Aiaa Aviation 2021 Forum 2021
DOI: 10.2514/6.2021-2144
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Numerical Investigation of Acoustic Liners Experimental Techniques using a Lattice-Boltzmann Solver

Abstract: The physics behind acoustic liners attenuation in the presence of flow and high sound pressure level is still a matter of debate. Similarly, discrepancies between experimental results and numerical data have been linked to the boundary conditions used to model the liner and boundary layer effects, and the reasons behind these discrepancies are still not clear. In this sense, to avoid the limitations of the boundary condition approach, fully resolved high fidelity computation models of the liner and its dissipa… Show more

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Cited by 3 publications
(7 citation statements)
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References 33 publications
(57 reference statements)
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“…It is worth mentioning that, in the experiments, results from the in-situ technique are obtained for the most upstream cavity. For such a configuration, local resistance decreases as reactance increases at downstream cavities [17]. Since the numerical results are averaged over all cavities, this could affect the numerical results' agreement to the experimental ones.…”
Section: A Acoustic Results: No-flow Casesmentioning
confidence: 99%
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“…It is worth mentioning that, in the experiments, results from the in-situ technique are obtained for the most upstream cavity. For such a configuration, local resistance decreases as reactance increases at downstream cavities [17]. Since the numerical results are averaged over all cavities, this could affect the numerical results' agreement to the experimental ones.…”
Section: A Acoustic Results: No-flow Casesmentioning
confidence: 99%
“…In this paper, we present a follow-up of the work presented by Schroeder et al [17], where the same multi-cavity SDOF liner is investigated in the presence of flow, and the comparison between eduction methods is extended by including the Prony-like Kumaresan-Tufts (KT) technique [21]. Numerical results are presented for acoustic plane wave with tonal frequency equal to 800, 1100, 1400, 1700, 2000 and 2300 Hz (i.e., above and below the resonant frequency) and amplitude equal to 130 dB and 145 dB.…”
Section: Introductionmentioning
confidence: 92%
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