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Jun 2009

Volume 3, Issue 2, Articles (02xxxx)

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Editorial: Changes to the journal and appointment of a new Co-Editor

Hsueh-Chia Chang

Biomicrofluidics 3, 020901 (2009); http://dx.doi.org/10.1063/1.3138045 (2 pages)

Online Publication Date: 8 May 2009

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Abstract Unavailable
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99.10.Np Editorial note
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Editorial: A note from the new Co-Editor

Leslie Y. Yeo

Biomicrofluidics 3, 020902 (2009); http://dx.doi.org/10.1063/1.3138046 (2 pages)

Online Publication Date: 8 May 2009

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Abstract Unavailable
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01.30.-y Physics literature and publications
87.80.Ek Mechanical and micromechanical techniques
87.85.Ox Biomedical instrumentation and transducers, including micro-electro-mechanical systems (MEMS)
85.85.+j Micro- and nano-electromechanical systems (MEMS/NEMS) and devices
47.85.Np Fluidics
47.61.Fg Flows in micro-electromechanical systems (MEMS) and nano-electromechanical systems (NEMS)
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Preface to Special Topic: Papers from the 2009 Conference on Advances in Microfluidics and Nanofluidics, The Hong Kong University of Science & Technology, Hong Kong, 2009

Leslie Y. Yeo

Biomicrofluidics 3, 022301 (2009); http://dx.doi.org/10.1063/1.3167278 (2 pages)

Online Publication Date: 26 June 2009

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The inaugural conference on Advances in Microfluidics and Nanofluidics was held at the Hong Kong University of Science and Technology on 5–7 January 2009 and brought together leading researchers from across a wide variety of disciplines from North America, Europe, Asia, and Oceania. This Special Topic section forms the second of the two issues dedicated to original contributions covering both fundamental physicochemical aspects of microfluidics and nanofluidics as well as their applications to the miniaturization of chemical and biological systems that were presented at the conference.
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85.85.+j Micro- and nano-electromechanical systems (MEMS/NEMS) and devices
87.80.Ek Mechanical and micromechanical techniques

Design and testing of a microfluidic biochip for cytokine enzyme-linked immunosorbent assay

Hongyan He, Yuan Yuan, Weixiong Wang, Nan-Rong Chiou, Arthur J. Epstein, and L. James Lee

Biomicrofluidics 3, 022401 (2009); http://dx.doi.org/10.1063/1.3116665 (17 pages) | Cited 11 times

Online Publication Date: 13 April 2009

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Enzyme-linked immunosorbent assay (ELISA) has been widely used in medical diagnostics, environmental analyses, and biochemical studies. To reduce assay time and lower consumption of reagents in cytokine ELISA analysis, a polymeric microfluidic biochip has been designed and fabricated via several new techniques: Polyaniline-based surface modification for superhydrophobic capillary valving and oxygen plasma-poly(ethyleneimine)-tyrosinase-protein A modification for high sensitivity protein detection. The proper flow sequencing was achieved using the superhydrophobic capillary valves. The burst frequency of each valve was experimentally determined and compared with two capillary force equations and the fluent finite element simulation. This fully automated microfluidic biochip with an analyzer is able to provide high fluorescence signal of ELISA with a wider linear detection range and a much shorter assay time than 96-well microtiter plates. It is applicable to a variety of nonclinic research and clinically relevant disease conditions. The modification technologies in this study can be implemented in other lab-on-a-chip systems, drug/gene delivery carriers, and other immunoassay biosensor applications.
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87.85.Ox Biomedical instrumentation and transducers, including micro-electro-mechanical systems (MEMS)
85.85.+j Micro- and nano-electromechanical systems (MEMS/NEMS) and devices
47.85.Np Fluidics
87.85.M- Biotechnology
87.14.ej Enzymes

A novel actuation method of transporting droplets by using electrical charging of droplet in a dielectric fluid

Yong-Mi Jung (정용미) and In Seok Kang (강인석)

Biomicrofluidics 3, 022402 (2009); http://dx.doi.org/10.1063/1.3122299 (11 pages) | Cited 6 times

