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Interface condition for the Darcy velocity at the water-oil flood front in the porous medium

Flood front is the jump interface where fluids distribute discontinuously, whose interface condition is the theoretical basis of a mathematical model of the multiphase flow in porous medium. The conventional interface condition at the jump interface is expressed as the continuous Darcy velocity and...

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Detalles Bibliográficos
Autores principales: Peng, Xiaolong, Liu, Yong, Liang, Baosheng, Du, Zhimin
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Public Library of Science 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5441608/
https://www.ncbi.nlm.nih.gov/pubmed/28542612
http://dx.doi.org/10.1371/journal.pone.0177187
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author Peng, Xiaolong
Liu, Yong
Liang, Baosheng
Du, Zhimin
author_facet Peng, Xiaolong
Liu, Yong
Liang, Baosheng
Du, Zhimin
author_sort Peng, Xiaolong
collection PubMed
description Flood front is the jump interface where fluids distribute discontinuously, whose interface condition is the theoretical basis of a mathematical model of the multiphase flow in porous medium. The conventional interface condition at the jump interface is expressed as the continuous Darcy velocity and fluid pressure (named CVCM). Our study has inspected this conclusion. First, it is revealed that the principle of mass conservation has no direct relation to the velocity conservation, and the former is not the true foundation of the later, because the former only reflects the kinetic characteristic of the fluid particles at one position(the interface), but not the different two parts of fluid on the different side of the interface which required by the interface conditions. Then the reasonableness of CVCM is queried from the following three aspects:(1)Using Mukat’s two phase seepage equation and the mathematical method of apagoge, we have disproved the continuity of each fluid velocity;(2)Since the analytical solution of the equation of Buckley-Leveret equations is acquirable, its velocity jumps at the flood front presents an appropriate example to disprove the CVCM;(3) The numerical simulation model gives impractical result that flood front would stop moving if CVCM were used to calculate the velocities at the interface between two gridcells. Subsequently, a new one, termed as Jump Velocity Condition Model (JVCM), is deduced from Muskat’s two phase seepage equations and Darcy’s law without taking account of the capillary force and compressibility of rocks and fluids. Finally, several cases are presented. And the comparisons of the velocity, pressure difference and the front position, which are given by JVCM, CVCM and SPU, have shown that the result of JVCM is the closest to the exact solution.
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spelling pubmed-54416082017-06-06 Interface condition for the Darcy velocity at the water-oil flood front in the porous medium Peng, Xiaolong Liu, Yong Liang, Baosheng Du, Zhimin PLoS One Research Article Flood front is the jump interface where fluids distribute discontinuously, whose interface condition is the theoretical basis of a mathematical model of the multiphase flow in porous medium. The conventional interface condition at the jump interface is expressed as the continuous Darcy velocity and fluid pressure (named CVCM). Our study has inspected this conclusion. First, it is revealed that the principle of mass conservation has no direct relation to the velocity conservation, and the former is not the true foundation of the later, because the former only reflects the kinetic characteristic of the fluid particles at one position(the interface), but not the different two parts of fluid on the different side of the interface which required by the interface conditions. Then the reasonableness of CVCM is queried from the following three aspects:(1)Using Mukat’s two phase seepage equation and the mathematical method of apagoge, we have disproved the continuity of each fluid velocity;(2)Since the analytical solution of the equation of Buckley-Leveret equations is acquirable, its velocity jumps at the flood front presents an appropriate example to disprove the CVCM;(3) The numerical simulation model gives impractical result that flood front would stop moving if CVCM were used to calculate the velocities at the interface between two gridcells. Subsequently, a new one, termed as Jump Velocity Condition Model (JVCM), is deduced from Muskat’s two phase seepage equations and Darcy’s law without taking account of the capillary force and compressibility of rocks and fluids. Finally, several cases are presented. And the comparisons of the velocity, pressure difference and the front position, which are given by JVCM, CVCM and SPU, have shown that the result of JVCM is the closest to the exact solution. Public Library of Science 2017-05-23 /pmc/articles/PMC5441608/ /pubmed/28542612 http://dx.doi.org/10.1371/journal.pone.0177187 Text en © 2017 Peng et al http://creativecommons.org/licenses/by/4.0/ This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/) , which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.
spellingShingle Research Article
Peng, Xiaolong
Liu, Yong
Liang, Baosheng
Du, Zhimin
Interface condition for the Darcy velocity at the water-oil flood front in the porous medium
title Interface condition for the Darcy velocity at the water-oil flood front in the porous medium
title_full Interface condition for the Darcy velocity at the water-oil flood front in the porous medium
title_fullStr Interface condition for the Darcy velocity at the water-oil flood front in the porous medium
title_full_unstemmed Interface condition for the Darcy velocity at the water-oil flood front in the porous medium
title_short Interface condition for the Darcy velocity at the water-oil flood front in the porous medium
title_sort interface condition for the darcy velocity at the water-oil flood front in the porous medium
topic Research Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5441608/
https://www.ncbi.nlm.nih.gov/pubmed/28542612
http://dx.doi.org/10.1371/journal.pone.0177187
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