2004
DOI: 10.1016/j.advwatres.2004.02.021
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On the non-linear behavior of a laminar single-phase flow through two and three-dimensional porous media

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Cited by 131 publications
(71 citation statements)
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“…2) is obtained for flow experiments on sand and gravel for a wide range of Reynold numbers (e.g., Moutsopoulos et al 2009;Sedghi-Asl et al 2014). Similar conclusions can be obtained from numerical studies, such as Firdaouss et al (1997) and Fourar et al (2004), which consider the Forchheimer equation (Eq. 2) valid over a wide range of Reynolds numbers.…”
Section: Nonlinear Laminar Flow and Fully Turbulent Flow In Porous Mediasupporting
confidence: 64%
“…2) is obtained for flow experiments on sand and gravel for a wide range of Reynold numbers (e.g., Moutsopoulos et al 2009;Sedghi-Asl et al 2014). Similar conclusions can be obtained from numerical studies, such as Firdaouss et al (1997) and Fourar et al (2004), which consider the Forchheimer equation (Eq. 2) valid over a wide range of Reynolds numbers.…”
Section: Nonlinear Laminar Flow and Fully Turbulent Flow In Porous Mediasupporting
confidence: 64%
“…More realistic flow simulations in three dimensions were performed by Hill and Koch (2002), by means of the lattice-Boltzmann method (which makes use of the relation between fluid flow and kinetic gas theory), and also by Fourar et al (2004). Fourar et al (2004), in their numerical study of high-velocity effects in periodic porous media, state that viscous dissipation in the recirculation area is not preponderant.…”
Section: Theoretical Background and Proposed Relationsmentioning
confidence: 99%
“…This equation was obtained by numerical simulations in a two-dimensional periodic porous medium, and by using the homogenization technique for an isotropic homogeneous 3D porous medium. In spite of the numerous attempts to clarify the physical reasons for the non-linear behavior described above, neither Forchheimer equation (2) nor the weak inertia equation (4) have received any physical justification (Fourar et al, 2004). The pressure gradient across the foam is thus a function of system geometry (porosity, pore and ligament size...), as well as physical properties of the fluid phase (viscosity, density).…”
Section: Flow Lawmentioning
confidence: 99%