PIV STUDY OF RADIAL WALL JET FORMED BY A NORMALLY IMPINGING TURBULENT SYNTHETIC JET

2019 ◽  
Vol 26 (2) ◽  
pp. 99-126 ◽  
Author(s):  
Udaysinh S. Bhapkar ◽  
Harekrishna Yadav ◽  
Amit Agrawal
Keyword(s):  
Wall Jet ◽  
1977 ◽  
Vol 28 (4) ◽  
pp. 247-258 ◽  
Author(s):  
Yutaka Tsuji ◽  
Yoshinobu Morikawa ◽  
Masaaki Sakou

SummaryMeasured stability characteristics in a radial wall jet were compared with calculated results for a two-dimensional wall jet. It was found that the stability of the radial wall jet is similar in many respects to that of the two-dimensional wall jet. An exception is that the local amplification rate of the disturbance velocity is much higher than in the two-dimensional case. It was also found that quarter-harmonics appear in the non-linear region, as well as half-harmonics, and that their amplitude distributions show profiles similar to that of the fundamental component. Further, vortex patterns were visualised in water flow, and results corresponding to measurements in air flow and to the linear stability calculation were obtained.


1975 ◽  
Vol 13 (3) ◽  
pp. 239-262 ◽  
Author(s):  
Anat Arbhabhirama ◽  
Wei-Chun Wan
Keyword(s):  
Wall Jet ◽  

1967 ◽  
Vol 34 (2) ◽  
pp. 457-463 ◽  
Author(s):  
M. Poreh ◽  
Y. G. Tsuei ◽  
J. E. Cermak

In this paper measurements are presented of mean velocities, turbulence intensities, Reynolds’ stresses, and the wall friction in a radial wall jet formed by an impinging circular jet on a smooth flat plate. The mean velocities of the wall jet are found to be similar and can be correlated with the maximum velocity and jet thickness at each station, except for a mild Reynolds number dependence near the wall. The dimensionless radial velocity profile is in good agreement with the form suggested by Glauert [1] although the variation of the thickness of the jet does not conform to his predictions. It is shown here that this discrepancy follows from Glauert’s use of the Prandtl eddy viscosity model in describing the Reynolds’ stress distribution. Our measurements show that the shear stress does not vanish where the velocity gradient is zero, as in the case with a free jet, or as required by the eddy viscosity model. The wall friction in the wall jet is found to be larger than the corresponding friction pipe flow. This increase is probably due to the large turbulent fluctuations in the outer region of the jet, which affect the structure of the wall region.


1987 ◽  
Vol 30 (266) ◽  
pp. 1243-1247
Author(s):  
Toshio TANAKA ◽  
Eiichi TANAKA ◽  
Yoshihiro INOUE
Keyword(s):  
Wall Jet ◽  

AIChE Journal ◽  
1963 ◽  
Vol 9 (4) ◽  
pp. 548-554 ◽  
Author(s):  
M. T. Scholtz ◽  
Olev Trass
Keyword(s):  
Wall Jet ◽  

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