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短距/垂直起降飞机近地面机腹温升影响特性数值模拟

李春 李广超

李春, 李广超. 短距/垂直起降飞机近地面机腹温升影响特性数值模拟[J]. 航空动力学报, 2024, 39(10):20220831 doi: 10.13224/j.cnki.jasp.20220831
引用本文: 李春, 李广超. 短距/垂直起降飞机近地面机腹温升影响特性数值模拟[J]. 航空动力学报, 2024, 39(10):20220831 doi: 10.13224/j.cnki.jasp.20220831
LI Chun, LI Guangchao. Numerical simulation on the effect characteristics of belly temperature rise for short/vertical takeoff and landing aircraft proximity of ground[J]. Journal of Aerospace Power, 2024, 39(10):20220831 doi: 10.13224/j.cnki.jasp.20220831
Citation: LI Chun, LI Guangchao. Numerical simulation on the effect characteristics of belly temperature rise for short/vertical takeoff and landing aircraft proximity of ground[J]. Journal of Aerospace Power, 2024, 39(10):20220831 doi: 10.13224/j.cnki.jasp.20220831

短距/垂直起降飞机近地面机腹温升影响特性数值模拟

doi: 10.13224/j.cnki.jasp.20220831
基金项目: 辽宁省自然科学基金(2022-MS-296)
详细信息
    作者简介:

    李春(1998-),男,硕士生,主要从事短距/垂直起降飞机近地面流场研究

    通讯作者:

    李广超(1979-),男,教授、博士生导师,博士,主要从事航空发动机热端部件传热与冷却技术方面的研究。E-mail:ligc706@163.com

  • 中图分类号: V233

Numerical simulation on the effect characteristics of belly temperature rise for short/vertical takeoff and landing aircraft proximity of ground

  • 摘要:

    通过计算流体力学方法和响应面法获得了机腹温升关于喷管落压比、来流速度及喷管出口离地高度的2阶响应曲面回归方程,以及显著影响飞机机腹温升的关键因素。分析了喷管落压比、来流速度和喷管出口离地高度对飞机机腹温升的交互影响作用,并得到了给定工况范围内机腹温升最大的工况。研究表明:仅考虑单因素影响时,机腹温升随落压比、来流速度和喷管出口离地高度的增大而减小;考虑两因素交互作用时,只有高度与落压比对机腹存在交互影响;考虑单因素2阶影响时,喷管出口离地高度、来流速度和喷管落压比均对机腹温升存在2阶效应。优化获得的机腹温升最大的工作点是尾喷管出口离地高度为3倍尾喷管出口直径、喷管落压比为2、来流速度为0 m/s,此时的机腹温度变化为13.92%。

     

  • 图 1  S/VTOL飞机缩比模型及边界条件

    Figure 1.  Scale model of S/VTOL aircraft and boundary conditions

    图 2  不同湍流模型下冲击面中轴线压力分布

    Figure 2.  Pressure distribution on the central axis of impact surface under different turbulence models

    图 3  冲击面中轴线压力分布

    Figure 3.  Pressure distribution of central line on impact plane

    图 4  机腹温升响应曲面

    Figure 4.  Respond surface of belly temperature rise

    图 5  喷泉流的形成

    Figure 5.  Formation of fountain flow

    图 6  不同落压比下计算域子午面速度及流线分布

    Figure 6.  Velocity and streamline distribution on meridian plane of computational domain under different nozzle pressure ratios

    图 7  不同落压比下机腹无量纲温度分布

    Figure 7.  Non-dimensional temperature distribution of belly under different nozzle pressure ratios

    图 8  不同流速下计算域子午面速度及流线分布

    Figure 8.  Velocity and streamline distribution on meridian plane of computational domain under different inflow velocities

    图 9  不同流速下机腹无量纲温度分布

    Figure 9.  Non-dimensional temperature distribution of belly under different inflow velocities

    图 10  H/D=9时计算域子午面速度及流线分布

    Figure 10.  Velocity an streamline distribution on meridian plane of computational domain when H/D=9

    图 11  不同高度时机腹无量纲温度分布

    Figure 11.  Non-dimensional temperature distribution of belly under different heights

    表  1  响应面法试验点

    Table  1.   Test point for respond surface method

    参数 数值
    H/D 3 6 9
    U/(m/s) 0 7.5 15
    π 2 2.5 3
    下载: 导出CSV

    表  2  机腹温度变化模型方差及显著性表格

    Table  2.   Variance and significance of belly temperature variation

    方差来源 方均根值/10−5 F P 结果
    回归模型 422.1 19.8 0.0004 显著
    A 652.5 30.61 0.0009 显著
    B 1400 64.54 <0.0001 显著
    C 165.1 7.75 0.0272 显著
    AB 0.269 0.013 0.9137
    AC 171.6 8.05 0.0251 显著
    BC 2.611 1.22 0.3050
    A2 537.7 25.23 0.0015 显著
    B2 144.4 6.77 0.0353 显著
    C2 591.2 27.74 0.0012 显著
    决定系数 0.9622
    下载: 导出CSV
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出版历程
  • 收稿日期:  2022-11-01
  • 网络出版日期:  2024-04-03

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