22nd AIAA/CEAS Aeroacoustics Conference 2016
DOI: 10.2514/6.2016-2844
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Landing Gear Noise Sources Identification through an Application of Array Methods to Experimental and Computational Data

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Cited by 7 publications
(8 citation statements)
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“…For the sake of conciseness, the section below summarizes only a fraction of these noise source localization efforts [29], focusing in particular on the sole baseline CFD-CAA computation (i.e. as-like F2 experiment).…”
Section: Further Investigation About the Nlg Noise Sourcesmentioning
confidence: 99%
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“…For the sake of conciseness, the section below summarizes only a fraction of these noise source localization efforts [29], focusing in particular on the sole baseline CFD-CAA computation (i.e. as-like F2 experiment).…”
Section: Further Investigation About the Nlg Noise Sourcesmentioning
confidence: 99%
“…This work, which was achieved by the present first and fourth authors, is detailed in Section 4. Finally, based on the CFD-CAA numerical signals acquired over dedicated microphone arrays, the NLG noise sources were further characterized through the use of advanced signal processing techniques [29]; more precisely, once acquired over virtual microphone arrays matching those used in the experiments, the CFD-CAA signals were processed following two distinct array methods of source localization, namely Classical Beam Forming (CBF) and Deconvolution Approach for the Mapping of Acoustic Sources (DAMAS). Such work, which was primarily achieved by the present third and first authors, was documented through the 22th AIAA Aeroacoustics Conference [29], and is recalled in Section 5.…”
Section: Introductionmentioning
confidence: 99%
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“…In other studies the phased array is located farther from the sources and the acoustic data has to be extrapolated from the flow solution. This extrapolation is most often performed using integral methods such as the Ffowcs Williams-Hawkings (FW-H) integral [12,13,14,15,16,17], but other approaches can be found [18]. Extrapolation is performed when the acoustic field is not expected to be sufficiently well-resolved at the location of the array.…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, extensive wind-tunnel or flyover test campaigns usually have a large economic cost, limiting the amount of configurations available to study. In practice, for numerical simulations, the geometry of the LG is normally simplified to some extent where the computational cost is acceptable, such as the realistic NLG geometry from the ALLEGRA project [27][28][29] or the more simplified LAGooN geometry from ONERA [30]. One advantage of computational simulations is that they allow for non-intrusive measurements in directions that are impossible to investigate in experiments (such as upwind of the model) and that the acoustic data are usually cleaner than those recorded in experiments, allowing for shorter recording times.…”
mentioning
confidence: 99%