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作 者:Miguel A. Barron Dulce Y. Medina Joan Reyes Miguel A. Barron;Dulce Y. Medina;Joan Reyes(Departamento de Materiales, Universidad Autonoma Metropolitana Azcapotzalco, Mexico City, Mexico)
机构地区:[1]Departamento de Materiales, Universidad Autonoma Metropolitana Azcapotzalco, Mexico City, Mexico
出 处:《World Journal of Engineering and Technology》2021年第4期793-803,共11页世界工程和技术(英文)
摘 要:The water-air and Wood’s metal-air systems are modeled by means of Computational Fluid Dynamics to study the interaction between a liquid surface and an impinging air jet under the near field blowing conditions. The effect of the air jet velocity, the height of the injection lance, and the density of the liquid on the depth of the formed cavity is numerically studied. The CFD results of the cavity depth are compared with results previously reported by other authors. The emergence of the splashing phenomenon is predicted in terms of the critical velocity for each liquid-air system. Besides, the blowing number indicates that the drop generation rate is not significant for jet velocities below the critical velocity, and therefore neither the splashing is significant.The water-air and Wood’s metal-air systems are modeled by means of Computational Fluid Dynamics to study the interaction between a liquid surface and an impinging air jet under the near field blowing conditions. The effect of the air jet velocity, the height of the injection lance, and the density of the liquid on the depth of the formed cavity is numerically studied. The CFD results of the cavity depth are compared with results previously reported by other authors. The emergence of the splashing phenomenon is predicted in terms of the critical velocity for each liquid-air system. Besides, the blowing number indicates that the drop generation rate is not significant for jet velocities below the critical velocity, and therefore neither the splashing is significant.
关 键 词:Cavity Depth CFD Impinging Gas Jet Lance Height Liquid-Gas Interaction SPLASHING
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