Abstract
The present study is focused on the development of the RIF (Representative Interactive Flamelet) model which can overcome the shortcomings of conventional approach based on the steady flamelet library. Due to the ability for interactively describing the transient behaviors of local flame structures with CFD solver, the RIF model can effectively account for the detailed mechanisms of NOx formation including thermal NO path, prompt and nitrous NOx formation, and reburning process by hydrocarbon radical without any ad-hoc procedure. The flamelet time of RIFs within a stationary turbulent flame may be thought to be Lagrangian flight time. In context with the RIF approach, this study adopts the Eulerian Particle Flamelet Model (EPFM) with mutiple flamelets which can realistically account for the spatial inhomogeneity of scalar dissipation rate. In order to systematically evaluate the capability of Eulerian particle flamelet model to predict the precise flame structure and NO formation in the multi-dimensional elliptic flames, two methanol bluffbody flames with two different injection velocities are chosen as the validation cases. Numerical results suggest that the present EPFM model has the predicative capability to realistically capture the essential features of flame structure and NOx formation in the bluff-body stabilized flames.
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Abbreviations
- ap,k :
-
Planck mean absorption coefficient for radiating speciesk
- Cp :
-
Specific heat of mixture at constant pressure
- Di :
-
Diffusion coefficient of speciesi
- d:
-
Fuel nozzle diameter
- h, hk :
-
Enthalpy of mixture and speciesk
- P:
-
Probability density function
- Yi :
-
Mass fraction of speciesi
- Z:
-
Mixture fraction
- ρ:
-
Density
- σb :
-
Stefan-Boltzmann constant
- Wk :
-
Chemical production rate of speciesk
- χ:
-
Scalar dissipation rate
- st:
-
Stoichiometry
- \(\bar \phi \) :
-
Reynolds-averaged (density-unweighted)
- \(\bar \phi \) :
-
Favre-averaged (density-weighted)
References
Barths, H., Hasse, C., Bikas, G. and Peters, N., 2000, “Simulation of Combustion in Direct Injection Diesel Engines Using an Eulerian particle Flamelet Model,”Proc. 28 th Symp. (Int.) Comb., Combustion Institute, Pittsburgh, pp. 1161–1168.
Barths, H., Peters, N., Brehm, N., Mack, A., Pfitzner, M. and Smiljanovski, V., 1998, “Simulation of Pollutant Formation in a Gas-Turbine Combustor using Unsteady Flamelets,”Proc. 27 th Symp. (Int.) Comb., Combustion Institute, Pittsburgh, pp. 1841–1847.
Chen, M., Herrmann, M. and Peters, N., 2000, “Flamelet Modeling of Lifted Turbulent Methane/Air and Propane/Air Jet Diffusion Flames,”Proc. 28 th Symp. (Int.) Comb., Combustion Institute, Pittsburgh, pp. 167–174.
Coelho, P. J. and Peters, N., 2001, “Numerical Simulation of a MILD Combustion Burner,”Combustion and Flame, Vol. 124, pp. 503–518.
Dally, B. B., Masri, A. R., Barlow, R. S., Fiechtner, G. J. and Fletcher, D. F., 1996, “Measurements of NO in Turbulent Non-premixed Flames Stabilized on a Bluff Body,”Proc. 26 th Symp.(Int.)Comb., Combustion Institute, Pittsburgh, pp. 2191–2197.
Dally, B. B., Masri, A. R., Barlow, R. S. and Fiechtner, G. J., 1998, “Instantaneous and Mean Compositional Structure of Bluff-Body Stabilized Nonpremixed Flames,”Combustion and Flame, Vol. 114, pp. 119–148.
Ferreira, J. C., 1996,Flamelet Modelling of Stabilization in Turbulent Non-premixed Combustion, PhD Thesis, ETHZ Zuerich Switzerland.
Grcar, J.F., 1992,The Twopnt Program for Boundary Value Problems, Sandia Report, SAND91-8320, Livermore.
Hewson, J. C., 1997,Pollutant Emissions from Nonpremixed Hydrocarbon Flames, PhD Thesis, University of California, San Diego.
Kang, S. M. and Kim, Y. M., 2003, “Parallel Unstructured-Grid Finite-Volume Method for Turbulent Nonpremixed Flames Using the Flamelet Model,”Numerical Heat Transfer, Part B, Vol. 43, pp. 525–547.
Kim, H. J. and Kim, Y. M., 2002, “Numerical Modeling for Combustion and Soot Formation Processes in Turbulent Diffusion Flames,”KSME Int. J., Vol. 16, No. 1, pp. 116–124.
