1999
DOI: 10.1016/s0301-9322(99)00042-7
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Drop formation at the surface of plane turbulent liquid jets in still gases

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Cited by 43 publications
(32 citation statements)
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“…For example, when scaling the characteristic droplet diameter of sprays from pressure atomisers on the surface tension, power law exponents ranging from −0.15 to 0.737 [9][10][11][12][13] have been quoted. While there are differences in the considered injector geometries and the flow conditions among the various investigation, from the breadth of the reported correlations, it is clear that no consensus exists.…”
Section: Introductionmentioning
confidence: 99%
“…For example, when scaling the characteristic droplet diameter of sprays from pressure atomisers on the surface tension, power law exponents ranging from −0.15 to 0.737 [9][10][11][12][13] have been quoted. While there are differences in the considered injector geometries and the flow conditions among the various investigation, from the breadth of the reported correlations, it is clear that no consensus exists.…”
Section: Introductionmentioning
confidence: 99%
“…Sallam et al [18] proposed correlations based on several previous pulsed photography and holography studies [4,17] (among others) to estimate the onset of primary breakup and mass flux from turbulent annular and round jets for nozzle exit conditions corresponding to unconditioned, fully developed turbulent pipe flow.…”
mentioning
confidence: 99%
“…The experimental results by Hussein et al [17], Pitts [43], Liepmann et al [31], and Van de Sande et al [57] state that the nozzle exit flow conditions or the Reynolds number of the jet flow allow for the description of the variation of the entrainment intensity in the two-phase air/liquid free jet flow with downstream distance. From experiments by Sallam et al [47], Wong et al [61], and Wygnanski et al [62] emerged accordingly that the intensity of the air entrainment process is expected to be significant for establishing the droplet size distribution. In particular, the primary breakup of the liquid in the Core/Transition region yields fragments that are intrinsically weakened against the impact of the relatively large vortical structures and, therefore, prone to further deformation, so that these vortical air flow structures govern the local self establishing droplet size distribution in a two-phase free jet flow.…”
Section: Literature Surveymentioning
confidence: 99%