2009
DOI: 10.1016/j.cageo.2008.05.004
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A new partial-bounceback lattice-Boltzmann method for fluid flow through heterogeneous media

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Cited by 102 publications
(108 citation statements)
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“…Equation (15) provides a subgrid-scale model for the membrane diffusion, and it is conveniently implemented even in arbitrarily complex geometries. Previously partialbounceback schemes have been used in the LBM context for modeling transport in porous media [15][16][17][18], thermal conduction across the boundary between two materials [19], or slip flows [20,21].…”
Section: Lattice-boltzmann Modeling Of Diffusion Across a Membranementioning
confidence: 99%
“…Equation (15) provides a subgrid-scale model for the membrane diffusion, and it is conveniently implemented even in arbitrarily complex geometries. Previously partialbounceback schemes have been used in the LBM context for modeling transport in porous media [15][16][17][18], thermal conduction across the boundary between two materials [19], or slip flows [20,21].…”
Section: Lattice-boltzmann Modeling Of Diffusion Across a Membranementioning
confidence: 99%
“…Individual lattice nodes on one length scale are assigned generic properties of the underlying material at that node without explicitly describing the underlying material structure at the shorter length scale. Amongst such methods, the partial bounce back, effective media, algorithm proposed by Dardis and McCloskey, [9], and refined by Walsh, Burwinkle and Saar, (WBS), [10], is particularly easy to implement and computationally efficient. It has the advantage that, unlike some other schemes, it conserves mass and an analytic expression exists relating the permeability to the effective media parameter.…”
Section: Introductionmentioning
confidence: 99%
“…To overcome this difficulty, we adopt LB effective media methods based on the ideas of partial bounce-back [22][23][24] to describe the C-S-H phase. Hence, each numerical node represents a permeable capillary pore, or an element of weakly-permeable nano-porous C-S-H, or an impermeable solid inclusion such as unhydrated cement.…”
Section: Introductionmentioning
confidence: 99%
“…noting that one of the methods that can be used to derive equation (13) starts by projecting the 3D lattice onto a 1D lattice (see Appendix A of [24]). The case of 0.5 σ = is a special case and may be interpreted as a checkerboard structure with 50% impermeable solids and 50% pores: the permeability of a checkerboard structure equals the permeability of a homogeneous medium for which ( ) 0.5 .…”
Section: Validation Of the Algorithmmentioning
confidence: 99%