BREAK-UP AND ATOMIZATION OF A ROUND WATER-JET BY A HIGH-SPEED ANNULARAIR-JET

Citation
Jc. Lasheras et al., BREAK-UP AND ATOMIZATION OF A ROUND WATER-JET BY A HIGH-SPEED ANNULARAIR-JET, Journal of Fluid Mechanics, 357, 1998, pp. 351-379
Citations number
52
Categorie Soggetti
Mechanics,"Phsycs, Fluid & Plasmas
Journal title
ISSN journal
00221120
Volume
357
Year of publication
1998
Pages
351 - 379
Database
ISI
SICI code
0022-1120(1998)357:<351:BAAOAR>2.0.ZU;2-C
Abstract
The near-and far-field break-up and atomization of a water jet by a hi gh-speed annular air jet are examined by means of high-speed flow visu alizations and phase Doppler particle sizing techniques. Visualization of the jet's near field and measurements of the frequencies associate d with the gas-liquid interfacial instabilities are used to study the underlying physical mechanisms involved in the primary breakup 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 d rops. An entrainment model of the near-field stripping of the liquid i s proposed, and shown to describe the measured liquid shedding frequen cies. This simplified model explains qualitatively the dependence of t he shedding frequency on the air/water momentum ratio in both initiall y laminar and turbulent water jets. The role of the secondary liquid b reak-up in the far-field atomization of the water jet is also investig ated, and an attempt is made to apply the classical concepts of local isotropy to explain qualitatively the measurement of the far-field dro plet size distribution and its dependence on the water to air mass and momentum ratios. Models accounting for the effect of the local turbul ent dissipation rate in the gas on both the break-up and coalescence o f the droplets are developed and compared with the measurements of the variation of the droplet size along the jet's centreline. The total f lux of kinetic energy supplied by the gas per unit total mass of the s pray jet was found to be the primary parameter determining the seconda ry break-up and coalescence of the droplets in the far field.