2010
DOI: 10.1103/physreve.82.046305
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Crossover from fingering to fracturing in deformable disordered media

Abstract: We investigate the displacement of one fluid by another in a deformable medium with pore-scale disorder. We develop a model that captures the dynamic pressure redistribution at the invasion front and the feedback between fluid invasion and microstructure rearrangement. Our results suggest how to collapse the transition between invasion percolation and viscous fingering in the presence of quenched disorder. We predict the emergence of a fracturing pattern for sufficiently deformable media, in agreement with obs… Show more

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Cited by 87 publications
(119 citation statements)
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References 35 publications
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“…Finally, a new regime was reported in the 2D experiment, with a transition between the growth of an air finger and the fracture of the above granular layer at a given height in the cell. Such patterns as fingering and fracturing have been reported in the literature in deformable, saturated porous media, when varying the grain volume fraction [40,55,56]. These patterns, however, were mainly described for horizontal Hele-Shaw cell, in which buoyancy does not govern the system dynamics.…”
Section: Discussionmentioning
confidence: 88%
“…Finally, a new regime was reported in the 2D experiment, with a transition between the growth of an air finger and the fracture of the above granular layer at a given height in the cell. Such patterns as fingering and fracturing have been reported in the literature in deformable, saturated porous media, when varying the grain volume fraction [40,55,56]. These patterns, however, were mainly described for horizontal Hele-Shaw cell, in which buoyancy does not govern the system dynamics.…”
Section: Discussionmentioning
confidence: 88%
“…To rationalize the results, we first define an effective capillary number Ca à that reflects the balance between viscous and capillary forces at the scale of the entire cell as the ratio between a characteristic capillary pressure difference for invasion along the displacement front, δP c , and the characteristic viscous pressure loss across the cell in the direction perpendicular to the front, δP v [18,27]. From simple arguments using the classical Laplace pressure and Darcy's law, we propose the scaling δP c ∼γ=r min −γ=r max ∼ γ=d, and δP v ∼ ðη liq QRÞ=ðγbd 3 Þ, leading to…”
Section: Resultsmentioning
confidence: 99%
“…Extensions to the Lenormand diagram have addressed the effects of gravity [16], pore-scale disorder [17,18], fluid compressibility [3,19], the crossover between regimes including the existence of a Ca-dependent crossover length scale [17,18,[20][21][22], and frictional forces between grains leading to a whole new set of displacement patterns [3,[23][24][25][26][27]]. Yet, this wealth of observations has been restricted to a drainage process.…”
Section: Introductionmentioning
confidence: 99%
“…Previous research shows that at φ ≈ 1, if confining pressures are high, the particle network can lock. Under these conditions, the gas front cannot mobilize the particles, because the mechanical forces that resist particle displacement are stronger than those generated by bubble expansion, and the gas must advance by invading the porespace [15,17,18]. Importantly, the fracture regime was not observed in experiments with in situ bubble generation.…”
Section: The Role Of Particles On Regime Transitionsmentioning
confidence: 97%
“…The transition from fingering to fracturing has been placed at a packing fraction of 0.9 * RCP [10,12]. At RCP, gas migration patterns depend on the confining pressure [15,17,18]. Specifically, low confining stress allows continued fracturing, while increasing the confining stress causes the granular material to become rigid, and forces the gas to invade the pore space in the form of capillary or viscous fingering.…”
Section: Introductionmentioning
confidence: 99%