Details

Electrowetting


Electrowetting

Fundamental Principles and Practical Applications
1. Aufl.

von: Frieder Mugele, Jason Heikenfeld

97,99 €

Verlag: Wiley-VCH
Format: EPUB
Veröffentl.: 12.12.2018
ISBN/EAN: 9783527412419
Sprache: englisch
Anzahl Seiten: 312

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Beschreibungen

Starting from the basic principles of wetting, electrowetting and fluid dynamics all the way up to those engineering aspects relevant for the development of specific devices, this is a comprehensive introduction and overview of the theoretical and practical aspects. <br> Written by two of the most knowledgeable experts in the field, the text covers both current as well as possible future applications, providing basic working principles of lab-on-a-chip devices and such optofluidic devices as adaptive lenses and optical switches. Furthermore, novel e-paper display technology, energy harvesting and supercapacitors as well as electrowetting in the nano-world are discussed. Finally, the book contains a series of exercises and questions for use in courses on microfluidics or electrowetting. <br> With its all-encompassing scope, this book will equally serve the growing community of students and academic and industrial researchers as both an introduction and a standard reference.<br>
<p>Preface xi</p> <p><b>1 Introduction to Capillarity and Wetting Phenomena</b> <b>1</b></p> <p>1.1 Surface Tension and Surface Free Energy 2</p> <p>1.1.1 The Microscopic Origin of Surface Energies 2</p> <p>1.1.2 Macroscopic Definition of Surface Energy and Surface Tension 5</p> <p>1.2 Young–Laplace Equation: The Basic Law of Capillarity 7</p> <p>1.2.1 Laplace’s Equation and the Pressure Jump Across Liquid Surfaces 7</p> <p>1.2.2 Applications of the Young–Laplace Equation: The Rayleigh–Plateau Instability 11</p> <p>1.3 Young–Dupré Equation: The Basic Law of Wetting 13</p> <p>1.3.1 To Spread or Not to Spread: From Solid Surface Tension to Liquid Spreading 13</p> <p>1.3.2 Partial Wetting: The Young Equation 16</p> <p>1.4 Wetting in the Presence of Gravity 19</p> <p>1.4.1 Bond Number and Capillary Length 21</p> <p>1.4.2 Case Studies 22</p> <p>1.4.2.1 The Shape of a Liquid Puddle 22</p> <p>1.4.2.2 The Pendant Drop Method: Measuring Surface Tension by Balancing Capillary and Gravity Forces 24</p> <p>1.4.2.3 Capillary Rise 25</p> <p>1.5 Variational Derivation of the Young–Laplace and the Young–Dupré Equation 26</p> <p>1.6 Wetting at the Nanoscale 29</p> <p>1.6.1 The Effective Interface Potential 30</p> <p>1.6.2 Case Studies 32</p> <p>1.6.2.1 The Effective Interface Potential for van der Waals Interaction 32</p> <p>1.6.2.2 Equilibrium Surface Profile Near the Three-Phase Contact Line 34</p> <p>1.7 Wetting of Heterogeneous Surfaces 35</p> <p>1.7.1 Young–Laplace and Young–Dupré Equation for Heterogeneous Surfaces 35</p> <p>1.7.2 Gibbs Criterion for Contact Line Pinning at Domain Boundaries 37</p> <p>1.7.3 From Discrete Morphology Transitions to Contact Angle Hysteresis 38</p> <p>1.7.4 Optimum Contact Angle on Heterogeneous Surfaces: The Laws of Wenzel and Cassie 43</p> <p>1.7.5 Superhydrophobic Surfaces 45</p> <p>1.7.6 Wetting of Heterogeneous Surfaces in Three Dimensions 48</p> <p>1.7.7 Wetting of Complex Surfaces in Three Dimensions: Morphology Transitions, Instabilities, and Symmetry Breaking 50</p> <p>1.A Mechanical Equilibrium and Stress Tensor 55</p> <p>Problems 56</p> <p>References 58</p> <p><b>2 Electrostatics</b> <b>61</b></p> <p>2.1 Fundamental Laws of Electrostatics 61</p> <p>2.1.1 Electric Fields and the Electrostatic Potential 61</p> <p>2.1.2 Specific Examples 64</p> <p>2.2 Materials in Electric Fields 66</p> <p>2.2.1 Conductors 66</p> <p>2.2.2 Dielectrics 68</p> <p>2.2.3 Dielectric