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Abstracts - KTH Mechanics

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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)

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