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Permeability of Self-Affine Aperture Fields

Authors :
Harold Auradou
Laurent Talon
Alex Hansen
Fluides, automatique, systèmes thermiques (FAST)
Université Paris-Sud - Paris 11 (UP11)-Université Pierre et Marie Curie - Paris 6 (UPMC)-Centre National de la Recherche Scientifique (CNRS)
Department of Physics [Trondheim] (Physics NTNU)
Norwegian University of Science and Technology [Trondheim] (NTNU)
Norwegian University of Science and Technology (NTNU)-Norwegian University of Science and Technology (NTNU)
PICS research project: 'The Physics of Geological Complex Systems'
Source :
Physical Review E : Statistical, Nonlinear, and Soft Matter Physics, Physical Review E : Statistical, Nonlinear, and Soft Matter Physics, American Physical Society, 2010, 82 (4), pp.046108. ⟨10.1103/PhysRevE.82.046108⟩, Physical Review E : Statistical, Nonlinear, and Soft Matter Physics, 2010, 82 (4), pp.046108. ⟨10.1103/PhysRevE.82.046108⟩
Publication Year :
2010
Publisher :
HAL CCSD, 2010.

Abstract

International audience; We introduce a model that allows for the prediction of the permeability of self-affine rough channels (one-dimensional fracture) and two-dimensional fractures over a wide range of apertures. In the lubrication approximation, the permeability shows three different scaling regimes. For fractures with a large mean aperture or an aperture small enough to the permeability being close to disappearing, the permeability scales as the cube of the aperture when the zero level of the aperture is set to coincide with the disappearance of the permeability. Between these two regimes, there is a third regime where the scaling is due to the self-affine roughness. For rough channels, the exponent is found to be $3-1/H$ where $H$ is the Hurst exponent. For two-dimensional fractures, it is necessary to introduce a new equivalent aperture $b_c$ to make the scaling regime apparent. $b_c$ is defined as the hydraulic aperture of the most restrective barrier crossing the fracture normal to the flow direction. This regime is characterized by an exponent higher than for the one-dimensional case: it is $2.25$ for $H=0.8$ and $2.16$ for $H=0.3$.

Details

Language :
English
ISSN :
15393755 and 15502376
Database :
OpenAIRE
Journal :
Physical Review E : Statistical, Nonlinear, and Soft Matter Physics, Physical Review E : Statistical, Nonlinear, and Soft Matter Physics, American Physical Society, 2010, 82 (4), pp.046108. ⟨10.1103/PhysRevE.82.046108⟩, Physical Review E : Statistical, Nonlinear, and Soft Matter Physics, 2010, 82 (4), pp.046108. ⟨10.1103/PhysRevE.82.046108⟩
Accession number :
edsair.doi.dedup.....44972f7172bc6e89b3c5fdd5ceda485c
Full Text :
https://doi.org/10.1103/PhysRevE.82.046108⟩