Liquids and Leaky Dielectrics 73</p> <p>2.3 Electrostatic Energy 76</p> <p>2.3.1 Energy of Charges, Conductors, and Electric Fields 76</p> <p>2.3.2 Capacitance Coefficients and Capacitance 78</p> <p>2.3.3 Thermodynamic Energy of Charged Systems: Constant Charge Versus Constant Potential 80</p> <p>2.4 Electrostatic Stresses and Forces 82</p> <p>2.4.1 Global Forces Acting on Rigid Bodies 82</p> <p>2.4.2 Local Forces: The Maxwell Stress Tensor 83</p> <p>2.4.3 Stress Boundary Condition at Interfaces 85</p> <p>2.5 Two Generic Case Studies 87</p> <p>2.5.1 Parallel Plate Capacitor 87</p> <p>2.5.2 Charge and Energy Distribution for Two Capacitors in Series 90</p> <p>Problems 92</p> <p>References 93</p> <p><b>3 Adsorption at Interfaces</b> <b>95</b></p> <p>3.1 Adsorption Equilibrium 96</p> <p>3.1.1 General Principles 96</p> <p>3.1.2 Langmuir Adsorption 96</p> <p>3.1.3 Reduction of Surface Tension 99</p> <p>3.2 Adsorption Kinetics 101</p> <p>3.3 Surface-Active Solutes: From Surfactants to Polymers, Proteins, and Particles 105</p> <p>3.A A StatisticalMechanics Model of Interfacial Adsorption 107</p> <p>Problems 110</p> <p>References 110</p> <p><b>4 From Electric Double Layer Theory to Lippmann’s Electrocapillary Equation</b> <b>113</b></p> <p>4.1 Electrocapillarity: the Historic Origins 113</p> <p>4.2 The Electric Double Layer at Solid–Electrolyte Interfaces 115</p> <p>4.2.1 Poisson–Boltzmann Theory and Gouy–Chapman Model of the EDL 116</p> <p>4.2.2 Total Charge and Capacitance of the Diffuse Layer 120</p> <p>4.2.3 Voltage Dependence of the Free Energy: Electrowetting 122</p> <p>4.3 Shortcomings of Poisson–Boltzmann Theory and the Gouy–Chapman Model 124</p> <p>4.4 Teflon–Water Interfaces: a Case Study 125</p> <p>4.A StatisticalMechanics Derivation of the Governing Equations 127</p> <p>Problems 130</p> <p>References 130</p> <p><b>5 Principles of Modern Electrowetting</b> <b>133</b></p> <p>5.1 The Standard Model of Electrowetting (on Dielectric) 133</p> <p>5.1.1 Electrowetting Phenomenology 133</p> <p>5.1.2 Macroscopic EW Response 136</p> <p>5.1.3 Microscopic Structure of the Contact Line Region 138</p> <p>5.2 Interpretation of the StandardModel of EW 145</p> <p>5.2.1 The Electromechanical Interpretation 145</p> <p>5.2.2 StandardModel of EW Versus Lippmann’s Electrocapillarity 145</p> <p>5.2.3 Limitations of the Standard Model: Nonlinearities and Contact Angle Saturation 149</p> <p>5.3 DC Versus AC Electrowetting 151</p> <p>5.3.1 General Principles 151</p> <p>5.3.2 Application Example: Parallel Plate Geometry 153</p> <p>Problems 156</p> <p>References 157</p> <p><b>6 Elements of Fluid Dynamics</b> <b>159</b></p> <p>6.1 Navier–Stokes Equations 159</p> <p>6.1.1 General Principles: from Newton to Navier–Stokes 160</p> <p>6.1.2 Boundary Conditions 163</p> <p>6.1.3 Nondimensional Navier–Stokes Equation: The Reynolds Number 166</p> <p>6.1.4 Example: Pressure-Driven Flow Between Two Parallel Plates 167</p> <p>6.2 Lubrication Flows 170</p> <p>6.2.1 General Lubrication Flows 170</p> <p>6.2.2 Lubrication Flows with a Free Liquid Surface 173</p> <p>6.2.3 Application I: Linear Stability Analysis of aThin Liquid Film 174</p> <p>6.2.4 Application II: Entrainment of Liquid Films 176</p> <p>6.3 Contact Line Dynamics 179</p> <p>6.3.1 Tanner’s Law and the Spreading of Drops on Macroscopic Scales 179</p> <p>6.3.2 Surface Profiles on the Mesoscopic Scale: The Cox–Voinov Law 181</p> <p>6.3.3 Dynamics of the Microscopic Contact Angle: The Molecular Kinetic Picture 182</p> <p>6.3.4 Comparison to Experimental Results 183</p> <p>6.4 SurfaceWaves and Drop Oscillations 185</p> <p>6.4.1 SurfaceWaves 187</p> <p>6.4.2 Oscillating Drops 188</p> <p>6.4.3 Example: Electrowetting-Driven Excitation of Eigenmodes of a Sessile Drop 