吉林大学学报(工学版)2024,Vol.54Issue(6) :1512-1518.DOI:10.13229/j.cnki.jdxbgxb.20220960

自激振荡喷嘴流动特性对近嘴区射流雾化的影响

Effect of fuel flow in self-excited oscillating nozzle on near-nozzle region jet atomization

高永强 周士谦 齐龙 尹迁齐 黄雪涛 张佳兴
吉林大学学报(工学版)2024,Vol.54Issue(6) :1512-1518.DOI:10.13229/j.cnki.jdxbgxb.20220960

自激振荡喷嘴流动特性对近嘴区射流雾化的影响

Effect of fuel flow in self-excited oscillating nozzle on near-nozzle region jet atomization

高永强 1周士谦 1齐龙 1尹迁齐 1黄雪涛 1张佳兴1
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作者信息

  • 1. 山东交通学院 汽车工程学院,济南 250357
  • 折叠

摘要

基于大涡模拟(LES)和流体体积分数法(VOF)模型,建立了自激振荡喷嘴流场的数学模型,仿真研究了自激振荡喷嘴内流动及射流破碎过程.结果表明:燃油流过自激振荡喷嘴能显著提高流体涡度和扰动强度,射流扰动强度的振荡幅值增大3倍多.射流扰动对近嘴区射流破碎的影响更加敏感,显著提高了射流破碎质量;近嘴区射流破碎距离(SL)明显减小,SL在距喷嘴出口(2~5)倍直径处变化;近嘴区喷雾锥角也随之增大,最大增幅超过60%,燃油雾化效果得到显著提高.本文计算结果可为自激振荡脉冲雾化喷嘴提供有力的理论依据.

Abstract

In order to further understand the mechanism of breakup of diesel jet,a mathematical model of fuel flow in self-excited oscillating nozzle was built based on large eddy simulation(LES)and Volume of Fluid(VOF)model.The results show that fluid vorticity and disturbance intensity in the self-excited oscillating nozzle is significantly increased,and it can increased by more than three times.The disturbance intensity is more sensitive to jet breakup in the near-nozzle region,which can significantly improve the jet breakup effect.The jet breakup length(SL)is greatly reduced,which can varies from 2 to 5 times of the outlet diameter at near-nozzle region.At the same time,the spray cone angle in the near-nozzle area is also increased,which can increase by more than 60%.The fuel jet atomization effect is greatly improved in the self-excited oscillating nozzle.The numerical simulation results is also provided a strong theoretical basis for the self-oscillating pulsed atomizing nozzle.

关键词

能源动力工程/自激振荡喷嘴/喷雾特性/射流破碎机理/湍流扰动

Key words

energy and power engineering/self-excited oscillating nozzle/atomization characteristic/breakup mechanism of jet/turbulence perturbation

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基金项目

山东交通学院博士启动基金项目(BS201901047)

出版年

2024
吉林大学学报(工学版)
吉林大学

吉林大学学报(工学版)

CSTPCD北大核心
影响因子:0.792
ISSN:1671-5497
参考文献量5
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