2016
DOI: 10.1016/j.pecs.2016.07.001
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State-of-the-art in premixed combustion modeling using flamelet generated manifolds

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Cited by 287 publications
(154 citation statements)
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“…However, the characteristic length scale is still sufficiently large compared to the mean free path for the combustion problem involved. Consequently, classical continuum descriptions are appropriate [66,67]. Additionally, the Reynolds number is found to be less than 680 in all of the cases examined.…”
Section: Mathematical Modelmentioning
confidence: 92%
“…However, the characteristic length scale is still sufficiently large compared to the mean free path for the combustion problem involved. Consequently, classical continuum descriptions are appropriate [66,67]. Additionally, the Reynolds number is found to be less than 680 in all of the cases examined.…”
Section: Mathematical Modelmentioning
confidence: 92%
“…Table 1 summarizes these cases. Following closely the analysis procedures discussed in Dasgupta et al [1], the "local" flame behavior is quantified via integrated flame sub-volumes, constructed to pass through localized sections of a triangulated isosurface that represents an instantaneous snapshot of the flame following the methodology in Ref. [18].…”
Section: Methodsmentioning
confidence: 99%
“…A significant increase of about four times is observed for Z 2 sgs , c 2 sgs and the magnitude of [ Z c ] sgs moving from + = 0.6 to 3. The magnitude of g Zc , however, drops from 0.9 to 0.68 and it is due to the faster increase of the denominator than the numerator in Equation (17). Although it seems that the value of [ Z c ] sgs compared to Z 2 sgs and c 2 sgs is smaller for larger + , the Z-c correlation effect on combustion is more important as the filter size increases because the subgrid scalar fluctuations and their interaction become more influential and they require closure models.…”
Section: Joint Subgrid Z -C Statistics 31 Analysis Of Single Snapshmentioning
confidence: 95%
“…However, in LES this correlation is partly resolved by the numerical grid and it is of interest to understand the effect of the remaining unresolved part, [ Z c ] sgs , in Equation (1) and its behaviour with the filter size. In many existing LES models for partially premixed combustion such as the flamelet-based approaches [14][15][16][17][18][19][20][21] and conditional moment closure (CMC) with doubleconditioning [22,23], a presumed JPDF is used to account for the subgrid fluctuations of mixture fraction and progress variable. This joint PDF is computed locally using the transported scalars, usually the Favre-filtered values and subgrid variances of Z and c. The filtered thermo-chemical quantities can then be obtained from the flamelet manifolds using Φ (x, t) = F Φ (ξ, ζ ) P (ξ, ζ ; x, t) dζ dξ,…”
Section: Introductionmentioning
confidence: 99%