2011
DOI: 10.1016/j.proci.2010.05.045
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Modeling chemical flame structure and combustion dynamics in LES

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Cited by 30 publications
(22 citation statements)
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“…Even though this perspective is exciting and will certainly become true in the next years for simplified lab-scale burners [205,278], it remains probably a very long term option in gas turbines. First, as pointed out in [190,279], conventional approximations provided for the filtered viscous stress tensor may not be sufficient to fully recover expected flame behaviors in the context of fully resolved premixed flames [191]. LES models do not converge to DNS when the number of grid points increases because SGS models usually neglect certain effects.…”
Section: Leadership-class Les Modeling and Predictionsmentioning
confidence: 99%
“…Even though this perspective is exciting and will certainly become true in the next years for simplified lab-scale burners [205,278], it remains probably a very long term option in gas turbines. First, as pointed out in [190,279], conventional approximations provided for the filtered viscous stress tensor may not be sufficient to fully recover expected flame behaviors in the context of fully resolved premixed flames [191]. LES models do not converge to DNS when the number of grid points increases because SGS models usually neglect certain effects.…”
Section: Leadership-class Les Modeling and Predictionsmentioning
confidence: 99%
“…More detailed combustion models are now commonly used to simulate the response of flames to flow forcing. [42][43][44][45] A different approach is undertaken in this work, where only the steady, reacting base flow is solved by direct simulation of the nonlinear Navier-Stokes equations assuming that chemistry proceeds through one irreversible reaction. The unsteady response of the flame is subsequently determined by solving a linearized version of these equations around this base state.…”
Section: Introductionmentioning
confidence: 99%
“…The flame is here modeled by a progress variable Y c , monotonically increasing from 0 in the fresh gases to Y eq c in the burnt gases. In practical meshes, the flame thickness, defined as d Y c ¼ Y eq c =maxðjrY c jÞ, is thinner than the mesh size D x [7,8]. Therefore, filtering the progress variable field at the width D introduces a resolved flame front of thickness d e Y c % D with D % 3D x .…”
Section: Introductionmentioning
confidence: 99%
“…Initially developed for infinitely thin flame front and for single-step chemistry [14][15][16], this strategy has recently been extended to tabulated chemistry by the Filtered Tabulated Chemistry for LES (F-TACLES) model [9,17]. Simulations of propagating filtered premixed planar flames show that the flame resolution criterion D=D x depends on numerical conditions [18]. For instance, the criteria D=D x P 8 is required in [9] to predict the proper propagation speed of a laminar premixed filtered flame.…”
Section: Introductionmentioning
confidence: 99%