Preface to the First Edition |
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xiii | |
Acknowledgments |
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xv | |
Preface to the Second Edition |
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xvii | |
Acknowledgments |
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xix | |
About the Authors |
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xxi | |
1 Surface Forces and Equilibrium of Liquids on Solid Substrates |
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1 | (24) |
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1 | (1) |
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1.1 Wetting and Neumann-Young's Equation |
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2 | (6) |
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1.2 Surface Forces and Derjaguin's Pressure |
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8 | (9) |
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Components of the Derjaguin's Pressure |
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10 | (7) |
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Molecular or Dispersion Component |
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10 | (2) |
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12 | (1) |
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13 | (1) |
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The Electrostatic Component of the Derjaguin's Pressure |
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13 | (2) |
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Structural Component of the Derjaguin's Pressure |
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15 | (2) |
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1.3 Static Hysteresis of Contact Angle |
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17 | (5) |
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Static Hysteresis of Contact Angles from the Microscopic Point of View: Surface Forces |
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20 | (2) |
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22 | (3) |
2 Equilibrium Wetting Phenomena |
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25 | (100) |
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25 | (1) |
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2.1 Thin Liquid Films on Flat Solid Substrates |
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25 | (7) |
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Equilibrium Droplets on the Solid Substrate under Oversaturation (Pe < 0) |
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29 | (1) |
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Flat Films at the Equilibrium with Menisci (Pe > 0) |
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30 | (2) |
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2.2 Non-flat Equilibrium Liquid Shapes on Flat Solid Surfaces |
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32 | (10) |
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33 | (3) |
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Microdrops: The Case Where Pe > 0 (The Case of Under-Saturation) |
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36 | (1) |
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Microscopic Quasi-equilibrium Periodic Films |
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37 | (4) |
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Microgcopic Equilibrium Depressions on β-Films |
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41 | (1) |
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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 |
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42 | (11) |
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Equilibrium of Liquid in a Flat Capillary: Partial Wetting Case |
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43 | (1) |
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Meniscus in a Flat Capillary |
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44 | (3) |
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Meniscus in a Flat Capillary: Profile of the Transition Zone |
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47 | (1) |
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Partial Wetting: Macroscopic Liquid Drops |
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48 | (3) |
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Profile of the Transition Zone in the Case of Droplets |
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51 | (21) |
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52 | (1) |
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Meniscus in a Cylindrical Capillary |
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53 | (1) |
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53 | (1) |
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2.4 Profile of the Transition Zone between a Wetting Film and the Meniscus of the Bulk Liquid in the Case of Complete Wetting |
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54 | (5) |
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2.5 Thickness of Equilibrium Wetting Films on Rough Solid Substrates |
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59 | (7) |
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2.6 Equilibrium Films on Locally Heterogeneous Surfaces: Hydrophilic Surface with Hydrophobic Inclusions |
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66 | (6) |
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2.7 Equilibrium of Droplets on a Deformable Substrate: Influence of the Derjaguin's Pressure |
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72 | (13) |
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73 | (1) |
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Derjaguin's Pressure and Deformation of Soft Substrates |
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73 | (2) |
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Mathematical Model and Derivation |
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75 | (3) |
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Spherical Region: h - hS > t1 |
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78 | (1) |
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Transitional Region: h - hS less or equal to t1 |
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78 | (4) |
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Equilibrium Contact Angle |
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82 | (1) |
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83 | (2) |
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2.8 Deformation of Fluid Particles in the Contact Zone |
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85 | (12) |
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Two Identical Cylindrical Drops/Bubbles |
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86 | (3) |
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Interaction of Cylindrical Droplets of Different Radii |
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89 | (3) |
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Shape of a Liquid Interlayer between Interacting Droplets: Critical Radius |
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92 | (5) |
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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 |
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97 | (7) |
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Liquid Profiles on Curved Surface: Derivation of Governing Equations |
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98 | (4) |
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Equilibrium Contact Angle of a Droplet on an Outer Surface of Cylindrical Capillaries |
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100 | (2) |
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Equilibrium Contact Angle of a Meniscus inside Cylindrical Capillaries |
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102 | (1) |
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Derjaguin's Pressure of Uniform Films in Cylindrical Capillaries |
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103 | (1) |
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104 | (10) |
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The Comparison with the Experimental Data and Discussion |
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113 | (1) |
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2.11 Capillary Interaction between Solid Bodies |
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114 | (5) |
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119 | (2) |
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121 | (4) |
3 Hysteresis of Contact Angles Based on Derjaguin's Pressure |
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125 | (36) |
