2016
DOI: 10.1007/s10404-016-1789-z
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Electrode-assisted trapping and release of droplets on hydrophilic patches in a hydrophobic microchannel

Abstract: a hydrophilic patch amidst a hydrophobic environment on the other. Two pairs of carefully aligned EW electrodes are used: one for drop adherence and another one for the subsequent release. We demonstrate these operations and discuss the required voltage signals in terms of the forces on the drop. Finally, we discuss possible steps for further improvement in the device.

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Cited by 12 publications
(7 citation statements)
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“…The surface properties of the glass microfluidic devices are important factors during the droplet synthesis [ 54 , 55 , 56 ]. In the case of hydrophilic glass, the surface is covered with hydroxyl groups.…”
Section: Hydrophilic Chip Applicationmentioning
confidence: 99%
“…The surface properties of the glass microfluidic devices are important factors during the droplet synthesis [ 54 , 55 , 56 ]. In the case of hydrophilic glass, the surface is covered with hydroxyl groups.…”
Section: Hydrophilic Chip Applicationmentioning
confidence: 99%
“…Trapping is a key process for sample preparation, observation, and detection. Passive droplet trapping using specific microchannel designs [37,38] and active droplet trapping using external energy [39,40] have been widely used for various microfluidic applications. However, trapping of LMs has not yet been studied.…”
Section: Introductionmentioning
confidence: 99%
“…F γ is modeled as a sum of two contributions: F γ,s due to the changes of the droplet surface area that pushes the droplet toward configurations with the minimal surface area and F γ,w that results from gradients of surface wettability and pulls an aqueous droplet toward the hydrophilic regions of the ablated track. F γ acts perpendicularly to the edges of the guiding track; it points into the track and its magnitude can be written as Here, γ is the interfacial tension (IFT) between the droplet and host liquids, D L and D R are the interaction lengths of the droplet with the left and right track edge, θ in and θ out are the droplet contact angles (CAs) inside and outside the track, R B is the radius of the contact area between the droplet and the bottom wall of the channel, w is the width of the track, and Δ A = A in – A out (Δ A = A out – A in ) represents the change in the droplet surface area upon moving into (out of) the center of the track. Except for Δ A , all the quantities that enter into eq can be either independently measured beforehand or analytically calculated from the droplet geometry at each time step during the simulation of droplet motion.…”
Section: Methodsmentioning
confidence: 99%