# S. Nambully, P. Domingo, V. Moureau, L. Vervisch (in press) A Filtered-Laminar-Flame PDF sub-grid scale closure for LES of premixed turbulent flames. Part I: Formalism and application to a bluff-body burner with differential diffusion. Combust. Flame.
# S. Nambully, P. Domingo, V. Moureau, L. Vervisch (in press) A Filtered-Laminar-Flame PDF sub-grid scale closure for LES of premixed turbulent flames: Part II: Application to a stratified bluff-body burner, Combust. Flame.
# B. Farcy, A. Abou-Taouk, L. Vervisch, P. Domingo, N. Perret (2014) Two approaches of chemistry downsizing for simulating Selective Non Catalytic Reduction DeNOx Process, Fuel, 118: 291-299, DOI 10.1016/j.fuel.2013.10.070.
# G. Ribert, L. Vervisch, P. Domingo, Y.-S. Niu (2014) Hybrid transported-tabulated strategy to downsize detailed chemistry for numerical simulation of premixed flames, FLow Turbulence and Combustion, 92(1/2): 175-200. DOI 10.1007/s10494-013-9520-6.
# F. Pecquery, V. Moureau, G. Lartigue, L. Vervisch, A. Roux (2014) Modelling nitrogen oxide emissions in turbulent flames with air dilution: Application to LES of a non-premixed jet-flame, Combust. Flame, 161(2): 496-509.
# X. Petit, G. Ribert, P. Domingo, G. Lartigue (2013) Large-eddy simulation of supercritical fluid injection, ''J. Supercritical Fluids'' '''(84)''': 61 - 73. doi:10.1016/j.supflu.2013.09.011 [http://www.sciencedirect.com/science?_ob=ArticleListURL&_method=list&_ArticleListID=-406086495&_sort=r&_st=13&view=c&_acct=C000032441&_version=1&_urlVersion=0&_userid=1071190&md5=1be41adf80142fdc4879c0665a695946&searchtype=a link].
# M. Sjostrand-Cuif, Y. D'Angelo & E. Albin (in press) No-slip Wall Acoustic Boundary Condition treatment in the Incompressible Limit, Computers and Fluids.
# Z. Pouransari, L. Vervisch, A. Johansson (2013) Heat release effects on mixing scales of non-premixed turbulent wall-jets: A direct numerical simulation study, Int. J. Heat and Fluid Flow, 40(4): 65-80 [http://dx.doi.org/10.1016/j.ijheatfluidflow.2012.12.005]
# N. Yi-Shuai, L. Vervisch, P.-D. Tao, An optimization-based approach to detailed chemistry tabulation: Automated progress variable definition, Combust. Flame, 160(4): 776-785 [http://dx.doi.org/10.1016/j.combustflame.2012.11.015]
# C. Merlin, P. Domingo, L. Vervisch (2013) Immersed boundaries in Large Eddy Simulation of compressible flows, FLow Turbulence and Combustion, 90(1): 29-68 [http://dx.doi.org/10.1007/s10494-012-9421-0]
# E. Albin, H. Nawroth, S. Göke, Y. D’Angelo, C.O Paschereit, Experimental investigation of burning velocities of ultra-wet methane-air-steam mixtures, Fuel Processing Technology, Fuel Processing Technology Volume 107, March 2013, Pages 27–35, [http://dx.doi.org/10.1016/j.fuproc.2012.06.027]
# RA Rego, Y D’Angelo & G Joulin, On nonlinear model equations for the response of premixed flames to acoustic like accelerations, Combustion Theory & Modelling, Volume 17, Issue 1, 2013. [http://dx.doi.org/10.1080/13647830.2012.721900]
# C. Merlin, P. Domingo, L. Vervisch (2012) Large Eddy Simulation of turbulent flames in a Trapped Vortex Combustor (TVC) - A flamelet presumed-pdf closure preserving laminar flame speed Comptes Rendus Mécanique, 340 (11/12): 917-932. [http://dx.doi.org/10.1016/j.crme.2012.10.039]
# G. Lodier, C. Merlin, P. Domingo, L. Vervisch, F. Ravet (2012) Self-ignition scenarios after rapid compression of a turbulent mixture weakly-stratified in temperature, Combust. Flame, 159(11), pp. 3358-3371. [http://dx.doi.org/10.1016/j.combustflame.2012.07.006]
# E. Albin, Y. D’Angelo, Assessment of the Evolution Equation Modelling approach for three-dimensional expanding wrinkled premixed flames, Combustion and Flame 2012[http://dx.doi.org/doi:10.1016/j.combustflame.2011.12.019]
# N. Enjalbert, P. Domingo, L. Vervisch (2012) Mixing time-history effects in Large Eddy Simulation of non-premixed turbulent flames: Flow-Controlled Chemistry Tabulation, Combust. Flame 159(1), pp. 336-352.2012 [http://dx.doi.org/doi:10.1016/j.combustflame.2011.06.005]
# G. Ribert, K. Wang and L. Vervisch, A multi-zone self-similar chemistry tabulation with application to auto-ignition including cool-flames effects, ''Fuel'' '''(91)''': 87 - 92, (2012). [http://www.sciencedirect.com/science/article/pii/S0016236111004339]
# J. Dombard, B. Leveugle, L. Selle, J. Réveillon, T. Poinsot & Y. D'Angelo, Modeling heat transfer in diluted two-phase flows using the Mesoscopic Eulerian Formalism, International Journal of Heat and Mass Transfer, 2011, [http://dx.doi.org/10.1016/j.ijheatmasstransfer.2011.10.050]
# G. Boury & Y. D’Angelo, On third order density contrast expansion of the evolution equation for wrinkled unsteady premixed flames, International Journal of Non-Linear Mechanics, 2011 [http://dx.doi.org/10.1016/j.ijnonlinmec.2011.05.018]
# E. Albin, Y. D'Angelo, L. Vervisch Flow streamline based Navier-Stokes Characteristic Boundary Conditions: modeling for transverse and corner outflows, Computers and Fluids, 2011 [http://dx.doi.org/10.1016/j.compfluid.2011.08.005]
# G. Lodier, L. Vervisch, V. Moureau, P. Domingo (2011) Composition-space premixed flamelet solution with differential diffusion for in situ flamelet-generated manifolds, Combust. Flame 158(10): 2009-2016. [http://dx.doi.org/doi:10.1016/j.combustflame.2011.03.011]
# V. Moureau, P. Domingo, L. Vervisch (2011) From Large-Eddy Simulation to Direct Numerical Simulation of a lean premixed swirl flame: Filtered Laminar Flame-PDF modeling, Combust. Flame 158(7): 1340-1357 [http://dx.doi.org/doi:10.1016/j.combustflame.2010.12.004]
# V. Moureau, P. Domingo, L. Vervisch (2011) Design of a massively parallel CFD code for complex geometries C.R. Mecanique 339(2/3): 141-148.
# E. Albin, Y. D'Angelo, L. Vervisch Using staggered grids with characteristic boundary conditions when solving compressible reactive Navier-Stokes equations Int. J. Numer. Meth. Fl. , Feb 2012, [http://dx.doi.org/doi:10.1002/fld.2520].
# G. Lecocq, S. Richard, J.-B. Michel, L. Vervisch (2011) A new LES model coupling flame surface density and tabulated kinetics approaches to investigate knock and pre-ignition in piston engines Proc. Combust. Inst., 33(2): 3105-3114.
# G. Lecocq, S. Richard, O. Colin, L. Vervisch (2011) Hybrid presumed pdf and flame surface density approaches for Large-Eddy Simulation of premixed turbulent combustion Part 1: Formalism and simulation of a quasi-steady burner Combust. Flame 158(6): 1201-1214.
# G. Lecocq, S. Richard, O. Colin, L. Vervisch (2011) Hybrid presumed pdf and flame surface density approaches for Large-Eddy Simulation of premixed turbulent combustion Part 2: Early flame development after sparking Combust. Flame 158(6): 1215-1226.
# D. Taïeb, G. Ribert, A. Hadjadj (2010) Shock focusing simulations using an optimized High-order WENO numerical scheme, AIAA J. (48,8): 1739-1747.
# K. Wang, G. Ribert, P. Domingo, L. Vervisch (2010) Self-similar behavior and chemistry tabulation of burnt-gases diluted premixed flamelets including heat-loss Combust. Theory and Modelling 14(4): 541-570.
# G. Lecocq, S. Richard, O. Colin, L. Vervisch (2010) Gradient and counter-gradient modelling in premixed flames: theoretical study and application to the LES of a Lean premixed turbulent swirl-burner Comb. Sci. Tech. 182(4-6): 465-479.
# D. Veynante, G. Lodato, P. Domingo, L. Vervisch, E. R. Hawkes (2010) Estimation of three-dimensional flame surface densities from planar images in turbulent premixed combustion Exp. in Fluids 49:267-278.
# L. Vervisch, P. Domingo, G. Lodato, D. Veynante (2010) Scalar energy fluctuations in Large-Eddy Simulation of turbulent flames: Statistical budgets and mesh quality criterion Combust. Flame 157(4): 778-789.
# V. Subramanian, P. Domingo, L. Vervisch (2010) Large-Eddy Simulation of forced ignition of an annular bluff-body burner Combust. Flame 157(3): 579-601.
# P.-D. Nguyen, L. Vervisch, V. Subramanian, P. Domingo (2010) Multi-dimensional flamelet-generated manifolds for partially premixed combustion Combust. Flame 157(1): 43-61.
# G. Lodato, L. Vervisch, P. Domingo (2009) A compressible wall-adapting similarity mixed model for large-eddy simulation of the impinging round jet Phys. Fluids 21:035102.
# L. Pons, N. Darabiha, S. Candel, G. Ribert, V. Yang (2009) Mass transfer and combustion in transcritical non-premixed counterflows, Combust. Theory Model. (13): 57-81.
# G. Godel, P. Domingo, L. Vervisch (2009) Tabulation of NOx chemistry for Large-Eddy Simulation of non-premixed turbulent flames Proc. Combust. Inst. 32: 1555-1551.
# F. Duchaine, A. Corpron, L. Pons, V. Moureau, F. Nicoud, and T. Poinsot (2009) Development and assessment of a coupled strategy for conjugate heat transfer with Large Eddy Simulation. Application to a cooled turbine blade, International Journal of Heat and Fluid Flow, 30(6), 1129-1141 [http://dx.doi.org/10.1016/j.ijheatfluidflow.2009.07.004].
# V. Moureau, B. Fiorina, and H. Pitsch (2009) A level set formulation for premixed combustion LES considering the turbulent flame structure., Comb. and Flame, 156, 801-812 [http://dx.doi.org/10.1016/j.combustflame.2009.01.019].
