3-D LDA study of a rectangular jet

1988 ◽  
Author(s):  
GERALD MORRISON ◽  
GARY TATTERSON
Keyword(s):  
2021 ◽  
Vol 6 (7) ◽  
Author(s):  
Surya Chakrabarti ◽  
Datta Gaitonde ◽  
S. Unnikrishnan
Keyword(s):  

1984 ◽  
Author(s):  
B. MCLACHLAN ◽  
A. KROTHAPALLI ◽  
K. NAGARAJA

2001 ◽  
Vol 44 (8-9) ◽  
pp. 2179-2182 ◽  
Author(s):  
V Shukla ◽  
G.S Elliott ◽  
B.H Kear ◽  
L.E McCandlish

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

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

2015 ◽  
Vol 779 ◽  
pp. 751-775 ◽  
Author(s):  
K. B. M. Q. Zaman ◽  
A. F. Fagan ◽  
J. E. Bridges ◽  
C. A. Brown

The interaction between an 8:1 aspect ratio rectangular jet and a flat plate, placed parallel to the jet, is addressed in this study. At high subsonic conditions and for certain relative locations of the plate, a resonance takes place with accompanying audible tones. Even when the tone is not audible the sound pressure level spectra are often marked by conspicuous peaks. The frequencies of these peaks, as functions of the plate’s length, its location relative to the jet as well as jet Mach number, are studied in an effort to understand the flow mechanism. It is demonstrated that the tones are not due to a simple feedback between the nozzle exit and the plate’s trailing edge; the leading edge also comes into play in determining the frequency. With parametric variation, it is found that there is an order in the most energetic spectral peaks; their frequencies cluster in distinct bands. The lowest frequency band is explained by an acoustic feedback involving diffraction at the plate’s leading edge. Under the resonant condition, a periodic flapping motion of the jet column is seen when viewed in a direction parallel to the plate. Phase-averaged Mach number data on a cross-stream plane near the plate’s trailing edge illustrate that the jet cross-section goes through large contortions within the period of the tone. Farther downstream a clear ‘axis switching’ takes place for the time-averaged cross-section of the jet that does not occur otherwise for a non-resonant condition.


1986 ◽  
Vol 14 (4) ◽  
pp. 327-359 ◽  
Author(s):  
Akira Shimizu ◽  
Hiroshi Ishii ◽  
Tsutomu Wada

1991 ◽  
Vol 18 (1) ◽  
pp. 1-9
Author(s):  
E. Rathakrishnan ◽  
T.J. Ignatius ◽  
Channa Raju

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