192</p> <p>6.4.4 General Consequences 193</p> <p>Problems 194</p> <p>References 196</p> <p><b>7 Electrowetting Materials and Fabrication</b> <b>197</b></p> <p>7.1 Practical Requirements 197</p> <p>7.2 Electrowetting Deviation: Caused by Non-obvious Materials Behavior 198</p> <p>7.2.1 Commonly Observed Temporal Deviations 199</p> <p>7.2.1.1 Dielectric Failure (Leakage Current) 199</p> <p>7.2.1.2 Dielectric Charging 201</p> <p>7.2.1.3 Charges into the Oil 202</p> <p>7.2.1.4 Oil Relaxation 202</p> <p>7.2.1.5 Surfactant Diffusion (Interface Absorption) 203</p> <p>7.2.1.6 Oil Film Trapping 203</p> <p>7.2.2 Commonly Observed Nontemporal Deviation 204</p> <p>7.2.2.1 Unexpected Young’s Angles: Gravity Effects 204</p> <p>7.2.2.2 Unexpected Young’s Angles: Surface and Interface Fouling 204</p> <p>7.2.2.3 Unexpected Young’s Angles: Dielectric Charging 205</p> <p>7.2.2.4 Wetting Hysteresis 205</p> <p>7.2.3 Deviation That Is Often Both Highly Temporal and Nontemporal 206</p> <p>7.2.3.1 Chemical/Surface Potentials 206</p> <p>7.3 Electrowetting Saturation 207</p> <p>7.4 The Invariant Onset of Deviation or Saturation and Lack of a Universal Theory for This Invariance 208</p> <p>7.4.1 The Invariance of Saturation for Aqueous Conducting Fluids 208</p> <p>7.4.2 The Invariance of the Onset of Deviation or Saturation for All Types of Conducting Fluids with 𝛾ci > 5 mNm−1 209</p> <p>7.4.3 Summary 209</p> <p>7.5 Choosing Materials: Large Young’s Angle and LowWetting Hysteresis 210</p> <p>7.5.1 Conventional Ultralow Surface Energy Coatings (Fluoropolymers) 211</p> <p>7.5.2 Hydrophilic Coatings Made HydrophobicThrough Proper Choice of Insulating Fluid 213</p> <p>7.5.3 Superhydrophobic Coatings: Larger Young’s Angle in Air but Small Modulation Range 213</p> <p>7.6 Choosing Materials: the Electrowetting Dielectric (Capacitor) 215</p> <p>7.6.1 Current State of the Art for Low Potential Electrowetting:Multilayer Dielectrics 218</p> <p>7.6.2 A Note of Critical Importance for the Topcoat in a Multilayer System 219</p> <p>7.6.3 Carefully Choosing the Best Materials for Each Individual Layer of the Dielectric Stack 219</p> <p>7.6.3.1 First Layer: Inorganic Dielectrics 219</p> <p>7.6.3.2 Second Layer: Organic Dielectrics 220</p> <p>7.6.3.3 Third Layer: Fluoropolymer 220</p> <p>7.6.3.4 The Simplest Approaches Available to Electrowetting Practitioners 220</p> <p>7.7 Choosing Materials: Insulating and Conducting Fluids 221</p> <p>7.7.1 The Insulating Fluid 221</p> <p>7.7.2 The Conducting Fluid 221</p> <p>7.7.2.1 Ionic Content 222</p> <p>7.7.2.2 Don’t UseWater! 223</p> <p>7.8 Summary of General Best Practices 224</p> <p>7.9 Mitigating Surface Fouling in Biological Applications 224</p> <p>7.10 Additional Issues for Complex or Integrated Devices 226</p> <p>Acknowledgement 227</p> <p>7.A Trapped Charge Derivation 227</p> <p>Problems 229</p> <p>References 231</p> <p><b>8 Fundamentals of Applied Electrowetting 235</b></p> <p>8.1 Introduction and Scope 235</p> <p>8.2 Droplet Transport 235</p> <p>8.2.1 Basic Force Balance Interpretation of Droplet Transport 235</p> <p>8.2.2 Advanced Droplet Transport Physics:Threshold and Velocity 237</p> <p>8.2.2.1 Advanced Droplet Transport Physics: Flow Field 239</p> <p>8.2.3 Additional Practical Notes on Implementation of Basic Droplet Transport 240</p> <p>8.3 Droplet Transport for Splitting, Dosing, Merging, and Mixing 240</p> <p>8.3.1 Simple Experimental Examples 241</p> <p>8.3.2 Fundamentals of Droplet Splitting 241</p> <p>8.3.2.1 Influence of Vertical Radii of Curvature 242</p> <p>8.3.2.2 Influence of Horizontal Radii of Curvature 242</p> <p>8.3.3 Fundamentals of Droplet Dosing (Dispensing) 243</p> <p>8.3.4 Fundamentals of Droplet Mixing 244</p> <p>8.4 Stationary Droplet Oscillation, Jumping, and