TY - GEN
T1 - Source mechanisms of jet crackle
AU - Anderson, Aaron T.
AU - Freund, Jonathan B.
PY - 2012
Y1 - 2012
N2 - Fighter jets and other aircraft with high specific thrust engines can make a particularly intense type of aerodynamic jet noise that has become known as crackle. It is distinguished from low-speed jet noise by its frequency content, extreme intensity, and sporadic character, all of which make it particularly annoying to people working and living near these aircraft. There is evidence that source mechanisms and nonlinear propagation mechanisms both lead to crackle. We use detailed simulations to study the turbulence source and near acoustic field of a crackling temporally developing planar free shear flows, with Mach numbers M = 1.5, M = 2.5, and M = 3.5. The skewness of the acoustic pressure being Sk > 0.4 has been correlated with the perception of crackle. The sound radiated from the M = 1.5 mixing layer had Sk = 0.13, which is well below this threshold. However, both the higher speed mixing layers have Sk that meet this nominal threshold: Sk = 0.46 for M = 2.5 and Sk = 0.61 for M = 3.5. Space-time correlations inside the mixing layer show convective Mach numbers corresponding to that anticipated based upon the Mach angle of the near-field acoustic waves. However, turbulence correlation statistics suggest that the Mach waves observed are longer than would be produced by typical correlated structure. The clumping together of shorter waves in the very near acoustic field leads to the obvious Mach waves of greater extent further from the turbulent mixing layer.
AB - Fighter jets and other aircraft with high specific thrust engines can make a particularly intense type of aerodynamic jet noise that has become known as crackle. It is distinguished from low-speed jet noise by its frequency content, extreme intensity, and sporadic character, all of which make it particularly annoying to people working and living near these aircraft. There is evidence that source mechanisms and nonlinear propagation mechanisms both lead to crackle. We use detailed simulations to study the turbulence source and near acoustic field of a crackling temporally developing planar free shear flows, with Mach numbers M = 1.5, M = 2.5, and M = 3.5. The skewness of the acoustic pressure being Sk > 0.4 has been correlated with the perception of crackle. The sound radiated from the M = 1.5 mixing layer had Sk = 0.13, which is well below this threshold. However, both the higher speed mixing layers have Sk that meet this nominal threshold: Sk = 0.46 for M = 2.5 and Sk = 0.61 for M = 3.5. Space-time correlations inside the mixing layer show convective Mach numbers corresponding to that anticipated based upon the Mach angle of the near-field acoustic waves. However, turbulence correlation statistics suggest that the Mach waves observed are longer than would be produced by typical correlated structure. The clumping together of shorter waves in the very near acoustic field leads to the obvious Mach waves of greater extent further from the turbulent mixing layer.
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U2 - 10.2514/6.2012-2251
DO - 10.2514/6.2012-2251
M3 - Conference contribution
AN - SCOPUS:85088185011
SN - 9781600869327
T3 - 18th AIAA/CEAS Aeroacoustics Conference (33rd AIAA Aeroacoustics Conference)
BT - 18th AIAA/CEAS Aeroacoustics Conference (33rd AIAA Aeroacoustics Conference)
PB - American Institute of Aeronautics and Astronautics Inc.
T2 - 18th AIAA/CEAS Aeroacoustics Conference 2012 (33rd AIAA Aeroacoustics Conference)
Y2 - 4 June 2012 through 6 June 2012
ER -