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Improving the operation of electrowetting-based digital microfluidic systems by using water-oil core-shell droplets

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Improving the operation of electrowetting-based digital microfluidic

systems by using water-oil core-shell droplets

Brassard, Daniel; Malic, Lidija; Normandin, François; Tabrizian, Maryam;

Veres, Teodor

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IMPROVING THE OPERATION OF

ELECTROWETTING-BASED DIGITAL

MICRO-FLUIDIC SYSTEMS BY USING WATER-OIL

CORE-SHELL DROPLETS

Daniel Brassard1,2, Lidija Malic1,3, François Normandin1, Maryam Tabrizian3 and Teodor Veres1,2

1

National Research Council, CANADA,

2

Laval University, CANADA and

3

McGill University, CANADA

ABSTRACT

In electrowetting-on-dielectric (EWOD)-based digital microfluidic devices, dis-crete droplets are typically transported either directly in air or in an immiscible fluid such as silicone oil. We propose herein an alternative mode of operation in which the droplets are enclosed in a thin oil shell. We show that such water-oil core-shell droplets offer several key advantages. Specifically, this mode of operation not only reduces the voltage required by the devices but also leads to higher transport veloci-ties when compared with the manipulation of droplets directly in air or oil.

KEYWORDS: Digital Microfluidics, Electrowetting, Droplet, Silicone Oil INTRODUCTION

Due to their high flexibility and dynamic reconfigurability, droplet-based micro-fluidic platforms (i.e., digital micromicro-fluidics) have emerged as a promising alternative to the traditional microfluidic devices based on continuous flow of liquid in channels [1]. In such devices, the droplets are manipulated on a 2D surface by means of an actuation force (such as EWOD) applied locally, thus eliminating the need for com-plex mechanical components or permanently etched microchannels.

In EWOD-based microfluidic devices, the aqueous droplets have traditionally been transported either directly in air or in immiscible fluid such as silicone oil. Un-til now, the choice of air or oil as the transporting medium has been a complex tradeoff as neither offers the flexibility required to fulfill the needs of several appli-cations. For example, while the presence of a silicone oil medium prevents droplet evaporation and minimizes the contamination of the devices, it also increases the viscous drag, complicates the fabrication and handling of the devices, and prevents the use of some on-chip detection or analysis techniques [1,2]. On the other hand, transporting the droplets directly in air requires significantly higher operation volt-ages than in oil, which can cause a rapid degradation of the dielectric layers [1,2]. In this paper, we report on an alternative mode of operation for EWOD-based micro-fluidic devices in which the droplets are enclosed in a thin oil shell (Fig. 1). This mode of operation has been recently proposed as a mean to reduce the evaporation in an EWOD-based airborne particle sampler [3]. Herein, we additionally show that, by using such water-oil core-shell droplets, it is possible to minimize the various drag forces that interfere with the operation of EWOD-based microfluidic devices.

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0 20 40 60 80 100 0 50 100 150 0 20 40 60 80 100 Switching frequ ency (Hz) THEORY

Both contact angle hysteresis and viscous drag are known to interfere with the transport of the droplets in EWOD-based microfluidics devices. Contact angle hys-teresis (Δθ) of the droplets, which causes contact line friction, is generally much higher in air (Δθ ~ 8o) than in oil (Δθ ~ 2o

). On the other hand, in a viscous medium such as oil, viscous drag can be significant when the droplets are actuated at high speeds. Core-shell droplets thus offers the interesting possibility to achieve simulta-neously a low viscous drag, as they are actuated in air, and reduced contact line fric-tion, as the water droplet is enclosed in oil.

EXPERIMENTAL

The electrowetting-based microfluidic devices were fabricated according to the layout of the chip shown in Fig.1. The electrodes were formed by patterning 1.5 mm interdigitated squares from Cr/Au layers deposited on a piece of glass. The dielectric layers consisted of a 3 μm thick SU-8 photoresist that was hydrophobized by spin-coating a 30 nm thick layer of Teflon-AF. A piece of glass coated with indium tin oxide and Teflon AF was used for the top electrode. The distance between the bot-tom and the top plates was of about 150 μm during the operation of the devices. The droplets were manipulated on-chip by applying a DC potential sequentially to the control electrodes with a home-made computer-controlled electronic interface.

