Comparison of FDS predictions by different combustion models with measured data for enclosure fires

Abstract The performance of mixture fraction models FDS4 and FDS5 is investigated under different global equivalence ratios (GER). Predictions of heat release rate (HRR), upper-layer temperature, and CO yield are compared with measurements considering their sensitivities to the lower limit of fuel, mixing time scale, and turbulence model constants. When using FDS4, the inclusion of an extinction model can result in significant variations in both total and volumetric HRR prediction. When using FDS5, the mixing model constant has significant effects on volumetric HRR prediction. At low GER (

[1]  Linda G. Blevins,et al.  Modeling of bare and aspirated thermocouples in compartment fires , 1999 .

[2]  Uri Vandsburger,et al.  An Evaluation of the Global Equivalence Ratio Concept for Compartment Fires: Data Analysis Methods , 2004 .

[3]  A. Tewarson Generation of Heat and Chemical Compounds in Fires , 2002 .

[4]  Kevin B. McGrattan,et al.  Validation of A CFD Fire Model Using Two Step Combustion Chemistry Using the NIST Reduced-Scale Ventilation-Limited Compartment Data , 2008 .

[5]  Clayton Huggett,et al.  Estimation of rate of heat release by means of oxygen consumption measurements , 1980 .

[6]  J. Quintiere,et al.  Numerical simulation of axi-symmetric fire plumes: accuracy and limitations , 2003 .

[7]  Michael A. Delichatsios,et al.  Heat fluxes and flame heights in façades from fires in enclosures of varying geometry , 2007 .

[8]  N. Peters Laminar flamelet concepts in turbulent combustion , 1988 .

[9]  William M. Pitts,et al.  The global equivalence ratio concept and the formation mechanisms of carbon monoxide in enclosure fires , 1995 .

[10]  D. Spalding Mixing and chemical reaction in steady confined turbulent flames , 1971 .

[11]  Uri Vandsburger,et al.  Evaluating the Global Equivalence Ratio Concept for Compartment Fires: Part II–Limitations for Correlating Species Yields: , 2004 .

[12]  William M. Pitts,et al.  Carbon Monoxide Production in Compartment Fires: Reduced-Scale Enclosure Test Facility (NISTIR 5568) , 1994 .

[13]  Craig L. Beyler,et al.  Major species production by diffusion flames in a two-layer compartment fire environment , 1986 .

[14]  Arnaud Trouvé,et al.  Towards large eddy simulations of flame extinction and carbon monoxide emission in compartment fires , 2007 .

[15]  Stephen B. Pope,et al.  PDF calculations of turbulent nonpremixed flames with local extinction , 2000 .

[16]  W. P. Jones,et al.  Large Eddy simulation of a turbulent non-premixed flame , 2001 .

[17]  Weigang Zhang,et al.  Turbulence statistics in a fire room model by large eddy simulation , 2002 .

[18]  H. Baum,et al.  Large eddy simulations of smoke movement , 1998 .

[19]  Vb Novozhilov,et al.  Computational fluid dynamics modeling of compartment fires , 2001 .

[20]  Craig L. Beyler,et al.  The role of temperature on carbon monoxide production in compartment fires , 1995 .

[21]  B. Hjertager,et al.  On mathematical modeling of turbulent combustion with special emphasis on soot formation and combustion , 1977 .

[22]  R. Lindstedt,et al.  Joint scalar probability density function modeling of pollutant formation in piloted turbulent jet diffusion flames with comprehensive chemistry , 2000 .

[23]  R. Lindstedt,et al.  Joint scalar transported probability density function modeling of turbulent methanol jet diffusion flames , 2002 .

[24]  Kevin B. McGrattan,et al.  Large eddy simulation of buoyant turbulent pool fires , 2002 .

[25]  James G. Quintiere,et al.  Enclosure Fire Dynamics , 1999 .

[26]  Johannes Janicka,et al.  Large Eddy Simulation of Turbulent Combustion Systems , 2005 .

[27]  Kevin B. McGrattan,et al.  Fire dynamics simulator (ver-sion 3) technical reference guide , 2001 .

[28]  Extending the mixture fraction concept to address under-ventilated fires , 2009 .

[29]  S. Toner,et al.  Entrainment, Chemistry, and Structure of Fire Plumes , 1987 .

[30]  Daniel T. Gottuk The generation of carbon monoxide in compartment fires , 1992 .

[31]  Akira Yoshizawa,et al.  Eddy‐viscosity‐type subgrid‐scale model with a variable Smagorinsky coefficient and its relationship with the one‐equation model in large eddy simulation , 1991 .

[32]  Yoshifumi Ohmiya,et al.  Effect of a facing wall on façade flames , 2008 .

[33]  N. Peters,et al.  Unsteady flamelet modeling of turbulent hydrogen-air diffusion flames , 1998 .

[34]  C. Wieczorek Carbon Monoxide Generation and Transport from Compartment Fires , 2003 .

[35]  Anders Lönnermark TOXFIRE - Fire characteristics and smoke gas analysis in under-ventilated large-scale combustion experiments. Tests in the ISO 9705 room. , 1996 .

[36]  Heinz Pitsch,et al.  Hybrid large-eddy simulation/Lagrangian filtered-density-function approach for simulating turbulent combustion , 2005 .

[37]  S. Pope,et al.  The effect of mixing models in PDF calculations of piloted jet flames , 2007 .

[38]  James G. Quintiere,et al.  A Perspective on Compartment Fire Growth , 1984 .

[39]  S. Frankel,et al.  Large eddy simulation of a nonpremixed reacting jet: Application and assessment of subgrid-scale combustion models , 1998 .

[40]  J. C. Ho,et al.  Comparison of different combustion models in enclosure fire simulation , 2001 .

[41]  K. V. Maele,et al.  Numerical simulations of full-scale enclosure fires in a small compartment with natural roof ventilation , 2008 .

[42]  Glenn P. Forney,et al.  Fire Dynamics Simulator (Version 2) -- Technical Reference Guide | NIST , 2001 .

[43]  L H Hu,et al.  Modeling fire-induced smoke spread and carbon monoxide transportation in a long channel: Fire Dynamics Simulator comparisons with measured data. , 2007, Journal of hazardous materials.