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Recent Advances in Electrowetting Microdroplet Technologies
Chapter 4 Recent Advances in Electrowetting Microdroplet Technologies Robert W. Barber and David R. Emerson 4.1 Introduction The ability to handle small volumes of liquid, typically from a few picolitres (pL) to a few microlitres (mL), has the potential to improve the performance of complex chemical and biological assays [1–6]. The benefits of miniaturisation are well documented [7–9] and include smaller sample requirements, reduced reagent con- sumption, decreased analysis time, lower power consumption, lower costs per assay and higher levels of throughput and automation. In addition, miniaturisation may offer enhanced functionality that cannot be achieved in conventional macroscale devices, such as the ability to combine sample collection, analyte extraction, preconcentration, filtration and sample analysis onto a single microfluidic chip [10]. Microfluidics-based lab-on-a-chip devices have received considerable attention in recent years, and are expected to revolutionise clinical diagnostics, DNA and protein analysis and many other laboratory procedures involving molecular biology [11–13]. Currently, most lab-on-a-chip devices employ continuous fluid flow through closed microchannels. However, an alternative approach, which is rapidly gaining popularity, is to mani- pulate the liquid in the form of discrete, unit-sized microdroplets—an approach which is often referred to as digital microfluidics [14–18]. The use of droplet-based microfluidics offers many benefits over continuous flow systems; one of the main advantages is that the reaction or assay can be performed sequentially in a similar manner to traditional (macroscale) laboratory techniques. Consequently, a wide range of established chemical and biological protocols can be transferred to the micro-scale without the need to establish continuous flow protocols for the same reaction. -
Colloidal Properties of Aqueous Suspensions of Acid-Treated, Multi-Walled Carbon Nanotubes Billy Smith, Kevin Wepasnick, K
Subscriber access provided by Johns Hopkins Libraries Article Colloidal Properties of Aqueous Suspensions of Acid-Treated, Multi-Walled Carbon Nanotubes Billy Smith, Kevin Wepasnick, K. E. Schrote, A. R. Bertele, William P. Ball, Charles O’Melia, and D. Howard Fairbrother Environ. Sci. Technol., 2009, 43 (3), 819-825 • DOI: 10.1021/es802011e • Publication Date (Web): 29 December 2008 Downloaded from http://pubs.acs.org on February 4, 2009 More About This Article Additional resources and features associated with this article are available within the HTML version: • Supporting Information • Access to high resolution figures • Links to articles and content related to this article • Copyright permission to reproduce figures and/or text from this article Environmental Science & Technology is published by the American Chemical Society. 1155 Sixteenth Street N.W., Washington, DC 20036 Environ. Sci. Technol. 2009, 43, 819–825 CNTs is enormous, providing the impetus for dramatic Colloidal Properties of Aqueous increases in their annual production rates: Bayer anticipates Suspensions of Acid-Treated, production rates of 200 tons/yr by 2009, and 3,000 tons/yr by 2012 (4). Multi-Walled Carbon Nanotubes Many CNT applications (e.g., as components of drug delivery agents, composite materials) require CNT suspen- sions that remain stable in polar mediums such as water or BILLY SMITH,† KEVIN WEPASNICK,† polymeric resins (5, 6). Due to strongly attractive van der K. E. SCHROTE,§ A. R. BERTELE,§ | | Waals forces between the hydrophobic graphene surfaces, WILLIAM P. BALL, CHARLES O’MELIA, AND D. HOWARD FAIRBROTHER*,†,‡ pristine CNTs minimize their surface free energy by forming settleable aggregates in solution. To prepare uniform, well- Department of Chemistry, The Johns Hopkins University, dispersed mixtures, the CNTs’ exterior surface must be Baltimore, Maryland 21218, Department of Materials Science modified. -
Opto-Electrowetting (OEW)
