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Abstract

In order to study the breakup process of liquid jet in gas film, the backlit photography technique and the VOF TO DPM method are used for experimental and simulation research respectively. Water and air are used as simulant media. Grid adaptive technology is used to refine the gas-liquid interface grid and improve the capture accuracy of the gas-liquid interface. The results show that there are two main breakup processes of liquid jet in gas film: column breakup and surface breakup. The local high-pressure zone in front of the liquid jet makes the jet have a large normal velocity gradient, which causes R-T instability. The surface wave that is generated by the R-T instability is mainly responsible for the liquid column breakup. When the thin liquid film reaches a column breakup point, the airflow penetrating the trough of the surface wave causes the jet column to break. The tangential velocity gradient is generated when the gas film bypasses the liquid jet surface, which causes K-H instability. The K-H surface waves cause ligaments and droplets to strip from the surface of the liquid jet. The local momentum ratio has an important influence on the breakup process of the liquid jet in gas film. When the local momentum ratio is low, the breakup of liquid jet is dominated by the K-H instability. As the local momentum ratio increases, the breakup of liquid jet is gradually dominated by R-T instability. The local momentum ratio plays an important role in the distribution range of the liquid jet in gas film. When the local momentum ratio is low, the ligaments and droplets caused by the liquid jet are mainly distributed within the range of gas film. As the local momentum ratio increases, part of the ligaments and droplets escape from the range of the gas film. The liquid jet penetrates the gas film when the local momentum ratio is greater than 0.74. The breakup length and the penetration depth are both affected by the local momentum ratio. The breakup length increases with the local momentum ratio increasing. The penetration depth also increases with the local momentum ratio, and the penetration depth increases significantly when the liquid jet penetrates the gas film.

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Authors and contacts

Corresponding author:Cheng Peng,imchengpeng@yeah.net; Li Qing-Lian,peakdreamer@163.com;

Funds:Project supported by the National Natural Science Foundation of China (Grant Nos. 11472303, 11402298), the Young Scientists Fund of the National Natural Science Foundation of China (Grant No. 11902351), and the National Basic Research Program of China (Grant No. 613239)

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总压/ MPa	静压/ MPa	质量流量/ (kg·s^–1)	速度/ (m·s^–1)	温度/K	膜厚/ mm
0.2	0.1	0.02	315.4	300	3

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密度/ (kg·m³)	速度/ (m·s^–1)	孔径/ mm	局部动量比LMR
998.2	12.5, 15.0, 17.5, 20.0, 22.5, 25.0	1.3	0.38, 0.55, 0.74, 0.97, 1.23, 1.52

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Vol. 70, Issue 5 - 2021-03-05

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