Mixing 244</p> <p>8.4.1 Droplet Oscillation 244</p> <p>8.4.2 Droplet Oscillation and Jumping 245</p> <p>8.4.3 Droplet Oscillation and Hysteresis 245</p> <p>8.4.4 Droplet Oscillation and Mixing 246</p> <p>8.5 Gating, Valving, and Pumping 247</p> <p>8.5.1 Fundamentals 247</p> <p>8.6 Generating Droplets and Channels 249</p> <p>8.6.1 Fundamentals for Droplet Generation 249</p> <p>8.6.2 Fundamentals for Channel Generation 250</p> <p>8.7 Shape Change in a Channel 251</p> <p>8.7.1 Fundamentals 251</p> <p>8.8 Control of Meniscus Curvature 252</p> <p>8.8.1 Fundamentals 252</p> <p>8.8.2 Additional Notes on Implementation 253</p> <p>8.9 Control of Meniscus Surface Area/Coverage 253</p> <p>8.9.1 Fundamentals 253</p> <p>8.9.2 Additional Notes on Implementation 254</p> <p>8.10 Control of Film Breakup and Oil Entrapment 255</p> <p>8.10.1 Fundamentals 255</p> <p>8.11 1D, 2D, and 3D Control of Rigid Objects 257</p> <p>8.11.1 Fundamentals 257</p> <p>8.12 Reverse Electrowetting and Energy Harvesting 258</p> <p>Problems 260</p> <p>References 261</p> <p><b>9 Related and Emerging Topics 265</b></p> <p>9.1 Introduction and Scope 265</p> <p>9.2 Dielectrophoresis and Dielectrowetting 265</p> <p>9.2.1 Basic Dielectrophoresis 265</p> <p>9.2.2 Dielectrowetting 267</p> <p>9.3 Innovations in Liquid Metal Electrowetting and Electrocapillarity 269</p> <p>9.3.1 Electrowetting of GaInSn Liquid Metal Alloys 269</p> <p>9.3.2 Giant Electrochemical Changes in Liquid Metal Interfacial Surface Tensions 270</p> <p>9.4 Nonequilibrium Electrical ControlWithout Contact Angle Modulation 271</p> <p>9.4.1 Some Limitations of Conventional Electrowetting 271</p> <p>9.4.2 ElectrowettingWithoutWetting 272</p> <p>Problems 273</p> <p>References 274</p> <p><b>Appendix Historical Perspective of Modern Electrowetting: </b><b>Individual Testimonials 277</b></p> <p>Introduction and Scope 277</p> <p>“CJ” Kim 277</p> <p>Authors Note from Heikenfeld 278</p> <p>Johan Feenstra 278</p> <p>Tom Jones 279</p> <p>FriederMugele 280</p> <p>Richard Fair 281</p> <p>Author’s Note from Heikenfeld 282</p> <p>Bruno Berge 282</p> <p>Glen McHale 285</p> <p>Stein Kuiper 286</p> <p>Jason Heikenfeld 288</p> <p>Kwan Hyung Kang: An Appreciation by T. B. Jones 289</p> <p>Author’s Note from Mugele 290</p> <p>References 290</p> <p>Index 293</p>
Frieder Mugele is the head of the Physics of Complex Fluids group at the University of Twente in Enschede, The Netherlands. Having obtained his academic degrees in physics at the University of Konstanz, Germany, he spent several years at the University of California in Berkeley, USA, and the University of Ulm, Germany, before his present appointment in Twente. Professor Mugele's research focuses on various aspects of solid-liquid interfaces and the properties of liquids on the micro- and nanoscale. He has been active in electrowetting since the late 1990s contributing in particular to the theoretical understanding and to fundamental concepts of electrowetting-driven microfluidics.<br> <br> Jason Heikenfeld is a Professor and Assistant Vice President for Commercialization at the Univ. of Cincinnati. He directs the Novel Devices Laboratory which has established highly-focused international leadership roles in an emergent technological paradigms including electrowetting, electronic paper, and most recently sweat biosensing technology. Prof. Heikenfeld's research approach centers on discovering and addressing the hidden challenges that can hinder the transition of innovative science into commercial application. Professor Heikenfeld is also a prolific inventor and serial entrepreneur, and during his teaching years was the highest-rated STEM educator at the University of Cincinnati.

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