2019
DOI: 10.1002/bit.27211
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Manipulation of micro‐ and nanoparticles in viscoelastic fluid flows within microfluid systems

Abstract: Manipulation of micro‐ and nanoparticles in complex biofluids is highly demanded in most biological and biomedical applications. A significant number of microfluidic platforms have been developed for inexpensive, rapid, accurate, and efficient particle manipulation. Due to the enormous potential of viscoelastic fluids (VEFs) for particle manipulation, various emerging microfluidic‐based VEFs techniques have been presented over the last decade. This review provides an intuitive understanding of VEF physics for … Show more

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Cited by 29 publications
(25 citation statements)
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“…Indeed, both forces are able to drive the flowing particles towards specific equilibrium positions depending on the channel geometry, flow rate, and properties of the suspending liquid, as well documented in several reviews. [72][73][74][75][76][77][78] Once the particles reached the equilibrium position, at sufficiently large concentrations, they begin to interact, possibly leading to the formation of crystal-like structures. In this stage, the overall dynamics depends upon the mutual distance between all the interacting particles.…”
Section: Particle Crystalsmentioning
confidence: 99%
“…Indeed, both forces are able to drive the flowing particles towards specific equilibrium positions depending on the channel geometry, flow rate, and properties of the suspending liquid, as well documented in several reviews. [72][73][74][75][76][77][78] Once the particles reached the equilibrium position, at sufficiently large concentrations, they begin to interact, possibly leading to the formation of crystal-like structures. In this stage, the overall dynamics depends upon the mutual distance between all the interacting particles.…”
Section: Particle Crystalsmentioning
confidence: 99%
“…In the case of a pressure-driven, non-Newtonian, viscoelastic flow, particles migrate towards the centreline of a microchannel due to a non-uniform distribution of the first normal stress between the centreline and the walls of microchannel 35 with non-negligible inertial effects in addition to the dominant elastic forces [36][37][38][39][40][41][42][43][44][45][46][47] . For 3D focusing of particles in rectangular geometries under similar conditions, the particles migrate towards the centreline and corners of the channel due to nonlinear effects of fluid inertia and fluid elasticity induced by the non-uniform distribution of normal stress.…”
Section: High Throughput Viscoelastic Particle Focusing and Separation In Spiral Microchannelsmentioning
confidence: 99%
“…Combination of inertial and elastic focusing at finite fluid inertia and elasticity regimes enables unique rigid particle or cell focusing at high throughput (Elasto‐inertial focusing). [ 7–11 ] Two non‐dimensional numbers, the channel Reynolds number ( Re ) and Weissenberg number ( Wi ), measure the inertial and elastic effect of the fluid, respectively: Re=ρnormalfVDnormalhη where ρ f is the fluid density; V is the average fluid velocity; D h is the hydraulic diameter of the channel; η is the dynamic viscosity of the fluid. Wi=λ γ.=λ2V/Dnormalh where λ is the relaxation time of the fluid; γ. is the characteristic shear rate.…”
Section: Theorectical Backgroundmentioning
confidence: 99%