2018
DOI: 10.1017/jfm.2017.906
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Vortex dynamics and sound emission in excited high-speed jets

Abstract: This work aims to study the dynamics of and noise generated by large-scale structures in a Mach 0.9 turbulent jet of Reynolds number $6.2\times 10^{5}$ using plasma-based excitation of shear layer instabilities. The excitation frequency is varied to produce individual or periodic coherent ring vortices in the shear layer. First, two-point cross-correlations are used between the acoustic near field and far field in order to identify the dominant noise source region. The large-scale structure interactions are th… Show more

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Cited by 15 publications
(14 citation statements)
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“…This is readily seen in irrotational near-field pressure spectra (Fig. 7) collected from an excited Mach 0.9 jet [107,165]. The high-amplitude nature of the LAFPA-produced perturbations ensures that at least one of the several harmonics has sufficient amplitude to excite natural instabilities.…”
Section: Actuatorsmentioning
confidence: 89%
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“…This is readily seen in irrotational near-field pressure spectra (Fig. 7) collected from an excited Mach 0.9 jet [107,165]. The high-amplitude nature of the LAFPA-produced perturbations ensures that at least one of the several harmonics has sufficient amplitude to excite natural instabilities.…”
Section: Actuatorsmentioning
confidence: 89%
“…Therefore, either multiple pairings must take place after the structure roll-up and before the end of potential core or the shear layer must grow sufficiently fast for f n θ to approach f p D. Consequently, the initial instability wave development and roll-up, and the potential pairing events, must occur (if at all) between the nozzle exit and the end of the potential core. The structures normally observed in experiments are those with passage frequency of f p , unless special effort is used to visualize the early part of the shear-layer development [107]. It has been shown experimentally that the pairing processes that take place in FSL [14,54] occur in jets as well and are responsible for decreasing the passage frequency of the LSS from the initial shear-layer value of St n f n θ 0 ∕U J ∼ 0.016 to the passage frequency at the end of the potential core, St p f p D∕U J ∼ 0.3 [25].…”
Section: A Shear Layer and Jet Column Modesmentioning
confidence: 99%
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“…Perhaps the most promising frequency-domain active control is the use of plasma actuators, the most successful example of which is arguably the Localized Arc-Filament Plasma Actuators developed at the Ohio State University. [141][142][143][144][145][146][147] These actuators are capable of forcing the flow across a range of frequencies and azimuthal modes. There have been some other novel attempts at forcing the jet away from its natural frequency using spinning valves and plugs, 148,149 though this technology is still in its relative infancy.…”
Section: Active Flow Controlmentioning
confidence: 99%
“…Our focus will be on the progress made in developing an integrated approach, in which nonlinear evolution of instability modes as a physical entity, and their acoustic radiation are both described on the basis of first principles. Experiments reveal that noise is emitted primarily as the wavepackets undergo growth and attenuation [36][37][38]. The emission is significantly enhanced by the jittering or intermittency of the wavepackets.…”
Section: Acoustic Radiation Of Instability Waves In Free Shear Flowsmentioning
confidence: 99%