# E. Riber, V. Moureau, M. Garcia, T. Poinsot and O. Simonin, (2009) Evaluation of numerical strategies for LES of particulate two-phase recirculating flows, J. Comp. Physics, 228, 539-564 [http://dx.doi.org/10.1016/j.jcp.2008.10.001].
# D. Veynante, B. Fiorina, P. Domingo L. Vervisch, (2008) Using self-similar properties of turbulent premixed flames to downsize chemical tables in high-performance numerical simulations Combust. Theory and Modeling 12(6): 1055-1088.
# G. Ribert, N. Zong, V. Yang, L. Pons, N. Darabiha, S. Candel (2008) Counterflow diffusion flames of general fluids: oxygen/hydrogen mixtures, Combust. Flame (154): 319-330.
# J. Galpin, A. Naudin, L. Vervisch, C. Angelberger, O. Colin, P. Domingo (2008) Large-Eddy Simulation of a fuel lean premixed turbulent swirl burner Combust. Flame 155(1): 247 266.
# G. Lodato, P. Domingo, L. Vervisch (2008) Three-dimensional boundary conditions for Direct and Large-Eddy Simulation of compressible flows J. of Comp. Phys. 227(10): 5105-5143.
# J. Galpin, C. Angelberger, A. Naudin, L. Vervisch (2008) Large-Eddy Simulation of H2-air auto-ignition using tabulated detailed chemistry J. of Turbulence 9(13).
# P. Domingo, L. Vervisch, D. Veynante (2008) Large-Eddy Simulation of a lifted methane jet flame in a vitiated coflow Combust. Flame 152(3): 415-432.
# O. Desjardins, V. Moureau and H. Pitsch (2008) An accurate conservative level set/ghost fluid method for simulating turbulent atomization, J. Comp. Physics, 227, 8395-8416 [http://dx.doi.org/10.1016/j.jcp.2008.05.027].
# O. Esnault, G. Joulin & Y. D'Angelo, Combustion fronts in nondiffusing disordered premixtures. I: Single-channel curved flames, Combustion Theory and Modelling, 12, 4, 739-768, 2008.
# J. Savre, N. Bertier, Y. D'Angelo & D. Gaffié, A chemical time scale approach for FPI modeling, Comptes-Rendus Mécanique, 336, 11-12, pp 807-812, 2008.
# G. Subramanian, R. Bounaceur, A. Pirez Da Cruz, L. Vervisch (2007) Chemical impact of CO and H2 addition on the auto-ignition delay of homogeneous n-heptane/air mixtures Comb. Sci. Tech. 179(9): 1937-1962.
# P. Domingo, L. Vervisch (2007) DNS of partially premixed flame propagating in a turbulent rotating flow Proc. Combust. Inst. 31:1657-1664.
# X. Paubel, A. Cessou, D. Honoré, L. Vevisch, R. Rsiava (2007) A flame stability diagram for piloted non-premixed oxycombustion of low calorific residual gases Proc. Combust. Inst. 31: 3385-3392.
# V. Moureau, C. Bérat and H. Pitsch (2007) An Efficient Semi-Implicit Compressible Solver for Large-Eddy Simulations, J. Comp. Physics, 226, 1256-1270 [http://dx.doi.org/10.1016/j.jcp.2007.05.035].
# V. Moureau, P. Minot, C. Bérat and H. Pitsch (2007) A Ghost-Fluid Method for Large-Eddy Simulations of Premixed Combustion in Complex Geometries, J. Comp. Physics, 221, 600--614 [http://dx.doi.org/10.1016/j.jcp.2006.06.031].
# C. Péra, J. Réveillon, L. Vervisch, P. Domingo (2006) Modeling subgrid scale mixture fraction variance in LES of evaporating spray Combust. Flame 146(4): 635-648.
# L. Vervisch, P. Domingo (2006) Two recent developments in numerical simulation of premixed and partially premixed turbulent flame C. R. Mecanique 334 (8/9): 523-530.
# G. Ribert, O. Gicquel, N. Darabiha, D. Veynante (2006) Tabulation of complex chemistry based on self-similar beahaviour of laminar premixed flames, Combust. Flame, (146): 649-664.
# G. Ribert, M. Champion, O. Gicquel, N. Darabiha, D. Veynante (2005) Modeling non adiabatic turbulent premixed reactive flows including tabulated chemistry, Combust. Flame, (141): 271-280.
# P. Domingo, L. Vervisch, S. Payet and R. Hauguel (2005) DNS of a Premixed Turbulent V-Flame and LES of a Ducted-Flame using a FSD-PDF subgrid scale closure with FPI tabulated chemistry Combust. Flame 143(4): 566-586.
# K.N.C. Bray, P. Domingo, L. Vervisch (2005) The role of progress variable in models for partially premixed turbulent combustion Combust. Flame 141(4): 431-437.
# J. Réveillon, L. Vervisch (2005) Analysis of weakly turbulent diluted-spray flames and combustion regimes J. Fluid Mech. 537: 317-347.
# P. Domingo, L. Vervisch, J. Réveillon (2005) DNS analysis of partially premixed combustion in spray and gaseous turbulent-flame bases stabilized in hot air. Combust. Flame 140(3): 172-195.
# B. Fiorina, O. Gicquel, L. Vervisch, S. Carpentier, N. Darabiha (2005) Approximating the chemical structure of partially-premixed and diffusion counter-flow flames using FPI flamelet tabulation Combust. Flame 140(3): 147-160.
# B. Fiorina, O. Gicquel, L. Vervisch, S. Carpentier, N. Darabiha (2005) Premixed turbulent combustion modeling using tabulated detailed chemistry and PDF Proc. Combust. Inst. 30(1): 867-874.
# R. Hauguel, L. Vervisch, P. Domingo (2005) DNS of premixed turbulent V-Flame: coupling spectral and finite difference methods C. R. Mecanique 333 (1): 95-102.
# V. Moureau, G. Lartigue, Y. Sommerer, C. Angelberger, O. Colin and T. Poinsot, (2005) Numerical methods for unsteady compressible multi-component reacting flows on fixed and moving grids, J. Comp. Physics, 202, 710--736 [http://dx.doi.org/10.1016/j.jcp.2004.08.003].
# L. Vervisch, P. Domingo, M. Rullaud, R. Hauguel (2004) Three facets of turbulent combustion modeling: DNS of Premixed V-flame, LES of lifted jet-flame, RANS of non premixed jet-flame J. of Turbulence, 5(4): 1-36.
# L. Vervisch, B. Labégorre, J. Réveillon (2004) Hydrogen-sulphur oxy-flame analysis and single-step flame tabulated chemistry Fuel 83(4-5): 605-614.
# G. Ribert, M. Champion, P. Plion (2004) Modeling turbulent reactive flows with variable equivalence ratio: application to the calculation of a reactive shear layer, Combust. Sci. and Tech. (176): 907 – 923.
# J. Boulanger, L. Vervisch, J. Réveillon, S. Ghosal (2003) Effects of heat release in laminar diffusion flames lifted on round jets Combust. Flame, 134(4): 355-368.
# L. Blin, A. Hadjadj, L. Vervisch, (2003) Large Eddy Simulation of turbulent flows in reversing systems J. of Turbulence, 4(1): 1-19.
# O. Gicquel, L. Vervisch, G. Joncquet, B. Labegorre, N. Darabiha (2003) Combustion of residual steel gases: Laminar flame analysis and turbulent flamelet modeling, Fuel 82(8): 983 - 991.
# P. Domingo, L. Vervisch, K.N.C. Bray (2002) Partially premixed flamelets in LES of nonpremixed turbulent combustion Combust. Theory and Modelling 6(4): 529-551.
# J. Boulanger, L. Vervisch (2002) Diffusion edge-flame: Approximation of the flame tip Damköhler number Combust. Flame, 130(1/2): 1-14.
# D. Veynante, L. Vervisch (2002) Turbulent Combustion Modeling Prog. Energ. Sci., 285(3): 193-266.
# V. Favier, L. Vervisch (2001) Edge flames and partially premixed combustion in diffusion flame quenching Combust. Flame. 125 (1/2): 788-803.
# S. Ghosal, L. Vervisch (2001) Stability diagram for lift-off and blowout of a round jet laminar diffusion flame Combust. Flame. 124(4): 646-655.
# S. Ghosal, L. Vervisch (2000) Theoretical and numerical study of a symmetrical triple flame using the parabolic flame path approximation J. Fluid Mech. 415: 227-260.
# J. Reveillon, L. Vervisch (2000) Accounting for spray vaporization in non-premixed turbulent combustion modeling: A Single Droplet Model (SDM) Combust. Flame 121(1/2): 75-90.
# L. Vervisch, D. Veynante (2000) Interlinks between approaches for modeling turbulent flames Proc. Combust. Inst. 28: 175-183.
# L. Vervisch (2000) Using numerics to help understand nonpremixed turbulent flames Proc. Combust. 28: 11-24.
# L. Vervisch, T. Poinsot (1998) Direct numerical simulation of non-premixed turbulent combustion Annu. Rev. Fluid Mech. 30: 655-92.
# J. Réveillon, L. Vervisch (1998) Subgrid-Scale Turbulent Micromixing: Dynamic Approach AIAA Journal 36 (3): 336-341.
# V. Favier, L. Vervisch (1998) Investigating the effects of Edge-flames in liftoff in non-premixed turbulent combustion Proc. Combust. Inst. 26: 1239-1245.
# L. Vervisch, J. Réveillon (1996) Dynamics of iso-concentration surfaces in weak shock turbulent mixing interaction AIAA Journal 34 (12): 2539-2544.
# L. Vervisch, J. Réveillon, L., Guichard (1996) Recent developments in turbulent combustion modeling Journal Européen des Eléments Finis 5 (2): 161-196.
# J. Réveillon, L. Vervisch (1996) Response of the dynamic model to heat release induced effects Phys. of Fluids 8(8): 2248-2250.
# P. Domingo, L. Vervisch (1996) Triple flames and partially premixed combustion in autoignition of nonpremixed turbulent mixtures Proc. Combust. Inst. 26: 233-240.
# G.R. Ruetsch, L. Vervisch, A. Linan (1995) Effects of heat release on triple flames Phys. Fluids 7(6): 1447-1454.
# S. Mahalingam, J. H. Chen, L. Vervisch (1995) Finite-rate chemistry and transient effects in direct numerical simulations of turbulent non-premixed flames Combust. Flame 102(3): 285-297.
# L. Vervisch, E. Bidaux, K.N.C. Bray, W. Kollmann (1995) Surface density function in premixed turbulent combustion modeling, similarities between probability density function and flame surface approaches Phys. Fluids 7(10): 2496-2503.
# L. Guichard, L. Vervisch, P. Domingo (1995) Two-dimensional weak-shock vortex interaction in a mixing zone AIAA Journal 33(10): 2539-2544.

