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Edouard Suillaud as a PhD student at IFPEN studied how to better describe the combustion in high Karlovitz1 number regimes such as those encountered in the new combustion chambers of spark-ignition engines. This description was limited by models that were not suitable for such regimes. The extension of the CFM model to “thin reaction zone regime” (TRZ) has produced promising results.
From one combustion regime to another, unsuitable combustion models
Nowadays, the car manufacturers rely on CFD2 tools for designing and optimising SI engines. However, the current models of turbulent combustion lose their predictivity when they simulate a highly diluted or very lean combustion involving high turbulent intensities.
Indeed, the current models were built based on the assumptions of the flamelet regime. Yet, the combustion in a diluted/lean boosted SI engine drifts from the flamelet regime to the thin reaction zone (TRZ3) regime.
Extending the coherent flame model (CFM) to TRZ regimes
The main aim of Edouard Suillaud’s PhD study was to provide a better description of the combustion in high Karlovitz regimes such as those encountered in the new combustion chambers of spark ignition engines. In particular, this thesis focused on extended the coherent flame model (CFM4) based on the concept of flame surface density (FSD5) to TRZ regimes.
DNS (Direct Numerical Simulation) of statistically planar turbulent premixed flames in three-dimensional turbulent fields were performed and analysed to investigate the validity of the FSD concept in the TRZ regime through the analyses of the flame surface, the flame structure, the characteristics of the flame stretch and of the displacement speed, which are considered as key factors in the modelling of high Karlovitz number flames. An example of numerical result for different combustion regimes is shown in the following figure.
An extension that has shown its potential
These results yielded an extension of the CFM model to TRZ regime through the definition of a new progress variable and a modelled transport equation for a fine-grained flame surface density. The developed CFM-HK raised the two main limitations of flamelet models in the TRZ regimes:
- It takes into account, in particular through the appropriate modelling of the displacement speed, the fact that the flame structure is disturbed by turbulence and that it can no longer be assimilated to a laminar flame structure;
- It takes into account the effect of differential fuel diffusion, which becomes a key factor in the estimation of the turbulent flame speed in the TRZ regime.
The encouraging results from a priori and a posteriori validation showed the potential of the extension of the CFM model proposed in this thesis. They were the subject of a paper submitted to the journal Combustion & Flame.
This work was supported by a grant overseen by the French National Research Agency (ANR) to the ANR-15-CE22-0014 MACDIL project coordinated by IFPEN.
This work was also granted access to the HPC resources of CINES from the GENCI (Grand Equipement National de Calcul Intensif) eDARI program, to resources of JSC (Germany) during the 17th Call of PRACE Project Access (Pra102) and to the HPC facilities at IFPEN.
This thesis has been defended on 12 March 2021 before a jury composed of:
Nilanjan CHAKRABORTY (Reporter, Professor Newcastle University, UK)
Pascale DOMINGO ( Reporter, Research Director CNRS/CORIA, France)
Andreas KEMPF (Examiner, Professor Duisburg-Essen University, Germany)
Benoît FIORINA (President, Professor CentraleSupelec, France)
Frédéric RAVET (Examiner, Engineer and Combustion expert, Renault)
This research was carried out at IFP Energies nouvelles in collaboration with CentraleSupelec, under the supervision of :
Denis Veynante (Co-supervisor, Professor CNRS/EM2C, France)
Olivier Colin (Supervisor and co-promoter, Research engineer, IFPEN, France)
Karine Truffin (Promoter, Research engineer, IFPEN, France)
1The Karlovitz number is a dimensionless number used in fluid mechanics to treat turbulent combustion problems. It measures the ratio of the chemical time scale to the turnover time of the smallest eddies in turbulent flows.
2CFD (Computational Fluid Dynamics)
3Thin reaction zone
4Coherent flame model
5Flame surface density