Comparison of a spectral model for premixed turbulent flame propagation to DNS and experiments
COMBUSTION THEORY AND MODELLING, cilt.4, sa.3, ss.241-264, 2000 (SCI-Expanded, Scopus)
- Yayın Türü: Makale / Tam Makale
- Cilt numarası: 4 Sayı: 3
- Basım Tarihi: 2000
- Doi Numarası: 10.1088/1364-7830/4/3/302
- Dergi Adı: COMBUSTION THEORY AND MODELLING
- Derginin Tarandığı İndeksler: Science Citation Index Expanded (SCI-EXPANDED), Scopus
- Sayfa Sayıları: ss.241-264
- Orta Doğu Teknik Üniversitesi Adresli: Hayır
Özet
A recently developed spectral model for premixed turbulent combustion in the flamelet regime (based on the EDQNM turbulence theory) has been compared with both direct numerical simulations (DNS) and experimental data. The 128(3) DNS is performed at a Reynolds number of 223 based on the integral length scale. Good agreement is observed for both single- and two-point quantities (i.e. ratio of the turbulent to laminar burning velocities, scalar autocorrelation. dissipation and scalar-velocity cross correlation spectral for the two different values of u'/s(LO) considered. The model also predicts the rapid transient behaviour of the flame at early times. An experimental set-up is then described for generating a lean methane-ah flame and measuring two- point spatial correlations along the midpoint of the flame brush (i.e. along the (C) over bar = 0.5 contour). The experimental measurements in the flamelet regime take the form of a discontinuous or 'telegraph' signal. The EDQNM model, in contrast, describes an 'ensemble' of flames, and thus is based solely on continuous variables. A theoretical relationship between the correlation obtained from the EDQNM model and the equivalent correlation for a discontinuous (experimental) flame is derived. The relationship is used to enable a meaningful comparison between experimentally observed and model correlations. In general, the agreement is good for the three different cases considered in this study, with most of the error occurring at the lowest Reynolds number (Re-L = 22). Furthermore, it is shown that considerably more error would result if no attempt is made to convert the ensemble representation in the model to an equivalent single-flame or 'telegraph' signal.