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Pore-network modelling of transverse dispersion in porous media under non-Darcy flow conditions

•Non-Darcy flow occurs in the pure mechanical dispersion transport regime.•Neglecting the flow inertial effects causes overestimation of the fluid velocity, Péclet number and transverse dispersion coefficient.•In the diffusion dominated and transition transport regimes, the distance needed to reach...

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Published in:Advances in water resources 2024-03, Vol.185, p.104626, Article 104626
Main Authors: El-Zehairy, A.A., Abdel-Gawad, H.A.A.
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description •Non-Darcy flow occurs in the pure mechanical dispersion transport regime.•Neglecting the flow inertial effects causes overestimation of the fluid velocity, Péclet number and transverse dispersion coefficient.•In the diffusion dominated and transition transport regimes, the distance needed to reach an asymptotic dispersion increases when Péclet number increases.•In the pure mechanical dispersion regime, the distance needed to reach an asymptotic dispersion state is a function of the medium characteristic length. This work is concerned, for the first time, with estimating the transverse dispersion coefficient under non-Darcy laminar flow conditions in porous media using pore-network modeling. The pore-network modelling approach and the mixed cell method are adopted to simulate both the steady laminar flow and the transient transport of solute for Berea and Bentheimer sandstone samples. For non-Darcy flow, the inertial effect is attributed to the quadratic increase of the pore throat mean velocity, which is embedded in the pressure head losses at either expansion or contraction located at the two ends of any pore throat. A time dependent function, based on both Péclet number and average residence time within the pore throat, is used to incorporate the effect of nonuniform pore throat velocity in the dispersion coefficient. A restrictive upper limit of the time step interval is introduced to prevent numerical overshoots of the concentrations calculated over time. For the same pressure gradient through the sample, the results show a decrease in both Péclet number and the coefficient of transverse dispersion in case of adopting the non-Darcy flow condition instead of the Darcy flow one. The percentage of decrease is up to 20 % for the maximum applied pressure gradient through the sample.
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This work is concerned, for the first time, with estimating the transverse dispersion coefficient under non-Darcy laminar flow conditions in porous media using pore-network modeling. The pore-network modelling approach and the mixed cell method are adopted to simulate both the steady laminar flow and the transient transport of solute for Berea and Bentheimer sandstone samples. For non-Darcy flow, the inertial effect is attributed to the quadratic increase of the pore throat mean velocity, which is embedded in the pressure head losses at either expansion or contraction located at the two ends of any pore throat. A time dependent function, based on both Péclet number and average residence time within the pore throat, is used to incorporate the effect of nonuniform pore throat velocity in the dispersion coefficient. A restrictive upper limit of the time step interval is introduced to prevent numerical overshoots of the concentrations calculated over time. For the same pressure gradient through the sample, the results show a decrease in both Péclet number and the coefficient of transverse dispersion in case of adopting the non-Darcy flow condition instead of the Darcy flow one. 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This work is concerned, for the first time, with estimating the transverse dispersion coefficient under non-Darcy laminar flow conditions in porous media using pore-network modeling. The pore-network modelling approach and the mixed cell method are adopted to simulate both the steady laminar flow and the transient transport of solute for Berea and Bentheimer sandstone samples. For non-Darcy flow, the inertial effect is attributed to the quadratic increase of the pore throat mean velocity, which is embedded in the pressure head losses at either expansion or contraction located at the two ends of any pore throat. A time dependent function, based on both Péclet number and average residence time within the pore throat, is used to incorporate the effect of nonuniform pore throat velocity in the dispersion coefficient. A restrictive upper limit of the time step interval is introduced to prevent numerical overshoots of the concentrations calculated over time. 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subjects Dispersion
Inertial flow
Non-Darcy flow
Pore-network modeling
Porous media
Solute transport
title Pore-network modelling of transverse dispersion in porous media under non-Darcy flow conditions
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