2021
DOI: 10.1115/1.4050701
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Lagrangian Transport and Chaotic Advection in Three-Dimensional Laminar Flows

Abstract: Transport and mixing of scalar quantities in fluid flows is ubiquitous in industry and Nature. Turbulent flows promote efficient transport and mixing by their inherent randomness. Laminar flows lack such a natural mixing mechanism and efficient transport is far more challenging. However, laminar flow is essential to many problems and insight into its transport characteristics of great importance. Laminar transport, arguably, is best described by the Lagrangian fluid motion ("advection") and the geometry, topol… Show more

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Cited by 31 publications
(26 citation statements)
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“…As far as the herringbone pattern in a duct flow is concerned, it has been demonstrated that two asymmetric counter-rotating flows are created by the herringbone-shaped grooves fabricated in a rectangular microchannel working in the creeping flow ( ) [ 22 , 37 , 38 , 39 , 40 , 41 , 42 ]. When the two flow portraits are projected onto a single plane normal to the ‒axis, the cross-sectional flow patterns from the two flows intersect each other, satisfying the necessary condition for chaotic advection in a three-dimensional geometrically periodic flow [ 20 , 21 , 43 ]. In the case of the flat membrane module ( Figure 1 ), unlike the two side walls of the microchannel, the two side surfaces of the computational domain (depicted in Figure 1 b) are not rigid walls but open boundaries, where a symmetric boundary condition is applied.…”
Section: Resultsmentioning
confidence: 99%
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“…As far as the herringbone pattern in a duct flow is concerned, it has been demonstrated that two asymmetric counter-rotating flows are created by the herringbone-shaped grooves fabricated in a rectangular microchannel working in the creeping flow ( ) [ 22 , 37 , 38 , 39 , 40 , 41 , 42 ]. When the two flow portraits are projected onto a single plane normal to the ‒axis, the cross-sectional flow patterns from the two flows intersect each other, satisfying the necessary condition for chaotic advection in a three-dimensional geometrically periodic flow [ 20 , 21 , 43 ]. In the case of the flat membrane module ( Figure 1 ), unlike the two side walls of the microchannel, the two side surfaces of the computational domain (depicted in Figure 1 b) are not rigid walls but open boundaries, where a symmetric boundary condition is applied.…”
Section: Resultsmentioning
confidence: 99%
“…It is an interesting subject to relate the chaotic behavior of the feed fluid to the fouling mitigation for the flat membrane module. If a flow system is chaotic, fluid elements exhibit strong deformations due to repeated stretching and folding, resulting in an exponential growth of the distance between two neighboring fluid particles [ 19 , 20 , 21 ]. Once chaotic advection occurs in a filtration module working in a laminar flow, it can uniformly distribute foulants via chaotic mixing, thereby mitigating membrane fouling if properly combined with downwelling flows [ 16 ].…”
Section: Resultsmentioning
confidence: 99%
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“…in the phase space related to chaotic advection (see e.g. Péntek et al, 1995;Cartwright et al, 1999;Tél et al, 2000;Speetjens et al, 2021). Recent important applications are connected to the exploration of Lagrangian coherent structures (Haller, 2015;Hadjighasem et al, 2017;Haller et al, 2018;Beron-Vera et al, 2018;Callies, 2021;Haller et al, 2021), mostly in the context of ocean flows.…”
Section: Introductionmentioning
confidence: 99%
“…In most cases, it is possible to reconstruct invariant sets of fractal nature in the phase space related to chaotic advection (see e.g. Péntek et al, 1995;Cartwright et al, 1999;Tél et al, 2000;Speetjens et al, 2021). Recent important applications are connected to the exploration of Lagrangian coherent structures (Haller, 2015;Hadjighasem et al, 2017;Haller et al, 2018;Beron-Vera et al, 2018;Callies, 2021;Haller et al, 2021), mostly in the context of ocean flows.…”
Section: Introductionmentioning
confidence: 99%