2022
DOI: 10.1016/j.sctalk.2022.100042
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On the determination of a generalized Darcy equation for yield stress fluid in porous media

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Cited by 4 publications
(2 citation statements)
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“…Howell and Atkinson (1976) showed that, in trickling filters, constant influent concentration and operating conditions can yield large fluctuations induced by sloughing events. Stewart and Scott Fogler (2002) found very large oscillations in the pressure signal due to the formation of successive stable or unstable dextran plugs of Leuconostoc mesenteroides biofilm, behaving in a way similar to a yield stress fluid, and allowing flow only through breakthrough channels -see also discussions on the flow of yield stress fluids through porous media in (Talon, 2022). Sharp et al (2005) showed that "the pore channels are dynamic, changing in sized, number and location with time" in a flat plate reactor colonized by Vibrio fischeri biofilm.…”
Section: Self-sustained Fluctuationsmentioning
confidence: 99%
“…Howell and Atkinson (1976) showed that, in trickling filters, constant influent concentration and operating conditions can yield large fluctuations induced by sloughing events. Stewart and Scott Fogler (2002) found very large oscillations in the pressure signal due to the formation of successive stable or unstable dextran plugs of Leuconostoc mesenteroides biofilm, behaving in a way similar to a yield stress fluid, and allowing flow only through breakthrough channels -see also discussions on the flow of yield stress fluids through porous media in (Talon, 2022). Sharp et al (2005) showed that "the pore channels are dynamic, changing in sized, number and location with time" in a flat plate reactor colonized by Vibrio fischeri biofilm.…”
Section: Self-sustained Fluctuationsmentioning
confidence: 99%
“…Nevertheless, in the intricate transport mechanism of yield-stress fluids through porous media, several mutual features can be identified regardless of the scales on which the previous studies are focused. In a number of studies (Talon & Bauer 2013;Liu et al 2019;Talon 2022), four regimes are detected in terms of flow rate (Q)-applied pressure gradient ( P/L): (i) when the applied pressure gradient is less than a critical pressure gradient ( P c /L), there is no flow (Q = 0); (ii) if the applied pressure gradient slightly exceeds the critical value, the flow is extremely localised in a channel and the flow rate linearly scales with the excessive pressure gradient where other parts of the fluid are quiescent; (iii) the third regime emerges when the applied pressure gradient increases, more and more channels appear (moderate values of pressure gradient) and the flow rate scales quadratically with the excessive applied pressure gradient; (iv) finally, when the applied pressure gradient is much higher than the critical value, the flow rate again scales linearly with the excessive pressure gradient.…”
Section: Introductionmentioning
confidence: 99%