2005
DOI: 10.1140/epjb/e2005-00288-x
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Dynamics and kinetic roughening of interfaces in two-dimensional forced wetting

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Cited by 14 publications
(38 citation statements)
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“…Finally, we claim that the existence of a singular behavior as v → 0 and the extent of the critical region v ≤ L −2 explain earlier numerical observations [5,10] that reported a dependence of the critical exponents α(v) and z(v) with the velocity in numerical results of forced-flow imbibition in finite systems. Table I summarizes the different interfacial scaling exponents we observed for different velocities.…”
supporting
confidence: 82%
See 1 more Smart Citation
“…Finally, we claim that the existence of a singular behavior as v → 0 and the extent of the critical region v ≤ L −2 explain earlier numerical observations [5,10] that reported a dependence of the critical exponents α(v) and z(v) with the velocity in numerical results of forced-flow imbibition in finite systems. Table I summarizes the different interfacial scaling exponents we observed for different velocities.…”
supporting
confidence: 82%
“…such that interface fluctuations are uncorrelated above this typical scale. Indeed, several numerical studies [8,10,12] have shown that the interface is asymptotically flat on length scales larger than ξ × , introducing then a natural cutoff in the system. For capillary-induced fluctuations we have ξ × ≪ ξ K , so that the permeability disorder can be ignored.…”
mentioning
confidence: 99%
“…This gives τ f = β ∞ + 1, which corresponds to the previously derived scaling relation (9). This allows us to immediately associate the ∞correlation moment (a global observable) with the distribution of the return times of activity at any given site (a local observable).…”
Section: A Multiscaling Of the Height-height Correlationssupporting
confidence: 62%
“…We now apply the above scaling theory to the problem of forced-flow imbibition in disordered media [7]. As it has been noted in the introduction, the main point in forced-flow imbibition lays in the existence of a natural characteristic length ξ × ∼ (1/v) 1/2 for the typical avalanche extent [7][8][9][10][11], which can be controlled by the liquid flow rate. In this way, we have a system whose activity can be made progressively fractal as the velocity is tuned from moderate to very low values.…”
Section: Case Study: Fluid Imbibition In Random Mediamentioning
confidence: 99%
“…The macroscopic variables and parameters are defined from the phase-field formulation as [25]: In our study, we will consider both situations of spontaneous and forced-flow imbibition by choosing conveniently the boundary conditions into the phase-field model [26]. For spontaneous imbibition an applied constant pressure is imposed at the origin of the cell µ(x, y = 0) = µ a .…”
Section: A the Macroscopic Description Of Imbibitionmentioning
confidence: 99%