Subgrid Linear Eddy Mixing and Combustion Modelling of a Turbulent Nonpremixed Piloted Jet Flame

2011 ◽  
Vol 89 (2) ◽  
pp. 295-309 ◽  
Author(s):  
José Salvador Ochoa ◽  
Alberto Sánchez-Insa ◽  
Norberto Fueyo
2021 ◽  
pp. 146808742110371
Author(s):  
Mattia Olcuire ◽  
Clara Iacovano ◽  
Alessandro d’Adamo ◽  
Sebastiano Breda ◽  
Tommaso Lucchini ◽  
...  

Turbulent jet ignition is seen as one of the most promising strategies to achieve stable lean-burn operation in modern spark-ignition engines thanks to its ability to promote rapid combustion. A nearly stoichiometric mixture is ignited in a small-volume pre-chamber, following which multiple hot turbulent jets are discharged in the main chamber to initiate combustion. In the present work, a detailed computational investigation on the turbulent combustion regime of premixed rich propane/air mixture in a quiescent divided chamber vessel is carried out, to study the characteristics of the jet flame without the uncertainties in mixing and turbulent conditions typical of real-engine operations. In particular, the paper investigates the dependency of flame propagation on nozzle diameter (4, 6, 8, 12 and 14 mm) and pre-chamber/main-chamber volume ratio (10% and 20%); CFD results are compared to the experimental outcomes. Results show that the combustion regime in the quiescent pre-chamber follows a well-stirred reaction mode, rendering the limitation in using conventional flamelet combustion models. Furthermore, due to the very high turbulence levels generated by the outflowing reacting jets, also the main chamber combustion develops in a well-stirred reactor type, confirming the need for a kinetics-based approach to combustion modelling. However, the picture is complicated by thickened flamelet conditions possibly being verified for some geometrical variations (nozzle diameter and pre-chamber volume). The results show a general good alignment with the experimental data in terms of both jet phasing and combustion duration, offering a renewed guideline for combustion simulations under quiescent and low Damköhler number conditions.


Author(s):  
Padmabhushana R. Desam ◽  
Philip J. Smith

Numerical prediction of Nitrogen Oxides (NOx) from combustion processes has been a challenging task to the combustion community, yet necessary to reduce environmental impact. Turbulent nonpremixed combustion is characterized by wide ranges of overlapping length and time scales associated with the mixing and chemical reaction processes. In practice, averaged governing equations are solved with subgrid scale models to account for the unresolved scales and interactions among them. A validation study of subgrid scale models is made for a turbulent nonpremixed CO/H2/N2 jet flame. Numerical predictions of Nitric Oxide (NO) quantities are compared with experimental data to evaluate the accuracy of subgrid scale models. Factors significantly affect NO formation are identified and studied thoroughly. In addition to thermal NO pathway, N2O-intermediate pathway is also dominant for this fuel composition. Even though this flame has a very low radiant fraction, the heat loss has a significant effect on NO formation because of the highly temperature dependent NO formation rates. Superequilibrium O-atom & OH radical levels showed high sensitivity to the thermal NO formation in high-temperature zones. An order of magnitude differences are observed in thermal NO by neglecting subgrid scale fluctuations on NO formation with some what less sensitivity to NO formation by the N2O pathway. For reliable and accurate NO numerical predictions, the following should be accounted for; NO formation pathways, radiation effects, nonequilibrium O-atom & OH-radicals and subgrid scale turbulence effects. Overall, the Zeldovich mechanism predicted thermal NO very closely and overpredictions resulted from the N2O-intermediate pathway.


2005 ◽  
Vol 30 (1) ◽  
pp. 549-556 ◽  
Author(s):  
M.R.H. Sheikhi ◽  
T.G. Drozda ◽  
P. Givi ◽  
F.A. Jaberi ◽  
S.B. Pope

2015 ◽  
Vol 156 ◽  
pp. 804-815 ◽  
Author(s):  
S. Gövert ◽  
D. Mira ◽  
J.B.W. Kok ◽  
M. Vázquez ◽  
G. Houzeaux

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