimental Part
249(2)
Conclusions
251(1)
4.9 Combined Heat and Mass Transfer in Tapered Capillaries with Bubbles under the Action of a Temperature Gradient
252(6)
Cylindrical Capillaries
255(1)
Tapered Capillaries
256(2)
4.10 Spreading of Non-Newtonian Liquids over Solid Substrates
258(11)
Governing Equation for the Evolution of the Profile of the Spreading Drop
258(4)
Gravitational Regime of Spreading
262(3)
Capillary Regime of Spreading
265(3)
Conclusions
268(1)
Reference
269(2)
5 Spreading over Porous Substrates 271(78)
Introduction
271(1)
5.1 Spreading of Liquid Drops over Saturated Porous Layers
272(10)
Theory
272(10)
Liquid inside the Drop (0 < z < h(t, r))
272(1)
Inside the Porous Layer beneath the Drop (- Δ < z < 0, 0 < r < L)
273(5)
Materials and Methods
278(1)
Results and Discussion. Experimental Determination of the "Effective Lubrication Coefficient" ω
279(3)
5.2 Spreading of Liquid Drops over a Thin Dry Porous Layer: Complete Wetting Case
282(13)
Theory
282(15)
Inside the Porous Layer outside the Drop (- Δ < z < 0, L < r < l)
287(3)
Experimental Part
290(1)
Independent Determination of Kppc
290(1)
Results and Discussion
291(4)
Appendix 1
295(2)
5.3 Spreading of Liquid Drops over Thick Porous Substrates: Complete Wetting Case
297(11)
Theory
298(10)
Inside the Porous Substrate
300(1)
Experimental Part
300(1)
Results and Discussion
301(2)
Spreading of Silicone Oil Drops of Different Viscosity over Identical Glass Filters
303(1)
Spreading of Silicone Oil Drops over Filters with Similar Properties but Made of Different Materials
304(1)
Spreading of Silicone Oil Drops with the Same Viscosity (η = 5 P) over Glass Filters with Different Porosity and Average Pore Size
305(3)
Conclusions
308(1)
5.4 Spreading of Liquid Drops from a Liquid Source
308(8)
Theory
309(7)
Experimental Setup and Results
312(3)
Materials and Methods
312(1)
Results and Discussion
313(2)
Conclusions
315(1)
Appendix 2
316(5)
Capillary Regime, Complete Wetting
316(3)
Gravitational Regime, Complete Wetting
319(2)
Partial Wetting
321(1)
5.5 Spreading of Non-Newtonian Liquids over Dry Porous Layer. Complete and Partial Wetting Cases
321(22)
Partial and Complete Wetting Cases
322(1)
5.5.1 Complete Wetting Case
323(14)
Introduction
323(1)
Theory
324(13)
Droplet Profile
325(1)
Spreading above Porous Substrate
326(2)
Inside the Porous Layer outside the Drop (- Δ < z < 0, L < r < l)
328(3)
Experimental Data
331(1)
Numerical Solution of Eqs. (5.132) and (5.133)
332(1)
Results and Discussion
333(3)
Conclusions on Section "Complete Wetting Case"
336(1)
5.5.2 Partial Wetting Case
337(6)
Theory
337(1)
Droplet Profile
338(1)
Pores of the Porous Substrate Are Large Enough and Red Blood Cells Penetrate into the Substrate with Plasma Flow
339(1)
The Second Stage of the Process
339(1)
Pores inside the Porous Substrate Are Small and Red Blood Cells Do Not Penetrate into the Porous Substrate
340(2)
Conclusions on Section "Partial Wetting Case"
342(1)
Appendix 3
343(1)
Capillary Imbibition of Non-Newtonian Liquid into a Thin Capillary
343(1)
One-Dimensional Penetration of a Non-Newtonian Liquid into a Porous Medium
344(1)
Appendix 4
344(1)
Reference
345(4)
6 Wetting of Wetting/Spreading in the Presence of Surfactants 349(72)
Introduction
349(1)
6.1 Spreading of Aqueous Surfactant Solutions over Porous Layers
349(11)
Experimental Methods and Materials
350(1)
Spreading on Porous Substrates
350(9)
Measurement of Static Advancing and Receding Contact Angles on Nonporous Substrates
351(1)
Results and Discussion
352(3)
Advancing and Hydrodynamic Receding Contact Angles on Porous Nitrocellulose Membranes
355(2)
Static Hysteresis of the Contact Angle of SDS Solution Drops on Smooth Nonporous Nitrocellulose Substrate
357(2)
Conclusions
359(1)
6.2 Spontaneous Capillary Imbibition of Surfactant Solutions into Hydrophobic Capillaries
360(12)
Theory
362(3)
Concentration below the CMC
365(2)
Concentration above the CMC
367(3)
Spontaneous Capillary Rise in Hydrophobic Capillaries
370(2)
Appendix 1
372(2)
Excess Free Energy of an Aqueous Surfactant Droplet on a Hydrophobic Substrate
372(2)
Appendix 2
374(2)
6.3 Capillary Imbibition of Surfactant Solutions in Porous Media and Thin Capillaries: The Partial Wetting Case
376(10)
Theory
376(1)
Concentration below the CMC
377(6)
Concentration above the CMC
383(1)
Experimental Part
384(1)
Results and Discussions
385(1)
6.4 Spreading of Surfactant Solutions over Hydrophobic Substrates
386(7)
Theory
387(3)
Experiment: Materials
390(1)
Monitoring Method
390(1)
Results and Discussion
390(3)
6.5 Spreading of Insoluble Surfactants over Thin Viscous Liquid Layers
393(9)
Theory and Relation to Experiment
394(6)
Experimental Results
400(2)
Appendix 3
402(1)
Derivation of Governing Equations for Time Evolution of Both Film Thickness and Surfactant Surface Concentration
402(1)
Appendix 4
403(1)
Influence of Capillary Forces during the Initial Stage of Spreading
403(1)
Appendix 5
404(1)
Derivation of Boundary Condition at the Moving Shock Front
404(1)
Appendix 6
405(1)