Publications

2014-01-28T14:27:08Z

Domingo:

# S. Nambully, P. Domingo, V. Moureau, L. Vervisch (in press) A Filtered-Laminar-Flame PDF sub-grid scale closure for LES of premixed turbulent flames. Part I: Formalism and application to a bluff-body burner with differential diffusion. Combust. Flame.
# S. Nambully, P. Domingo, V. Moureau, L. Vervisch (in press) A Filtered-Laminar-Flame PDF sub-grid scale closure for LES of premixed turbulent flames: Part II: Application to a stratified bluff-body burner, Combust. Flame.
# B. Farcy, A. Abou-Taouk, L. Vervisch, P. Domingo, N. Perret (2014) Two approaches of chemistry downsizing for simulating Selective Non Catalytic Reduction DeNOx Process, Fuel, 118: 291-299, DOI 10.1016/j.fuel.2013.10.070.
# G. Ribert, L. Vervisch, P. Domingo, Y.-S. Niu (2014) Hybrid transported-tabulated strategy to downsize detailed chemistry for numerical simulation of premixed flames, FLow Turbulence and Combustion, 92(1/2): 175-200. DOI 10.1007/s10494-013-9520-6.
# F. Pecquery, V. Moureau, G. Lartigue, L. Vervisch, A. Roux (2014) Modelling nitrogen oxide emissions in turbulent flames with air dilution: Application to LES of a non-premixed jet-flame, Combust. Flame, 161(2): 496-509.
# X. Petit, G. Ribert, P. Domingo, G. Lartigue}} (2013) Large-eddy simulation of supercritical fluid injection, ''J. Supercritical Fluids'' '''(84)''': 61 - 73. doi:10.1016/j.supflu.2013.09.011 [http://www.sciencedirect.com/science?_ob=ArticleListURL&_method=list&_ArticleListID=-406086495&_sort=r&_st=13&view=c&_acct=C000032441&_version=1&_urlVersion=0&_userid=1071190&md5=1be41adf80142fdc4879c0665a695946&searchtype=a link].
# M. Sjostrand-Cuif, Y. D'Angelo & E. Albin (in press) No-slip Wall Acoustic Boundary Condition treatment in the Incompressible Limit, Computers and Fluids.
# Z. Pouransari, L. Vervisch, A. Johansson (2013) Heat release effects on mixing scales of non-premixed turbulent wall-jets: A direct numerical simulation study, Int. J. Heat and Fluid Flow, 40(4): 65-80 [http://dx.doi.org/10.1016/j.ijheatfluidflow.2012.12.005]
# N. Yi-Shuai, L. Vervisch, P.-D. Tao, An optimization-based approach to detailed chemistry tabulation: Automated progress variable definition, Combust. Flame, 160(4): 776-785 [http://dx.doi.org/10.1016/j.combustflame.2012.11.015]
# C. Merlin, P. Domingo, L. Vervisch (2013) Immersed boundaries in Large Eddy Simulation of compressible flows, FLow Turbulence and Combustion, 90(1): 29-68 [http://dx.doi.org/10.1007/s10494-012-9421-0]
# E. Albin, H. Nawroth, S. Göke, Y. D’Angelo, C.O Paschereit, Experimental investigation of burning velocities of ultra-wet methane-air-steam mixtures, Fuel Processing Technology, Fuel Processing Technology Volume 107, March 2013, Pages 27–35, [http://dx.doi.org/10.1016/j.fuproc.2012.06.027]
# RA Rego, Y D’Angelo & G Joulin, On nonlinear model equations for the response of premixed flames to acoustic like accelerations, Combustion Theory & Modelling, Volume 17, Issue 1, 2013. [http://dx.doi.org/10.1080/13647830.2012.721900]
# C. Merlin, P. Domingo, L. Vervisch (2012) Large Eddy Simulation of turbulent flames in a Trapped Vortex Combustor (TVC) - A flamelet presumed-pdf closure preserving laminar flame speed Comptes Rendus Mécanique, 340 (11/12): 917-932. [http://dx.doi.org/10.1016/j.crme.2012.10.039]
# G. Lodier, C. Merlin, P. Domingo, L. Vervisch, F. Ravet (2012) Self-ignition scenarios after rapid compression of a turbulent mixture weakly-stratified in temperature, Combust. Flame, 159(11), pp. 3358-3371. [http://dx.doi.org/10.1016/j.combustflame.2012.07.006]
# E. Albin, Y. D’Angelo, Assessment of the Evolution Equation Modelling approach for three-dimensional expanding wrinkled premixed flames, Combustion and Flame 2012[http://dx.doi.org/doi:10.1016/j.combustflame.2011.12.019]
# N. Enjalbert, P. Domingo, L. Vervisch (2012) Mixing time-history effects in Large Eddy Simulation of non-premixed turbulent flames: Flow-Controlled Chemistry Tabulation, Combust. Flame 159(1), pp. 336-352.2012 [http://dx.doi.org/doi:10.1016/j.combustflame.2011.06.005]
# G. Ribert, K. Wang and L. Vervisch, A multi-zone self-similar chemistry tabulation with application to auto-ignition including cool-flames effects, ''Fuel'' '''(91)''': 87 - 92, (2012). [http://www.sciencedirect.com/science/article/pii/S0016236111004339]
# J. Dombard, B. Leveugle, L. Selle, J. Réveillon, T. Poinsot & Y. D'Angelo, Modeling heat transfer in diluted two-phase flows using the Mesoscopic Eulerian Formalism, International Journal of Heat and Mass Transfer, 2011, [http://dx.doi.org/10.1016/j.ijheatmasstransfer.2011.10.050]
# G. Boury & Y. D’Angelo, On third order density contrast expansion of the evolution equation for wrinkled unsteady premixed flames, International Journal of Non-Linear Mechanics, 2011 [http://dx.doi.org/10.1016/j.ijnonlinmec.2011.05.018]
# E. Albin, Y. D'Angelo, L. Vervisch Flow streamline based Navier-Stokes Characteristic Boundary Conditions: modeling for transverse and corner outflows, Computers and Fluids, 2011 [http://dx.doi.org/10.1016/j.compfluid.2011.08.005]
# G. Lodier, L. Vervisch, V. Moureau, P. Domingo (2011) Composition-space premixed flamelet solution with differential diffusion for in situ flamelet-generated manifolds, Combust. Flame 158(10): 2009-2016. [http://dx.doi.org/doi:10.1016/j.combustflame.2011.03.011]
# V. Moureau, P. Domingo, L. Vervisch (2011) From Large-Eddy Simulation to Direct Numerical Simulation of a lean premixed swirl flame: Filtered Laminar Flame-PDF modeling, Combust. Flame 158(7): 1340-1357 [http://dx.doi.org/doi:10.1016/j.combustflame.2010.12.004]
# V. Moureau, P. Domingo, L. Vervisch (2011) Design of a massively parallel CFD code for complex geometries C.R. Mecanique 339(2/3): 141-148.
# E. Albin, Y. D'Angelo, L. Vervisch Using staggered grids with characteristic boundary conditions when solving compressible reactive Navier-Stokes equations Int. J. Numer. Meth. Fl. , Feb 2012, [http://dx.doi.org/doi:10.1002/fld.2520].
# G. Lecocq, S. Richard, J.-B. Michel, L. Vervisch (2011) A new LES model coupling flame surface density and tabulated kinetics approaches to investigate knock and pre-ignition in piston engines Proc. Combust. Inst., 33(2): 3105-3114.
# G. Lecocq, S. Richard, O. Colin, L. Vervisch (2011) Hybrid presumed pdf and flame surface density approaches for Large-Eddy Simulation of premixed turbulent combustion Part 1: Formalism and simulation of a quasi-steady burner Combust. Flame 158(6): 1201-1214.
# G. Lecocq, S. Richard, O. Colin, L. Vervisch (2011) Hybrid presumed pdf and flame surface density approaches for Large-Eddy Simulation of premixed turbulent combustion Part 2: Early flame development after sparking Combust. Flame 158(6): 1215-1226.
# D. Taïeb, G. Ribert, A. Hadjadj (2010) Shock focusing simulations using an optimized High-order WENO numerical scheme, AIAA J. (48,8): 1739-1747.
# K. Wang, G. Ribert, P. Domingo, L. Vervisch (2010) Self-similar behavior and chemistry tabulation of burnt-gases diluted premixed flamelets including heat-loss Combust. Theory and Modelling 14(4): 541-570.
# G. Lecocq, S. Richard, O. Colin, L. Vervisch (2010) Gradient and counter-gradient modelling in premixed flames: theoretical study and application to the LES of a Lean premixed turbulent swirl-burner Comb. Sci. Tech. 182(4-6): 465-479.
# D. Veynante, G. Lodato, P. Domingo, L. Vervisch, E. R. Hawkes (2010) Estimation of three-dimensional flame surface densities from planar images in turbulent premixed combustion Exp. in Fluids 49:267-278.
# L. Vervisch, P. Domingo, G. Lodato, D. Veynante (2010) Scalar energy fluctuations in Large-Eddy Simulation of turbulent flames: Statistical budgets and mesh quality criterion Combust. Flame 157(4): 778-789.
# V. Subramanian, P. Domingo, L. Vervisch (2010) Large-Eddy Simulation of forced ignition of an annular bluff-body burner Combust. Flame 157(3): 579-601.
# P.-D. Nguyen, L. Vervisch, V. Subramanian, P. Domingo (2010) Multi-dimensional flamelet-generated manifolds for partially premixed combustion Combust. Flame 157(1): 43-61.
# G. Lodato, L. Vervisch, P. Domingo (2009) A compressible wall-adapting similarity mixed model for large-eddy simulation of the impinging round jet Phys. Fluids 21:035102.
# L. Pons, N. Darabiha, S. Candel, G. Ribert, V. Yang (2009) Mass transfer and combustion in transcritical non-premixed counterflows, Combust. Theory Model. (13): 57-81.
# G. Godel, P. Domingo, L. Vervisch (2009) Tabulation of NOx chemistry for Large-Eddy Simulation of non-premixed turbulent flames Proc. Combust. Inst. 32: 1555-1551.
# F. Duchaine, A. Corpron, L. Pons, V. Moureau, F. Nicoud, and T. Poinsot (2009) Development and assessment of a coupled strategy for conjugate heat transfer with Large Eddy Simulation. Application to a cooled turbine blade, International Journal of Heat and Fluid Flow, 30(6), 1129-1141 [http://dx.doi.org/10.1016/j.ijheatfluidflow.2009.07.004].
# V. Moureau, B. Fiorina, and H. Pitsch (2009) A level set formulation for premixed combustion LES considering the turbulent flame structure., Comb. and Flame, 156, 801-812 [http://dx.doi.org/10.1016/j.combustflame.2009.01.019].