Nano-Bio-Sens ing Summer Sc hoo l @ EPFL June 29 – July 3, 2009 Introduction to Optofluidics Ming C. Wu University of California, Berkeley Electrical Engineering & Computer Sciences Dept. Berkeley Sensor and Actuator Center (BSAC) [email protected] .edu Wu-1 ©2009. University of California Optofluidics • Electrowetting optics • Tunable lenses • Electronic papers • Optical trapping and manipulation • Optofluidic lab-on-a-chip • Microresonators • Photonic crystals Wu-2 ©2009. University of California Optofluidics • Integration of optics and fluidics to synthesize novel functionalities • Applications: Li, et. al., Opt. Express, 2006 – Use microfluidics to control light • Optical switches, tunable lenses • Display • Sensors – Use light t o cont rol micro flu idics, micro/nanoparticles, cells, … Wolfe, et. al., Proc. Natl. Acad. Sci. , 2004 • Optical trapping, sorting, and assembly • Non-invasive optical actuation Psaltis, et. al., Nature, 2006 Domachuck, et. al., Nature, 2005 Wu-3 ©2009. University of California “Bubble” Switches Agilent Champaign Switch • Optical crossbar switch using total internal reflection by a thermally generated bubble • 32x32 switches have been demonstrated • J. E. Fouquet, "Compact optical cross-connect switch based on total internal reflection in a fluid- containing planar lightwave circuit,“ OFC 2006 Wu-4 ©2009. University of California Optofludic Microscopy • Low-cost, high-resolution (0.8 !m), lensless on-chip microscopes • Use micro flu idic flow to de liver specimens across apertures on a metal-coated CMOS sensor X. Cui, L. M. Lee, X. Heng, W. Zhong, P. W. Sternberg, D. Psaltis, and C. Yang, "Lensless high-resolution on-chip optofluidic microscopes for Caenorhabditis elegans and cell imaging," Proceedings of the National Academy of Sciences, vol. -
Combining Electrowetting and Magnetic Bead Manipulations for Use in Microfluidic Immunoassays
Combining Electrowetting and Magnetic Bead Manipulations for Use in Microfluidic Immunoassays Amanda Barbour Ronit Langer [email protected] [email protected] Tiffany Li Katherine Tsang [email protected] [email protected] Rose Yin [email protected] Abstract afford to lose large amounts of blood.1 It This experiment investigated reducing the also takes 2 days of incubation time, which cost of microfluidic immunoassays. places a risk on patients with urgent health Magnetic microbeads are used in these concerns.1 Technologies in microfluidics assays to increase the efficiency of have created a different type of immunoassays, but they also raise the cost. immunoassay that uses magnetic This experiment aims to reduce the number microbeads. It can be performed within of magnetic beads necessary by using minutes with only 5-10 µL of blood, making electrowetting in conjunction with the beads. it safer for patients who cannot afford to lose Single and parallel plate electrowetting blood, and more efficient for doctors.2 devices were tested individually and the However, this process is very expensive due magnetic microbeads. The devices did not to the large number of microbeads needed. succeed in separating the beads from the During the assay, the microbeads need to be droplets, but the results show many separated from each sample and pulled promising options for further investigation. through microchannels into a new solution. In order to separate, the microbeads need to 1. Introduction break the surface tension of the sample, and 3 With the increasing pace of today’s society, this requires thousands of microbeads. current medicine requires fast and accurate This project aims to create a method diagnoses for patients. -
Towards Automated Optoelectrowetting on Dielectric Devices for Multi-Axis Droplet Manipulation
2013 IEEE International Conference on Robotics and Automation (ICRA) Karlsruhe, Germany, May 6-10, 2013 Towards Automated Optoelectrowetting on Dielectric Devices for Multi-Axis Droplet Manipulation Vasanthsekar Shekar, Matthew Campbell, and Srinivas Akella Abstract— Lab-on-a-chip technology scales down multiple layout of electrodes, and layout design restrictions arising laboratory processes to a chip capable of performing automated from electrode addressing constraints. We can overcome biochemical analyses. Electrowetting on dielectric (EWOD) is a these limitations by light-actuated droplet manipulation. digital microfluidic lab-on-a-chip technology that uses patterned electrodes for droplet manipulation. The main limitations of EWOD devices are the restrictions in volume and motion of Optoelectrowetting (OEW) is a light-actuated droplet ma- droplets due to the fixed size, layout, and addressing scheme of nipulation technique using optical sources and electric fields. the electrodes. Optoelectrowetting on dielectric (OEWOD) is a A projected pattern of light, which acts as a virtual electrode, recent technology that uses optical sources and electric fields for is moved to manipulate the droplet. The optical source droplet actuation on a continuous surface. We describe an open surface light–actuated OEWOD device that can manipulate generating the patterns ranges from a laser [6] to an LCD droplets of multiple volumes ranging from 1 to 50 µL at screen [7]. The main advantages of OEW devices are the voltages below 45 V. To achieve lower voltage droplet actuation simplicity in fabrication process and the large continuous than previous open configuration devices, we added a dedicated droplet manipulation region compared to EWOD devices. dielectric layer of high dielectric constant (Al2O3 with εr of 9.1) Devices that use OEW on a dielectric surface for droplet and significantly reduced the thickness of the hydrophobic layer. -
