2015
DOI: 10.1016/j.combustflame.2015.06.001
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Abstract: a b s t r a c tDirect numerical simulations of premixed n-heptane/air flames at different Karlovitz numbers are performed using detailed chemistry. Differential diffusion effects are systematically isolated by performing simulations with both non-unity and unity Lewis numbers. Different unburnt temperatures and turbulence intensities are used and their effects on the flame structure and chemical source terms are investigated. As the unburnt gases are preheated, the viscosity ratio across the flame is reduced a… Show more

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Cited by 109 publications
(130 citation statements)
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“…Little work has been done on direct numerical simulation of high molecular weight hydrocarbon fuels, particularly for high Karlovitz number premixed flames. In a sequence of papers, Savard et al [9,10] and Lapointe et al [11] discuss simulations of premixed heptane flames at high Karlovitz numbers with detailed chemistry and transport, building on previous work [12] based on the hydrogen simulations in [1]. The focus of these papers is on the impact of differential diffusion on flame response, even at high Karlovitz numbers; the authors note a broadening of the flame and a transition to composition versus temperature profiles characteristic of a unity Lewis number flame and a reduction in heat release and fuel consumption rates.…”
Section: Introductionmentioning
confidence: 99%
“…Little work has been done on direct numerical simulation of high molecular weight hydrocarbon fuels, particularly for high Karlovitz number premixed flames. In a sequence of papers, Savard et al [9,10] and Lapointe et al [11] discuss simulations of premixed heptane flames at high Karlovitz numbers with detailed chemistry and transport, building on previous work [12] based on the hydrogen simulations in [1]. The focus of these papers is on the impact of differential diffusion on flame response, even at high Karlovitz numbers; the authors note a broadening of the flame and a transition to composition versus temperature profiles characteristic of a unity Lewis number flame and a reduction in heat release and fuel consumption rates.…”
Section: Introductionmentioning
confidence: 99%
“…All simulations were performed in the work of Bobbitt et al 6 and were originally based on the previous work of Savard et al 11 and Lapointe et al 13 Only cases A, B, B Tab,1 , B 4 Tab,1 , C * , and D performed by Bobbitt et al 6 are considered here. All necessary information about the different simulations is provided in Table I.…”
Section: A Physical Configurationmentioning
confidence: 99%
“…9,10,12,15 In order to isolate the effects of the flame on the turbulence and to reach high Karlovitz numbers, the DNSs analyzed here were statistically planar and used turbulence forcing to prevent the decay of turbulence. Similar methods have been used in the past to investigate both the dynamics of the flame 12,13,[45][46][47] and small scale turbulence. 6,15,16,22 Further analysis and justification of the current configuration were performed by Bobbitt et al 6 The evolution of enstrophy through the flame was in agreement with the unforced, shear-driven, high Karlovitz number slot Bunsen flames of Sankaran et al 43 In the simulations under consideration, linear forcing, adapted from the work of Carroll and Blanquart, 27 was employed by appending the following term to the momentum equation:…”
Section: Turbulence Forcingmentioning
confidence: 99%
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“…The local flame geometries were also investigated, and the effects of strain rate and curvature on different regions across the flame were analyzed in detail [7,8]. Large scale DNS at higher Reynolds and Karlovitz numbers considering detailed chemistry have also been conducted [9][10][11][12][13], with an emphasis on the fractal characteristics.…”
Section: Introductionmentioning
confidence: 99%