rectangular jet
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2022 ◽  
pp. 1-16
Author(s):  
Surya Chakrabarti ◽  
Datta V. Gaitonde ◽  
Sasidharan Nair Unnikrishnan ◽  
Cory Stack ◽  
Florian Baier ◽  
...  

Aerospace ◽  
2021 ◽  
Vol 8 (11) ◽  
pp. 314
Author(s):  
Colby Niles Horner ◽  
Adrian Sescu ◽  
Mohammed Afsar ◽  
Eric Collins

Multiple competing factors are forcing aircraft designers to reconsider the underwing engine pod configuration typically seen on most modern commercial aircraft. One notable concern is increasing environmental regulations on noise emitted by aircraft. In an attempt to satisfy these constraints while maintaining or improving vehicle performance, engineers have been experimenting with some innovative aircraft designs which place the engines above the wings or embedded in the fuselage. In one configuration, a blended wing concept vehicle utilizes rectangular jet exhaust ports exiting from above the wing ahead of the trailing edge. While intuitively one would think that this design would reduce the noise levels transmitted to the ground due to the shielding provided by the wing, experimental studies have shown that this design can actually increase noise levels due to interactions of the jet exhaust with the aft wing surface and flat trailing edge. In this work, we take another look at this rectangular exhaust port configuration with some notional modifications to the geometry of the trailing edge to determine if the emitted noise levels due to jet interactions can be reduced with respect to a baseline configuration. We consider various horizontal and vertical offsets of the jet exit with respect to a flat plate standing in for the aft wing surface. We then introduce a series of sinusoidal deformations to the trailing edge of the plate of varying amplitude and wave number. Our results show that the emitted sound levels due to the jet–surface interactions can be significantly altered by the proposed geometry modifications. While sound levels remained fairly consistent over many configurations, there were some that showed both increased and decreased sound levels in specific directions. We present results here for the simulated configurations which showed the greatest decrease in overall sound levels with respect to the baseline. These results provide strong indications that such geometry modifications can potentially be tailored to optimize for further reductions in sound levels.


2021 ◽  
Author(s):  
Gao Jun Wu ◽  
Sanjiva K. Lele ◽  
Jinah Jeun

2021 ◽  
Vol 6 (7) ◽  
Author(s):  
Surya Chakrabarti ◽  
Datta Gaitonde ◽  
S. Unnikrishnan
Keyword(s):  

2021 ◽  
Author(s):  
Jinah Jeun ◽  
Gao Jun Wu ◽  
Sanjiva K. Lele ◽  
Aatresh Karnam ◽  
Florian Baier ◽  
...  

2021 ◽  
Vol 2021.58 (0) ◽  
pp. F023
Author(s):  
Naoki KAJITANI ◽  
Takahiro KIWATA ◽  
Takaaki KONO ◽  
Nobuyoshi KOMATSU ◽  
Riku OUCHI

IEEE Access ◽  
2021 ◽  
pp. 1-1
Author(s):  
Vignesh Kumar Murugesan ◽  
Aravindh Kumar Suseela Moorthi ◽  
Ganapathy Subramanian L. Ramachandran

2020 ◽  
Vol 86 ◽  
pp. 108723
Author(s):  
Iftekhar Z. Naqavi ◽  
Paul G. Tucker ◽  
Eric Savory ◽  
Robert J. Martinuzzi

2020 ◽  
Vol 14 (1) ◽  
pp. 6322-6333
Author(s):  
Hassan Hasan Assoum ◽  
Jana Hamdi ◽  
Mouhammad El Hassan ◽  
Kamel Abed-Meraim ◽  
M. El Kheir ◽  
...  

Impinging jets are widely used in ventilation systems to improve the mixing and diffusion of airflows. When a rectangular jet hits a slotted plate, an acoustic disturbance can be generated and self-sustained tones produced. Few studies have looked at the Turbulent Kinetic Energy (TKE) produced by the aerodynamic field in such configurations and in the presence of self-sustaining tones. The aim of this work is to investigate the energy transfer between the aerodynamic and acoustic fields generated in a rectangular jet impinging on a slotted plate. The present paper methodology is based on experimental data measurements using 3D tomographic Particle Image Velocimetry (PIV) technique and microphones. It was found that the spectrum of the TKE for Re=5294 (configuration of self-sustained tones) is    which is smaller than that of the acoustic signal . A negative peak of correlation  is obtained between the acoustic signal and TKE for   These results may lead to conclude that the acoustic cycle should be covered by the TKE period and the two signals of both fields are in opposition of phase in order to obtain an optimal configuration for energy transfer.


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