Chaotic advection at the pore scale: Mechanisms, upscaling and implications for macroscopic transport

被引:18
|
作者
Lester, D. R. [1 ]
Trefry, M. G. [2 ,3 ,4 ]
Metcalfe, G. [5 ,6 ,7 ]
机构
[1] RMIT Univ, Sch Engn, Discipline Chem & Environm Engn, Melbourne, Vic 3001, Australia
[2] CSIRO Land & Water, Floreat, WA 6014, Australia
[3] CSIRO Mineral Resources, Floreat, WA 6014, Australia
[4] Univ Western Australia, Sch Math & Stat, Perth, WA 6009, Australia
[5] Swinburne Univ Technol, Dept Mech & Prod Design Engn, Hawthorn, Vic 3122, Australia
[6] CSIRO Mfg, Clayton, Vic 3169, Australia
[7] Monash Univ, Sch Math Sci, Clayton, Vic 3800, Australia
关键词
Porous media; Dispersion; Dilution; Mixing; Upscaling; Chaotic advection; POROUS-MEDIA; FLOW; DIFFUSION; LAMINAR; DISPERSION; IMAGES; FLUIDS; MIXER;
D O I
10.1016/j.advwatres.2016.09.007
中图分类号
TV21 [水资源调查与水利规划];
学科分类号
081501 ;
摘要
The macroscopic spreading and mixing of solute plumes in saturated porous media is ultimately controlled by processes operating at the pore scale. Whilst the conventional picture of pore-scale mechanical dispersion and molecular diffusion leading to persistent hydrodynamic dispersion is well accepted, this paradigm is inherently two-dimensional (2D) in nature and neglects important three-dimensional (3D) phenomena. We discuss how the kinematics of steady 3D flow at the pore scale generate chaotic advection-involving exponential stretching and folding of fluid elements-the mechanisms by which it arises and implications of microscopic chaos for macroscopic dispersion and mixing. Prohibited in steady 2D flow due to topological constraints, these phenomena are ubiquitous due to the topological complexity inherent to all 3D porous media. Consequently 3D porous media flows generate profoundly different fluid deformation and mixing processes to those of 2D flow. The interplay of chaotic advection and broad transit time distributions can be incorporated into a continuous-time random walk (CTRW) framework to predict macroscopic solute mixing and spreading. We show how these results may be generalised to real porous architectures via a CTRW model of fluid deformation, leading to stochastic models of macroscopic dispersion and mixing which both honour the pore-scale kinematics and are directly conditioned on the pore-scale architecture. Crown Copyright (C) 2016 Published by Elsevier Ltd. All rights reserved.
引用
收藏
页码:175 / 192
页数:18
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