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1.
Philos Trans A Math Phys Eng Sci ; 362(1818): 1037-58, 2004 May 15.
Artigo em Inglês | MEDLINE | ID: mdl-15306483

RESUMO

The recent introduction of actuation mechanisms for microfluidic transport based on free surface flows raises a number of interesting questions involving efficient mixing configurations, especially in systems with small aspect ratios. This work investigates the characteristics of convective and diffusive mixing in continuous-mode streaming of thermocapillary microflows on chemically micropatterned surfaces. Mixing times and mixing lengths relevant to chemical microreactors or gas sensors are investigated for various geometries and parameter ranges. Scaling arguments and full numerical solutions are presented to extract optimal operating conditions. Confocal fluorescence microscopy measurements of the interfacial diffusive broadening in adjacent flowing streams confirm numerical predictions. Three important mixing regimes, based on analogues of purely diffusive dynamics, Rhines-Young shear-augmented diffusion and Taylor-Aris dispersion are identified and investigated for use in free surface flows with large surface-to-volume ratios.


Assuntos
Misturas Complexas/química , Microquímica/métodos , Microfluídica/métodos , Modelos Químicos , Nanotecnologia/métodos , Ação Capilar , Simulação por Computador , Desenho de Equipamento , Análise de Falha de Equipamento , Manufaturas , Microquímica/instrumentação , Microfluídica/instrumentação , Movimento (Física) , Nanotecnologia/instrumentação , Soluções , Propriedades de Superfície
2.
Phys Rev E Stat Nonlin Soft Matter Phys ; 64(3 Pt 1): 031603, 2001 Sep.
Artigo em Inglês | MEDLINE | ID: mdl-11580345

RESUMO

We have studied the capillary spreading of a Newtonian liquid along hydrophilic microstripes that are chemically defined on a hydrophobic substrate. The front of the spreading film advances in time according to a power law x=Bt(1/2). This exponent of 1/2 is much larger than the value 1/10 observed in the axisymmetric spreading of a wetting droplet. It is identical to the exponent found for wicking in open or closed microchannels. Even though no wicking occurs in our system, the influence of surface curvature induced by the lateral confinement of the liquid stripe also leads to an exponent of 1/2 but with a strongly modified prefactor B. We obtain excellent experimental agreement with the predicted time dependence of the front location and the dependence of the front speed on the stripe width. Additional experiments and simulations reveal the influence of the reservoir volume, liquid material parameters, edge roughness, and nonwetting defects. These results are relevant to liquid dosing applications or microfluidic delivery systems based on free-surface flow.

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