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125 | (1) |
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3.1 Hysteresis of Contact Angle of a Meniscus inside a Capillary with Smooth Homogeneous Non-deformable Walls |
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125 | (12) |
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The Derjaguin's Pressure Components |
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127 | (1) |
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The Derjaguin's Pressure and Wetting Phenomena |
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128 | (1) |
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Hysteresis of Contact Angle in Capillaries |
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129 | (5) |
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134 | (3) |
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137 | (1) |
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3.2 Hysteresis of Contact Angle of Sessile Droplets on Non-deformable Substrates |
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137 | (9) |
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137 | (2) |
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Equilibrium Contact Angle and Derjaguin's Pressure for Sessile Droplets |
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139 | (2) |
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Static Hysteresis of the Contact Angle of Sessile Droplets on Smooth Homogeneous Substrates |
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141 | (1) |
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Expressions for the Advancing Contact Angle |
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142 | (3) |
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Expressions for the Receding Contact Angle |
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145 | (1) |
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146 | (1) |
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3.3 Hysteresis of Contact Angle of Sessile Droplets on Deformable Substrates |
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146 | (9) |
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147 | (1) |
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Equilibrium Contact Angle of Droplet on Deformable Substrates and the Surface Forces Action: A Simplified Model Adopted in this Section |
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147 | (2) |
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Theory and Model for Hysteresis of Contact Angle on a Deformable Substrate |
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149 | (4) |
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153 | (2) |
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155 | (1) |
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Appendix: Advancing Contact Angle |
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155 | (2) |
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157 | (4) |
4 Kinetics of Wetting |
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161 | (110) |
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161 | (7) |
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4.1 Spreading of Nonvolatile Liquid Drops over Flat Solid Substrates: Qualitative Analysis |
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168 | (17) |
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Capillary Regime of Spreading |
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172 | (5) |
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Gravitational Spreading as a Continuation of the Capillary Spreading Regime |
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177 | (1) |
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178 | (2) |
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Spreading of Very Thin Droplets |
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180 | (5) |
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4.2 Spreading of Nonvolatile Liquid Drops over Dry Surfaces: Influence of Surface Forces |
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185 | (11) |
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191 | (1) |
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191 | (3) |
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Comparison with Experiments |
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194 | (2) |
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196 | (1) |
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196 | (1) |
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197 | (1) |
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198 | (1) |
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199 | (1) |
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4.3 Spreading of Drops over a Surface Covered with a Thin Layer of the Same Liquid |
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200 | (6) |
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4.4 Quasi-Steady-State Approach in the Kinetics of Spreading |
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206 | (7) |
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4.5 Dynamic Advancing Contact Angle and the Form of the Moving Meniscus in Flat Capillaries in the Case of Complete Wetting |
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213 | (4) |
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217 | (3) |
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Asymptotic Behavior of Solution of y3 d3y/dx3 = y - 1 at y right arrow infinity |
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217 | (3) |
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4.6 Motion of Long Drops in Thin Capillaries in the Case of Complete Wetting |
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220 | (8) |
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228 | (3) |
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4.7 Liquid Film Coating of a Moving Thin Cylindrical Fiber |
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231 | (7) |
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232 | (1) |
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Derivation of the Equation for the Liquid-Liquid Interface Profile |
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232 | (2) |
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Equilibrium Configuration |
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234 | (1) |
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Matching of Asymptotic Solutions in Zones I and II |
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234 | (2) |
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Equilibrium Case (Ca = 0) |
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236 | (1) |
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237 | (1) |
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4.8 Blow-off Method for Investigating Boundary Viscosity of Volatile Liquids |
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238 | (14) |
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238 | (1) |
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239 | (12) |
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249 | (2) |
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251 | (1) |
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4.9 Combined Heat and Mass Transfer in Tapered Capillaries with Bubbles under the Action of a Temperature Gradient |
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252 | (6) |
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255 | (1) |
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256 | (2) |
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4.10 Spreading of Non-Newtonian Liquids over Solid Substrates |
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258 | (11) |
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Governing Equation for the Evolution of the Profile of the Spreading Drop |
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258 | (4) |
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Gravitational Regime of Spreading |
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262 | (3) |
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Capillary Regime of Spreading |
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265 | (3) |
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268 | (1) |
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269 | (2) |
5 Spreading over Porous Substrates |
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271 | (78) |
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271 | (1) |
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5.1 Spreading of Liquid Drops over Saturated Porous Layers |
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272 | (10) |
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272 | (10) |
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Liquid inside the Drop (0 < z < h(t, r)) |