In this study, DI water was used for the droplets and, unless otherwise noted, the oil phase consisted of 1 cSt viscosity silicone oil. For the core-shell configuration, a small amount of oil was dispensed along with the water in the reservoirs of the chip. Due to the relative interfacial tension between the water, oil, and air, we found that the oil phase forms spontaneously a shell enclosing the water phase. As discussed next, the core-shell droplets were then formed on-chip from the reservoirs.

RESULTS AND DISCUSSION

As shown in figure 2, we found that, for a given operation voltage, water-oil core-shell droplets can be actuated at much higher velocities that water droplets ma-nipulated in either air or oil. Additionally, as shown in figure 3, significantly lower

Figure 1. Schematic of an EWOD-based digital microfluidic device ma-nipulating a water-oil core-shell droplet

Air Aqueous droplet

(core) Silicone oil

V Glass substrate Glass substrate Insulation Control electrodes Ground electrode Hydrophobic coatings Air Oil Core-shell D roplet veloc it y ( mm /s) Operation voltage (V)

Figure 2. Effect of the operation volt-age on the actuation dynamics of water droplets transported in air, in oil and in the core-shell configuration

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operation voltages are achieved in the core-shell configuration than in air despite the absence of a continuous oil medium. We could also successfully dispense, merge, mix and split water-oil core-shell droplets on-chip with the same procedure as for water droplets manipulated directly in air or oil [1]. For example, we found that, dur-ing the dispensdur-ing of a core-shell droplet from a large reservoir, a part of the oil shell around the reservoir is transferred spontaneously to the dispensed droplet. Fi-nally, our results confirm that, when a non volatile oil is used for the shell (for e.g., 10 cSt silicone oil), the evaporation rate of the water-oil core-shell droplets is drasti-cally reduced compared to water droplets in air (Fig. 4).

CONCLUSIONS

We have investigated the manipulation of water-oil core-shell droplets as an al-ternative mode of operation for EWOD-based digital microfluidic devices. Our re-sults indicate that, despite being extremely simple to implement, this novel mode of operation offers an increased flexibility toward the realization of high-throughput and high reliability EWOD-based digital microfluidic devices.

ACKNOWLEDGEMENTS

This work was supported financially by the Natural Sciences and Engineering Research Council of Canada and the National Research Council of Canada.

REFERENCES

[1]R. B. Fair, Digital microfluidics: is a true lab-on-a-chip possible?, Microfluid Nanofluid 3, pp. 245 - 281, (2007).

[2]H. Moon, A. R. Wheeler, R. L. Garrell, J. A. Loo, and C.-J. Kim, An integrated

digital microfluidic chip for multiplexed proteomic sample preparation and analysis by MALDI-MS, Lab Chip 6, pp. 1213-1219, (2006).

[3]R. B. Fair, A. Khlystov, V. Srinivasan, V. K. Pamula, and K. N. Weaver,

Inte-grated chemical/biochemical sample collection, pre-concentration, and analysis on a digital microfluidic lab-on-a-chip platform, Lab-on-a-Chip: Platforms,

De-vices, and Applications, Proceedings of SPIE, Philadelphia, pp. 113-124, (2004).

Actuation Dispensing Splitting

0 20 40 60 80 100 Min imum oper ation vo lt age ( V ) Air Oil Core-shell t = 60 min t = 0 min t = 30 min t = 120 min

Figure 3. Minimum operation voltage re-quired to perform various fluidic opera-tions for water droplets transported in air, in oil, and in the core-shell configuration.

Figure 4. Comparative evaporation rate of a water-oil core-shell drop-let (top left) and a water dropdrop-let in air (bottom right).

Figure

Figure 4.  Comparative evaporation  rate of a water-oil core-shell  drop-let (top left) and a water dropdrop-let in  air (bottom right)

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