2017
DOI: 10.1002/aic.15704
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Experimental investigations of non‐Newtonian/Newtonian liquid‐liquid flows in microchannels

Abstract: The plug flow of a non-Newtonian and a Newtonian liquid was experimentally investigated in a quartz microchannel (200-mm internal diameter). Two aqueous glycerol solutions containing xanthan gum at 1000 and 2000 ppm were the non-Newtonian fluids and 0.0046 Pa s silicone oil was the Newtonian phase forming the dispersed plugs. Two-color particle image velocimetry was used to obtain the hydrodynamic characteristics and the velocity profiles in both phases under different fluid flow rates. The experimental result… Show more

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Cited by 40 publications
(19 citation statements)
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“…The intensity fields for Qtot= 5 μL/min in the aqueous slug and in the organic plug are lower and higher, respectively, when compared to the other two flow rates. The concentration fields in the main channel seem to follow the internal circulation patterns expected in both the slugs and plugs [33]. This is more evident from the concentration field of 〈I org 〉 at Qtot=10 μL/min.…”
Section: Extraction Efficiency (%Eeff)mentioning
confidence: 63%
“…The intensity fields for Qtot= 5 μL/min in the aqueous slug and in the organic plug are lower and higher, respectively, when compared to the other two flow rates. The concentration fields in the main channel seem to follow the internal circulation patterns expected in both the slugs and plugs [33]. This is more evident from the concentration field of 〈I org 〉 at Qtot=10 μL/min.…”
Section: Extraction Efficiency (%Eeff)mentioning
confidence: 63%
“…Note that the film thickness h is the only free parameter of the problem and can be determined, for example, by experiments (see, e.g., Roumpea et al, 2017) or by theory-based correlations (see Bretherton, 1961;Hodges et al, 2004;Picchi et al, 2018), where the film thickness is expressed as a function of the capillary number and the dimensionless parameters of the system, h = h (Ca, M, …). The problem then is closed with the following relation between the average velocities:…”
Section: 1029/2018wr023172mentioning
confidence: 99%
“…Note that the film thickness h is the only free parameter of the problem and can be determined, for example, by experiments (see, e.g., Roumpea et al, ) or by theory‐based correlations (see Bretherton, ; Hodges et al, ; Picchi et al, ), where the film thickness is expressed as a function of the capillary number and the dimensionless parameters of the system, h = h ( C a , M ,…). The problem then is closed with the following relation between the average velocities: truebold-italicu¯11=truebold-italicu¯11normalP+false(1false)truebold-italicu¯11normalS, truebold-italicu¯22=truebold-italicu¯22normalP, where truebold-italicu¯11normalS is the average velocity in the single‐phase region, (1 − ℓ ), equal to the mixture velocity (Fabre & Line, ; Picchi et al, ) as truebold-italicu¯11boldS=S1boldPtruebold-italicu¯11boldP+false(1S1boldPfalse)truebold-italicu¯22boldP. …”
Section: Impact Of Pore‐scale Flow Regimes On the Upscaled Equationmentioning
confidence: 99%
“…However, they identified a transition point at a critical value of capillary number, above which the shear stress effect has to be accounted for. Extensive work has been performed over the last decades in an attempt to describe and characterise the break-up mechanism in a microfluidic T-junction, both in Newtonian and non-Newtonian systems [1][2][3][4][5][6][7][8][9]. Droplets are detached from the dispersed phase threads penetrating the continuous phase, either near the junction or several widths downstream, depending on the flow rates, the fluid properties, and the geometrical characteristics of the system [4,5].…”
Section: Introductionmentioning
confidence: 99%