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272 | (1) |
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Inside the Porous Layer beneath the Drop (- Δ < z < 0, 0 < r < L) |
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273 | (5) |
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278 | (1) |
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Results and Discussion. Experimental Determination of the "Effective Lubrication Coefficient" ω |
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279 | (3) |
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5.2 Spreading of Liquid Drops over a Thin Dry Porous Layer: Complete Wetting Case |
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282 | (13) |
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282 | (15) |
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Inside the Porous Layer outside the Drop (- Δ < z < 0, L < r < l) |
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287 | (3) |
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290 | (1) |
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Independent Determination of Kppc |
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290 | (1) |
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291 | (4) |
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295 | (2) |
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5.3 Spreading of Liquid Drops over Thick Porous Substrates: Complete Wetting Case |
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297 | (11) |
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298 | (10) |
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Inside the Porous Substrate |
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300 | (1) |
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300 | (1) |
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301 | (2) |
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Spreading of Silicone Oil Drops of Different Viscosity over Identical Glass Filters |
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303 | (1) |
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Spreading of Silicone Oil Drops over Filters with Similar Properties but Made of Different Materials |
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304 | (1) |
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Spreading of Silicone Oil Drops with the Same Viscosity (η = 5 P) over Glass Filters with Different Porosity and Average Pore Size |
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305 | (3) |
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308 | (1) |
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5.4 Spreading of Liquid Drops from a Liquid Source |
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308 | (8) |
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309 | (7) |
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Experimental Setup and Results |
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312 | (3) |
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312 | (1) |
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313 | (2) |
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315 | (1) |
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316 | (5) |
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Capillary Regime, Complete Wetting |
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316 | (3) |
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Gravitational Regime, Complete Wetting |
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319 | (2) |
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321 | (1) |
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5.5 Spreading of Non-Newtonian Liquids over Dry Porous Layer. Complete and Partial Wetting Cases |
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321 | (22) |
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Partial and Complete Wetting Cases |
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322 | (1) |
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5.5.1 Complete Wetting Case |
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323 | (14) |
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323 | (1) |
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324 | (13) |
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325 | (1) |
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Spreading above Porous Substrate |
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326 | (2) |
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Inside the Porous Layer outside the Drop (- Δ < z < 0, L < r < l) |
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328 | (3) |
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331 | (1) |
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Numerical Solution of Eqs. (5.132) and (5.133) |
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332 | (1) |
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333 | (3) |
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Conclusions on Section "Complete Wetting Case" |
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336 | (1) |
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5.5.2 Partial Wetting Case |
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337 | (6) |
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337 | (1) |
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338 | (1) |
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Pores of the Porous Substrate Are Large Enough and Red Blood Cells Penetrate into the Substrate with Plasma Flow |
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339 | (1) |
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The Second Stage of the Process |
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339 | (1) |
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Pores inside the Porous Substrate Are Small and Red Blood Cells Do Not Penetrate into the Porous Substrate |
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340 | (2) |
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Conclusions on Section "Partial Wetting Case" |
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342 | (1) |
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343 | (1) |
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Capillary Imbibition of Non-Newtonian Liquid into a Thin Capillary |
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343 | (1) |
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One-Dimensional Penetration of a Non-Newtonian Liquid into a Porous Medium |
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344 | (1) |
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344 | (1) |
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345 | (4) |
6 Wetting of Wetting/Spreading in the Presence of Surfactants |
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349 | (72) |
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349 | (1) |
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6.1 Spreading of Aqueous Surfactant Solutions over Porous Layers |
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349 | (11) |
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Experimental Methods and Materials |
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350 | (1) |
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Spreading on Porous Substrates |
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350 | (9) |
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Measurement of Static Advancing and Receding Contact Angles on Nonporous Substrates |
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351 | (1) |
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352 | (3) |
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Advancing and Hydrodynamic Receding Contact Angles on Porous Nitrocellulose Membranes |
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355 | (2) |
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Static Hysteresis of the Contact Angle of SDS Solution Drops on Smooth Nonporous Nitrocellulose Substrate |
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357 | (2) |
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359 | (1) |
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6.2 Spontaneous Capillary Imbibition of Surfactant Solutions into Hydrophobic Capillaries |
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360 | (12) |
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362 | (3) |
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Concentration below the CMC |
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365 | (2) |
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Concentration above the CMC |
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367 | (3) |
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Spontaneous Capillary Rise in Hydrophobic Capillaries |
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370 | (2) |
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372 | (2) |
