2019
DOI: 10.1103/physrevfluids.4.034305
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Disorder characterization of porous media and its effect on fluid displacement

Abstract: We investigate the effects of topological disorder and wettability on fluid displacement in porous media. A modified disorder index I v is proposed to characterize the disorder of porous media. By changing I v , different displacement patterns (stable displacement and fingering) under the same flow condition and fluid property are obtained. We analytically demonstrate how increase in disorder promotes fingering due to uneven distribution of local capillary pressure. It is shown that the displacement efficiency… Show more

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Cited by 61 publications
(54 citation statements)
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“…Recent research focused on the impact of wettability on fluid pattern formation and on capillary trapping (Wang et al, 2019). In their classical work Cieplak and Robbins (1988) discussed an interesting dynamical phase transition associated with changes in local growth modes at the displacement front .…”
Section: Introductionmentioning
confidence: 99%
“…Recent research focused on the impact of wettability on fluid pattern formation and on capillary trapping (Wang et al, 2019). In their classical work Cieplak and Robbins (1988) discussed an interesting dynamical phase transition associated with changes in local growth modes at the displacement front .…”
Section: Introductionmentioning
confidence: 99%
“…Recent research has focused on capillary trapping and the impact of wettability on fluid pattern formation. Wang et al (2019) studied the combined effect of viscous and capillary forces, local disorder, and wettability using Lattice-Boltzmann simulations. The 2-D triangular stochastic lattice consisted of circular grains with a uniformly distributed grain diameter.…”
Section: Introductionmentioning
confidence: 99%
“…This increase in e↵ective contact angle suppresses cooperative pore filling events, promoting trapping 16,65 , consistent with past results. [11][12][13][14]16 Moreover, the volume of trapped ganglia for cases with large Dy (Dy = 12, slow wetting transition) can be very close to the one with Dy = 1 where wetting transition does not take place. However, from Fig.3(B The interfacial length in lattice unit l l can be defined as the total front length between the defending fluid and the union of invading fluid and grains, as shown by the white-solid curve in Fig.3(A).…”
Section: Displacement E Ciencymentioning
confidence: 80%