Matching of Asymptotic Solutions at the Moving Shock Front
405(1)
Appendix 7
406(1)
Solution of the Governing Equations for the Second Stage of Spreading
406(1)
6.6 Spreading of Aqueous Droplets Induced by Overturning of Amphiphilic Molecules or Their Fragments in the Surface Layer of an Initially Hydrophobic Substrate
406(14)
Theory, Derivation of Basic Equations
407(4)
Boundary Conditions
411(4)
Solution of the Problem
415(3)
Comparison between Theory and Experimental Data
418(2)
Reference
420(1)
7 Kinetics of Simultaneous Spreading and Evaporation 421(44)
Introduction
421(1)
7.1 Basic Properties of Simultaneous Spreading/Evaporation
422(4)
The Partial Wetting Case
422(1)
The Complete Wetting Case
423(2)
Dependence of Evaporation Flux on Droplet Size
424(1)
Thermal Phenomena at Evaporation
425(1)
7.2 Spreading and Evaporation of Sessile Droplets: Universal Behavior in the Case of Complete Wetting
426(15)
Introduction
426(1)
Theory
427(9)
Experimental
436(3)
Materials
436(1)
Methodology
436(1)
Results and Discussions
436(1)
Extracting Theoretical Parameters from Experimental Data
437(1)
Comparison of Experimental Data and Predicted Universal Behavior
438(1)
Conclusions
439(1)
List of Main Symbols
440(1)
Latin
440(1)
Greek
440(1)
Subscripts
440(1)
Superscripts
440(1)
7.3 Evaporation of Sessile Droplets: Universal Behavior in the Presence of Contact Angle Hysteresis
441(6)
Introduction
441(1)
Theory
442(2)
Problem Statement
442(1)
Two Stages of Evaporation of a Sessile Droplet
442(2)
Validation against Experimental Data
444(3)
Conclusions
447(1)
7.4 Spreading and Evaporation of Surfactant Solutions
447(7)
Introduction
447(1)
Experimental
448(1)
Results and Discussion
449(3)
Theory Presented in Section 7.3 and Used in This Section for the Spreading/Evaporation of Surfactant Solutions
450(1)
Comparison of the Experimental Data for Evaporation of Surfactant Solutions with the Theoretical Predictions for Pure Liquids
450(2)
Conclusions
452(2)
7.5 Evaporation of Microdroplets
454(9)
Introduction
454(1)
Problem Statement
454(1)
Governing Equations in the Bulk Phases
455(1)
Boundary Conditions
455(4)
Computer Simulations
459(1)
Results and Discussion
459(3)
Isothermal Evaporation
459(2)
Influence of Thermal Effects
461(1)
Conclusions
462(1)
Reference
463(2)
8 Main Problems in Kinetics of Wetting and Spreading to Be Solved 465(2)
Index 467
Victor Starov, PhD, DSc, Fellow of the Royal Society of Chemistry, Professor. Victor Starov has been a Professor at the Department of Chemical Engineering, Loughborough University, UK, since 1999. He received his PhD from the USSR Academy of Sciences in 1970 on "Capillary hysteresis in porous bodies." He received his DSc degree from St. Petersburg University in 1981 on "Equilibrium and kinetics of thin liquid layers in dispersed systems." Victor Starov is working on the influence of surface forces on kinetics of wetting and spreading over rigid and soft solids and the kinetics of spreading over porous and hydrophobic surfaces. He has published more than 300 scientific papers. Some of his research results are summarized in this book. He currently serves on the editorial board of 10 journals. He has participated in numerous organizing and scientific committees of international conferences and was a chairman of ECIC XVII in 2005. For more information, please visit https://doi.org/10.1016/j.cis.2007.04.016 (Manuel G. Velarde. "Honorary Note," Advances in Colloid and Interface Science, 134135 (2007), 12; and https://doi.org/10.1016/j.colsurfa.2016.11.028Get (N. M. Kovalchuk, R. Miller, Manuel G. Velarde. "Honorary Note," Colloids and Surfaces A: Physicochemical and Engineering Aspects, 521 (2017), 12.

Manuel G. Velarde, PhD Physics (UCM, Spain, 1968; ULB, Belgium, 1970), Honorary Doctor (Aix-Marseille, Saratov), is an Emeritus Professor at the Instituto Pluridisciplinar, Universidad Complutense Madrid (Spain). He is a member of Academia Europaea and the European Academy of Sciences. He has published numerous papers and book chapters, and six research frontier monographs and has edited several other books dealing with interfacial phenomena, wetting and spreading processes, waves and convective instabilities, and nonlinear dynamics as applied to various fields of science (patterns, waves, solitons, and chaos). He has over two decades of collaboration with V. M. Starov on wetting and spreading processes. At present he is mostly engaged in a theory of soliton-assisted electron transport (mechanical control of electrons at the nanolevel). He is the co inventor (with E. G. Wilson) of a novel field effect transistor, not using silicon, designed to operate with extremely low dissipation and huge mobility (UK Patent application published GB 2533105 A-15/6/2016). For further details see http://www.ucm.es/info/fluidos; see also R. G. Rubio et al., Without Bounds: A Scientific Canvas of Nonlinearity and Complex Dynamics, Springer, Berlin (2013) and R. Miller, R. G. Rubio and V. M. Starov, Advances in Colloid and Interface Science 206 (2014).