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Excess Free Energy of an Aqueous Surfactant Droplet on a Hydrophobic Substrate |
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372 | (2) |
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374 | (2) |
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6.3 Capillary Imbibition of Surfactant Solutions in Porous Media and Thin Capillaries: The Partial Wetting Case |
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376 | (10) |
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376 | (1) |
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Concentration below the CMC |
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377 | (6) |
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Concentration above the CMC |
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383 | (1) |
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384 | (1) |
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385 | (1) |
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6.4 Spreading of Surfactant Solutions over Hydrophobic Substrates |
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386 | (7) |
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387 | (3) |
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390 | (1) |
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390 | (1) |
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390 | (3) |
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6.5 Spreading of Insoluble Surfactants over Thin Viscous Liquid Layers |
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393 | (9) |
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Theory and Relation to Experiment |
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394 | (6) |
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400 | (2) |
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402 | (1) |
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Derivation of Governing Equations for Time Evolution of Both Film Thickness and Surfactant Surface Concentration |
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402 | (1) |
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403 | (1) |
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Influence of Capillary Forces during the Initial Stage of Spreading |
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403 | (1) |
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404 | (1) |
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Derivation of Boundary Condition at the Moving Shock Front |
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404 | (1) |
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405 | (1) |
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Matching of Asymptotic Solutions at the Moving Shock Front |
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405 | (1) |
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406 | (1) |
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Solution of the Governing Equations for the Second Stage of Spreading |
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406 | (1) |
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6.6 Spreading of Aqueous Droplets Induced by Overturning of Amphiphilic Molecules or Their Fragments in the Surface Layer of an Initially Hydrophobic Substrate |
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406 | (14) |
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Theory, Derivation of Basic Equations |
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407 | (4) |
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411 | (4) |
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415 | (3) |
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Comparison between Theory and Experimental Data |
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418 | (2) |
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420 | (1) |
7 Kinetics of Simultaneous Spreading and Evaporation |
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421 | (44) |
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421 | (1) |
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7.1 Basic Properties of Simultaneous Spreading/Evaporation |
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422 | (4) |
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422 | (1) |
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The Complete Wetting Case |
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423 | (2) |
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Dependence of Evaporation Flux on Droplet Size |
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424 | (1) |
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Thermal Phenomena at Evaporation |
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425 | (1) |
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7.2 Spreading and Evaporation of Sessile Droplets: Universal Behavior in the Case of Complete Wetting |
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426 | (15) |
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426 | (1) |
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427 | (9) |
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436 | (3) |
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436 | (1) |
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436 | (1) |
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436 | (1) |
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Extracting Theoretical Parameters from Experimental Data |
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437 | (1) |
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Comparison of Experimental Data and Predicted Universal Behavior |
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438 | (1) |
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439 | (1) |
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440 | (1) |
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440 | (1) |
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440 | (1) |
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440 | (1) |
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440 | (1) |
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7.3 Evaporation of Sessile Droplets: Universal Behavior in the Presence of Contact Angle Hysteresis |
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441 | (6) |
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441 | (1) |
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442 | (2) |
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442 | (1) |
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Two Stages of Evaporation of a Sessile Droplet |
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442 | (2) |
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Validation against Experimental Data |
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444 | (3) |
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447 | (1) |
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7.4 Spreading and Evaporation of Surfactant Solutions |
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447 | (7) |
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447 | (1) |
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448 | (1) |
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449 | (3) |
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Theory Presented in Section 7.3 and Used in This Section for the Spreading/Evaporation of Surfactant Solutions |
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450 | (1) |
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Comparison of the Experimental Data for Evaporation of Surfactant Solutions with the Theoretical Predictions for Pure Liquids |
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450 | (2) |
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452 | (2) |
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7.5 Evaporation of Microdroplets |
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454 | (9) |
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454 | (1) |
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454 | (1) |
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Governing Equations in the Bulk Phases |
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455 | (1) |
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455 | (4) |
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459 | (1) |
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459 | (3) |
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459 | (2) |
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Influence of Thermal Effects |
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461 | (1) |
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462 | (1) |
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463 | (2) |
8 Main Problems in Kinetics of Wetting and Spreading to Be Solved |
|
465 | (2) |
Index |
|
467 | |