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复合坐标系跨临界液滴表面Kelvin-Helmholtz不稳定增长高效预测方法

崔海港 闫啸宇 高岩飞 陈飞 杨世春

崔海港,闫啸宇,高岩飞,等. 复合坐标系跨临界液滴表面Kelvin-Helmholtz不稳定增长高效预测方法[J]. 北京航空航天大学学报,2024,50(9):2835-2842 doi: 10.13700/j.bh.1001-5965.2022.0701
引用本文: 崔海港,闫啸宇,高岩飞,等. 复合坐标系跨临界液滴表面Kelvin-Helmholtz不稳定增长高效预测方法[J]. 北京航空航天大学学报,2024,50(9):2835-2842 doi: 10.13700/j.bh.1001-5965.2022.0701
CUI H G,YAN X Y,GAO Y F,et al. Efficient prediction method for Kelvin-Helmholtz instability growth on transcritical droplet surface in composite coordinate system[J]. Journal of Beijing University of Aeronautics and Astronautics,2024,50(9):2835-2842 (in Chinese) doi: 10.13700/j.bh.1001-5965.2022.0701
Citation: CUI H G,YAN X Y,GAO Y F,et al. Efficient prediction method for Kelvin-Helmholtz instability growth on transcritical droplet surface in composite coordinate system[J]. Journal of Beijing University of Aeronautics and Astronautics,2024,50(9):2835-2842 (in Chinese) doi: 10.13700/j.bh.1001-5965.2022.0701

复合坐标系跨临界液滴表面Kelvin-Helmholtz不稳定增长高效预测方法

doi: 10.13700/j.bh.1001-5965.2022.0701
基金项目: 国家自然科学基金(T2241003)
详细信息
    通讯作者:

    E-mail:yangshichun@buaa.edu.cn

  • 中图分类号: U469

Efficient prediction method for Kelvin-Helmholtz instability growth on transcritical droplet surface in composite coordinate system

Funds: National Natural Science Foundation of China (T2241003)
More Information
  • 摘要:

    针对混合动力专用内燃机实际运行的跨临界条件,传统方法对于主导可燃混合气形成质量的液滴表面Kelvin-Helmholtz不稳定性分析方法难以实现跨临界宽范围的有效预测。采用复合坐标系方法,建立跨临界强对流环境的等效液滴不稳定性高效预测模型,分别采用全局扩散动力学模型、热力学控制模型及局部液滴表面切向不稳定模型。在全局坐标系模型可以通过模态坐标变换求得解析解,局部坐标系引入势函数等,提高求解速度。而对于可实用性流体计算仿真模型,可通过无量纲物理参数描述不同跨临界条件下空气动力、惯性力、黏性力、表面张力、加速度等控制因素的变化规律,以及其对液滴表面切向和法向不稳定波增长的影响规律。结果表明:液滴表面的空气动力仍然支配着跨临界条件液滴表面切向不稳定波的发展;压力增大时,液相雷诺数控制的流动特性减小与欧尼索控制的液滴黏性力减弱基本抵消;环境温度增加时,雷诺数表征的流动特性对Kelvin-Helmholtz波增长的贡献越来越小,液滴的惯性力影响也越来越弱。

     

  • 图 1  跨临界复合坐标系统液滴切向不稳定模型示意

    Figure 1.  Tangential instability model of droplet in transcritical composite coordinate system

    图 2  局部表面坐标系K-H不稳定表面波示意

    Figure 2.  K-H unstable surface waves in local surface coordinate system

    图 3  液滴迎风面破碎高速摄影图像

    Figure 3.  High-speed photographic image of droplets breaking up on the windward side

    图 4  不同环境压力下各参数随无量纲时间的变化曲线

    Figure 4.  Variation of variables with dimensionless time under different ambient pressures

    图 5  不同环境压力下最大K-H增长率随无量纲时间的变化曲线

    Figure 5.  Variation of maximum K-H growth rate with dimensionless time under different environmental pressures

    图 6  不同环境温度下各参数随无量纲时间的变化曲线

    Figure 6.  Variation of variables with dimensionless time under different ambient temperatures

    图 7  不同环境温度下最大K-H增长率随无量纲时间的变化曲线

    Figure 7.  Variation of maximum K-H growth rate with dimensionless time under different ambient temperatures

    表  1  不稳定波长与初始粒径比的试验与数值模拟结果

    Table  1.   Experimental and numerical simulation results of ratio of unstable wavelength to initial particle size

    对比态环境压力Pr 对比态初始液滴温度Trdrop0 对比态环境温度Tramb 气流速度urel /(m·s−1) λ/d0计算值 λ/d0试验值
    1.1 0.53 0.95 80 0.53 0.6
    1.6 0.53 0.95 80 0.4 0.4
    1.0 0.59 0.95 80 0.62 0.7
    1.0 0.78 0.95 80 0.3 0.3
    1.0 0.53 0.66 80 0.60 0.7
    1.0 0.53 1.15 80 0.56 0.6
    1.0 0.53 0.95 80 0.59 0.6
    1.0 0.53 0.95 100 0.43 0.5
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出版历程
  • 收稿日期:  2022-08-10
  • 录用日期:  2022-11-12
  • 网络出版日期:  2023-05-05
  • 整期出版日期:  2024-09-27

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