Jump conditions for filtered quantities at an under-resolved discontinuous interface. Part 1: Theoretical development
暂无分享,去创建一个
O. Lebaigue | D. Jamet | Adrien Toutant | M. Chandesris | M. Chandesris | O. Lebaigue | A. Toutant | D. Jamet
[1] Célia Fouillet. Généralisation à des mélanges binaires de la méthode du second gradient et application à la simulation numérique directe de l'ébullition nucléée , 2003 .
[2] Said Elghobashi,et al. Prediction of the particle-laden jet with a two-equation turbulence model , 1984 .
[3] Santiago Laín,et al. Modelling hydrodynamics and turbulence in a bubble column using the Euler-Lagrange procedure , 2002 .
[4] Kyle D. Squires,et al. Preferential concentration of marine particles in isotropic turbulence , 1995 .
[5] D. Homescu,et al. Forced Convection Condensation on a Horizontal Tube: Influence of Turbulence in the Vapor and , 1999 .
[6] Donald M. Anderson,et al. A phase-field model with convection: sharp-interface asymptotics , 2001 .
[7] Lian Shen,et al. Large-eddy simulation of free-surface turbulence , 2001, Journal of Fluid Mechanics.
[8] D. Zwillinger. Handbook of differential equations , 1990 .
[9] K. Squires,et al. On the prediction of gas–solid flows with two-way coupling using large eddy simulation , 2000 .
[10] D. Jamet,et al. Boundary conditions at a fluid–porous interface: An a priori estimation of the stress jump coefficients , 2007 .
[11] Olivier Simonin,et al. DNS of the interaction between a deformable buoyant bubble and a spatially decaying turbulence: A priori tests for LES two-phase flow modelling , 2008 .
[12] O. Lebaigue,et al. Jump conditions for filtered quantities at an under-resolved discontinuous interface. Part 2: A priori tests , 2009 .
[13] D. Jamet,et al. Boundary conditions at a planar fluid–porous interface for a Poiseuille flow , 2006 .
[14] Benoît Mathieu. Etudes physique, expérimentale et numérique des mécanismes de base intervenant dans les écoulements diphasiques , 2003 .
[15] Pierre Sagaut,et al. On the filtering paradigm for LES of flows with discontinuities , 2005 .
[16] R. Aris. Vectors, Tensors and the Basic Equations of Fluid Mechanics , 1962 .
[17] Djamel Lakehal,et al. Large-eddy simulation of bubbly turbulent shear flows , 2002 .
[18] Y. Sato,et al. Liquid velocity distribution in two-phase bubble flow , 1975 .
[19] G. Hetsroni. Handbook of hydraulic resistance , 1990 .
[20] Erik Damgaard Christensen,et al. Large eddy simulation of breaking waves , 2001 .
[21] Pierre Sagaut,et al. Towards large eddy simulation of isothermal two-phase flows: Governing equations and a priori tests , 2007 .
[22] John R. Fessler,et al. Preferential concentration of particles by turbulence , 1991 .
[23] Donald A. Drew,et al. The virtual mass and lift force on a sphere in rotating and straining inviscid flow , 1987 .
[24] J. M. Delhaye,et al. Jump conditions and entropy sources in two-phase systems , 1974 .
[25] Isabelle Calmet,et al. Statistical structure of high-Reynolds-number turbulence close to the free surface of an open-channel flow , 2003, Journal of Fluid Mechanics.
[26] D. Drew,et al. Theory of Multicomponent Fluids , 1998 .
[27] Hiroshi Saeki,et al. Velocity field after wave breaking , 2002 .
[28] P. Sagaut. Large Eddy Simulation for Incompressible Flows , 2001 .
[29] S. Menon,et al. Effect of subgrid models on the computed interscale energy transfer in isotropic turbulence , 1994 .
[30] Howard Brenner,et al. Interfacial transport processes and rheology , 1991 .