Digital Microfluidics
Microfluid Nanofluid DOI 10.1007/s10404-007-0161-8 REVIEW Digital microfluidics: is a true lab-on-a-chip possible? R. B. Fair Received: 10 February 2007 / Accepted: 14 February 2007 Ó Springer-Verlag 2007 Abstract The suitability of electrowetting-on-dielectric elemental operations, such as transport, mixing, or dis- (EWD) microfluidics for true lab-on-a-chip applications is pensing. These elemental operations are performed on an discussed. The wide diversity in biomedical applications elemental set of components, such as electrode arrays, can be parsed into manageable components and assembled separation columns, or reservoirs. Examples of the incor- into architecture that requires the advantages of being poration of these principles in complex biomedical appli- programmable, reconfigurable, and reusable. This capa- cations are described. bility opens the possibility of handling all of the protocols that a given laboratory application or a class of applications Keywords Lab-on-a-chip Á Digital microfluidics Á would require. And, it provides a path toward realizing the Biomedical applications Á Detection Á Analysis Á true lab-on-a-chip. However, this capability can only be Electrowetting realized with a complete set of elemental fluidic compo- nents that support all of the required fluidic operations. Architectural choices are described along with the reali- 1 Introduction zation of various biomedical fluidic functions implemented in on-chip electrowetting operations. The current status of Historically, microfluidic devices have been designed from this EWD toolkit is discussed. However, the question re- the bottom up, whereby various fluidic components are mains: which applications can be performed on a digital combined together to achieve a device that performs a microfluidic platform? And, are there other advantages particular application. -
Fundamentals and Applications of Electrowetting: a Critical Review
Fundamentals and Applications of Electrowetting: A Critical Review Ya-Pu Zhao* and Ying Wang State Key Laboratory of Nonlinear Mechanics, Institute of Mechanics Chinese Academy of Sciences, Beijing 100190, China Abstract: We have witnessed rapid and exciting development in electrowetting (EW) or electrowetting-on-dielectric (EWOD) since 1990s. Owing to its great advantages such as easy operation, sensitive response and electrical reversibility, EW has found many applications in various fi elds, especially in micro- and nano-fl uidics, electronic display, etc. The aim of this review is to inspire new investigations on EW, not only in theory and numerical simulation, but also in experiments, and spur further research on EW for more practical applications. A comprehensive review is presented on the EW research progress, and experiments, theoretical modeling and numerical simulations are covered. After a brief look at the development history, some latest experimental and simulation methods, such as Lattice Boltzmann method, phase-fi eld method and molecular dynamics (MD), are introduced. Some representative practical applications are then presented. Unresolved issues and prospects on EW as the fi nal part of this review are expected to attract more attention and inspire more in-depth studies in this fascinating area. Keywords: Electrowetting (EW), electrowetting-on-dielectric (EWOD), Lippmann- Young (L-Y) equation, curvature effect, elasto-electro-capillarity (EEC), Lattice Boltzmann method (LBM), phase-fi eld model, molecular dynamics (MD) simulations, coffee stain ring, electronic display, liquid lens, Micro Total Analysis Systems (μ-TAS), cell-based digital microfl uidics 1 Motivation Electrowetting (EW) or electrowetting-on-dielectric (EWOD) is an indispensable and versatile means for droplet manipulation. -
Coalescence and Particle Self-Assembly of Inkjet-Printed Colloidal Drops
Coalescence and Particle Self-assembly of Inkjet-printed Colloidal Drops A Thesis Submitted to the Faculty of Drexel University by Xin Yang in partial fulfillment of the requirements for the degree of Doctor of Philosophy December 2014 ii © Copyright 2014 Xin Yang. All Rights Reserved. iii Acknowledgements I would like to thank my advisor Prof. Ying Sun. During the last 3 years, she supports and guides me throughout the course of my Ph.D. research with her profound knowledge and experience. Her dedication and passion for researches greatly encourages me in pursuing my career goals. I greatly appreciate her contribution to my growth during my Ph.D. training. I would like to thank my parents, my girlfriend, my colleagues (Brandon, Charles, Dani, Gang, Dong-Ook, Han, Min, Nate, and Viral) and friends (Abraham, Mahamudur, Kewei, Patrick, Xiang, and Yontae). I greatly appreciate Prof. Nicholas Cernansky, Prof. Bakhtier Farouk, Prof. Adam Fontecchio, Prof. Frank Ji, Prof. Alan Lau, Prof. Christopher Li, Prof. Mathew McCarthy, and Prof. Hongseok (Moses) Noh for their critical assessments and positive suggestions during my candidacy exam, proposal and my defense. I also appreciate the financial supports of National Science Foundation (Grant CAREER-0968927 and CMMI-1200385). iv TABLE OF CONTENTS LIST OF TABLES ............................................................................................................ vii LIST OF FIGURES ......................................................................................................... viii -
Electrical Double Layer Interactions with Surface Charge Heterogeneities
Electrical double layer interactions with surface charge heterogeneities by Christian Pick A dissertation submitted to Johns Hopkins University in conformity with the requirements for the degree of Doctor of Philosophy Baltimore, Maryland October 2015 © 2015 Christian Pick All rights reserved Abstract Particle deposition at solid-liquid interfaces is a critical process in a diverse number of technological systems. The surface forces governing particle deposition are typically treated within the framework of the well-known DLVO (Derjaguin-Landau- Verwey-Overbeek) theory. DLVO theory assumes of a uniform surface charge density but real surfaces often contain chemical heterogeneities that can introduce variations in surface charge density. While numerous studies have revealed a great deal on the role of charge heterogeneities in particle deposition, direct force measurement of heterogeneously charged surfaces has remained a largely unexplored area of research. Force measurements would allow for systematic investigation into the effects of charge heterogeneities on surface forces. A significant challenge with employing force measurements of heterogeneously charged surfaces is the size of the interaction area, referred to in literature as the electrostatic zone of influence. For microparticles, the size of the zone of influence is, at most, a few hundred nanometers across. Creating a surface with well-defined patterned heterogeneities within this area is out of reach of most conventional photolithographic techniques. Here, we present a means of simultaneously scaling up the electrostatic zone of influence and performing direct force measurements with micropatterned heterogeneously charged surfaces by employing the surface forces apparatus (SFA). A technique is developed here based on the vapor deposition of an aminosilane (3- aminopropyltriethoxysilane, APTES) through elastomeric membranes to create surfaces for force measurement experiments. -
Supplementary Information 1. Theory When an Electric Potential Is
Supplementary Information 1. Theory When an electric potential is applied between a metal-electrolyte interface, charges are redistributed and accumulate at the solid-liquid interface, forming an electrical double layer (EDL), which changes the surface energy of the solid-liquid interface [1]. Repulsion of like charges at the solid-liquid interface reduces the work required to expand the surface area, leading to a decrease in the associated surface tension and induces a change in the contact angle [1]. This phenomenon is called electrowetting [2]. The relationship between contact angle and applied electric potential is described using the Lippmann-Young equation, which can be derived using different approaches – the classical thermodynamic approach, the energy minimization approach, and the electromechanical approach. Here we present the classical thermodynamic approach in detail. The other two approaches can be found elsewhere [3]. a. The classical Thermodynamic Approach Consider a droplet of conductive liquid (electrolyte) placed on a smooth metal surface. The metal surface is in direct contact with the electrolyte, and a small potential difference is applied such that no current flows through the liquid and no Faradaic reactions take place on the metal surface [3]. Due to the application of an electric field, an electrical double layer (EDL) is formed in the liquid which is in contact with the metal surface [3]. The mathematical relationship between the surface charge distribution, surface tension and electric potential can be derived from Gibb’s interfacial thermodynamics [3], which yields: − = (1) Here is the effective surface tension of the solid-liquid interface, is the electric-field induced surface charge density at the solid-liquid interface, and V is the electric potential [3]. -
Shear Thickening in Colloidal Silica Chemical Mechanical
SHEAR THICKENING IN COLLOIDAL SILICA CHEMICAL MECHANICAL POLISHING SLURRIES by Anastasia Krasovsky A thesis submitted to the Faculty and the Board of Trustees of the Colorado School of Mines in partial fulfillment of the requirements for the degree of Master of Science (Chemical Engineering). Golden, Colorado Date _________________________ Signed: _________________________ Anastasia Krasovsky Signed: _________________________ Dr. Matthew W. Liberatore Thesis Advisor Golden, Colorado Date _________________________ Signed: _________________________ Dr. David W. M. Marr Professor and Head Department of Chemical and Biological Engineering ii ABSTRACT Chemical mechanical polishing (CMP) is used by the semiconductor manufacturing industry to polish materials under high shear for the fabrication of microelectronic devices such as computer chips. Under these high shear conditions, slurry particles can form agglomerates causing defects, which cost the semiconductor industry billions of dollars annually. The shear thickening behavior of colloidal silica CMP slurries (28-38 wt%) under high shear was studied using a rotating rheometer with parallel-plate geometry. The colloidal silica slurries showed continuous thickening and irreversible behavior at high shear rates (>10,000 s-1). Changing the silica concentration, adding monovalent chloride salts (NaCl, KCl, CsCl, and LiCl), adjusting the pH (pH 4 to pH 10.5), and mixing two particle sizes (d = 20 nm and 100 nm) within the slurry altered the thickening behavior of the slurries. Shear thickening behavior can be eliminated with certain large to small particle ratios. iii TABLE OF CONTENTS ABSTRACT…………………………………………………………………………………….. iii LIST OF FIGURES……………………………………………………………………………... vi LIST OF TABLES…………………………………………………………………………...... viii LIST OF SYMBOLS……………………………………………………………………………. ix LIST OF ABBREVIATIONS……………………………………………………………………. x CHAPTER 1 BACKGROUND………………………………………………………………… 1 1.1 Chemical Mechanical Polishing…………………………………………………. -
Understanding Adhesion: a Means for Preventing Fouling
ELSEVIER Understanding Adhesion: A Means for Preventing Fouling R. Oliveira • Adhesion of particulate materials is an important step in the formation Engenharia Biol6gica, of fouling. Because the size of such materials is generally less than 1 tzm, Unicersidade do Minho, the phenomenon can be described in terms of colloid chemistry. Accord- Braga, Portugal ingly, the net force of interaction between foulants and the surface has been described in terms of DLVO theory (van der Waals attraction and electrostatic double-layer repulsion). However, those forces are sometimes not sufficient to describe the formation of fouling. Recent works have made it possible to calculate the effect of hydrophobic interactions and steric forces, which can also be taken into account. In aqueous media, the various types of interactions can be strongly affected by the pH, the ionic strength, the type of ions, and the presence of polymeric molecules. The objective of this work is to give a general overview of the basic physicochemical factors playing a role in fouling and to outline some practical aspects related to the theoretical reasoning to help prevent or at leasl[ mitigate fouling. © Elsevier Science Inc., 1997 Keywords: adhesion, DLVO theory, surface free energy, hydrophobic interactions, steric forces, ionic strength, ion bridging INTRODUCTION tant roles. In bifouling, the adhesion of microorganisms can be strongly dependent on their external appendages. The accumulation of inorganic particles, microorganisms, The net effect is a balance between all possible interac- macromolecules, and corrosion products on heat ex- tions. A knowledge of the roles of the main variables changer surfaces gives rise to the so-called fouling phe- affecting the interactions outlined above is of great impor- nomenon.