# E. Riber, V. Moureau, M. Garcia, T. Poinsot and O. Simonin, (2009) Evaluation of numerical strategies for LES of particulate two-phase recirculating flows, J. Comp. Physics, 228, 539-564 [http://dx.doi.org/10.1016/j.jcp.2008.10.001].
# D. Veynante, B. Fiorina, P. Domingo L. Vervisch, (2008) Using self-similar properties of turbulent premixed flames to downsize chemical tables in high-performance numerical simulations Combust. Theory and Modeling 12(6): 1055-1088.
# G. Ribert, N. Zong, V. Yang, L. Pons, N. Darabiha, S. Candel (2008) Counterflow diffusion flames of general fluids: oxygen/hydrogen mixtures, Combust. Flame (154): 319-330.
# J. Galpin, A. Naudin, L. Vervisch, C. Angelberger, O. Colin, P. Domingo (2008) Large-Eddy Simulation of a fuel lean premixed turbulent swirl burner Combust. Flame 155(1): 247 266.
# G. Lodato, P. Domingo, L. Vervisch (2008) Three-dimensional boundary conditions for Direct and Large-Eddy Simulation of compressible flows J. of Comp. Phys. 227(10): 5105-5143.
# J. Galpin, C. Angelberger, A. Naudin, L. Vervisch (2008) Large-Eddy Simulation of H2-air auto-ignition using tabulated detailed chemistry J. of Turbulence 9(13).
# P. Domingo, L. Vervisch, D. Veynante (2008) Large-Eddy Simulation of a lifted methane jet flame in a vitiated coflow Combust. Flame 152(3): 415-432.
# O. Desjardins, V. Moureau and H. Pitsch (2008) An accurate conservative level set/ghost fluid method for simulating turbulent atomization, J. Comp. Physics, 227, 8395-8416 [http://dx.doi.org/10.1016/j.jcp.2008.05.027].
# O. Esnault, G. Joulin & Y. D'Angelo, Combustion fronts in nondiffusing disordered premixtures. I: Single-channel curved flames, Combustion Theory and Modelling, 12, 4, 739-768, 2008.
# J. Savre, N. Bertier, Y. D'Angelo & D. Gaffié, A chemical time scale approach for FPI modeling, Comptes-Rendus Mécanique, 336, 11-12, pp 807-812, 2008.
# G. Subramanian, R. Bounaceur, A. Pirez Da Cruz, L. Vervisch (2007) Chemical impact of CO and H2 addition on the auto-ignition delay of homogeneous n-heptane/air mixtures Comb. Sci. Tech. 179(9): 1937-1962.
# P. Domingo, L. Vervisch (2007) DNS of partially premixed flame propagating in a turbulent rotating flow Proc. Combust. Inst. 31:1657-1664.
# X. Paubel, A. Cessou, D. Honoré, L. Vevisch, R. Rsiava (2007) A flame stability diagram for piloted non-premixed oxycombustion of low calorific residual gases Proc. Combust. Inst. 31: 3385-3392.
# V. Moureau, C. Bérat and H. Pitsch (2007) An Efficient Semi-Implicit Compressible Solver for Large-Eddy Simulations, J. Comp. Physics, 226, 1256-1270 [http://dx.doi.org/10.1016/j.jcp.2007.05.035].
# V. Moureau, P. Minot, C. Bérat and H. Pitsch (2007) A Ghost-Fluid Method for Large-Eddy Simulations of Premixed Combustion in Complex Geometries, J. Comp. Physics, 221, 600--614 [http://dx.doi.org/10.1016/j.jcp.2006.06.031].
# C. Péra, J. Réveillon, L. Vervisch, P. Domingo (2006) Modeling subgrid scale mixture fraction variance in LES of evaporating spray Combust. Flame 146(4): 635-648.
# L. Vervisch, P. Domingo (2006) Two recent developments in numerical simulation of premixed and partially premixed turbulent flame C. R. Mecanique 334 (8/9): 523-530.
# G. Ribert, O. Gicquel, N. Darabiha, D. Veynante (2006) Tabulation of complex chemistry based on self-similar beahaviour of laminar premixed flames, Combust. Flame, (146): 649-664.
# G. Ribert, M. Champion, O. Gicquel, N. Darabiha, D. Veynante (2005) Modeling non adiabatic turbulent premixed reactive flows including tabulated chemistry, Combust. Flame, (141): 271-280.
# P. Domingo, L. Vervisch, S. Payet and R. Hauguel (2005) DNS of a Premixed Turbulent V-Flame and LES of a Ducted-Flame using a FSD-PDF subgrid scale closure with FPI tabulated chemistry Combust. Flame 143(4): 566-586.
# K.N.C. Bray, P. Domingo, L. Vervisch (2005) The role of progress variable in models for partially premixed turbulent combustion Combust. Flame 141(4): 431-437.
# J. Réveillon, L. Vervisch (2005) Analysis of weakly turbulent diluted-spray flames and combustion regimes J. Fluid Mech. 537: 317-347.
# P. Domingo, L. Vervisch, J. Réveillon (2005) DNS analysis of partially premixed combustion in spray and gaseous turbulent-flame bases stabilized in hot air. Combust. Flame 140(3): 172-195.
# B. Fiorina, O. Gicquel, L. Vervisch, S. Carpentier, N. Darabiha (2005) Approximating the chemical structure of partially-premixed and diffusion counter-flow flames using FPI flamelet tabulation Combust. Flame 140(3): 147-160.
# B. Fiorina, O. Gicquel, L. Vervisch, S. Carpentier, N. Darabiha (2005) Premixed turbulent combustion modeling using tabulated detailed chemistry and PDF Proc. Combust. Inst. 30(1): 867-874.
# R. Hauguel, L. Vervisch, P. Domingo (2005) DNS of premixed turbulent V-Flame: coupling spectral and finite difference methods C. R. Mecanique 333 (1): 95-102.
# V. Moureau, G. Lartigue, Y. Sommerer, C. Angelberger, O. Colin and T. Poinsot, (2005) Numerical methods for unsteady compressible multi-component reacting flows on fixed and moving grids, J. Comp. Physics, 202, 710--736 [http://dx.doi.org/10.1016/j.jcp.2004.08.003].
# L. Vervisch, P. Domingo, M. Rullaud, R. Hauguel (2004) Three facets of turbulent combustion modeling: DNS of Premixed V-flame, LES of lifted jet-flame, RANS of non premixed jet-flame J. of Turbulence, 5(4): 1-36.
# L. Vervisch, B. Labégorre, J. Réveillon (2004) Hydrogen-sulphur oxy-flame analysis and single-step flame tabulated chemistry Fuel 83(4-5): 605-614.
# G. Ribert, M. Champion, P. Plion (2004) Modeling turbulent reactive flows with variable equivalence ratio: application to the calculation of a reactive shear layer, Combust. Sci. and Tech. (176): 907 – 923.
# J. Boulanger, L. Vervisch, J. Réveillon, S. Ghosal (2003) Effects of heat release in laminar diffusion flames lifted on round jets Combust. Flame, 134(4): 355-368.
# L. Blin, A. Hadjadj, L. Vervisch, (2003) Large Eddy Simulation of turbulent flows in reversing systems J. of Turbulence, 4(1): 1-19.
# O. Gicquel, L. Vervisch, G. Joncquet, B. Labegorre, N. Darabiha (2003) Combustion of residual steel gases: Laminar flame analysis and turbulent flamelet modeling, Fuel 82(8): 983 - 991.
# P. Domingo, L. Vervisch, K.N.C. Bray (2002) Partially premixed flamelets in LES of nonpremixed turbulent combustion Combust. Theory and Modelling 6(4): 529-551.
# J. Boulanger, L. Vervisch (2002) Diffusion edge-flame: Approximation of the flame tip Damköhler number Combust. Flame, 130(1/2): 1-14.
# D. Veynante, L. Vervisch (2002) Turbulent Combustion Modeling Prog. Energ. Sci., 285(3): 193-266.
# V. Favier, L. Vervisch (2001) Edge flames and partially premixed combustion in diffusion flame quenching Combust. Flame. 125 (1/2): 788-803.
# S. Ghosal, L. Vervisch (2001) Stability diagram for lift-off and blowout of a round jet laminar diffusion flame Combust. Flame. 124(4): 646-655.
# S. Ghosal, L. Vervisch (2000) Theoretical and numerical study of a symmetrical triple flame using the parabolic flame path approximation J. Fluid Mech. 415: 227-260.
# J. Reveillon, L. Vervisch (2000) Accounting for spray vaporization in non-premixed turbulent combustion modeling: A Single Droplet Model (SDM) Combust. Flame 121(1/2): 75-90.
# L. Vervisch, D. Veynante (2000) Interlinks between approaches for modeling turbulent flames Proc. Combust. Inst. 28: 175-183.
# L. Vervisch (2000) Using numerics to help understand nonpremixed turbulent flames Proc. Combust. 28: 11-24.
# L. Vervisch, T. Poinsot (1998) Direct numerical simulation of non-premixed turbulent combustion Annu. Rev. Fluid Mech. 30: 655-92.
# J. Réveillon, L. Vervisch (1998) Subgrid-Scale Turbulent Micromixing: Dynamic Approach AIAA Journal 36 (3): 336-341.
# V. Favier, L. Vervisch (1998) Investigating the effects of Edge-flames in liftoff in non-premixed turbulent combustion Proc. Combust. Inst. 26: 1239-1245.
# L. Vervisch, J. Réveillon (1996) Dynamics of iso-concentration surfaces in weak shock turbulent mixing interaction AIAA Journal 34 (12): 2539-2544.
# L. Vervisch, J. Réveillon, L., Guichard (1996) Recent developments in turbulent combustion modeling Journal Européen des Eléments Finis 5 (2): 161-196.
# J. Réveillon, L. Vervisch (1996) Response of the dynamic model to heat release induced effects Phys. of Fluids 8(8): 2248-2250.
# P. Domingo, L. Vervisch (1996) Triple flames and partially premixed combustion in autoignition of nonpremixed turbulent mixtures Proc. Combust. Inst. 26: 233-240.
# G.R. Ruetsch, L. Vervisch, A. Linan (1995) Effects of heat release on triple flames Phys. Fluids 7(6): 1447-1454.
# S. Mahalingam, J. H. Chen, L. Vervisch (1995) Finite-rate chemistry and transient effects in direct numerical simulations of turbulent non-premixed flames Combust. Flame 102(3): 285-297.
# L. Vervisch, E. Bidaux, K.N.C. Bray, W. Kollmann (1995) Surface density function in premixed turbulent combustion modeling, similarities between probability density function and flame surface approaches Phys. Fluids 7(10): 2496-2503.
# L. Guichard, L. Vervisch, P. Domingo (1995) Two-dimensional weak-shock vortex interaction in a mixing zone AIAA Journal 33(10): 2539-2544.

