期刊
INTERNATIONAL JOURNAL OF MULTIPHASE FLOW
卷 147, 期 -, 页码 -出版社
PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.ijmultiphaseflow.2021.103863
关键词
Lattice Boltzmann method; Emulsion dynamics; Microfludics
类别
资金
- Natural Sciences and Engineering Research Council of Canada (NSERC) Discovery Grant [T02-P05]
- Compute Canada [RGPIN-2020-05511]
- Canada First Research Excellence Fund (CFREF)
- Future Energy System (FES) at University of Alberta
- Alberta Innovates (AI), Canada
- NSERC, Canada Discovery grant
Surface wettability significantly affects the dynamics and stability of liquid-liquid dispersion in microfluidic channels. In this study, simulations were conducted to investigate these effects in a microchannel with heterogeneous surface wettability. Different flow patterns were observed depending on drop length and Capillary number, and the results matched well with experimental data. The presence of an intervening thin film of the continuous phase was found to be crucial in capturing the observed drop behavior.
Surface wettability plays a vital role in various natural phenomena and technical applications, such as coating, printing, membrane technology, microfluidic devices, and porous media flow. We numerically investigate the dynamics and stability of liquid-liquid dispersion flowing in a microfluidic channel with heterogeneous surface wettability, using a conservative phase-field lattice Boltzmann method. First, we validate the implementation of the wetting boundary conditions. We then perform three-dimensional simulations of a single drop motion immersed in another immiscible liquid in a square microchannel with alternating surface wettability: hydrophilic, hydrophobic, and again hydrophilic sections. The viscosity of the dispersed liquid (oil) is ten times higher than that of the continuous one (water), while the two liquids have equal densities. Depending on the drop length and Capillary number, calculated based on the drop velocity and the dynamic viscosity of the continuous phase, four different flow patterns are observed when the drop passes through the hydrophobic section. The distinct flow patterns include passing without any changes in drop shape or dynamics, adhesion of the dispersed liquid to the walls, phase inversion (i.e., water becomes the dispersed phase), and drop breakage. These outcomes are in close agreement with the experimental data. A detailed explanation of the choice of the numerical parameters is presented. The critical aspect of capturing the observed drop behavior is introducing an intervening thin-film of the continuous phase of at least three diffuse interface thicknesses (between the drop and channel walls).
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