The Dynamic Evolution of Cavitation Vacuolar Cloud with High-Speed Camera

被引:0
作者
Joseph Sekyi-Ansah
Yun Wang
Zhongrui Tan
Jun Zhu
Fuzhu Li
机构
[1] Jiangsu University,School of Mechanical Engineering
来源
Arabian Journal for Science and Engineering | 2020年 / 45卷
关键词
Vacuolar cloud; Grayscale; FDM; Nozzle diameter; Cavitation;
D O I
暂无
中图分类号
学科分类号
摘要
The dynamic model of a single cavitation bubble in the submerged cavitation water jet was established and solved by MATLAB to obtain its motion characteristics and pressure pulse change rules. Numerical simulation based on FLUENT to closer wall, empty bubble breaking form then influences the law of mechanics effect, with the increase in empty bubble, and the breaking time is reduced, but the maximum jet velocity and pressure increase gradually, on the mechanism of action of the solid wall by the fact that the combination of microfluidic and shock wave gradually plays a leading role, while plastic deformation and basic cavitation erosion are avoided. The maximum pressure and maximum jet velocity increase little, and the collapse time of cavitation is reduced. By comparing the grayscale images of the two combinations of jets, it can be found that the brightness of the vacuolar clouds in diameter (d) = 1.6 mm and pressure (P) = 15 MPa is slightly less than that in d = 1.2 mm and P = 30 MPa, indicating that the density of the vacuolar clouds and the dispersion is relatively high, while the increase in nozzle diameter leads to the increase in flow rate, which increases the shear layer of high-speed submerged jet in a static water. The pressure pulse generated by cavitating water jet hollow bubble failure is far greater than the linear superposition value of a single cavitation bubble. But the high-pressure shock wave value on the fixed wall and water hammer pressure are generated by microjet. The conclusion is also corresponding to the simulation results.
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页码:4907 / 4919
页数:12
相关论文
共 121 条
  • [1] Fujisawa N(2017)Time-resolved observations of pit formation and cloud behavior in cavitating jet Wear 386–387 99-105
  • [2] Kikuchi T(2018)Simultaneous observation of cavitation collapse and shock wave formation in cavitating jet Exp. Thermal Fluid Sci. 94 159-167
  • [3] Fujisawa K(2008)Frequency in shedding/discharging cavitation clouds determined by visualization of a submerged cavitating jet J. Fluids Eng. 130 021304-021304-8-26
  • [4] Yamagata T(2015)Visualisation and les simulation of cavitation cloud formation and collapse in an axisymmetric geometry Int. J. Multiph. Flow 68 14-251
  • [5] Fujisawa N(1995)High-speed observations of the cavitation cloud around a high-speed submerged water jet. JSME Int J. Ser. B Fluids Therm. Eng. 38 245-79
  • [6] Fujita Y(2016)Simultaneous shadowgraph imaging and acceleration pulse measurement of cavitating jet Wear 358–359 72-911
  • [7] Yanagisawa K(2000)Flow structure and modeling issues in the closure region of attached cavitation Phys. Fluids 12 895-902
  • [8] Fujisawa K(2013)Effect of nozzle geometry on a standard cavitation erosion test using a cavitating jet Wear 297 895-64
  • [9] Yamagata T(2008)Frequency in shedding/discharging cavitation clouds determined by visualization of a submerged cavitating jet J. Fluids Eng. 130 021304-1184
  • [10] Hutli EAF(2013)Simultaneous observation of cavitation structures and cavitation erosion Wear 300 55-17