Kim, H. J., Kim, Y. M. and Ahn, K. Y., 2004a, “Numerical Modeling of Turbulent Nonpremixed Lifted Flames,”KSME Int. J., Vol. 18, No. 1, pp. 167–172.
Kim, S. H., Huh, K. Y. and Tao, L., 2000, “Application of the Elliptic Conditional Moment Closure Model to a Two-Dimensional Nonpremixed Methanol Bluff-Body Flame,”Combustion and Flame, Vol. 120, pp. 75–90.
Kim, S. K., Kang, S. M. and Kim, Y. M., 2001, “Flamelet Modeling for Combustion Processes and NOx Formation in the Turbulent Nonpremexed CO/H2/N2 Jet Flames,”Combustion Science and Technology, Vol. 168, pp. 47–83.
Kim, S. K., Yu, Y., Ahn, J. and Kim, Y. M., 2004b, “Numerical Investigation of the Autoignition of Turbulent Gaseous Jets in a High-Pressure Environment Using the Multiple-RIF Model,”Fuel, Vol. 83, pp. 375–386.
Klimenko, A. Y. and Bilger, R. W., 1999, “Conditional Moment Closure for Turbulent Combustion,”Prog. Energy Combust. Sci., Vol. 25, pp. 595–687.
Kronenburg, A., Bilger, R. W. and Kent, J. H., 2000, “Computation of Conditional Average Scalar Dissipation in Turbulent Jet Diffusion Flames,”Flow, Turbulence and Combustion, Vol. 64, pp. 145–159.
Libby, P.A. and Williams, F. A., eds, 1994,Turbulent Reacting Flows, New York, Academic Press.
Marracino, B. and Lentini, D., 1997, “Radiation Modelling in Non-Luminous Nonpremixed Turbulent Flames,”Combustion Science and Technology, Vol. 128, p. 23.
Peters, N., 1986, “Laminar Flamelet Concepts in Turbulent Combustion,”Proc. 21 st Symp. (Int.) Comb., Combustion Institute, Pittsburgh, pp. 1231–1250.
Peters, N., 2000,Turbulent Combustion, Cambridge University Press.
Pitsch, H. and Steiner, H., 2000, “Large-Eddy Simulation of a Turbulent Piloted Methane/Air Diffusion Flame (Sandia Flame D),”Physics of Fluids, Vol. 12, pp. 2541–2554.
Pitsch, H., 2000, “Unsteady Flamelet Modeling of Differential Diffusion in Turbulent Jet Diffusion Flames,”Combustion and Flame, Vol. 123, pp. 358–374.
Pitsch, H., Barths, H. and Peters, N., 1996, “Three-Dimensional Modeling of NOx and Soot Formation in DI-Diesel Engines Using Detailed Chemistry Based on the Interactive Flamelet Approach,” SAE paper 962057.
Pitsch, H., Chen, M. and Peters, N., 1998, “Unsteady Flamelet Modeling of Turbulent Hydrogen-Air Diffusion Flames,”Proc. 27 th Symp. (Int.) Comb., Combustion Institute, Pittsburgh, pp. 1057–1064.
Pitsch, H., Riesmeier, E. and Peters, N., 2000, “Unsteady Flamelet Modeling of Soot Formation in Turbulent Jet Diffusion Flames,”Combustion Science and Technology, Vol. 158, pp. 389–406.
Pope, S. B., 2000,Turbulent Flows, Cambridge University Press.
Radhakrishnan, K. and Hindmarsh, A. C., 1993, “Description and Use of LSODE, the Livermore Solver for Ordinary Differential Equations,”Lawrence Livermore National Laboratory Report, UCRL-ID-113855.
Roquemore, W. M., Tankin, R. S., Chiu, H. H. and Lottes, S. A., 1984, “The Role of Vortex Shedding in a Bluff-Body Combustor,”Experimental Measurement and Techniques in Turbulent Reactive and Nonreactive Flows, Vol. 66, pp. 159–174.
Turpin, G. and Troyes, J., 2000, “Validation of a Two-Equation Turbulence Model for Axisymmetric Reacting and Nonreacting Flows,” AIAA paper 2000-3463.
Vervisch, L. and Veynante, D., 2002, “Turbulent Combustion Modeling,”Prog. Energy Combust. Sci., Vol. 28, pp. 193–266.
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Kim, SK., Kang, S. & Kim, Y. Eulerian particle flamelet modeling for combustion processes of bluff-body stabilized methanol-air turbulent nonpremixed flames. J Mech Sci Technol 20, 1459–1474 (2006). https://doi.org/10.1007/BF02915969
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DOI: https://doi.org/10.1007/BF02915969