16th AIAA/CEAS Aeroacoustics Conference 2010
DOI: 10.2514/6.2010-3833
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CAA-RPM Prediction and Validation of Slat Setting Influence on Broadband High-Lift Noise Generation

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Cited by 20 publications
(21 citation statements)
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“…The second step consists of two parts, (a) the stochastic unsteady 3D modeling of the turbulence by DLR's stochastic turbulence generator fRPM (fast Random Particle Mesh Method) [11,12] and (b) the actual CAA computation of the (acoustic) perturbation field about the given RANS flow field by means of DLR's CAA code PIANO [13], see Figure 2. The approach requires an appropriate modeling of the unsteadiness of turbulence, which means that it has to cover those features of the turbulence which are relevant for the sound generation, see [14,15]. The respective turbulence representation is realized with the stochastic turbulence generator "fRPM" which takes the flow field and one point turbulence statistics from a pre-cursor RANS mean flow simulation as an input.…”
Section: Noise Assessment Of An Aircraft Component (Level 1)mentioning
confidence: 99%
See 1 more Smart Citation
“…The second step consists of two parts, (a) the stochastic unsteady 3D modeling of the turbulence by DLR's stochastic turbulence generator fRPM (fast Random Particle Mesh Method) [11,12] and (b) the actual CAA computation of the (acoustic) perturbation field about the given RANS flow field by means of DLR's CAA code PIANO [13], see Figure 2. The approach requires an appropriate modeling of the unsteadiness of turbulence, which means that it has to cover those features of the turbulence which are relevant for the sound generation, see [14,15]. The respective turbulence representation is realized with the stochastic turbulence generator "fRPM" which takes the flow field and one point turbulence statistics from a pre-cursor RANS mean flow simulation as an input.…”
Section: Noise Assessment Of An Aircraft Component (Level 1)mentioning
confidence: 99%
“…Turbulence is only realized in the relevant source domain (called "fRPM source patch", see [14,15]) as shown in Figure 3a. A snapshot of the resulting sound pressure field is plotted in Figure 3b for illustration.…”
Section: Noise Assessment Of An Aircraft Component (Level 1)mentioning
confidence: 99%
“…This mechanism (referred to as an edge-dipole source [79]) is regarded as a major contributor to slat noise generation. High-fidelity simulation of the multi-element aerofoil flow, and in particular of the slat flow, using improved versions of DES (see [6,88]), implicit DES [89,90], with wallmodel LES (see [10]) and stochastic source models coupled with acoustic perturbation equation solution [91,92] has provided important insights into slat noise generation and radiation. Strong collaboration between the computations and laboratory measurements (see [93]) even when simulations were limited to two-dimensional unsteady RANS, has resulted in faster progress.…”
Section: (I) Slat Noisementioning
confidence: 99%
“…Initially frozen, the behavior of the turbulence carried by the mean flow in the RPM method is now driven by a Langevin equation [31,34,35], which is massively used to describe turbulence temporal evolution [34,36,37]. Working with a Langevin equation, random particles carrying the stream function are placed along the streamlines according to the time step and the mean flow.…”
Section: Doi: 102514/1j052368mentioning
confidence: 99%
“…Many formulations have been proposed to improve the former works of Careta et al [29], who generated a stochastic field from a random stream function. The random particle mesh (RPM) method developed by Ewert and Edmunds [30], followed by Ewert [13], has been applied to investigate slat [31] and jet [32] noise. In RPM, the streamlines are discretized regarding the time step and the local mean velocity of the flow.…”
Section: Doi: 102514/1j052368mentioning
confidence: 99%