User:Domingo

2014-01-28T14:16:04Z

Domingo: /* Recent Publications */

User:Domingo

2014-01-28T14:12:35Z

Domingo: /* Recent Publications */

Publications

2014-01-28T14:10:00Z

Domingo:

# S. Nambully, P. Domingo, V. Moureau, L. Vervisch (in press) A Filtered-Laminar-Flame PDF sub-grid scale closure for LES of premixed turbulent flames. Part I: Formalism and application to a bluff-body burner with differential diffusion. Combust. Flame.
# S. Nambully, P. Domingo, V. Moureau, L. Vervisch (in press) A Filtered-Laminar-Flame PDF sub-grid scale closure for LES of premixed turbulent flames: Part II: Application to a stratified bluff-body burner, Combust. Flame.
# B. Farcy, A. Abou-Taouk, L. Vervisch, P. Domingo, N. Perret (2014) Two approaches of chemistry downsizing for simulating Selective Non Catalytic Reduction DeNOx Process, Fuel, 118: 291-299, DOI 10.1016/j.fuel.2013.10.070.
# G. Ribert, L. Vervisch, P. Domingo, Y.-S. Niu (2014) Hybrid transported-tabulated strategy to downsize detailed chemistry for numerical simulation of premixed flames, FLow Turbulence and Combustion, 92(1/2): 175-200. DOI 10.1007/s10494-013-9520-6.
# F. Pecquery, V. Moureau, G. Lartigue, L. Vervisch, A. Roux (2014) Modelling nitrogen oxide emissions in turbulent flames with air dilution: Application to LES of a non-premixed jet-flame, Combust. Flame, 161(2): 496-509.
# M. Sjostrand-Cuif, Y. D'Angelo & E. Albin (in press) No-slip Wall Acoustic Boundary Condition treatment in the Incompressible Limit, Computers and Fluids.
# Z. Pouransari, L. Vervisch, A. Johansson (2013) Heat release effects on mixing scales of non-premixed turbulent wall-jets: A direct numerical simulation study, Int. J. Heat and Fluid Flow, 40(4): 65-80 [http://dx.doi.org/10.1016/j.ijheatfluidflow.2012.12.005]
# N. Yi-Shuai, L. Vervisch, P.-D. Tao, An optimization-based approach to detailed chemistry tabulation: Automated progress variable definition, Combust. Flame, 160(4): 776-785 [http://dx.doi.org/10.1016/j.combustflame.2012.11.015]
# C. Merlin, P. Domingo, L. Vervisch (2013) Immersed boundaries in Large Eddy Simulation of compressible flows, FLow Turbulence and Combustion, 90(1): 29-68 [http://dx.doi.org/10.1007/s10494-012-9421-0]
# E. Albin, H. Nawroth, S. Göke, Y. D’Angelo, C.O Paschereit, Experimental investigation of burning velocities of ultra-wet methane-air-steam mixtures, Fuel Processing Technology, Fuel Processing Technology Volume 107, March 2013, Pages 27–35, [http://dx.doi.org/10.1016/j.fuproc.2012.06.027]
# RA Rego, Y D’Angelo & G Joulin, On nonlinear model equations for the response of premixed flames to acoustic like accelerations, Combustion Theory & Modelling, Volume 17, Issue 1, 2013. [http://dx.doi.org/10.1080/13647830.2012.721900]
# C. Merlin, P. Domingo, L. Vervisch (2012) Large Eddy Simulation of turbulent flames in a Trapped Vortex Combustor (TVC) - A flamelet presumed-pdf closure preserving laminar flame speed Comptes Rendus Mécanique, 340 (11/12): 917-932. [http://dx.doi.org/10.1016/j.crme.2012.10.039]
# G. Lodier, C. Merlin, P. Domingo, L. Vervisch, F. Ravet (2012) Self-ignition scenarios after rapid compression of a turbulent mixture weakly-stratified in temperature, Combust. Flame, 159(11), pp. 3358-3371. [http://dx.doi.org/10.1016/j.combustflame.2012.07.006]
# E. Albin, Y. D’Angelo, Assessment of the Evolution Equation Modelling approach for three-dimensional expanding wrinkled premixed flames, Combustion and Flame 2012[http://dx.doi.org/doi:10.1016/j.combustflame.2011.12.019]
# N. Enjalbert, P. Domingo, L. Vervisch (2012) Mixing time-history effects in Large Eddy Simulation of non-premixed turbulent flames: Flow-Controlled Chemistry Tabulation, Combust. Flame 159(1), pp. 336-352.2012 [http://dx.doi.org/doi:10.1016/j.combustflame.2011.06.005]
# G. Ribert, K. Wang and L. Vervisch, A multi-zone self-similar chemistry tabulation with application to auto-ignition including cool-flames effects, ''Fuel'' '''(91)''': 87 - 92, (2012). [http://www.sciencedirect.com/science/article/pii/S0016236111004339]
# J. Dombard, B. Leveugle, L. Selle, J. Réveillon, T. Poinsot & Y. D'Angelo, Modeling heat transfer in diluted two-phase flows using the Mesoscopic Eulerian Formalism, International Journal of Heat and Mass Transfer, 2011, [http://dx.doi.org/10.1016/j.ijheatmasstransfer.2011.10.050]
# G. Boury & Y. D’Angelo, On third order density contrast expansion of the evolution equation for wrinkled unsteady premixed flames, International Journal of Non-Linear Mechanics, 2011 [http://dx.doi.org/10.1016/j.ijnonlinmec.2011.05.018]
# E. Albin, Y. D'Angelo, L. Vervisch Flow streamline based Navier-Stokes Characteristic Boundary Conditions: modeling for transverse and corner outflows, Computers and Fluids, 2011 [http://dx.doi.org/10.1016/j.compfluid.2011.08.005]
# G. Lodier, L. Vervisch, V. Moureau, P. Domingo (2011) Composition-space premixed flamelet solution with differential diffusion for in situ flamelet-generated manifolds, Combust. Flame 158(10): 2009-2016. [http://dx.doi.org/doi:10.1016/j.combustflame.2011.03.011]
# V. Moureau, P. Domingo, L. Vervisch (2011) From Large-Eddy Simulation to Direct Numerical Simulation of a lean premixed swirl flame: Filtered Laminar Flame-PDF modeling, Combust. Flame 158(7): 1340-1357 [http://dx.doi.org/doi:10.1016/j.combustflame.2010.12.004]
# V. Moureau, P. Domingo, L. Vervisch (2011) Design of a massively parallel CFD code for complex geometries C.R. Mecanique 339(2/3): 141-148.
# E. Albin, Y. D'Angelo, L. Vervisch Using staggered grids with characteristic boundary conditions when solving compressible reactive Navier-Stokes equations Int. J. Numer. Meth. Fl. , Feb 2012, [http://dx.doi.org/doi:10.1002/fld.2520].
# G. Lecocq, S. Richard, J.-B. Michel, L. Vervisch (2011) A new LES model coupling flame surface density and tabulated kinetics approaches to investigate knock and pre-ignition in piston engines Proc. Combust. Inst., 33(2): 3105-3114.
# G. Lecocq, S. Richard, O. Colin, L. Vervisch (2011) Hybrid presumed pdf and flame surface density approaches for Large-Eddy Simulation of premixed turbulent combustion Part 1: Formalism and simulation of a quasi-steady burner Combust. Flame 158(6): 1201-1214.
# G. Lecocq, S. Richard, O. Colin, L. Vervisch (2011) Hybrid presumed pdf and flame surface density approaches for Large-Eddy Simulation of premixed turbulent combustion Part 2: Early flame development after sparking Combust. Flame 158(6): 1215-1226.
# D. Taïeb, G. Ribert, A. Hadjadj (2010) Shock focusing simulations using an optimized High-order WENO numerical scheme, AIAA J. (48,8): 1739-1747.
# K. Wang, G. Ribert, P. Domingo, L. Vervisch (2010) Self-similar behavior and chemistry tabulation of burnt-gases diluted premixed flamelets including heat-loss Combust. Theory and Modelling 14(4): 541-570.
# G. Lecocq, S. Richard, O. Colin, L. Vervisch (2010) Gradient and counter-gradient modelling in premixed flames: theoretical study and application to the LES of a Lean premixed turbulent swirl-burner Comb. Sci. Tech. 182(4-6): 465-479.
# D. Veynante, G. Lodato, P. Domingo, L. Vervisch, E. R. Hawkes (2010) Estimation of three-dimensional flame surface densities from planar images in turbulent premixed combustion Exp. in Fluids 49:267-278.
# L. Vervisch, P. Domingo, G. Lodato, D. Veynante (2010) Scalar energy fluctuations in Large-Eddy Simulation of turbulent flames: Statistical budgets and mesh quality criterion Combust. Flame 157(4): 778-789.
# V. Subramanian, P. Domingo, L. Vervisch (2010) Large-Eddy Simulation of forced ignition of an annular bluff-body burner Combust. Flame 157(3): 579-601.
# P.-D. Nguyen, L. Vervisch, V. Subramanian, P. Domingo (2010) Multi-dimensional flamelet-generated manifolds for partially premixed combustion Combust. Flame 157(1): 43-61.
# G. Lodato, L. Vervisch, P. Domingo (2009) A compressible wall-adapting similarity mixed model for large-eddy simulation of the impinging round jet Phys. Fluids 21:035102.
# L. Pons, N. Darabiha, S. Candel, G. Ribert, V. Yang (2009) Mass transfer and combustion in transcritical non-premixed counterflows, Combust. Theory Model. (13): 57-81.
# G. Godel, P. Domingo, L. Vervisch (2009) Tabulation of NOx chemistry for Large-Eddy Simulation of non-premixed turbulent flames Proc. Combust. Inst. 32: 1555-1551.
# F. Duchaine, A. Corpron, L. Pons, V. Moureau, F. Nicoud, and T. Poinsot (2009) Development and assessment of a coupled strategy for conjugate heat transfer with Large Eddy Simulation. Application to a cooled turbine blade, International Journal of Heat and Fluid Flow, 30(6), 1129-1141 [http://dx.doi.org/10.1016/j.ijheatfluidflow.2009.07.004].
# V. Moureau, B. Fiorina, and H. Pitsch (2009) A level set formulation for premixed combustion LES considering the turbulent flame structure., Comb. and Flame, 156, 801-812 [http://dx.doi.org/10.1016/j.combustflame.2009.01.019].
# E. Riber, V. Moureau, M. Garcia, T. Poinsot and O. Simonin, (2009) Evaluation of numerical strategies for LES of particulate two-phase recirculating flows, J. Comp. Physics, 228, 539-564 [http://dx.doi.org/10.1016/j.jcp.2008.10.001].
# D. Veynante, B. Fiorina, P. Domingo L. Vervisch, (2008) Using self-similar properties of turbulent premixed flames to downsize chemical tables in high-performance numerical simulations Combust. Theory and Modeling 12(6): 1055-1088.
# G. Ribert, N. Zong, V. Yang, L. Pons, N. Darabiha, S. Candel (2008) Counterflow diffusion flames of general fluids: oxygen/hydrogen mixtures, Combust. Flame (154): 319-330.
# J. Galpin, A. Naudin, L. Vervisch, C. Angelberger, O. Colin, P. Domingo (2008) Large-Eddy Simulation of a fuel lean premixed turbulent swirl burner Combust. Flame 155(1): 247 266.
# G. Lodato, P. Domingo, L. Vervisch (2008) Three-dimensional boundary conditions for Direct and Large-Eddy Simulation of compressible flows J. of Comp. Phys. 227(10): 5105-5143.
# J. Galpin, C. Angelberger, A. Naudin, L. Vervisch (2008) Large-Eddy Simulation of H2-air auto-ignition using tabulated detailed chemistry J. of Turbulence 9(13).
# P. Domingo, L. Vervisch, D. Veynante (2008) Large-Eddy Simulation of a lifted methane jet flame in a vitiated coflow Combust. Flame 152(3): 415-432.
# O. Desjardins, V. Moureau and H. Pitsch (2008) An accurate conservative level set/ghost fluid method for simulating turbulent atomization, J. Comp. Physics, 227, 8395-8416 [http://dx.doi.org/10.1016/j.jcp.2008.05.027].
# O. Esnault, G. Joulin & Y. D'Angelo, Combustion fronts in nondiffusing disordered premixtures. I: Single-channel curved flames, Combustion Theory and Modelling, 12, 4, 739-768, 2008.
# J. Savre, N. Bertier, Y. D'Angelo & D. Gaffié, A chemical time scale approach for FPI modeling, Comptes-Rendus Mécanique, 336, 11-12, pp 807-812, 2008.
# G. Subramanian, R. Bounaceur, A. Pirez Da Cruz, L. Vervisch (2007) Chemical impact of CO and H2 addition on the auto-ignition delay of homogeneous n-heptane/air mixtures Comb. Sci. Tech. 179(9): 1937-1962.
# P. Domingo, L. Vervisch (2007) DNS of partially premixed flame propagating in a turbulent rotating flow Proc. Combust. Inst. 31:1657-1664.
# X. Paubel, A. Cessou, D. Honoré, L. Vevisch, R. Rsiava (2007) A flame stability diagram for piloted non-premixed oxycombustion of low calorific residual gases Proc. Combust. Inst. 31: 3385-3392.
# V. Moureau, C. Bérat and H. Pitsch (2007) An Efficient Semi-Implicit Compressible Solver for Large-Eddy Simulations, J. Comp. Physics, 226, 1256-1270 [http://dx.doi.org/10.1016/j.jcp.2007.05.035].
# V. Moureau, P. Minot, C. Bérat and H. Pitsch (2007) A Ghost-Fluid Method for Large-Eddy Simulations of Premixed Combustion in Complex Geometries, J. Comp. Physics, 221, 600--614 [http://dx.doi.org/10.1016/j.jcp.2006.06.031].
# C. Péra, J. Réveillon, L. Vervisch, P. Domingo (2006) Modeling subgrid scale mixture fraction variance in LES of evaporating spray Combust. Flame 146(4): 635-648.
# L. Vervisch, P. Domingo (2006) Two recent developments in numerical simulation of premixed and partially premixed turbulent flame C. R. Mecanique 334 (8/9): 523-530.
# G. Ribert, O. Gicquel, N. Darabiha, D. Veynante (2006) Tabulation of complex chemistry based on self-similar beahaviour of laminar premixed flames, Combust. Flame, (146): 649-664.
# G. Ribert, M. Champion, O. Gicquel, N. Darabiha, D. Veynante (2005) Modeling non adiabatic turbulent premixed reactive flows including tabulated chemistry, Combust. Flame, (141): 271-280.
# P. Domingo, L. Vervisch, S. Payet and R. Hauguel (2005) DNS of a Premixed Turbulent V-Flame and LES of a Ducted-Flame using a FSD-PDF subgrid scale closure with FPI tabulated chemistry Combust. Flame 143(4): 566-586.
# K.N.C. Bray, P. Domingo, L. Vervisch (2005) The role of progress variable in models for partially premixed turbulent combustion Combust. Flame 141(4): 431-437.
# J. Réveillon, L. Vervisch (2005) Analysis of weakly turbulent diluted-spray flames and combustion regimes J. Fluid Mech. 537: 317-347.
# P. Domingo, L. Vervisch, J. Réveillon (2005) DNS analysis of partially premixed combustion in spray and gaseous turbulent-flame bases stabilized in hot air. Combust. Flame 140(3): 172-195.
# B. Fiorina, O. Gicquel, L. Vervisch, S. Carpentier, N. Darabiha (2005) Approximating the chemical structure of partially-premixed and diffusion counter-flow flames using FPI flamelet tabulation Combust. Flame 140(3): 147-160.
# B. Fiorina, O. Gicquel, L. Vervisch, S. Carpentier, N. Darabiha (2005) Premixed turbulent combustion modeling using tabulated detailed chemistry and PDF Proc. Combust. Inst. 30(1): 867-874.
# R. Hauguel, L. Vervisch, P. Domingo (2005) DNS of premixed turbulent V-Flame: coupling spectral and finite difference methods C. R. Mecanique 333 (1): 95-102.
# V. Moureau, G. Lartigue, Y. Sommerer, C. Angelberger, O. Colin and T. Poinsot, (2005) Numerical methods for unsteady compressible multi-component reacting flows on fixed and moving grids, J. Comp. Physics, 202, 710--736 [http://dx.doi.org/10.1016/j.jcp.2004.08.003].
# L. Vervisch, P. Domingo, M. Rullaud, R. Hauguel (2004) Three facets of turbulent combustion modeling: DNS of Premixed V-flame, LES of lifted jet-flame, RANS of non premixed jet-flame J. of Turbulence, 5(4): 1-36.
# L. Vervisch, B. Labégorre, J. Réveillon (2004) Hydrogen-sulphur oxy-flame analysis and single-step flame tabulated chemistry Fuel 83(4-5): 605-614.
# G. Ribert, M. Champion, P. Plion (2004) Modeling turbulent reactive flows with variable equivalence ratio: application to the calculation of a reactive shear layer, Combust. Sci. and Tech. (176): 907 – 923.
# J. Boulanger, L. Vervisch, J. Réveillon, S. Ghosal (2003) Effects of heat release in laminar diffusion flames lifted on round jets Combust. Flame, 134(4): 355-368.
# L. Blin, A. Hadjadj, L. Vervisch, (2003) Large Eddy Simulation of turbulent flows in reversing systems J. of Turbulence, 4(1): 1-19.
# O. Gicquel, L. Vervisch, G. Joncquet, B. Labegorre, N. Darabiha (2003) Combustion of residual steel gases: Laminar flame analysis and turbulent flamelet modeling, Fuel 82(8): 983 - 991.
# P. Domingo, L. Vervisch, K.N.C. Bray (2002) Partially premixed flamelets in LES of nonpremixed turbulent combustion Combust. Theory and Modelling 6(4): 529-551.
# J. Boulanger, L. Vervisch (2002) Diffusion edge-flame: Approximation of the flame tip Damköhler number Combust. Flame, 130(1/2): 1-14.
# D. Veynante, L. Vervisch (2002) Turbulent Combustion Modeling Prog. Energ. Sci., 285(3): 193-266.
# V. Favier, L. Vervisch (2001) Edge flames and partially premixed combustion in diffusion flame quenching Combust. Flame. 125 (1/2): 788-803.
# S. Ghosal, L. Vervisch (2001) Stability diagram for lift-off and blowout of a round jet laminar diffusion flame Combust. Flame. 124(4): 646-655.
# S. Ghosal, L. Vervisch (2000) Theoretical and numerical study of a symmetrical triple flame using the parabolic flame path approximation J. Fluid Mech. 415: 227-260.
# J. Reveillon, L. Vervisch (2000) Accounting for spray vaporization in non-premixed turbulent combustion modeling: A Single Droplet Model (SDM) Combust. Flame 121(1/2): 75-90.
# L. Vervisch, D. Veynante (2000) Interlinks between approaches for modeling turbulent flames Proc. Combust. Inst. 28: 175-183.
# L. Vervisch (2000) Using numerics to help understand nonpremixed turbulent flames Proc. Combust. 28: 11-24.
# L. Vervisch, T. Poinsot (1998) Direct numerical simulation of non-premixed turbulent combustion Annu. Rev. Fluid Mech. 30: 655-92.
# J. Réveillon, L. Vervisch (1998) Subgrid-Scale Turbulent Micromixing: Dynamic Approach AIAA Journal 36 (3): 336-341.
# V. Favier, L. Vervisch (1998) Investigating the effects of Edge-flames in liftoff in non-premixed turbulent combustion Proc. Combust. Inst. 26: 1239-1245.
# L. Vervisch, J. Réveillon (1996) Dynamics of iso-concentration surfaces in weak shock turbulent mixing interaction AIAA Journal 34 (12): 2539-2544.
# L. Vervisch, J. Réveillon, L., Guichard (1996) Recent developments in turbulent combustion modeling Journal Européen des Eléments Finis 5 (2): 161-196.
# J. Réveillon, L. Vervisch (1996) Response of the dynamic model to heat release induced effects Phys. of Fluids 8(8): 2248-2250.
# P. Domingo, L. Vervisch (1996) Triple flames and partially premixed combustion in autoignition of nonpremixed turbulent mixtures Proc. Combust. Inst. 26: 233-240.
# G.R. Ruetsch, L. Vervisch, A. Linan (1995) Effects of heat release on triple flames Phys. Fluids 7(6): 1447-1454.
# S. Mahalingam, J. H. Chen, L. Vervisch (1995) Finite-rate chemistry and transient effects in direct numerical simulations of turbulent non-premixed flames Combust. Flame 102(3): 285-297.
# L. Vervisch, E. Bidaux, K.N.C. Bray, W. Kollmann (1995) Surface density function in premixed turbulent combustion modeling, similarities between probability density function and flame surface approaches Phys. Fluids 7(10): 2496-2503.
# L. Guichard, L. Vervisch, P. Domingo (1995) Two-dimensional weak-shock vortex interaction in a mixing zone AIAA Journal 33(10): 2539-2544.

