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基于相界面数据交换的结冰多相传热过程研究

高轩 邓文豪 刘松 陈胜广 李海旺

高轩, 邓文豪, 刘松, 等. 基于相界面数据交换的结冰多相传热过程研究[J]. 航空动力学报, 2023, 38(7):1561-1570 doi: 10.13224/j.cnki.jasp.20220763
引用本文: 高轩, 邓文豪, 刘松, 等. 基于相界面数据交换的结冰多相传热过程研究[J]. 航空动力学报, 2023, 38(7):1561-1570 doi: 10.13224/j.cnki.jasp.20220763
GAO Xuan, DENG Wenhao, LIU Song, et al. Study on icing multiphase heat transfer process based on phase interface data exchange[J]. Journal of Aerospace Power, 2023, 38(7):1561-1570 doi: 10.13224/j.cnki.jasp.20220763
Citation: GAO Xuan, DENG Wenhao, LIU Song, et al. Study on icing multiphase heat transfer process based on phase interface data exchange[J]. Journal of Aerospace Power, 2023, 38(7):1561-1570 doi: 10.13224/j.cnki.jasp.20220763

基于相界面数据交换的结冰多相传热过程研究

doi: 10.13224/j.cnki.jasp.20220763
基金项目: 国家自然科学基金(52206066)
详细信息
    作者简介:

    高轩(1987-),男,副研究员、博士生导师,博士,主要从事发动机结冰与防冰方面的研究。E-mail:xuangao@buaa.edu.cn

    通讯作者:

    李海旺(1980-),男,教授、博士生导师,博士,主要从事航空发动机高温部件冷却技术方面的研究。E-mail:lihaiwang@buaa.edu.cn

  • 中图分类号: V211.3

Study on icing multiphase heat transfer process based on phase interface data exchange

  • 摘要:

    发动机结冰会对飞行安全造成影响,研究发动机结冰过程机理可以帮助提高飞行安全性能和完成适航验证。使用欧拉法计算了水滴运动过程,使用能量平衡法计算了结冰的多相传热流动过程,使用一维导热模型矫正了壁面导热过程,并提出了基于相界面导热平衡方程的数据交换模型。基于此模型进行了发动机进口部件的冰风洞实验数据数值验证,模拟计算最大结冰厚度与试验误差能够控制在10%左右。相界面数据交换模型能够对近壁的水膜流动和温度梯度进行精细化模拟,并且将用户自定义函数(UDF)与求解器进行流场参数的实时交换,经验证后表明该模型在计算结冰最大厚度时具有较好的精度。

     

  • 图 1  结冰传热流动过程

    Figure 1.  Heat transfer and flow process of icing

    图 2  当量导热系数随时间变化

    Figure 2.  Equivalent heat conductivity coefficient varies with time

    图 3  当量导热系数随冰层厚度变化

    Figure 3.  Equivalent heat conductivity coefficient varies with ice thickness

    图 4  相界面导热平衡模型

    Figure 4.  Heat conduction balance model of phase interface

    图 5  结冰过程计算模型

    Figure 5.  Numerical model of icing process

    图 6  计算流程

    Figure 6.  Solving process

    图 7  数据交换模型冰形与实验、LEWICE软件、CIRA软件冰形比较

    Figure 7.  Ice shape comparison of data exchange model, test, LEWICE software and CIRA software

    图 8  几何模型

    Figure 8.  Geometric model

    图 9  液态水收集系数

    Figure 9.  Water collection coefficient

    图 10  支板冰形验证

    Figure 10.  Ice shape verification of strut

    图 11  表面温度分布

    Figure 11.  Surface temperature distribution

    图 12  支板冰形比较

    Figure 12.  Ice shapes comparison of strut

    表  1  不同冰层厚度当量导热系数

    Table  1.   Equivalent heat conductivity coefficient with different ice thicknesses

    时间/s$ \kappa $/(W/(m3·K))
    δ=0.5 mmδ=1 mmδ=2 mmδ=4 mmδ=6 mm
    0.21239411704786478517851
    0.487607468459345804580
    0.676245912344634233420
    0.870785119284828132813
    167254654247924302430
    下载: 导出CSV
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出版历程
  • 收稿日期:  2022-10-03
  • 网络出版日期:  2023-04-29

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