Mixing Enhancement in Subsonic Jet Flow Using the Air-Tab Technique

AIAA Journal ◽  
2008 ◽  
Vol 46 (11) ◽  
pp. 2966-2969 ◽  
Author(s):  
S. C. M. Yu ◽  
K. S. Lim ◽  
W. Chao ◽  
X. P. Goh
Author(s):  
Peter Jordan ◽  
Francois Coiffet ◽  
Joel Delville ◽  
Yves Gervais ◽  
Fabienne Ricaud

1996 ◽  
Author(s):  
D. Parekh ◽  
V. Kibens ◽  
A. Glezer ◽  
J. Wiltse ◽  
D. Smith

2016 ◽  
Vol 32 (5) ◽  
pp. 1095-1103 ◽  
Author(s):  
Qitai Eri ◽  
Liang Hong ◽  
Ting Li ◽  
Qiang Wang ◽  
Mengjie Wang

Author(s):  
Sathish Kumar K ◽  
Senthilkumar Chidambaram

Abstract This investigation aims to present the jet mixing characteristics and thrust variations of the subsonic jet employed with plain triangular tab and semi-circular corrugated tab by numerical simulation. A triangular tab with semi-circular corrugations is used in this regard at the exit plane of a convergent nozzle, to study the behavior of the jet and its structure. The near jet flow field is studied for different Mach numbers of 0.6, 0.8 and 1, and the comparisons were done for the jet employed with plain triangular tab. To validate the numerical results, experimental validation is carried out for 0.6 Mach jet. The thrust and the potential core length of any jet depend mainly on the percentage of blockage ratio. Since the relationship between the thrust and blockage ratio is such that, the blockage ratio increases, the thrust and the potential core length decreases and vice-versa. The blockage ratio is kept 8.27 % for both the corrugated and plain triangular tabs. From the results, it is found that the Potential core length of the free jet is cut down to 66 % by the jet employed with plain triangular tab, whereas it is 64.5 % for the corrugated tab enabled jet. It is also concluded that the corrugated tab enhances the thrust by 4.43 % for the same blockage ratio and increases potential core length by 3.33 % when compared with the plain triangular tab. This increase in thrust is there by an added advantage of this investigation.


1981 ◽  
Vol 103 (4) ◽  
pp. 378-384 ◽  
Author(s):  
S. W. Rienstra

Asymptotic approximations for small Strouhal number are derived for the solution of the problem of the interaction between an acoustic wave and a subsonic jet flow issuing from a semi-infinite pipe. Density and sound speed differences between the jet flow and the (slowly moving) ambient medium, and a general edge condition are included. The approximations relate to the field inside the jet flow, to the far field, to the reflection coefficient, end-impedance and end correction for the reflected wave inside the pipe, and to the transmitted and radiated sound power. Within the range of parameters considered, the effect of the density and sound speed differences and ambient flow is found to be appreciable, although the character of the solution is not changed. However, the choice of the edge condition does have important implications; specifically, the phase of the reflected wave is most sensitive to only slight deviations from the Kutta condition.


1971 ◽  
Vol 46 (3) ◽  
pp. 477-500 ◽  
Author(s):  
P. A. Lush

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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