SiTCom-B Gallery

2014-01-28T13:59:26Z

Domingo: /* Electric field and edge-flame */

== Chemistry downsizing for simulating selective non catalytic reduction DeNOx process ==

The introduction of strongly non-linear chemistry effects in numerical simulation of flows in Selective Non Catalytic Reduction (SNCR) DeNOx is addressed. In these systems of large dimensions, NOx in flue gas is reduced by injecting either ammonia or urea as a reducing agent. First, an analysis is performed to seek out with detailed chemistry (207 elementary reactions, 33 species by Klippenstein et al. (2011) ) the importance of global parameters in the performance of NO removal, such as temperature and major species concentration levels. Then, this detailed reaction mechanism needs to be simplified for its subsequent introduction in flow simulations. In this paper, two different methods relying on auto- mated optimization tools for reducing the cost of chemistry are discussed. The first one is based on the tabulation of the detailed chemical response from canonical problems, using automatically defined progress variables. In the second one, a large sample set of detailed chemistry solution points is processed by an iterative optimization procedure, leading to a reduced two-step chemistry reproducing the response of the global parameters characterizing NO removal.

{| class="wikitable"
|+ NO / NH3 chemistry for LES
|-
| [[File:NO_NH3_optim.png|center|400px]]
| [[File:NO_NH3_scheme.png|center|400px]]
|-
| Optimal conditions for NO removal from NH3
| Novel reduced kinetics for Large-Eddy Simulation of DeNOx
|}

* B. Farcy, A. Abou-Taouk, L. Vervisch, P. Domingo, N. Perret (2014) Two approaches of chemistry downsizing for simulating Selective Non Catalytic Reduction DeNOx Process, Fuel, 118: 291-299.

== An optimization-based approach to detailed chemistry tabulation ==
Finding a progress variable so that all relevant species can be retrieved from its knowledge, is not always straightforward; specifically for fuel mixtures composed of more than a single hydrocarbon, or for simpler fuels but under conditions where the global reaction progress is not continuous, for instance in the case of cool-flame ignition. To overcome these difficulties, automated methods are discussed to define progress variables in which all species of a chemical scheme, even minor ones, are involved. This is done formulating constraints applied to progress variables definition: they should evolve in a monotonic manner from fresh to burnt gases and species derivative in progress variable-space should stay moderate for tabulation accuracy. This set of constraints is discretized along chemical trajectories observed in laminar canonical flames, to be formulated in terms of an ensemble of inequalities, which are solved using optimization tools. The outcome is a set of weighting coefficients to be applied to every species of the detailed chemical scheme, in order to construct the progress variable-space. The methods have been successfully applied to methane and kerosene premixed flamelets and to n-heptane self-ignition, under conditions with cool-flame effects.

{| class="wikitable"
|+ Automated progress variable definition
|-
| [[File:CF_160_4_YS_TAB.png|center|400px]]
| [[File:YC_alpha_optim.png|center|200px]]
| [[File:OH_Optim.png|center|300px]]
|-
| Coefficients of the optimized progress variable for CH4/Air combustion
| Progress variable is expressed from all species mass fraction
| OH tabulation valid at all equivalence ratios
|}

* N. Yi-Shuai, L. Vervisch, P.-D. Tao (2013) An optimization-based approach to detailed chemistry tabulation: Automated progress variable definition, Combust. Flame, 160(4): 776-785.

== LES of a Trapped Vortex Combustor ==
Flow and flame dynamics inside a trapped vortex combustor are analyzed from Large Eddy Simulation (LES) results compared against measurements. The Navier-Stokes equations are solved in their fully compressible form over a cartesian grid resorting to immersed boundaries to account for the complex geometry, composed of an annular flow impacting a set of axisymmetric rods (flame holders) before interacting with a cavity. Various cases are considered, varying the main flow rate, the length of the cavity, injecting secondary-air and also adding a swirling motion. From these cases, three main cavity flow regimes emerge. The modeling of molecular diffusion in LES with presumed probability density function (pdf), as filter of premixed flamelets, is also discussed. It is shown that a dynamic correction to molecular diffusion may be computed from the pdf control parameters to ensure the correct laminar flame speed, whatever the mesh used. Finally, the study of the turbulent flame evolution within the cavity in the various cases, suggests that swirling motion is mandatory to favor the global burner stability.

