The evolution from an unsteady to a steady mixing zone between two groundwater flow systems with different concentrations

Heat and mass transport through porous media is governed by the advection-dispersion equation. Near the forward moving mixing front the longitudinal and transversal dispersion lengths are non-zero; only dispersion by molecular diffusion remains. The present paper presents mathematical-physical argum...

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Main Authors: Wouter Zijl, Mustafa El-Rawy
Format: Article
Language:English
Published: Elsevier 2019-06-01
Series:Alexandria Engineering Journal
Online Access:http://www.sciencedirect.com/science/article/pii/S1110016819300523
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spelling doaj-9c31e841a7c6456889a69f331f071d942021-06-02T16:02:35ZengElsevierAlexandria Engineering Journal1110-01682019-06-01582725731The evolution from an unsteady to a steady mixing zone between two groundwater flow systems with different concentrationsWouter Zijl0Mustafa El-Rawy1Dept. of Hydrology and Hydraulic Engineering, Vrije Universiteit Brussel, Pleinlaan 2, 1050 Brussels, BelgiumDept. of Civil Engineering, Faculty of Engineering, Minia University, Minia 61111, Egypt; Civil Engineering Department, College of Engineering, Shaqra University, 11911 Dawadmi, Ar Riyadh, Saudi Arabia; Corresponding author at: Dept. of Civil Engineering, Faculty of Engineering, Minia University, Minia 61111, Egypt.Heat and mass transport through porous media is governed by the advection-dispersion equation. Near the forward moving mixing front the longitudinal and transversal dispersion lengths are non-zero; only dispersion by molecular diffusion remains. The present paper presents mathematical-physical arguments why in steady transport the dispersion lengths are equal to zero. In conventional models the dispersion lengths are generally assumed to be process-independent. To interpolate between the relatively large dispersion lengths near time-dependent moving front and the steady transport conditions far away from the front, a mathematical model is proposed to describe the process-dependent time-evolution of the dispersion lengths. In this model, the dispersion lengths near the forward moving front are equal to the well-established conventional dispersion lengths that correctly represent the mixing near the front. However, further behind the moving front, where the mass transport has become (almost) steady, the process-dependent model results in vanishing dispersion lengths and, consequently, in a substantially smaller transversal mixing zone. Keywords: Advection, Flow systems, Mixing, Steady transport, Transversal dispersionhttp://www.sciencedirect.com/science/article/pii/S1110016819300523
collection DOAJ
language English
format Article
sources DOAJ
author Wouter Zijl
Mustafa El-Rawy
spellingShingle Wouter Zijl
Mustafa El-Rawy
The evolution from an unsteady to a steady mixing zone between two groundwater flow systems with different concentrations
Alexandria Engineering Journal
author_facet Wouter Zijl
Mustafa El-Rawy
author_sort Wouter Zijl
title The evolution from an unsteady to a steady mixing zone between two groundwater flow systems with different concentrations
title_short The evolution from an unsteady to a steady mixing zone between two groundwater flow systems with different concentrations
title_full The evolution from an unsteady to a steady mixing zone between two groundwater flow systems with different concentrations
title_fullStr The evolution from an unsteady to a steady mixing zone between two groundwater flow systems with different concentrations
title_full_unstemmed The evolution from an unsteady to a steady mixing zone between two groundwater flow systems with different concentrations
title_sort evolution from an unsteady to a steady mixing zone between two groundwater flow systems with different concentrations
publisher Elsevier
series Alexandria Engineering Journal
issn 1110-0168
publishDate 2019-06-01
description Heat and mass transport through porous media is governed by the advection-dispersion equation. Near the forward moving mixing front the longitudinal and transversal dispersion lengths are non-zero; only dispersion by molecular diffusion remains. The present paper presents mathematical-physical arguments why in steady transport the dispersion lengths are equal to zero. In conventional models the dispersion lengths are generally assumed to be process-independent. To interpolate between the relatively large dispersion lengths near time-dependent moving front and the steady transport conditions far away from the front, a mathematical model is proposed to describe the process-dependent time-evolution of the dispersion lengths. In this model, the dispersion lengths near the forward moving front are equal to the well-established conventional dispersion lengths that correctly represent the mixing near the front. However, further behind the moving front, where the mass transport has become (almost) steady, the process-dependent model results in vanishing dispersion lengths and, consequently, in a substantially smaller transversal mixing zone. Keywords: Advection, Flow systems, Mixing, Steady transport, Transversal dispersion
url http://www.sciencedirect.com/science/article/pii/S1110016819300523
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