2017
DOI: 10.1016/j.jcis.2017.01.034
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Dynamics of rigid microparticles at the interface of co-flowing immiscible liquids in a microchannel

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Cited by 10 publications
(10 citation statements)
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“…Sorting of droplets based on size contrast is demonstrated as well. Later, they reported the dynamical migration behavior of rigid polystyrene microparticles at an interface of coflowing streams of primary (aqueous) and secondary (oils) immiscible phases at low Reynolds numbers in a microchannel 104 . They found that the migration criterion depends on the sign of the spreading parameter and the presence of surfactant at the interface, and the interfacial perturbation can cause detachment of microparticles from the interface.…”
Section: Particle Solution Exchangementioning
confidence: 99%
“…Sorting of droplets based on size contrast is demonstrated as well. Later, they reported the dynamical migration behavior of rigid polystyrene microparticles at an interface of coflowing streams of primary (aqueous) and secondary (oils) immiscible phases at low Reynolds numbers in a microchannel 104 . They found that the migration criterion depends on the sign of the spreading parameter and the presence of surfactant at the interface, and the interfacial perturbation can cause detachment of microparticles from the interface.…”
Section: Particle Solution Exchangementioning
confidence: 99%
“…This is because at higher droplet velocity the residence time of a droplet in the electric-field region becomes smaller and the droplet does not spend enough time for the complete drainage of the thin film between the droplet and interface. At a higher droplet velocity, the flow capillary number Ca = μ m γa /γ̇ increases due to which the coalescence time also increases . Here μ m is the viscosity of continuous phase CP 1 , γ is the interfacial tension of droplet–CP 1 interface, a is the droplet radius, and γ̇ is the shear rate.…”
Section: Results and Discussionmentioning
confidence: 99%
“…Here μ m is the viscosity of continuous phase CP 1 , γ is the interfacial tension of droplet–CP 1 interface, a is the droplet radius, and γ̇ is the shear rate. However, to coalesce the faster moving droplets within this short residence time available, the droplet electrocapillary number Ca E = ε m aE 0 2 /γ needs to be higher . Here ε m is the permittivity of continuous phase CP 1 and E 0 is the applied electric field.…”
Section: Results and Discussionmentioning
confidence: 99%
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“…The viscosity of CP 1 ( μ CP1 ) is much greater than the viscosity of CP 2 ( μ CP2 ); thus, irrespective of the flow rates, the maximum velocity (i.e., region of zero shear) of the coflow always lies in the CP 2 . Using a coflowing system of two immiscible phases, extraction of rigid polystyrene particles (from aqueous phase to oil phase) 23 and soft hydrogel microparticles (from oil phase to aqueous phase) 24 has been demonstrated, at low Re, in which the working principle was based on the interfacial properties of the liquid phases and the particle. In contrast, here, we have employed hydrodynamic (noninertial lift) force that acts on the deformable objects at low Re to selectively sort droplets of interest.…”
Section: Sorting Of Positive and Negative Droplets Encapsulating Particles And Cells Based On Size Contrastmentioning
confidence: 99%