Bubble Dynamics in Stationary Two-phase Flow Through Disordered Porous Media

Two-phase flow through porous media leads to the formation of drops and fingers, which eventually break and merge or may be trapped behind obstacles. This complex dynamical behavior highly influences macroscopic properties such as the effective permeability and it also creates characteristic fluctua...

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Main Authors: J. M. A. Sales, H. J. Seybold, C. L. N. Oliveira, J. S. Andrade
Format: Article
Language:English
Published: Frontiers Media S.A. 2022-03-01
Series:Frontiers in Physics
Subjects:
Online Access:https://www.frontiersin.org/articles/10.3389/fphy.2022.860190/full
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author J. M. A. Sales
H. J. Seybold
H. J. Seybold
C. L. N. Oliveira
J. S. Andrade
author_facet J. M. A. Sales
H. J. Seybold
H. J. Seybold
C. L. N. Oliveira
J. S. Andrade
author_sort J. M. A. Sales
collection DOAJ
description Two-phase flow through porous media leads to the formation of drops and fingers, which eventually break and merge or may be trapped behind obstacles. This complex dynamical behavior highly influences macroscopic properties such as the effective permeability and it also creates characteristic fluctuations in the velocity fields of the two phases, as well as in their relative permeability curves. In order to better understand how the microscopic behavior of the flow affects macroscopic properties of two phases, we simulate the velocity fields of two immiscible fluids flowing through a two-dimensional porous medium. By analyzing the fluctuations in the velocity fields of the two phases, we find that the system is ergodic for large volume fractions of the less viscous phase and high capillary numbers Ca. We also see that the distribution of drop sizes m follows a power-law scaling, P(m)∝m−ξ. The exponent ξ depends on the capillary number. Below a characteristic capillary number, namely Ca* ≈ 0.046, the drops are large and cohesive with a constant scaling exponent ξ ≈ 1.23 ± 0.03. Above the characteristic capillary number Ca*, the flow is dominated by many small droplets and few finger-like spanning clusters. In this regime the exponent ξ increases approaching 2.05 ± 0.03 in the limit of infinite capillary number. Our analysis also shows that the temporal mean velocity of the entire mixture can be described by a generalization of Darcy’s law of the form v̄(m)∝(∇P)β where the exponent β is sensitive to the surface tension between the two phases. In the limit of infinite capillary numbers the mobility term increases exponentially with the saturation of the less viscous phase. This result agrees with previous observations for effective permeabilities found in dissolved-gas-driven reservoirs.
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spelling doaj.art-a2cb4d27dc1540c8a9dd0a02ec9b8d272022-12-21T23:51:12ZengFrontiers Media S.A.Frontiers in Physics2296-424X2022-03-011010.3389/fphy.2022.860190860190Bubble Dynamics in Stationary Two-phase Flow Through Disordered Porous MediaJ. M. A. Sales0H. J. Seybold1H. J. Seybold2C. L. N. Oliveira3J. S. Andrade4Departamento de Física, Universidade Federal do Ceará, Fortaleza, BrazilDepartamento de Física, Universidade Federal do Ceará, Fortaleza, BrazilDepartment of Environmental Systems Science, ETH Zurich, Zurich, SwitzerlandDepartamento de Física, Universidade Federal do Ceará, Fortaleza, BrazilDepartamento de Física, Universidade Federal do Ceará, Fortaleza, BrazilTwo-phase flow through porous media leads to the formation of drops and fingers, which eventually break and merge or may be trapped behind obstacles. This complex dynamical behavior highly influences macroscopic properties such as the effective permeability and it also creates characteristic fluctuations in the velocity fields of the two phases, as well as in their relative permeability curves. In order to better understand how the microscopic behavior of the flow affects macroscopic properties of two phases, we simulate the velocity fields of two immiscible fluids flowing through a two-dimensional porous medium. By analyzing the fluctuations in the velocity fields of the two phases, we find that the system is ergodic for large volume fractions of the less viscous phase and high capillary numbers Ca. We also see that the distribution of drop sizes m follows a power-law scaling, P(m)∝m−ξ. The exponent ξ depends on the capillary number. Below a characteristic capillary number, namely Ca* ≈ 0.046, the drops are large and cohesive with a constant scaling exponent ξ ≈ 1.23 ± 0.03. Above the characteristic capillary number Ca*, the flow is dominated by many small droplets and few finger-like spanning clusters. In this regime the exponent ξ increases approaching 2.05 ± 0.03 in the limit of infinite capillary number. Our analysis also shows that the temporal mean velocity of the entire mixture can be described by a generalization of Darcy’s law of the form v̄(m)∝(∇P)β where the exponent β is sensitive to the surface tension between the two phases. In the limit of infinite capillary numbers the mobility term increases exponentially with the saturation of the less viscous phase. This result agrees with previous observations for effective permeabilities found in dissolved-gas-driven reservoirs.https://www.frontiersin.org/articles/10.3389/fphy.2022.860190/fullporous mediatwo phase flowOnsager symmetrycomputational fluid dynamicsgeneralized Darcy’s law
spellingShingle J. M. A. Sales
H. J. Seybold
H. J. Seybold
C. L. N. Oliveira
J. S. Andrade
Bubble Dynamics in Stationary Two-phase Flow Through Disordered Porous Media
Frontiers in Physics
porous media
two phase flow
Onsager symmetry
computational fluid dynamics
generalized Darcy’s law
title Bubble Dynamics in Stationary Two-phase Flow Through Disordered Porous Media
title_full Bubble Dynamics in Stationary Two-phase Flow Through Disordered Porous Media
title_fullStr Bubble Dynamics in Stationary Two-phase Flow Through Disordered Porous Media
title_full_unstemmed Bubble Dynamics in Stationary Two-phase Flow Through Disordered Porous Media
title_short Bubble Dynamics in Stationary Two-phase Flow Through Disordered Porous Media
title_sort bubble dynamics in stationary two phase flow through disordered porous media
topic porous media
two phase flow
Onsager symmetry
computational fluid dynamics
generalized Darcy’s law
url https://www.frontiersin.org/articles/10.3389/fphy.2022.860190/full
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