SAE Technical Paper Series 2006
DOI: 10.4271/2006-01-1194
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Applicability of Large Eddy Simulation to the Fluid Mechanics in a Real Engine Configuration by Means of an Industrial Code

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Cited by 33 publications
(18 citation statements)
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“…This particular SGS model was used due to not using any additional space filtering or transport equations hence reducing the computational cost and increasing solution instability. The Smagorinsky constant (C s ) was set to 0.02 [12] and the filter width was defined by the cube root of the cell volume.…”
Section: The Les Sgs Turbulence Modelmentioning
confidence: 99%
“…This particular SGS model was used due to not using any additional space filtering or transport equations hence reducing the computational cost and increasing solution instability. The Smagorinsky constant (C s ) was set to 0.02 [12] and the filter width was defined by the cube root of the cell volume.…”
Section: The Les Sgs Turbulence Modelmentioning
confidence: 99%
“…The Smagorinsky constant (C s ) was set to 0.02 [15] and the filter width (Δ) was defined by equation (7), where V is the cell volume. …”
Section: Computational Setupmentioning
confidence: 99%
“…Actually, this efficiency function adaptation was performed in a very empirical way in several former computations on different engine configurations, in particular the F7P engine considered in this work and the XU10 engine described in [9,17] where authors found that b ¼ 2 gives very satisfactory results with LW. Indeed, Figure 12 shows that with this value, the expected behavior is retrieved: the resolved part is still lower with LW compared to TTGC or TTG4A but this loss is balanced by an increased contribution of SGS surface.…”
Section: Tfles and Efficiency Functionmentioning
confidence: 99%
“…In particular, ICE simulations usually use low order and/or dissipative numerical schemes as well as simple Sub-Grid-Scale (SGS) turbulence models. Concerning numerical schemes, two classes of convective schemes are generally found in the literature: upwind-biased schemes are used by Jhavar and Rutland [8], Dugue et al [9] or Goryntsev et al [10] for instance while the Lax-Wendroff total discretization approach [11] (second order accurate in space and time) is used by Richard et al [12], Vermorel et al [6] or Granet et al [13]. Both of them are known to be very dissipative and a priori not well suited for LES [10].…”
Section: Introductionmentioning
confidence: 99%