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the contrary, the global behavior of the flow seems to be correctly reproduced using mo<strong>de</strong>l<br />

UM2. Moreover, reasonable agreement with experimental data is obtained on streamwise<br />

velocity profile in the perforated zone. However, the velocity is slightly un<strong>de</strong>r-estimated near<br />

the wall, which is consistent with the comparison of the mo<strong>de</strong>l with the reference small-scale<br />

wall-resolved LES data. Despite this un<strong>de</strong>r-estimation, the mo<strong>de</strong>l UM2 is consi<strong>de</strong>red to be<br />

correct enough to be used in full combustion chamber flow computations. The mo<strong>de</strong>l can be<br />

used in the presented form in non-isothermal computations: in this case, the wall is implicitly<br />

assumed to be adiabatic.<br />

D<strong>et</strong>ailed information of the flow around multi-perforated plated is crucial not only to d<strong>et</strong>ermine<br />

which physical characteristics have to be mo<strong>de</strong>led but also to evaluate the exactness<br />

of the mo<strong>de</strong>ling assumptions. The comparison with the reference small-scale wall-resolved<br />

LES data indicates that improvements to the UM2 mo<strong>de</strong>l can be obtained by refining the<br />

mo<strong>de</strong>ling of the time- and spatial-averaged streamwise velocity at the hole inl<strong>et</strong>/outl<strong>et</strong> and by<br />

being able to evaluate the shape of the time-averaged velocity field at the hole inl<strong>et</strong>/outl<strong>et</strong>.<br />

Acknowledgments<br />

The authors are grateful to the European Community for funding this work un<strong>de</strong>r the<br />

project INTELLECT-DM (Contract No. FP6 - AST3 - CT - 2003 - 502961), and to<br />

the CINES (Centre Informatique National pour l’Enseignement Supérieur) and the BSC<br />

(Barcelona Supercomputing Center) for the access to supercomputer facilities. The authors<br />

would also like to thank Turbomeca and P<strong>et</strong>re Miron for the access to the LARA experimental<br />

database.<br />

References<br />

1 Lefebvre, A. H., Gas Turbines Combustion, Taylor & Francis, 1999.<br />

2 Simpson, R. L., “Characteristics of turbulent boundary layers at low Reynolds numbers with and<br />

without transpiration,” J. Fluid Mech., Vol. 42, No. 4, 1970, pp. 769–802.<br />

3 Piomelli, U., Ferziger, J. H., Moin, P., and Kim, J., “New approximate boundary conditions for large<br />

eddy <strong>simulation</strong>s of wall-boun<strong>de</strong>d flows,” Phys. Fluids A, Vol. 1, No. 6, 1989, pp. 1061–68.<br />

4 MacManus, D. G. and Eaton, J. A., “Flow physics of discr<strong>et</strong>e boundary layer suction - measurements<br />

and predictions,” J. Fluid Mech., Vol. 417, 2000, pp. 47–75.<br />

5 P<strong>et</strong>erson, S. D. and Plesniak, M. W., “Evolution of j<strong>et</strong>s emanating from short holes into crossflow,”<br />

J. Fluid Mech., Vol. 503, 2004, pp. 57–91.<br />

6 Pe<strong>et</strong>, Y. V., Film cooling from inclined cylindrical holes using Large-Eddy Simulations, Ph.D. thesis,<br />

Stanford University, 2006.<br />

7 Margason, R. J., “Fifty years of j<strong>et</strong> in crossflow research,” Computational and Experimental Assessment<br />

of J<strong>et</strong>s in Crossflow, edited by U. Winchester, Vol. AGARD-CP-534, 1993, pp. 1–41.<br />

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