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Volumn 53, Issue 1, 1996, Pages 743-750

Simulation of multicomponent fluids in complex three-dimensional geometries by the lattice Boltzmann method

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Indexed keywords


EID: 1842650686     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.53.743     Document Type: Article
Times cited : (864)

References (39)
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    • F. A. L. Dullien, Porous Media: Fluid Transport and Pore Structure (Academic, San Diego, 1992).
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  • 2
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    • T. Vicsek, Fractal Growth Phenomena (World Scientific, Singapore, 1989); Dynamics of Fractal Surfaces, edited by F. Family and T. Vicsek (World Scientific, Singapore, 1991).
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  • 6
    • 25744459324 scopus 로고    scopus 로고
    • G. McNamara and G. Zanetti, Phys. Rev. Lett. 61, 2332 91988);
    • G. McNamara and G. Zanetti, Phys. Rev. Lett. 61, 2332 91988);
  • 15
    • 0040455481 scopus 로고
    • Discrete Kinetic Theory, Lattice Gas Dynamics and Foundations of Hydrodynamics
    • R. Monaco World Scientific, Singapore
    • K. Molvig, P. Donis, J. Myczkowski, and G. Vichniac, in Discrete Kinetic Theory, Lattice Gas Dynamics and Foundations of Hydrodynamics, edited by R. Monaco (World Scientific, Singapore, 1988).
    • (1988)
    • Molvig, K.1    Donis, P.2    Myczkowski, J.3    Vichniac, G.4
  • 24
    • 85035213873 scopus 로고    scopus 로고
    • Los Alamos Science, Mail Stop M708, Los Alamos National Laboratory, Los Alamos, NM 87545.
    • Los Alamos Science, Mail Stop M708, Los Alamos National Laboratory, Los Alamos, NM 87545.
  • 29
    • 0002005819 scopus 로고
    • For a lattice gas approach to modeling phase transitions see C. Appert and S. Zaleski, Phys. Rev. Lett. 64, 1 (1990).
    • (1990) Phys. Rev. Lett. , vol.64 , pp. 1
    • Appert, C.1    Zaleski, S.2
  • 30
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    • An Introduction to Fluid Dynamics
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    • (1967)
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  • 36
    • 85035221774 scopus 로고    scopus 로고
    • Experimental data provided by courtesy of T. S. Ramakrishnan of Schlumberger-Doll. The relative permeability was obtained for the case of water displacing dodecane (wetting displacement) or dodecane displacing water (nonwetting displacement). The viscosity ratio between dodecane and water is about 1.5. In our simulations our viscosity ratio was 1. Since in both experiment and simulation the capillary number was very low, of order [Formula Presented] and [Formula Presented], respectively, we do not believe viscous effects (such as viscous fingering) were very important.
    • Experimental data provided by courtesy of T. S. Ramakrishnan of Schlumberger-Doll. The relative permeability was obtained for the case of water displacing dodecane (wetting displacement) or dodecane displacing water (nonwetting displacement). The viscosity ratio between dodecane and water is about 1.5. In our simulations our viscosity ratio was 1. Since in both experiment and simulation the capillary number was very low, of order 10-4 and 10-3, respectively, we do not believe viscous effects (such as viscous fingering) were very important.


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