Heat interaction in a resonance tube

2002 ◽  
Vol 14 (5) ◽  
pp. 1812-1815 ◽  
Author(s):  
A. Alexeev ◽  
A. Goldshtein ◽  
C. Gutfinger
Author(s):  
Abubakar Kawuwa Sani ◽  
Rao Martand Singh ◽  
Ignazio Cavarretta ◽  
Cristina de Hollanda Cavalcanti Tsuha ◽  
Subhamoy Bhattacharya

2020 ◽  
Vol 34 (6) ◽  
pp. 962.e19-962.e25
Author(s):  
Mayara Carneiro Bonette ◽  
Vanessa Veis Ribeiro ◽  
Congeta Bruniere Xavier-Fadel ◽  
Cintia da Conceição Costa ◽  
Ana Paula Dassie-Leite
Keyword(s):  

1983 ◽  
Vol 22 (Part 1, No. 6) ◽  
pp. 1072-1072
Author(s):  
Kiichiro Matsuzawa ◽  
Naoki Inoue ◽  
Takahi Hasegawa

1970 ◽  
Vol 43 (2) ◽  
pp. 369-384 ◽  
Author(s):  
E. Brocher ◽  
C. Maresca ◽  
M.-H. Bournay

Using a simplified wave-diagram and the gas-speed/sound-speed diagram, it is shown how the oscillations start and grow within a resonance tube. It is found that the oscillation amplitude tends to a limiting value which is obtained when the jet is fully swallowed by the tube during the phase of compression of the cycle. Experiments are carried out for jet Mach numbers from 0·1 up to 2. To achieve an adequate evacuation of the tube in the expansion phase, a thin cylindrical body must be used, which is laid along the axis of the jet to produce a wake and a correlative local deficiency of the kinetic energy of the jet. Measured amplitudes of pressure fluctuations are in good agreement with theoretical values.


10.2514/1.144 ◽  
2004 ◽  
Vol 41 (6) ◽  
pp. 1306-1314 ◽  
Author(s):  
Ganesh Raman ◽  
Andrew Mills ◽  
Valdis Kibens

Author(s):  
Ramlala P. Sinha

A solution of the highly complex unsteady compressible flow field inside a cylindrical resonance tube has been obtained numerically, assuming one dimensional, viscous, and heat conducting flow, by solving the appropriate fluid dynamic and energy equations. The resonance tube is approximated by a right circular cylinder closed at one end with a piston oscillating at resonant frequency at the other end. An iterative implicit finite difference scheme is employed to obtain the solution. The scheme permits arbitrary boundary conditions at the piston and the end wall and allows assumptions for transport properties. For the example considered herein, the solution predicts a rise of 95°F in the mean end wall temperature, from 60°F to 155°F, in 14.313 milliseconds which is in good agreement with the experimentally observed values. The solution would also be valid for tapered tubes if the variations in the cross-sectional area are small. In successfully predicting the resonance tube results, an innovative simple but stable solution of unsteady fluid dynamic and energy equations is provided here for wide ranging research, development, and industrial applications in solving a variety of complex fluid flow heat transfer problems. The method is directly applicable to pulsed or pulsating flow and wave motion thermal energy transport, fluid-structure interaction heat transfer enhancement, and fluidic pyrotechnic initiation devices.


2019 ◽  
Vol 72 (1) ◽  
pp. 22-28
Author(s):  
Lorena Sanz López ◽  
Natasha Pérez Marrero ◽  
Teresa Rivera Rodriguez

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