Modelling thermal radiation in buoyant turbulent diffusion flames
被引:14
作者:
Consalvi, J. L.
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Univ Aix Marseille 1, IUSTI, UMR 6595, CNRS, F-13453 Marseille 13, France
UAM I II, CNRS, IRSN, ETIC Lab, F-13453 Marseille 13, FranceUniv Aix Marseille 1, IUSTI, UMR 6595, CNRS, F-13453 Marseille 13, France
Consalvi, J. L.
[1
,2
]
Demarco, R.
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机构:
Univ Aix Marseille 1, IUSTI, UMR 6595, CNRS, F-13453 Marseille 13, France
UAM I II, CNRS, IRSN, ETIC Lab, F-13453 Marseille 13, France
CEA Cadarache, SEMIC, DPAM, IRSN, F-13115 St Paul Les Durance, FranceUniv Aix Marseille 1, IUSTI, UMR 6595, CNRS, F-13453 Marseille 13, France
Demarco, R.
[1
,2
,3
]
Fuentes, A.
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Univ Tecn Federico Santa Maria, Dept Ind, Valparaiso, ChileUniv Aix Marseille 1, IUSTI, UMR 6595, CNRS, F-13453 Marseille 13, France
Fuentes, A.
[4
]
机构:
[1] Univ Aix Marseille 1, IUSTI, UMR 6595, CNRS, F-13453 Marseille 13, France
[2] UAM I II, CNRS, IRSN, ETIC Lab, F-13453 Marseille 13, France
[3] CEA Cadarache, SEMIC, DPAM, IRSN, F-13115 St Paul Les Durance, France
[4] Univ Tecn Federico Santa Maria, Dept Ind, Valparaiso, Chile
This work focuses on the numerical modelling of radiative heat transfer in laboratory-scale buoyant turbulent diffusion flames. Spectral gas and soot radiation is modelled by using the Full-Spectrum Correlated-k (FSCK) method. Turbulence-Radiation Interactions (TRI) are taken into account by considering the Optically-Thin Fluctuation Approximation (OTFA), the resulting time-averaged Radiative Transfer Equation (RTE) being solved by the Finite Volume Method (FVM). Emission TRIs and the mean absorption coefficient are then closed by using a presumed probability density function (pdf) of the mixture fraction. The mean gas flow field is modelled by the Favre-averaged Navier-Stokes (FANS) equation set closed by a buoyancy-modified k-epsilon model with algebraic stress/flux models (ASM/AFM), the Steady Laminar Flamelet (SLF) model coupled with a presumed pdf approach to account for Turbulence-Chemistry Interactions, and an acetylene-based semi-empirical two-equation soot model. Two sets of experimental pool fire data are used for validation: propane pool fires 0.3 m in diameter with Heat Release Rates (HRR) of 15, 22 and 37 kW and methane pool fires 0.38 m in diameter with HRRs of 34 and 176 kW. Predicted flame structures, radiant fractions, and radiative heat fluxes on surrounding surfaces are found in satisfactory agreement with available experimental data across all the flames. In addition further computations indicate that, for the present flames, the gray approximation can be applied for soot with a minor influence on the results, resulting in a substantial gain in Computer Processing Unit (CPU) time when the FSCK is used to treat gas radiation.