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viii<br />
Premixed Turbulent combustion based on the Level Set Approach<br />
N. Peters a and J. Ewald b<br />
In premixed turbulent combustion a thin flame front interacts with a turbulent<br />
flow field at many scales, ranging from the integral length scale down to the<br />
Kolmogorov scale. Depending on whether the flame thickness lF is larger or smaller<br />
than the Kolmogorov scale lk, two different regimes of interaction can be defined:<br />
1. the corrugated flamelet regime where lF lk and 2. the thin reaction zones regime<br />
where lF lk. In the first case the entire flame structure including the preheat zone can<br />
be assumed as quasi-steady with the consequence that its interaction with the flow its<br />
characterized by the laminar burning velocity alone. In the second case Kolmogorov<br />
eddies may enter into the preheat zone but not into the thin reaction zone, which now<br />
may be assumed as quasi-steady. Since the smallest eddies will wrinkle the reaction<br />
zone, its curvature will become large. The product of the molecular diffusivity and the<br />
curvature represents a velocity. This velocity is of the same order of magnitude or<br />
larger than the laminar burning velocity and therefore determines the interaction with<br />
the flow in the second regime.<br />
Modelling premixed turbulent combustion is traditionally based on the progress<br />
variable as the dependent scalar. It will be argued that this approach is physically not<br />
sound. Therefore a level set formulation is proposed to derive suitable model<br />
equations. In these equations a better distinction can be made between the physical<br />
phenomena occurring in the two regimes mentioned above. Finally a joint formulation<br />
for the turbulent burning velocity is derived which contains the two regimes as<br />
distinet limits.<br />
The resulting combustion model is applied to two premixed configurations with<br />
spark ignition, a cylindrical vessel and a SI engine with complex geometry. For the<br />
latter case simulations are shown for engines for homogeneous and as well as for<br />
stratified charge. At the end of the talk a LES simulation of a turbulent flame on a slot<br />
burner will be presented.<br />
a Institut für Technische Verbrennung, RWTH, D-52056 Aachen, Germany<br />
b FEV, D-52078 Aachen, Germany<br />
1 Peters, J. Fluid Mech. 384, 107 (1999)<br />
2 Wenzel and Peters, Combust. Sci. and Techn. 158, 273 (2000)<br />
3 Peters et al., Proceedings of the Combustion Institute 28, 235 (2000)<br />
4 Peters et al., Combust. Theory Modelling 5, 363 (2001)<br />
5 Wenzel and Peters, Combust. Sci. Tech. 177, 1095 (2005)