2012
DOI: 10.1016/j.compfluid.2011.12.011
|View full text |Cite
|
Sign up to set email alerts
|

Broadband trailing-edge noise prediction with a stochastic source model

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

1
9
0

Year Published

2016
2016
2022
2022

Publication Types

Select...
5
4

Relationship

0
9

Authors

Journals

citations
Cited by 11 publications
(10 citation statements)
references
References 33 publications
1
9
0
Order By: Relevance
“…However, this simple integer is unsuitable for the flap noise prediction.The power is N SL = 5.5 for low frequency side-edge component and N SH = 6.5 for high frequency side-edge component. For the trailing-edge component, the power is set to N T = 5.5, which is in good agreement with the fitted result 5.4 and 5.6, respectively provided by Cozza et al [31] and Ewert et al [32], based on CFD solutions and experimental data. To close the prediction model, we also need to formulate the normalized spectrum F (St), the flow energy conversion efficiency β and the directivity factor D (θ).…”
Section: Prediction Modelsupporting
confidence: 75%
“…However, this simple integer is unsuitable for the flap noise prediction.The power is N SL = 5.5 for low frequency side-edge component and N SH = 6.5 for high frequency side-edge component. For the trailing-edge component, the power is set to N T = 5.5, which is in good agreement with the fitted result 5.4 and 5.6, respectively provided by Cozza et al [31] and Ewert et al [32], based on CFD solutions and experimental data. To close the prediction model, we also need to formulate the normalized spectrum F (St), the flow energy conversion efficiency β and the directivity factor D (θ).…”
Section: Prediction Modelsupporting
confidence: 75%
“…A synthetic turbulent spectra is generated by an advanced digital filter method. 16 Digital filter methods have been extensively used for CAA applications 23,24,25 due to their ability to reproduce realistic turbulence spectra with a low computational cost. In the current work, an advanced digital filter method 16 is used to generate a two-dimensional, isotropic, and frozen turbulence with a Gaussian energy spectrum, which is specified by the integral length scale Λ, and the turbulent intensity I xx .…”
Section: Ivb Broadband Turbulencementioning
confidence: 99%
“…Computational aeroacoustic (CAA) work-flows, based on stochastic sound source generation and sound propagation in the frequency domain, have previously been investigated in the literature. For instance, in Cozza et al [9], the sound sources are calculated using a digital filter-based stochastic turbulence method and the acoustic field is computed from the APE equations in the frequency domain. In Casalino et al [10], a stochastic Fourier method is used to compute the source terms of Howe's acoustic analogy [11], which is solved in frequency domain using a finite element method (FEM).…”
Section: Introductionmentioning
confidence: 99%