aiaa2011 presentation
TRANSCRIPT
Qualitative validation: n = 0, StD = 1.1
0246
r/R
0 10 20 30 40 50 60 70z/R
DNS
0246
r/R
0 10 20 30 40 50 60 70z/R
LEE
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Conclusion
1 Algorithm to compute the NRBF sources at multiple frequencies
2 In laminar jet: linear shear noise term is major source
3 NRBF decomposition and sources for a fully turbulent jet
wavepackets
monopole
vortex pairing
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Pressure in Fourier domain (ω = 1.2)
1
2
kr
0 1 2kz
0 0.25 0.5
Pressure P1.2(k)
0
1
2
3
kr
0 1 2 3kz
0 0.5 1
Gaussian filter W(k)
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Pressure in Fourier domain (ω = 1.2)
1
2
kr
0 1 2kz
0 0.25 0.5
Pressure P1.2(k)
0
1
2
3
kr
0 1 2 3kz
0 0.5 1
Gaussian filter W(k)
30 / 31
Pressure in Fourier domain (ω = 1.2)
Decomposition
1
2
kr
0 1 2kz
0 0.25 0.5
Radiating pressure
P �1.2 = WP
0
1
2
3
kr
0 1 2 3kz
0 0.25 0.5
Non-radiating pressure
P1.2 = (1 − W)P1.2
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Pressure in Fourier domain (ω = 1.2)
Decomposition
1
2
kr
0 1 2kz
0 0.25 0.5
Radiating pressure
P �1.2 = WP
0
1
2
3
kr
0 1 2 3kz
0 0.25 0.5
Non-radiating pressure
P1.2 = (1 − W)P1.2
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