Flame Broadening and its Impact on the Apparent Lewis Number in Premixed Turbulent Reacting Flows

Dulger, Mark; Sher, Eran

doi:10.1080/00102209608951990

Cited by 6 publications

(3 citation statements)

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“…The reader is referred to [34] for a scholarly review on Lewis number effects in turbulent combustion. Here our objective is more limited and addresses the question, discussed in [30], whether the effective Lewis number tends to one for large values of u , as argued in [6], or further deviates from one, as argued in [31]. This controversial question has a clear answer in our well defined framework.…”

Section: Dependence Of the Effective Lewis Number On The Flowmentioning

confidence: 94%

“…The third question is related to the characterization of the effective Lewis number in turbulent combustion. This controversial question, discussed in [30], concerns whether the effective Lewis number tends to one for large values of u , as argued in [6], or further deviates from one, as argued in [31]. We will provide a clear and somewhat surprising answer to this question posed within our laminar flow model based on a simple analytical formula to be derived.…”

Section: Introductionmentioning

confidence: 91%

“…The inner problem can now be simplified further, by noting that F 1 = −Le eff 1 identically; this is seen by adding (30) to (31) and using (32). Eliminating F 1 , the inner problem becomes…”

Section: -10mentioning

confidence: 99%

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Taylor dispersion in premixed combustion: Questions from turbulent combustion answered for laminar flames

2018

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We present a study of Taylor dispersion in premixed combustion and use it to clarify fundamental issues related to flame propagation in a flow field. In particular, simple analytical formulas are derived for variable density laminar flames with arbitrary Lewis number Le providing clear answers to important questions arising in turbulent combustion, when these questions are posed for the case of one-scale laminar parallel flows. Exploiting, in the context of a laminar Poiseuille flow model, a thick flame distinguished asymptotic limit for which the flow amplitude is large with the Reynolds number Re fixed, three main contributions are made. First, a link is established between Taylor dispersion [G. Taylor, Proc. R. Soc. London Ser. A 219, 186 (1953)] and Damköhler's second hypothesis [G. Damköhler, Ber. Bunsen. Phys. Chem. 46, 601 (1940)] by describing analytically the enhancement of the effective propagation speed U T due to small flow scales. More precisely, it is shown that Damköhler's hypothesis is only partially correct for one-scale parallel laminar flows. Specifically, while the increase in U T due to the flow is shown to be directly associated with the increase in the effective diffusivity as suggested by Damköhler, our results imply that U T ∼ Re (for Re 1) rather than U T ∼ √ Re, as implied by Damköhler's hypothesis. Second, it is demonstrated analytically and confirmed numerically that, when U T is plotted versus the flow amplitude for fixed values of Re, the curve levels off to a constant value depending on Re. We may refer to this effect as the laminar bending effect as it mimics a similar bending effect known in turbulent combustion. Third, somewhat surprising implications associated with the dependence of U T and of the effective Lewis number Le eff on the flow are reported. For example, Le eff is found to vary from Le to Le −1 as Re varies from small to large values. Also, U T is found to be a monotonically increasing function of Re if Le < √ 2 and a nonmonotonic function if Le > √ 2.

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