{| class="wikitable"
|+ Immersed boundaries are used to optimize the geometry of a trapped vortex combustor
|-
| [[File:TVC1.png|center|450px]]
| [[File:TVC2.png|center|500px]]
|-
| Geometry of the Trapped Vortex Combustion chamber
| Q-critrion - Visualisation of the turbulent flow topology
|-
| [[File:TVC3.png|center|400px]]
|-
| Comparison against experiments
|}

* C. Merlin, P. Domingo, L. Vervisch (2012) Large Eddy Simulation of turbulent flames in a Trapped Vortex Combustor (TVC) - A flamelet presumed-pdf closure preserving laminar flame speed, Comptes Rendus Mecanique, 340 (11/12), pp. 917-932.

== Immersed boundaries in LES of compressible flows==
Methods to immerse walls in a structured mesh are examined in the context of fully compressible solutions of the Navier Stokes equations. The ghost cell approach is tested along with compressible conservative immersed boundaries in canonical flow configurations; the reflexion of pressure waves on walls arbitrarily inclined on a cartesian mesh is studied, and mass conservation issues examined in both a channel flow inclined at various angles and flow past a cylinder. Then, results from Large Eddy Simulation of a flow past a rectangular cylinder and a transonic cavity flow are compared against experiments, using either a multi-block mesh conforming to the wall or immersed boundaries. Different strategies to account for unresolved transport by velocity fluctuations in LES are also compared. It is found that immersed boundaries allow for reproducing most of the coupling between flow instabilities and pressure-signal properties observed in the transonic cavity flow. To conclude, the complex geometry of a trapped vortex combustor, including a cavity, is simulated and results compared against experiments.

{| class="wikitable"
|+ Immersed boundaries are developed for fully compressible simulations
|-
| [[File:IBM1.png|center|400px]]
| [[File:IBM2.png|center|400px]]
|-
| Pressure wave reflection on inclined walls
| Transonic cavity flow simulation
|-
| [[File:IBM3.png|center|500px]]
|-
| Comparison of pressure spectra against measurements
|}

* C. Merlin, P. Domingo, L. Vervisch (2013) Immersed Boundaries in Large Eddy Simulation of Compressible Flows, Flow Turbulence and Combustion, 90(1), pp. 29-68.

== DNS of a Rapid Compression Machine ==
Turbulence and combustion inside a compression machine, experimentally studied by Guibert et al. [Flow Turbulence and Combust. 84(1):~79-85, 2010], are simulated to get some insight on flow-physics and ignition scenarios of a reactive-gas mixture pushed by a piston through a turbulence-grid, to be compressed in a fifty-five cubic-centimeter volume. Large Eddy Simulation (LES) with a structured-mesh solver and immersed boundaries are first performed for an inert mixture undergoing the compression, to validate the simulation procedure against experimental results. Then, keeping the flow admission-sequence the same, but downsizing its geometry, a Direct Numerical Simulation (DNS) analysis of the compression/ignition sequence is reported. Simulation parameters are varied for ignition to occur in mixtures featuring various temperature stratification patterns, due to wall cooling and turbulence characteristics. As previously discussed in the literature, conditions favoring spotty- or homogeneous-ignition are evidenced. Depending on characteristic times (coherent structure residence time, flow engulfment and mixing times) ignition may occur within localized compression zones, between vortical structures leading to spotty-ignition, or more homogeneously within large scale flow structures. Very small differences in local temperature and flow topology appear to lead to different routes toward successful auto-ignition. The underlying mechanisms are analyzed from an internal energy budget expressed as a temperature balance equation, to delineate between the contribution of the global adiabatic compression and localized flow divergence induced by turbulence velocity fluctuations. After primary ignition, the propagation phase of ignition is strongly influenced by the acoustic field and the specific temperature scalar dissipation-rate patterns. It is also shown that three-dimensional vortex stretching plays a crucial role, hence two and three-dimensional DNS lead to different ignition scenarios under similar chemical and turbulence intensity conditions.

{| class="wikitable"
|+ Analysis of ignition regimes after rapid compression - Homogeneous mixture stratified in temperature
|-
| [[File:RCM1.png|center|400px]]
| [[File:RCM2.png|center|400px]]
|-
| Flow injection sequence - Resolution of <math>20 \mu m </math>
| Ignition patterns
|-
| [[File:RCM3.png|center|400px]]
|-
| Regime Diagram
|}

* G. Lodier, C. Merlin, P. Domingo, L. Vervisch, F. Ravet (2012) Self-ignition scenarios after rapid compression of a turbulent mixture weakly-stratified in temperature, Combust. Flame 159(11): 3358-3371.

== Mixing time-history effects: Flow-Controlled Chemistry Tabulation ==
The time history of mixing is known to play a crucial and non-trivial role in non-premixed turbulent combustion. In a first part, Eulerian balance equations are derived for both a flow residence time and a characteristic time of the mixing which the particles gathered in a fluid element have been subjected to in their flow histories. These equations are analyzed and solved in a Large Eddy Simulation (LES) context for a fuel jet mixing with an oxidizer coflow. Typical responses of filtered mixture fraction versus flow residence time are highlighted. In a second part, a Flow-Controlled Chemistry Tabulation (FCCT) is devised in which the effects of unresolved fluctuations of thermochemical variables in LES are simulated, combining partially-stirred reactors with tabulated chemistry. The reactor evolutions are organized to mimick flow engulfment and micro-mixing, so as to reproduce the observed filtered mixture fraction versus residence time response. This allows for dynamically building sub-grid scale joint probability density functions, and thereby the sub-filter response of the non-premixed flames, according to four control parameters: the filtered mixture fraction, the progress of reaction, the flow residence time and a mixing time. Finally, LES of the Cabra et al. [Combust. Flame 143 (2005) 491--506] fuel-jet lifted-flame developing in a vitiated oxidizer environment is performed and results are compared against measurements.

{| class="wikitable"
|+ Analysis of time-history of turbulent mixing and fully new approach to turbulent combustion modeling
|-
| [[File:FCCT1.png|center|400px]]
| [[File:FCCT2.png|center|400px]]
|-
| FCCT procedure
| Dynamic construction of advanced chemistry tabulation
|-
| [[File:FCCT3.png|center|400px]]
|-
| Turbulent flame response to micro-mixing history
|}

* N. Enjalbert, P. Domingo, L. Vervisch (2012) Mixing time-history effects in Large Eddy Simulation of non-premixed turbulent flames: Flow-Controlled Chemistry Tabulation, Combust. Flame 159(1): 336-352.

== Flame base stabilization in vitiated partially-premixed mixture ==

The impact of burned gases on flame stabilization is analyzed
under the conditions of a laboratory jet flame in vitiated coflow
(Cabra~et al. 2005).
In this experiment, mass flow
rate, temperature, and the exact chemical composition of hot products mixed with air
sent toward the turbulent flame base are fully determined.
Auto-ignition and partially premixed flame propagation are investigated for these
operating conditions
from simulations of prototype combustion problems using fully detailed chemistry.
Using available instantaneous species and temperature measurements,
a priori tests are then performed to estimate
the prediction capabilities of chemistry tabulations built from these archetypal
reacting flows.
The links between auto-ignition and premixed flamelet
tables are discussed, along with their
controlling parameters.
Using these results,
Large-Eddy Simulation of the turbulent diluted jet flame
is performed,
a new closure for the scalar dissipation rate of reactive species is discussed,
and numerical predictions are successfully compared with experiments.

[[File:nice_QW.png]]

* P. Domingo, L. Vervisch, D. Veynante (2008) Large-Eddy Simulation of a lifted methane jet flame in a vitiated coflow Combust. Flame 152(3): 415-432.

== Electric field and edge-flame ==

The role of electric fields in stabilising combustion is a well-known phenomenon. Among the possible mechanisms favouring the anchorage of the flame base, the ion-driven wind acting directly on flow momentum ahead of the flame base could be the leading one. Direct numerical simulation has been used to verify this hypothesis and lead to a better understanding of diffusion flame base anchoring in the pres- ence of an externally applied voltage. In this context, a simplified modelling approach is proposed to describe combustion in the presence of electric body forces. The model reproduces the tendencies of experimental observations found in the literature. The sensitivity of the flame lift-off height to the applied voltage is studied and the modification of the velocity field ahead of the flame base induced by the electric volume forces is highlighted.

[[File:electric_edges_1.png|500px]]

* M. Belhi, P. Domingo, P. Vervisch (2010) Direct numerical simulation of the effect of an electric field on flame stability Combust. Flame 157 2286–2297.
* M. Belhi, P. Domingo, P. Vervisch (2013) Modeling of the Effect of DC and AC Electric Fields on the Stability of a Lifted Diffusion Methane/Air Flame, Combustion Theory and Modelling}, http://dx.doi.org/10.1080/13647830.2013.802415

== NSCBC vs 3D-NSCBC in jets ==

Navier-Stokes Characteristic Boundary Conditions (NSCBC) usually assume
the flow to be normal to the boundary plane. In this paper, NSCBC is extended to
account for convection and pressure gradients in boundary planes,
resulting in a 3D-NSCBC approach.
The introduction of these additional transverse terms requires a specific treatment for the computational domain's edges and corners, as well as a suited set of compatibility conditions for boundaries joining regions associated to different flow
properties, as inlet, outlet or wall.
A systematic strategy for dealing with edges and corners is derived and compatibility conditions for inlet/outlet and wall/outlet boundaries are proposed.
Direct Numerical Simulation (DNS) tests are carried out on simplified
flow configurations at first.
3D-NSCBC brings a drastic reduction of flow distortion and numerical reflection, even in regions of strong transverse convection; the accuracy and convergence rate toward target values of flow quantities is also improved.
Then, 3D-NSCBC is used for Large-Eddy Simulation (LES)
of a free jet and an impinging round-jet.
Edge and corner boundary treatment, combining multidirectional characteristics and compatibility conditions, yields stable and accurate solutions even with mixed boundaries characterized by bad posedness issues (e.g. inlet/outlet).
LES confirms the effectiveness of the proposed boundary treatment in reproducing mean flow velocity and turbulent fluctuations up to the computational domain limits.

[[File:jet_NSCBC_1D.png|500px]] [[File:jet_3DNSCBC_bis.png|300px]]

* G. Lodato, P. Domingo, L. Vervisch (2008) Three-dimensional boundary conditions for Direct and Large-Eddy Simulation of compressible flows J. of Comp. Phys. 227(10): 5105-5143.