Online Publication Date: 20 April 2009

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We evaluate the feasibility of manipulating droplets in two dimensions by exploiting Coulombic forces acting on conductive droplets immersed in a dielectric fluid. When a droplet suspended in an immiscible fluid is located near an electrode under a dc voltage, the droplet can be charged by direct contact, by charge transfer along an electrically conducting path, or by both mechanisms. This process is called electrical charging of droplet (ECOD). This charged droplet may then be transported rapidly by exploiting Coulombic forces. We experimentally demonstrate electrical actuation of a charged droplet by applying voltage sequences. A charged droplet is two dimensionally actuated by following the direction of the electrical field signal. The droplet does not contact the surface of the microfluidic chip when it moves. This characteristic is very advantageous because treatments of the substrate surfaces of microfluidic chip become simpler. In order to test the feasibility of using ECOD in a droplet-based microreactor, electrocoalescence of two oppositely charged droplets is also studied. When two droplets approach each other due to Coulombic attraction, a liquid bridge is formed between them. We postulate that if the applied electric field is weaker than a certain critical level, the two droplets coalesce instantaneously when the charges are exchanged and redistributed through this liquid bridge.
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47.85.Np Fluidics
07.10.Cm Micromechanical devices and systems
87.85.Ox Biomedical instrumentation and transducers, including micro-electro-mechanical systems (MEMS)
85.85.+j Micro- and nano-electromechanical systems (MEMS/NEMS) and devices

Fabricating scaffolds by microfluidics

Kuo-yuan Chung, Narayan Chandra Mishra, Chen-chi Wang, Feng-hui Lin, and Keng-hui Lin

Biomicrofluidics 3, 022403 (2009); http://dx.doi.org/10.1063/1.3122665 (8 pages) | Cited 10 times

Online Publication Date: 21 April 2009

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In this paper, we demonstrate for the first time the technique to using microfluidics to fabricate tissue engineering scaffolds with uniform pore sizes. We investigate both the bubble generation of the microfluidic device and the application of foam as a tissue engineering scaffold. Our microfluidic device consists of two concentric tapered channels, which are made by micropipettes. Nitrogen gas and aqueous alginate solution with Pluronic® F127 surfactant are pumped through the inner and the outer channels, respectively. We observe rich dynamic patterns of bubbles encapsulated in the liquid droplets. The size of the bubble depends linearly on the gas pressure and inversely on the liquid flow rate. In addition, monodisperse bubbles self-assemble into crystalline structures. The liquid crystalline foams are further processed into open-cell solid foams. The novel foam gel was used as a scaffold to culture chondrocytes.
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87.80.Ek Mechanical and micromechanical techniques
87.85.Ox Biomedical instrumentation and transducers, including micro-electro-mechanical systems (MEMS)
47.85.Np Fluidics
87.85.Lf Tissue engineering
82.70.Gg Gels and sols
87.17.Ee Growth and division

Pressure-driven transport of particles through a converging-diverging microchannel

Ye Ai, Sang W. Joo, Yingtao Jiang, Xiangchun Xuan, and Shizhi Qian

Biomicrofluidics 3, 022404 (2009); http://dx.doi.org/10.1063/1.3122594 (14 pages) | Cited 12 times

Online Publication Date: 22 April 2009

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Pressure-driven transport of particles through a symmetric converging-diverging microchannel is studied by solving a coupled nonlinear system, which is composed of the Navier–Stokes and continuity equations using the arbitrary Lagrangian–Eulerian finite-element technique. The predicted particle translation is in good agreement with existing experimental observations. The effects of pressure gradient, particle size, channel geometry, and a particle’s initial location on the particle transport are investigated. The pressure gradient has no effect on the ratio of the translational velocity of particles through a converging-diverging channel to that in the upstream straight channel. Particles are generally accelerated in the converging region and then decelerated in the diverging region, with the maximum translational velocity at the throat. For particles with diameters close to the width of the channel throat, the usual acceleration process is divided into three stages: Acceleration, deceleration, and reacceleration instead of a monotonic acceleration. Moreover, the maximum translational velocity occurs at the end of the first acceleration stage rather than at the throat. Along the centerline of the microchannel, particles do not rotate, and the closer a particle is located near the channel wall, the higher is its rotational velocity. Analysis of the transport of two particles demonstrates the feasibility of using a converging-diverging microchannel for passive (biological and synthetic) particle separation and ordering.
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87.80.Ek Mechanical and micromechanical techniques
47.10.A- Mathematical formulations
47.60.Dx Flows in ducts and channels
47.85.Np Fluidics
87.16.-b Subcellular structure and processes

Experimental verification of Faradaic charging in ac electrokinetics

Wee Yang Ng, Yee Cheong Lam, and Isabel Rodríguez

Biomicrofluidics 3, 022405 (2009); http://dx.doi.org/10.1063/1.3120273 (11 pages) | Cited 6 times

Online Publication Date: 23 April 2009

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This paper investigates the phenomenon of Faradaic charging in ac electrokinetics. Faradaic reactions were suggested as a key effect responsible for the reversal of pumping direction in ac micropumps. However, this hypothesis has yet to be proven convincingly and directly. Here we present an ion detection strategy to determine the production of ions through Faradaic hydrolytic reactions originating from direct application of voltage to electrolytic solutions during ac electrokinetics. Experiments were performed with symmetrical planar electrodes aligned along a microfluidic channel. Fluorescein, a pH-dependent dye, was employed as the pH indicator for the detection of ion production. Images were captured for analysis at various voltage levels. From analyzing the fluorescence intensity and its distribution, it can be concluded that the production of ions from hydrolytic reactions takes place and increases with the ac voltage. The coefficient of deviation indicates a significant enhancement at ac voltage above 11 Vpp. Lastly, we demonstrate a strategy using dc-biased ac electrokinetics to achieve controllability in direction and magnitude of the net fluid flow in pumping application.
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47.85.Np Fluidics
47.85.L- Flow control
47.61.Fg Flows in micro-electromechanical systems (MEMS) and nano-electromechanical systems (NEMS)
82.45.Fk Electrodes
85.85.+j Micro- and nano-electromechanical systems (MEMS/NEMS) and devices
87.80.Ek Mechanical and micromechanical techniques
87.85.Ox Biomedical instrumentation and transducers, including micro-electro-mechanical systems (MEMS)

Electrowetting on a lotus leaf

Jiang-Tao Feng, Feng-Chao Wang, and Ya-Pu Zhao

Biomicrofluidics 3, 022406 (2009); http://dx.doi.org/10.1063/1.3124822 (10 pages) | Cited 5 times

Online Publication Date: 24 April 2009

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Electrowetting on dielectrics has been widely used to manipulate and control microliter or nanoliter liquids in micro-total-analysis systems and laboratory on a chip. We carried out experiments on electrowetting on a lotus leaf, which is quite different from the equipotential plate used in conventional electrowetting. This has not been reported in the past. The lotus leaf is superhydrophobic and a weak conductor, so the droplet can be easily actuated on it through electrical potential gradient. The capillary motion of the droplet was recorded by a high-speed camera. The droplet moved toward the counterelectrode to fulfill the actuation. The actuation speed could be of the order of 10 mm/s. The actuation time is of the order of 10 ms.
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87.80.Ek Mechanical and micromechanical techniques
47.61.-k Micro- and nano- scale flow phenomena
47.85.Np Fluidics
87.80.Fe Micromanipulation of biological structures

Rapid on-chip genetic detection microfluidic platform for real world applications

Satyajyoti Senapati, Andrew R. Mahon, Jason Gordon, Carsten Nowak, Shramik Sengupta, Thomas H. Q. Powell, Jeffrey Feder, David M. Lodge, and Hsueh-Chia Chang

Biomicrofluidics 3, 022407 (2009); http://dx.doi.org/10.1063/1.3127142 (7 pages) | Cited 11 times

Online Publication Date: 4 May 2009

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The development of genetic detection protocols for field applications is an important aspect of modern medical diagnostic technology and environmental monitoring. In this paper, we report a rapid, portable, and inexpensive DNA hybridization technique using a bead-based microfluidic platform that functions by passing fluorescently labeled target DNA through a chamber packed with functionalized beads within a microfluidic channel. DNA hybridization is then assessed using a digital camera attached to a Clare Chemical DR-45M dark reader non-UV transilluminator that uses visible light as an excitation source and a blue and amber filter to reveal fluorescence. This microfluidic approach significantly enhances hybridization by reducing the diffusion time between target DNA and the silica surface. The use of probe-functionalized beads as solid support also enhances the sensitivity and limit of detection due to a larger surface area per unit volume. This platform could be adapted for use in medical applications and environmental monitoring, including the detection of harmful organisms in the ballast water of ships.
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85.85.+j Micro- and nano-electromechanical systems (MEMS/NEMS) and devices
87.80.Ek Mechanical and micromechanical techniques
47.85.Np Fluidics

Surface charge density of the track-etched nanopores in polyethylene terephthalate foils

Jianming Xue, Yanbo Xie, Yu Yan, Jin Ke, and Yugang Wang

Biomicrofluidics 3, 022408 (2009); http://dx.doi.org/10.1063/1.3130988 (8 pages) | Cited 7 times

Online Publication Date: 13 May 2009

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Surface charge is one of the most important properties of nanopores, which determines the nanopore performance in many practical applications. We report the surface charge densities of track-etched nanopores, which were obtained by measuring the streaming current and pore conductance, respectively. Experimental results reveal that surface charge densities depend significantly on the salt concentrations. In addition the values obtained with the pore conductance were always several times higher than those calculated with the streaming current, and the gel-like surface layer on the nanopore was considered to be responsible for this discrepancy.
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73.90.+f Other topics in electronic structure and electrical properties of surfaces, interfaces, thin films, and low-dimensional structures (Restricted to new topics in section 73)
82.70.Gg Gels and sols

An atomistic-continuum hybrid simulation of fluid flows over superhydrophobic surfaces

Qiang Li and Guo-Wei He

Biomicrofluidics 3, 022409 (2009); http://dx.doi.org/10.1063/1.3137674 (8 pages) | Cited 5 times

Online Publication Date: 13 May 2009

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Recent experiments have found that slip length could be as large as on the order of 1 μm for fluid flows over superhydrophobic surfaces. Superhydrophobic surfaces can be achieved by patterning roughness on hydrophobic surfaces. In the present paper, an atomistic-continuum hybrid approach is developed to simulate the Couette flows over superhydrophobic surfaces, in which a molecular dynamics simulation is used in a small region near the superhydrophobic surface where the continuum assumption is not valid and the Navier-Stokes equations are used in a large region for bulk flows where the continuum assumption does hold. These two descriptions are coupled using the dynamic coupling model in the overlap region to ensure momentum continuity. The hybrid simulation predicts a superhydrophobic state with large slip lengths, which cannot be obtained by molecular dynamics simulation alone.
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47.15.-x Laminar flows
47.10.A- Mathematical formulations
47.11.-j Computational methods in fluid dynamics

Unfolding polyelectrolytes in trivalent salt solutions using dc electric fields: A study by Langevin dynamics simulations

Yu-Fu Wei and Pai-Yi Hsiao

Biomicrofluidics 3, 022410 (2009); http://dx.doi.org/10.1063/1.3129563 (9 pages) | Cited 5 times

Online Publication Date: 19 May 2009

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We study the behavior of single linear polyelectrolytes condensed by trivalent salt under the action of electric fields through computer simulations. The chain is unfolded when the strength of the electric field is stronger than a critical value. This critical electric field follows a scaling law against chain length, and the exponent of the scaling law is −0.77(1), smaller than the theoretical prediction, −3ν/2 [ R. R. Netz, Phys. Rev. Lett. 90, 128104 (2003) ], and the one obtained by simulations in tetravalent salt solutions, −0.453(3) [ P.-Y. Hsiao and K.-M. Wu, J. Phys. Chem. B 112, 13177 (2008) ]. It demonstrates that the scaling exponent depends sensitively on the salt valence. Hence, it is easier to unfold chains condensed by multivalent salt of a smaller valence. Moreover, the absolute value of chain electrophoretic mobility increases drastically when the chain is unfolded in an electric field. The fact that the mobility depends on electric field and on chain length provides a plausible way to impart chain-length dependence in free-solution electrophoresis via chain unfolding transition induced by electric fields. Finally, we show that, in addition to an elongated structure, a condensed chain can be unfolded into a U-shaped structure. The formation of this structure in our study is purely a result of the electric polarization, not of the elastohydrodynamics dominated in sedimentation of polymers.
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61.25.he Polymer solutions
87.15.N- Properties of solutions of macromolecules
36.20.Ey Conformation (statistics and dynamics)

Transport properties and induced voltage in the structure of water-filled single-walled boron-nitrogen nanotubes

Quanzi Yuan and Ya-Pu Zhao

Biomicrofluidics 3, 022411 (2009); http://dx.doi.org/10.1063/1.3158618 (6 pages) | Cited 5 times

Online Publication Date: 18 June 2009

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Density functional theory/molecular dynamics simulations were employed to give insights into the mechanism of voltage generation based on a water-filled single-walled boron-nitrogen nanotube (SWBNNT). Our calculations showed that (1) the transport properties of confined water in a SWBNNT are different from those of bulk water in view of configuration, the diffusion coefficient, the dipole orientation, and the density distribution, and (2) a voltage difference of several millivolts would generate between the two ends of a SWBNNT due to interactions between the water dipole chains and charge carriers in the tube. Therefore, this structure of a water-filled SWBNNT can be a promising candidate for a synthetic nanoscale power cell as well as a practical nanopower harvesting device.
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73.63.Fg Nanotubes
07.10.Cm Micromechanical devices and systems
66.30.Pa Diffusion in nanoscale solids
61.48.De Structure of carbon nanotubes, boron nanotubes, and other related systems
47.60.Dx Flows in ducts and channels
47.61.Fg Flows in micro-electromechanical systems (MEMS) and nano-electromechanical systems (NEMS)

Modeling the coalescence of sessile droplets

M. Sellier and E. Trelluyer

Biomicrofluidics 3, 022412 (2009); http://dx.doi.org/10.1063/1.3154552 (14 pages) | Cited 4 times

Online Publication Date: 19 June 2009

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This paper proposes a simple scenario to describe the coalescence of sessile droplets. This scenario predicts a power-law growth of the bridge between the droplets. The exponent of this power law depends on the driving mechanism for the spreading of each droplet. To validate this simple idea, the coalescence is simulated numerically and a basic experiment is performed. The fluid dynamics problem is formulated in the lubrication approximation framework and the governing equations are solved in the commercial finite element software COMSOL. Although a direct comparison of the numerical results with experiment is difficult because of the sensitivity of the coalescence to the initial and operating conditions, the key features of the event are qualitatively captured by the simulation and the characteristic time scale of the dynamics recovered. The experiment consists of inducing coalescence by pumping a droplet through a substrate which grows and ultimately coalesces with another droplet resting on the substrate. The coalescence was recorded using high-speed imaging and also confirmed the power-law growth of the neck.
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47.63.-b Biological fluid dynamics
47.85.-g Applied fluid mechanics
47.55.D- Drops and bubbles

Induced charge electro osmotic mixer: Obstacle shape optimization

Mranal Jain, Anthony Yeung, and K. Nandakumar

Biomicrofluidics 3, 022413 (2009); http://dx.doi.org/10.1063/1.3167279 (15 pages) | Cited 5 times

Online Publication Date: 30 June 2009

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Efficient mixing is difficult to achieve in miniaturized devices due to the nature of low Reynolds number flow. Mixing can be intentionally induced, however, if conducting or nonconducting obstacles are embedded within the microchannel. In the case of conducting obstacles, vortices can be generated in the vicinity of the obstacle due to induced charge electro-osmosis (ICEO) which enhances mixing of different streams: the obstacle shape affects the induced zeta potential on the conducting surface, which in turn influences the flow profile near the obstacle. This study deals with optimization of the geometric shape of a conducting obstacle for the purpose of micromixing. The obstacle boundary is parametrically represented by nonuniform rational B-spline curves. The optimal obstacle shape, which maximizes the mixing for given operating conditions, is found using genetic algorithms. Various case studies at different operating conditions demonstrated that the near right triangle shape provides optimal mixing in the ICEO flow dominant regime, whereas rectangular shape is the optimal shape in diffusion dominant regime. The tradeoff between mixing and transport is examined for symmetric and nonsymmetric obstacle shapes.
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87.80.Ek Mechanical and micromechanical techniques
85.85.+j Micro- and nano-electromechanical systems (MEMS/NEMS) and devices
87.85.Ox Biomedical instrumentation and transducers, including micro-electro-mechanical systems (MEMS)
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