Journal of Fluid Mechanics · 1971 · 315 citations · 5 references
Natural SciencesPhysicsAcousticsOcean AcousticsTheoretical PhysicsAcoustic MeasurementAcoustic RadiationAeroacousticsCritical FrequencyExperimental AeroacousticsJet InteractionsJet NoiseJet Noise PredictionJet PhysicsJets
The authors measured the noise field of a 25 mm subsonic jet, analyzed velocity dependence and directivity in 1/3‑octave bands using the parameter \((fD/V_J)(1-M_c\cos\theta)\), and compared the results with Lighthill’s convected quadrupole theory. The measurements confirm that Lighthill’s theory accurately predicts intensity variation with jet velocity and angle below a critical frequency, but overestimates the noise above this threshold, indicating reduced convective amplification when the sound wavelength becomes shorter than the jet flow path length.
Measurements of the noise field from a 25 mm diameter subsonic air jet are presented. These results are analysed in some detail by determining both the jet velocity dependence and the directivity of the intensity of the radiation in 1/3-octave bands at particular values of the frequency parameter, \[ (fD/V_J)(1-M_c\cos\theta). \] This procedure should ensure that a particular source in a geometrically similar position in the jet is always observed, whatever the jet velocity, diameter and emission angle. These results are compared with the predictions of Lighthil's (1952) theory of convected quadrupoles. It is shown that the theory predicts the variation of the intensity with jet velocity and emission angle provided that the observed frequency is below a certain critical value, which depends on jet diameter and emission angle and is independent of jet velocity. Above this critical frequency, the predicted variations overestimate the measurements and it appears that the convective amplification predicted by the theory is much reduced. The variation of this critical frequency is explained by assuming that substantial interaction occurs between the radiated sound and the jet flow when the wavelength of the sound becomes shorter than the sound path length in the jet flow.
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