Correction: Investigation of water jet break up by supersonic rocket exhaust

Author(s):  
Hansen J. Jones ◽  
Vaibhav Rajora ◽  
Shyam K. Menon
Keyword(s):  
Break Up ◽  
1996 ◽  
Vol 24 (4) ◽  
pp. 229-234
Author(s):  
Kenneth C. Weston ◽  
Jianrong Wang

High-velocity jets of fluid are encountered in both natural and man-made settings. The geyser, the fireman's hose, and the rocket exhaust are notable examples. Study of the fluid mechanics literature reveals the axisymmetric fluid jet as a fundamental fluid configuration that is rich in physical features. It is the purpose of this paper to discuss a few basic, but important, aspects of the behaviour of a water jet and ways that they may be directly observed by the senses, without recourse to sophisticated measuring devices, to the benefit of science and engineering students of all ages. These are observations which may be readily performed in undergraduate laboratories or even as homework assignments.


2004 ◽  
Vol 36 (6) ◽  
pp. 919-927 ◽  
Author(s):  
P. Couty ◽  
�. Spiegel ◽  
N. V�g� ◽  
B. I. Ugurtas ◽  
P. Hoffmann
Keyword(s):  

2019 ◽  
Vol 113 ◽  
pp. 129-141
Author(s):  
Enrico Fuchs ◽  
Sebastian Kricke ◽  
Enrico Schöhl ◽  
Jens-Peter Majschak

2019 ◽  
Vol 58 (49) ◽  
pp. 22389-22398
Author(s):  
Paolo Trucillo ◽  
Roberta Campardelli ◽  
Iolanda De Marco

1998 ◽  
Vol 357 ◽  
pp. 351-379 ◽  
Author(s):  
J. C. LASHERAS ◽  
E. VILLERMAUX ◽  
E. J. HOPFINGER

The near- and far-field break-up and atomization of a water jet by a high-speed annular air jet are examined by means of high-speed flow visualizations and phase Doppler particle sizing techniques. Visualization of the jet's near field and measurements of the frequencies associated with the gas–liquid interfacial instabilities are used to study the underlying physical mechanisms involved in the primary break-up of the water jet. This process is shown to consist of the stripping of water sheets, or ligaments, which subsequently break into smaller lumps or drops. An entrainment model of the near-field stripping of the liquid is proposed, and shown to describe the measured liquid shedding frequencies. This simplified model explains qualitatively the dependence of the shedding frequency on the air/water momentum ratio in both initially laminar and turbulent water jets. The role of the secondary liquid break-up in the far-field atomization of the water jet is also investigated, and an attempt is made to apply the classical concepts of local isotropy to explain qualitatively the measurement of the far-field droplet size distribution and its dependence on the water to air mass and momentum ratios. Models accounting for the effect of the local turbulent dissipation rate in the gas on both the break-up and coalescence of the droplets are developed and compared with the measurements of the variation of the droplet size along the jet's centreline. The total flux of kinetic energy supplied by the gas per unit total mass of the spray jet was found to be the primary parameter determining the secondary break-up and coalescence of the droplets in the far field.


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