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...
Main Authors: | , |
---|---|
Format: | Article |
Language: | English |
Published: |
Elsevier
2019-06-01
|
Series: | Alexandria Engineering Journal |
Online Access: | http://www.sciencedirect.com/science/article/pii/S1110016819300523 |
id |
doaj-9c31e841a7c6456889a69f331f071d94 |
---|---|
record_format |
Article |
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 |
work_keys_str_mv |
AT wouterzijl theevolutionfromanunsteadytoasteadymixingzonebetweentwogroundwaterflowsystemswithdifferentconcentrations AT mustafaelrawy theevolutionfromanunsteadytoasteadymixingzonebetweentwogroundwaterflowsystemswithdifferentconcentrations AT wouterzijl evolutionfromanunsteadytoasteadymixingzonebetweentwogroundwaterflowsystemswithdifferentconcentrations AT mustafaelrawy evolutionfromanunsteadytoasteadymixingzonebetweentwogroundwaterflowsystemswithdifferentconcentrations |
_version_ |
1721403018660806656 |