2012
DOI: 10.1103/physreve.85.061403
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Packings of monodisperse emulsions in flat microfluidic channels

Abstract: In the lateral confinement of a flat microfluidic channel, monodisperse emulsion droplets spontaneously self-organize in a variety of topologically different packings. The explicit construction of mechanically equilibrated arrangements of effectively two-dimensional congruent droplet shapes reveals the existence of multiple mechanical equilibria depending on channel width W, droplet area A{d}, and volume fraction φ of the dispersed phase. The corresponding boundaries of local or global stability are summarized… Show more

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Cited by 8 publications
(7 citation statements)
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“…As they flowed, the drops arranged into a hexagonally packed crystal (Fig. 1A) (23). Due to the tapered channel geometry, the emulsion experienced gradual, elastic compression in the transverse direction as it moved along the channel, except at specific locations where the number of rows of drops N (counted at 60°relative to the x axis across the width of the channel) decreased by one (Fig.…”
Section: Resultsmentioning
confidence: 99%
“…As they flowed, the drops arranged into a hexagonally packed crystal (Fig. 1A) (23). Due to the tapered channel geometry, the emulsion experienced gradual, elastic compression in the transverse direction as it moved along the channel, except at specific locations where the number of rows of drops N (counted at 60°relative to the x axis across the width of the channel) decreased by one (Fig.…”
Section: Resultsmentioning
confidence: 99%
“…6, we analytically computed the dimensionless elastic force f ¼ F e /s from the interfacial energy of the considered droplet packing as function of the droplet confinement A/W 2 and the area fraction u. The calculated elastic force f(u) is plotted as solid lines in Fig.…”
mentioning
confidence: 99%
“…Based on these rules, we analytically constructed the three relevant droplet packing and determined the perimeter ' d of the droplet contour, the area A enclosed by it, and the corresponding area fraction u. 6 This allowed us to compute the interfacial energy E d ¼ s effective line tension of the two dimensional droplet contour in a flat Hele-Shaw geometry. 6,8 The elastic force F e of the droplet packing can be obtained as the derivative of the interfacial energy E ¼ NE d of a train of N droplets with respect to the length L of the droplet train for fixed A…”
mentioning
confidence: 99%
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“…The reservoir with a wide 2D space was replaced with parallelized microfluidic channels to produce droplet arrays. Droplets formed a hexagonal array without grain boundaries in each channel as the width of the channel was much smaller than crystal domain size. , This enabled patterning on two distinct scales and shapes: the line pattern was a few hundreds of micrometers in scale, whereas the hexagonal dot pattern was a few tens of micrometers in scale. This structure was demonstrated by generating droplets with diameters of 44 μm in the drop makers.…”
Section: Resultsmentioning
confidence: 99%