长江科学院院报 ›› 2021, Vol. 38 ›› Issue (11): 86-93.DOI: 10.11988/ckyyb.20200670

• 水力学 • 上一篇    下一篇

液滴倾斜撞击液膜液冠演化规律

郭平措1, 何小泷2, 袁浩3   

  1. 1.青海省水利厅引黄济宁工程建设管理局,西宁 810001;
    2.四川大学 水力学及山区河流开发保护国家重点实验室,成都 610065;
    3.重庆交通大学 重庆西南水运工程科学研究所,重庆 400074
  • 收稿日期:2020-07-06 修回日期:2020-11-17 出版日期:2021-11-01 发布日期:2021-11-08
  • 通讯作者: 袁 浩(1989-),男,四川巴中人,助理研究员,博士,主要从事水力学及河流动力学方向研究。E-mail:yuanhao@cqjtu.edu.cn
  • 作者简介:郭平措(1990-),男,青海民和人,工程师,主要从事水利水电工程研究。E-mail:sweatcreature@outlook.com
  • 基金资助:
    国家重点研发计划项目(2016YFC0402006);国家自然科学基金项目(51979183);贵州省交通运输厅科技项目(2018221007)

Evolution of Liquid Crown During Oblique Droplet Impact on Liquid Film

GUO Ping-cuo1, HE Xiao-long2, YUAN Hao3   

  1. 1. Management Office of Yellow River Diversion into Xining, Department of Water Resources of Qinghai Province,Xining 810001,China;
    2. State Key Laboratory of Hydraulics and Mountain River Engineering, Sichuan University, Chengdu 610065, China;
    3. Chongqing Southwest Research Institute for Water Transport Engineering, Chongqing Jiaotong University, Chongqing 400074, China
  • Received:2020-07-06 Revised:2020-11-17 Published:2021-11-01 Online:2021-11-08

摘要: 采用可调节表面张力的大密度比格子玻尔兹曼伪势模型模拟了液滴倾斜撞击液膜的过程,分析了不同雷诺数、韦伯数、液膜厚度和碰撞角对液冠演化的影响。结果表明: 碰撞时能量损失随着雷诺数增大而减小,但随着液膜厚度增大而增大;上下游液冠高度均随着雷诺数、韦伯数和碰撞角的增大而增大;同时上下游液冠高度随着液膜厚度的变化呈现先增大后减小的趋势,液膜厚度为0.25倍液滴半径时达到最大值。液冠延伸长度同样随着雷诺数和碰撞角增大而增大,但并不随着韦伯数的增大而变化,同时液冠延伸长度随着液膜厚度增加而减小。

关键词: 格子玻尔兹曼方法, 伪势模型, 倾斜撞击, 液冠演化, 液冠飞溅

Abstract: The process of droplets splashing on liquid film is simulated using a large-density lattice Boltzmann pseudo-potential model with tunable surface tension. The effects of Reynolds number, Weber number, liquid film thickness, and collision angle on the evolution of the liquid crown are analyzed. Results demonstrate that the energy loss during the impact decreases with the increase of Reynolds number, but augments with the thickening of liquid film; the upstream and downstream crown heights both rise with the increase of Reynolds number, Weber number, and collision angle, but reduce after increment with the change of film thickness, and peaks when liquid film thickness is 0.25 times of droplet radius. The crown extension length also increases with the growing of Reynolds number and collision angle, but does not vary with the increase of Weber number, and meanwhile shrinks with the thickening of liquid film.

Key words: lattice Boltzmann method, pseudo-potential model, oblique impact, crown evolution, crown splashing

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