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Droplet size and velocity distribution function in sprays based on maximum entropy principle

CAO Jian-ming HE Jian LI Xian-guo

曹建明, 何建, 李献国. 基于最大熵原理的喷雾液滴尺寸和速度联合分布函数[J]. 交通运输工程学报, 2008, 8(5): 1-8.
引用本文: 曹建明, 何建, 李献国. 基于最大熵原理的喷雾液滴尺寸和速度联合分布函数[J]. 交通运输工程学报, 2008, 8(5): 1-8.
CAO Jian-ming, HE Jian, LI Xian-guo. Droplet size and velocity distribution function in sprays based on maximum entropy principle[J]. Journal of Traffic and Transportation Engineering, 2008, 8(5): 1-8.
Citation: CAO Jian-ming, HE Jian, LI Xian-guo. Droplet size and velocity distribution function in sprays based on maximum entropy principle[J]. Journal of Traffic and Transportation Engineering, 2008, 8(5): 1-8.

基于最大熵原理的喷雾液滴尺寸和速度联合分布函数

基金项目: 

natural science fund project of PRC 50676012

详细信息
  • 中图分类号: U473

Droplet size and velocity distribution function in sprays based on maximum entropy principle

Funds: 

natural science fund project of PRC 50676012

More Information
    Author Bio:

    CAO Jian-ming (1962-), male, Changyit Shandong, Professor of Chang'an University, research on power engineering. +86-29-8233596l, jcao@chd.edu.cn

  • 摘要: 应用最大熵原理和动量守恒定律, 从理论上建立了喷雾液滴尺寸和速度联合分布函数。应用该方程编制数值计算程序, 对纯柴油与质量掺混比为30%(L30)的柴油/液化石油气(LPG)混合燃料的喷雾液滴尺寸和速度联合分布进行了数值计算, 比较了两种燃料的雾化特性。比较结果表明: 由于L30闪急沸腾效应的影响, 其液滴尺寸分布曲线的峰值明显高于柴油的分布曲线峰值, 且峰值和曲线整体趋势都向小颗粒方向偏移, 说明喷射L30产生的液滴颗粒比柴油颗粒小; L30的速度分布曲线峰值较高, 且位于小速度范围, 说明小速度液滴所占的比例更大。液滴尺寸与速度(D-u)等高线图表明: 液滴颗粒越小, 其速度分布范围越广; 液滴速度越小, 其尺寸分布范围越大。L30液滴尺寸与速度联合分布的收敛速度较快, 说明L30喷雾所产生的小颗粒和小速度液滴更加密集, 雾化质量更佳。

     

  • 图  1  柴油液滴尺寸/速度联合数目分布

    Figure  1.  Droplet size and velocity distributions of diesel

    图  2  柴油液滴尺寸数目分布

    Figure  2.  Droplet size distributions of diesel

    图  3  柴油液滴速度数目分布

    Figure  3.  Droplet velocity distributions of diesel

    图  4  L30液滴尺寸/速度联合数目分布

    Figure  4.  Droplet size and velocity distributions of L30

    图  5  L30喷滴尺寸数目分布

    Figure  5.  Droplet size distributions of L30

    图  6  L30液滴速度数目分布

    Figure  6.  Droplet velocity distributions of L30

    图  7  柴油D-u等高线

    Figure  7.  D-u contour map of diesel

    图  8  L30 D-u等高线

    Figure  8.  D-u contour map of L30

    表  1  Computational parameters

    Table  1.   Computational parameters

    density/(kg·m-3) vaporization heat/(kJ·kg-1) specific heat of diesel-air mixture/[kJ·(kg·K)-1] heat conduct coefficient/[kW·(m·K)-1] injected duration/ms injected mass/mg spray core angle/(°)
    845 251 1.005 1.28×10-4 9 5 19.3
    下载: 导出CSV

    表  2  Computational parameters of LPG

    Table  2.   Computational parameters of LPG

    density/(kg·m-3) vaporization heat/(kJ·kg-1) specific heat of L30-air mixture/[kJ·(kg·K)-1] heat conduct coefficient/[kW·(m·K)-1]
    557 propane 426 2.480 1.511 9×10-5
    butane 385 2.360 1.349 1×10-5
    LPG 410 2.432 1.444 4×10-5
    下载: 导出CSV
  • [1] 曹建明. 喷雾学[M]. 北京: 机械工业出版社, 2005.
    [2] CAO Jian-ming, BI AN Yao-zhang, QI Dong-hui, et al. Comparative investigation of diesel and mixed liquefied petroleum gas/diesel injection engines[J]. Journal of Automobile Engi-neering, 2004, 218(D5): 557-565. doi: 10.1243/095440704774061219
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    [7] LI Xian-guo, TANKIN R S. Droplet size distribution: a derivation of a Nukiyama-Tanasawa type distribution function[J]. Combustion Science and Technology, 1987, 56: 65-76. doi: 10.1080/00102208708947081
    [8] CAOJian-ming. On the theoretical prediction of fuel droplet size distribution in nonreactive diesel sprays[J]. Journal of Fluids Engineering, 2002, 124: 182-185. doi: 10.1115/1.1445140
    [9] LEVY N, AMARA S, CHAMPOUSSI N J C, et al. Nonreactive diesel spray computations supported by PDA measurements[J]. SAE Paper: 970049.
    [10] LI Mei-sen. Initial droplet size and velocity distribution for liquid sprays based on maxi mization of entropy generation[D]. Waterloo: University of Waterloo, 2005.
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出版历程
  • 收稿日期:  2008-04-25
  • 刊出日期:  2008-10-25

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