scholarly journals Water-in-water droplets by passive microfluidic flow focusing

Author(s):  
Byeong-Ui Moon ◽  
Niki Abbasi ◽  
Steven G. Jones ◽  
Dae Kun Hwang ◽  
Scott S. H. Tsai

We present a simple microfluidic system that generates water-in-water, aqueous two phase system (ATPS) droplets, by passive flow focusing. ATPS droplet formation is achieved by applying weak hydrostatic pressures, with liquid-filled pipette tips as fluid columns at the inlets, to introduce low speed flows to the flow focusing junction. To control the size of the droplets, we systematically vary the interfacial tension and viscosity of the ATPS fluids, and adjust the fluid column height at the fluid inlets. The size of the droplets scales with a power-law of the ratio of viscous stresses in the two ATPS phases. Overall, we find a drop size coefficient of variation (CV; i.e. polydispersity) of about 10 %. We also find that when drops form very close to the flow focusing junction, the drops have CV of less than 1 %. Our droplet generation method is easily scalable: we demonstrate a parallel system that generates droplets simultaneously, and improves the droplet production rate by up to one order-of-magnitude. Finally, we show the potential application of our system for encapsulating cells in water-in-water emulsions, by encapsulating microparticles and cells. To the best of our knowledge, our microfluidic technique is the first that forms low interfacial tension ATPS droplets without applying external perturbations. We anticipate that this simple approach will find utility in drug and cell delivery applications because of the all-biocompatible nature of the water-in-water ATPS environment.

Lab on a Chip ◽  
2015 ◽  
Vol 15 (11) ◽  
pp. 2437-2444 ◽  
Author(s):  
Byeong-Ui Moon ◽  
Steven G. Jones ◽  
Dae Kun Hwang ◽  
Scott S. H. Tsai

Simple microfluidic flow focusing generation of droplets from ultralow interfacial tension aqueous two phase systems (ATPS).


Author(s):  
Mohammad Mastiani ◽  
Seokju Seo ◽  
Sofia Melgar Jimenez ◽  
Nick Petrozzi ◽  
Myeongsub (Mike) Kim

Recent advent of Aqueous-Two-Phase-System (ATPS), more biologically friendly compared to conventional oil-water systems, has shown great potential to rapidly generate aqueous droplets without tedious post-processing. However, understanding of underlying physics of droplet formation in ATPS is still in its infancy. In this paper, we investigate hydrodynamic behaviors and mechanisms of all-aqueous droplet formation in two flow-focusing droplet generators. Two incompatible polymers namely polyethylene glycol (PEG) and dextran (DEX) are mixed in water to make ATPS. The influence of inlet pressures and flow-focusing configurations on droplet sizes, and thread breakup length is studied. Flow regime mapping for two different configurations of droplet generators possessing junction angles of 30° and 90° is also obtained. The results show that droplet size is very susceptible to the junction angle while inlet pressures of the PEG and DEX flows readily control four main flow regimes including back flow, dripping, jetting and stratified.


Author(s):  
Mohammad Mastiani ◽  
Seokju Seo ◽  
Sofia Melgar Jimenez ◽  
Nicholas Petrozzi ◽  
Myeongsub Mike Kim

2019 ◽  
Vol 876 ◽  
pp. 1052-1076 ◽  
Author(s):  
Krishne Gowda. V ◽  
Christophe Brouzet ◽  
Thibault Lefranc ◽  
L. Daniel Söderberg ◽  
Fredrik Lundell

An interface between two miscible fluids is transient, existing as a non-equilibrium state before complete molecular mixing is reached. However, during the existence of such an interface, which typically occurs at relatively short time scales, composition gradients at the boundary between the two liquids cause stresses effectively mimicking an interfacial tension. Here, we combine numerical modelling and experiments to study the influence of an effective interfacial tension between a colloidal fibre dispersion and its own solvent on the flow in a microfluidic system. In a flow-focusing channel, the dispersion is injected as core flow that is hydrodynamically focused by its solvent as sheath flows. This leads to the formation of a long fluid thread, which is characterized in three dimensions using optical coherence tomography and simulated using a volume of fluid method. The simulated flow and thread geometries very closely reproduce the experimental results in terms of thread topology and velocity flow fields. By varying the interfacial tension numerically, we show that it controls the thread development, which can be described by an effective capillary number. Furthermore, we demonstrate that the applied methodology provide the means to measure the ultra-low but dynamically highly significant effective interfacial tension.


1970 ◽  
Vol 10 (04) ◽  
pp. 327-327 ◽  
Author(s):  
H.G. Warren ◽  
E.W. Hough

The interfacial tension values for the methane-n heptane two-phase system were determined by the pendeant-drop method on eight isotherms from 100 degrees pendeant-drop method on eight isotherms from 100 degrees to 310 degrees F. The pressure range was from 215 to 3,415 psia. Direct measurements of the maximum and minimum drop diameters were made. The tables of Winkel and the density difference data of Reamer et al. were used to calculate experimental values of interfacial tension. The experimental data varied from 16.64 dynes/cm at 217 psia at 100 degrees F to 0.081 dynes/cm at 3,415 psia at 130 degrees F. The smooth data is given in Table 1. Fig. 1 is a plot of smoothed data at 0.1, 1.0, 5.0 and 10.0 dynes/cm over the range of 100 degrees to 310 degrees F and 0 to 3,618 psia. The dashed lines are extrapolation of the data. A correlation of these data along with other hydrocarbon systems has been published. The data are taken from the PhD dissertation of one of the authors. The supplement of the American Chemical Society Research Fund Grant No. 635-A is gratefully acknowledged. TABLE 1 - INTERFACIAL TENSION OF THE METHANE - NORMAL HEPTANE SYSTEM SMOOTHED DATA Interfacial Tension (dynes/cm) Pressure Pressure psia 100 F 130 F 160F 190 F 220 F 250 F 280 F 310 F psia 100 F 130 F 160F 190 F 220 F 250 F 280 F 310 F 400 14.88 13.75 12.50 11.28 9.97 8.83 7.74 6.60800 11.33 10.60 9.88 8.96 7.96 6.98 6.07 5.111,200 8.50 8.00 7.55 6.88 6.18 5.32 4.55 3.711,600 6.16 5.85 5.53 5.04 4.54 3.80 3.16 2.482,000 4.21 4.06 3.83 3.47 3.04 0.45 1.90 1.352,200 3.35 3.83 3.47 3.04 2.37 1.85 1.39 0.872,400 2.57 2.50 2.36 2.13 1.76 1.30 0.91 0.472,600 1.85 1.82 1.73 1.54 1.23 0.83 0.50 0.132,800 1.22 1.22 1.15 1.00 0.74 0.41 0.17 2709*3,000 0.73 0.73 0.67 0.56 0.34 0.13 2927*3,100 0.53 0.53 0.47 0.37 0.19 0.033,200 0.35 0.35 0.31 0.23 0.07 3122*3,300 0.22 0.22 0.19 0.12 3298*3,400 0.13 0.13 0.10 0.033,500 0.06 0.02 3549*3,600 3606* 3618* *Critical pressure at temperature. P. 227


Lab on a Chip ◽  
2017 ◽  
Vol 17 (2) ◽  
pp. 286-292 ◽  
Author(s):  
Van Bac Dang ◽  
Sung-Jin Kim

This paper presents the mechanism of a water-head-driven oscillator and shows the generation of droplets with low interfacial tension.


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