CERFACS CERFACS Scientific Activity Report Jan. 2010 â Dec. 2011
CERFACS CERFACS Scientific Activity Report Jan. 2010 â Dec. 2011
CERFACS CERFACS Scientific Activity Report Jan. 2010 â Dec. 2011
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ADVANCED METHODS AND MULTIPHYSICS<br />
(a) Near-field vorticity magnitude and far-field sound(b) Influence of the perturbation intensity imposed at the jet<br />
(shown using dilatation contours).<br />
inlet.<br />
FIG. 4.6: Noise computation of a subsonic jet.<br />
was adapted to simulate shocks.<br />
4.2.5 Airfoil noise (H. Deniau, G. Dufour, J.-F. Boussuge)<br />
Broadband noise generation and radiation from rotating blades due to the ingestion of turbulence is a<br />
topic of major interest for fan manufacturers. It becomes the main broadband noise source when the<br />
ingested turbulence is at least stronger than two or three % of the relative mean flow on the blades. In<br />
that context, turbulence-interaction noise due to isotropic turbulence impacting a thick cambered airfoil has<br />
been simulated for the first time at high Reynolds number (Rec = 6.5 10 5 ) by a compressible Large Eddy<br />
Simulation (LES) accounting for the installation effects. The full wind-tunnel has been simulated by a two<br />
dimensional Unsteady Reynolds-Averaged Navier-Stokes (URANS) simulation that provides the realistic<br />
boundary conditions for the LES on a restricted domain embedded in the potential core of the wind-tunnel<br />
jet (Fig. 4.7a). Radiative boundary conditions are applied around the LES domain to prevent reflection or<br />
drift of flow parameters. Synthetic turbulence is injected at the inlet of the LES domain. Comparison with<br />
experimental data shows excellent agreement for the noise level and directivity if the sources are restricted<br />
to the leading edge area (Fig. 4.7b). Yet LES also shows some extra noise sources at the trailing edge caused<br />
by a large recirculation bubble close to the leading edge yielding some large vorticity up to the trailing edge,<br />
and a late transition on the suction side [CFD27, CFD53].<br />
4.2.6 Landing-gear noise (J-C. Giret, J-C. Jouhaud, J.-F. Boussuge)<br />
Understanding and predicting aerodynamic noise generation is nowadays of a great importance. Particularly,<br />
since huge progresses have been made on the noise reduction of turbofan engines through high bypass ratios,<br />
the design of new aircraft requires the prediction and if needed the reduction of airframe noise (landing gear<br />
and high-lift devices), which is a major source in approach conditions.<br />
A requirement for such simulations is the ability to handle complex geometries. Most numerical<br />
aeroacoustics studies have been performed on structured meshes as it enables the use of high-order schemes.<br />
However, meshing a complex geometry with a block-structured mesh can be at least difficult and at worst<br />
impossible. In order to overcome such limitations, overset grids or unstructured meshes can be used. This<br />
study focuses on the use of unstructured meshes with a special care on accuracy issues.<br />
162 <strong>Jan</strong>. <strong>2010</strong> – <strong>Dec</strong>. <strong>2011</strong>