== Impinging round jets ==

Wall-jet interaction is studied with Large Eddy Simulation (LES) in which
a mixed similarity Sub-Grid Scale (SGS) closure is combined with
the Wall-Adapting Local Eddy-viscosity (WALE) model for the eddy-viscosity term.
A macrotemperature and macropressure are introduced to
deduce a weakly compressible form of the mixed similarity model and the
relevant formulation for the energy equation is deduced accordingly.
LES prediction capabilities are assessed by comparing flow statistical properties against experiment of an unconfined impinging round-jet at Reynolds number of 23,000 and 70,000.
To quantify the benefit of the proposed WALE Similarity Mixed (WSM) model,
the lower Reynolds number simulations are also performed using the standard WALE and Lagrangian Dynamic Smagorinsky approaches.
The unsteady compressible Navier-Stokes equations are integrated over 2.9 M, 3.5 M and 5.5 M nodes cartesian grids with an explicit fourth-order finite volume solver.
Non-reflecting boundary conditions are enforced using a methodology
accounting for the three-dimensional character of the turbulent flow at boundaries.
A correct wall scaling is achieved from the combination of similarity and WALE approaches; for this wall-jet interaction, the SGS closure terms can be computed in the near-wall region without the necessity of resorting to additional specific treatments.
The possible impact of turbulent energy backscatter in such flow configurations is also addressed. It is found that, for the present configuration, the correct reproduction of reverse energy transfer plays a key role in the estimation of near-wall statistics, especially when the viscous sub-layer is not properly resolved.

[[File:jet_wall_1.png|400px]]]]

[[File:jet_wall_2.png|400px]]
[[File:jet_wall_3.png|300px]]

* G. Lodato, L. Vervisch, P. Domingo (2009) A compressible wall-adapting similarity mixed model for large-eddy simulation of the impinging round jet Phys. Fluids 21:035102.

== Ignition of a bluff-body burner ==

The optimization of the ignition process is a crucial issue in the design of many combustion systems. Large-Eddy Simulation (LES) of a conical shaped bluff body turbulent non-premixed burner has been performed to study the impact of spark location on ignition success. This burner was experimentally investigated by Ahmed et al. (2007). The present work focuses on the case without swirl for which detailed measurements are available. First, cold flow measurements of velocities and mixture fraction are compared with their LES counterparts, to assess the prediction capabilities of simulations in terms of flow and turbulent mixing. Time history of velocities and mixture fraction are recorded at selected spots, to probe the resolved probability density function (pdf) of flow variables, in an attempt to reproduce, from the knowledge of LES resolved instantaneous flow conditions, the experimentally observed reasons of success or failure of spark ignition. A flammability map is also constructed from the resolved mixture fraction pdf and compared with its experimental counterpart. LES of forced ignition is then performed using flamelet fully detailed tabulated chemistry combined with presumed pdfs. Various scenarios of flame kernel development are analyzed and correlated with typical flow conditions observed in this burner. The correlations between, velocities and mixture fraction values at the sparking time, and, the success or failure of ignition, are then further discussed and analysed.

[[File:igni_bluff_1.png]]

* V. Subramanian, P. Domingo, L. Vervisch (2010) Large-Eddy Simulation of forced ignition of an annular bluff-body burner Combust. Flame 157(3): 579-601.

== Jet flame-surface & Scalar SGS variance in LES ==

* Turbulence motions are, by nature, three-dimensional while planar imaging techniques, widely used in turbulent combustion, give only access to two-dimensional information. For example, to extract flame surface densities, a key ingredient of some turbulent combustion models, from planar images implicitly assumes an instantaneously two-dimensional flow, neglecting the unresolved flame front wrinkling. The objective here is to estimate flame surface densities in statistically two-dimensional flows, modelling unknown flame front wrinkling from known quantities. An excellent agreement is achieved against direct numerical simulation (DNS) data where all three-dimensional quantities are known, but validations in other conditions (larger DNS, experiments) are required.

* Large-Eddy Simulation (LES) provides space-filtered quantities to compare with measurements, which usually have been obtained using a different filtering operation; hence, numerical and experimental results can be examined side-by-side in a statistical sense only. Instantaneous, space-filtered and statistically time-averaged signals feature different characteristic length scales, which can be combined in dimensionless ratios. From two canonical manufactured turbulent solutions, a turbulent flame and a passive scalar turbulent mixing layer, the critical values of these ratios under which measured and computed variances (resolved plus subgrid scale) can be compared without resorting to additional residual terms are first determined. It is shown that actual Direct Numerical Simulation can hardly accommodate a sufficiently large range of length scales to perform statistical studies of LES filtered reactive scalar-fields energy budget based on sub-grid scale variances; an estimation of the minimum Reynolds number allowing for such DNS studies is given. From these developments, a reliability mesh criterion emerges for scalar LES and scaling for scalar sub-grid scale energy is discussed.

{| class="wikitable"
|-
| [[File:jet_flame_DNS.png|400px]]
| [[File:bunsen.png|400px]]
|-
| Premixed jet flame
| Bunsen flame
|}

* L. Vervisch, P. Domingo, G. Lodato, D. Veynante (2010) Scalar energy fluctuations in Large-Eddy Simulation of turbulent flames: Statistical budgets and mesh quality criterion Combust. Flame 157(4): 778-789.
* D. Veynante, G. Lodato, P. Domingo, L. Vervisch, E. R. Hawkes (2010) Estimation of three-dimensional flame surface densities from planar images in turbulent premixed combustion Exp. in Fluids 49:267-278.

== Nonpremixed jet flame ==
Detailed chemistry tabulations are mostly based on reaction progress
variables used to track species evolutions along
trajectories in composition space, which in some cases are
obtained from simulations of prototype combustion problems.
For hydrocarbon chemistry,
these progress variables are usually built from major species,
as CO, CO2, H2O to which reactants are sometimes added.
Prediction of NO mass fraction is first evaluated
by comparing results from single progress variable and flamelet based chemical look-up tables against simulations of
reference flames performed with the detailed chemistry mechanism
that was used to generate the tabulations.
Nitric oxides mainly formed in the burnt
gases still evolve once major species have almost reached their equilibrium levels,
then large errors in the predictions of NO mass fractions are unavoidable when
using a progress variable based on major species only.
It is concluded that the time scale separation inherent to NOx species
must be included in the progress variable definition.
A novel definition of progress variable is proposed for flame based tabulation
and tested, which allows for reproducing
both major species as well as NO, NO2 and N2O.
Large-Eddy Simulation (LES) of a jet flame in a vitiated coflow is performed with
the new tabulation and results are compared against experiments.

[[File:sandia_flame.png|400px]]

* G. Godel, P. Domingo, L. Vervisch (2009) Tabulation of NOx chemistry for Large-Eddy Simulation of non-premixed turbulent flames Proc. Combust. Inst. 32: 1555-1551.

== DNS of a non-reacting HIT ==

This is a very simple DNS computation of a HIT with a constant-properties gas. 
The main parameters of the simulation are:
* temporal integration: RK3,
* spatial scheme: 4th order skew symmetric
* no AV.

In this series of computations, the number of cell is increased from 64^3 to 256^3.

{| class="wikitable"
|+ HIT on increasing number of cells. The displayed field is <math>\nabla \wedge U</math>
|-
| [[File:HIT_0064cube.png|center|400px]]
| [[File:HIT_0128cube.png|center|400px]]
| [[File:HIT_0256cube.png|center|400px]]
|-
|<math>N_c=64^3 \quad Re_t = 40</math>
|<math>N_c=128^3 \quad Re_t = 100</math>
|<math>N_c=256^3 \quad Re_t = 250</math>
|}

== DNS of a non-reacting supercritical mixing layer ==

This simulation is a DNS of a HIT non-reacting supercritical mixing layer with real-gas properties (equation of state, thermodynamic laws and transport laws). 
The main parameters of the simulation are:
* temporal integration: RK3,
* spatial scheme: 4th order skew symmetric
* 2D / Periodic in all directions
* 3.2 Million cells
* EOS: Soave-Redlich-Kwong.
* Transport laws: Chung et al.

[[Image:supercritical_mixing_layer_rho_mixness.png|800px|Supercritical Mixing Layer]]

The fields that are displayed are:
* '''up :''' the density which varies from 80 kg/m3 in the cold stream to 800 kg/m3 in the hot stream.
* '''down :''' the mixness ratio which varies from 0 in pure constitutents to 1 for perfect mixness.

 

----

 

[[Media:supercritical_mixing_layer_mix.avi]]

 

This video shows the temporal evolution of mixness ratio during the simulation. 
'''Warning''':
* no Artificial Viscosity was used and the mesh was slightly too coarse: a few "wiggles" are visible from time to time near the steepest gradients...
* this video is best visualized with [http://www.videolan.org/ VLC].

SiTCom-B

2014-01-28T13:53:34Z

Domingo:

== SiTCom-B ==

[[File:SITCOMB.png|right|thumb|400px|Image of a 128^3 HIT]]

SiTCom-B (Simulation of Turbulent Combustion with Billions of points) is a finite volume code that solves the unsteady compressible reacting Navier-Stokes equations system on cartesian meshes.

It uses a structured formalism, which means that the data is organized in multidimensional arrays, according to the corresponding cell position in the physical space.

It is mainly design to perform DNS and highly resolved LES on thousands of processors.

It is a totally new version of the previous SiTCom code, written by P. Domingo and which has been the main tool over the past ten years to conduct numerical combustion research at CORIA.

The main interest of this version is that it uses the full power of the fortran 90/95 language : pointers, dynamic allocation and most important, object oriented programming.

== Main features ==

* Finite volume discretization of Navier-Stokes equations
* 4th and 2nd order central difference schemes
* Runge-Kutta time-discretization (3rd and 4th order)
* Full multispecies formulation
* Realistic thermodynamics (CHEMKIN)
* Realistic transport properties (Hirschfelder & Curtiss)
* Complex chemistry
* Tabulated chemistry
* Perfect gas, Peng-Robinson or SRK equation of state
* NSCBC boundary treatment
* Immersed Boundary Method

== Implementation ==

The code is actually a library of '''modules''' which implements '''objects'''.

Examples of such modules/objects are:
* data
* block
* inpufile
* parameters
* probes
* species
* numerics
* ...

The main programs are simply built from this module library.

== Important concepts ==

=== Keywords ===
All input files make an extensive use of keywords.
This is possible thanks to a simple parser implemented in parser_m

=== Chained lists ===
Nearly all objects can be put in chained lists which are very flexible and much easier to manipulate than arrays.

=== Blocks ===
Blocks are sets of cells assigned to a single processor.
Each cell of the blocks can be described by a set of 3 indices (ix,iy,iz) that represent its position in the block.
Another important concept is the block_bound structure: it is an object that contains two sets of three indices (one for the lower corner and one for the upper corner).
It is used everywhere to perform loops on the blocks.

=== Probes ===
It is possible to put numerical probes into the flow that will record the value of some variables at given positions for each time step.

=== Statistics ===
Both Reynolds and Favre averaging are implemented, for any variables.

=== Numerics ===
Second and Fourth order centered-interpolations are implemented in SiTCom-B.
Moreover, convective fluxes can be computed in either convective, divergence or skew-symmetric form.
Artificial Viscosity (based on Jameson formulation) is also available to stabilize the computation near steep gradients.

=== Parallelism ===
The code has been thought to work on thousands of processors via the MPI protocol.
Parallel communications and I/O have been optimized to achieve this goal.

=== I/O ===
When running on thousands of processors, I/O may be a major bottleneck.
I/O in SiTCom-B have been designed to overcome this limitation.
Moreover, the HDF format is used to store meshes, solutions, ... which makes it easy to share on various platforms and people.

== Gallery ==

A few pictures of SiTCom-B computations are available in this [[SiTCom-B Gallery|gallery]].


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User:Domingo

2014-01-28T13:49:52Z

Domingo: