2017
DOI: 10.1016/j.compfluid.2016.09.015
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Pore-scale study on reactive mixing of miscible solutions with viscous fingering in porous media

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Cited by 28 publications
(16 citation statements)
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“…Here ρ p is a variable related to the fluid pressure as p = c 2 s ρ p , with c s = e/ √ 3 being the lattice sound velocity. To avoid discrete lattice effects in the LB model, the forcing and reactive distribution functionsF i andR i are [18,20]…”
Section: Methodsmentioning
confidence: 99%
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“…Here ρ p is a variable related to the fluid pressure as p = c 2 s ρ p , with c s = e/ √ 3 being the lattice sound velocity. To avoid discrete lattice effects in the LB model, the forcing and reactive distribution functionsF i andR i are [18,20]…”
Section: Methodsmentioning
confidence: 99%
“…, ψ 8 ) T to the moment space asψ = M • ψ. With this transformation, the evolution equations (20) and (21) can be implemented in the moment space aŝ…”
Section: Methodsmentioning
confidence: 99%
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“…The study of flow through confined porous media is of great importance in geology (Lei et al 2017), petroleum (Song et al 2014) and industry (Rahimi et al 2017). Flow through pressurized porous media has been studied experimentally and numerically by (Ingham and 119 Pop 2005;Sheikh and Pak 2015;and Zhu et al 2016).…”
Section: K = 65mentioning
confidence: 99%
“…Here ρ p is a variable related to fluid pressure as ρ p = p/c 2 s , with c s = e/ √ 3 being the lattice sound velocity. This LB model for incompressible fluid flows can reduce compressible errors [40,41]. Different from the original model [5], the distribution function F i accounts for both the body force F and the source term M as…”
Section: A Lb Equation For the Flow Fieldmentioning
confidence: 99%