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超声速盘收口盘缝带伞不同收口比下气动性能

代雨柔 李健 荣伟 薛晓鹏 黄明星 方康

代雨柔,李健,荣伟,等. 超声速盘收口盘缝带伞不同收口比下气动性能[J]. 北京航空航天大学学报,2026,52(3):864-873
引用本文: 代雨柔,李健,荣伟,等. 超声速盘收口盘缝带伞不同收口比下气动性能[J]. 北京航空航天大学学报,2026,52(3):864-873
DAI Y R,LI J,RONG W,et al. Aerodynamic characteristics of supersonic mid-gore reefing disk-gap-band parachute under different reefing ratios[J]. Journal of Beijing University of Aeronautics and Astronautics,2026,52(3):864-873 (in Chinese)
Citation: DAI Y R,LI J,RONG W,et al. Aerodynamic characteristics of supersonic mid-gore reefing disk-gap-band parachute under different reefing ratios[J]. Journal of Beijing University of Aeronautics and Astronautics,2026,52(3):864-873 (in Chinese)

超声速盘收口盘缝带伞不同收口比下气动性能

doi: 10.13700/j.bh.1001-5965.2023.0813
基金项目: 

国家自然科学基金(12072377);湖南省自然科学基金(2022JJ30678)

详细信息
    通讯作者:

    E-mail:lijian_bbmouth@163.com

  • 中图分类号: V445.2+3

Aerodynamic characteristics of supersonic mid-gore reefing disk-gap-band parachute under different reefing ratios

Funds: 

National Natural Science Foundation of China (12072377); Hunan Provincial Natural Science Foundation of China (2022JJ30678)

More Information
  • 摘要:

    火星着陆探测器的质量提升要求降落伞增大面积以保障稳降性能,同时,需控制开伞力以避免探测器结构负担过大质量。超声速盘缝带伞盘收口技术可同时满足上述2点需求。基于此,以火星环境为背景,采用流固耦合仿真分析,得到收口比与阻力系数比、投影面积比、收口绳载荷的函数关系;采用计算流体力学仿真分析方法,研究盘缝带伞的稳定性特征。研究表明,超声速盘收口盘缝带伞能够实现阻力性能的受控变化,提供满足工程应用的稳定性能。研究结果可为超声速盘收口盘缝带伞的工程设计提供参考。

     

  • 图 1  盘缝带伞

    Figure 1.  Disk-gap-band parachute

    图 2  盘收口盘缝带伞[11-12]

    Figure 2.  Disk-gap-band parachute with mid-gore reefing[11-12]

    图 3  盘缝带伞结构[13]

    Figure 3.  Disk-gap-band parachute structure[13]

    图 4  DUAL CE/SE方法一维求解步骤[16]

    Figure 4.  DUAL CE/SE one-dimensional solution procedure [16]

    图 5  流场域及盘缝带伞模型

    Figure 5.  Fluid and disk-gap-band parachute model

    图 6  盘收口盘缝带伞平均气动外形

    Figure 6.  Average aerodynamic shape of mid-gore reefing disk-gap-band parachute

    图 7  盘收口盘缝带伞外形对比

    Figure 7.  Shape comparison of mid-gore reefing disk-gap-band parachute

    图 8  投影面积与时间的关系

    Figure 8.  Relation between projected area and time

    图 9  投影面积比与收口比的关系

    Figure 9.  Relation between projected area ratio and reefing ratio

    图 10  阻力系数比与收口比的关系

    Figure 10.  Relation between drag coefficients ratio and reefing ratio

    图 11  盘收口盘缝带伞受力图

    Figure 11.  Mid-gore reefing disk-gap-band parachute force diagram

    图 12  局部受力图

    Figure 12.  Local stress diagram

    图 13  载荷比与收口比的关系

    Figure 13.  Relation between load ratio and reefing ratio

    图 14  盘缝带伞力矩方向示意图

    Figure 14.  Diagram of moment direction of disk-gap-band parachute

    图 15  轴向力系数与攻角的关系

    Figure 15.  Relation between axial force coefficient and angle of attack

    图 16  力矩系数与攻角的关系

    Figure 16.  Relation between moment coefficient and angle of attack

    图 17  力矩系数导数与攻角的关系

    Figure 17.  Relation between the derivative of the moment coefficient and the angle of attack

    图 18  力矩系数随时间变化曲线

    Figure 18.  Curve of moment coefficient with time

    图 19  速度云图

    Figure 19.  Velocity cloud map

    表  1  盘缝带伞结构尺寸[13]

    Table  1.   Structural size of the disk-gap-band parachute[13]

    名义
    直径/m
    顶孔
    直径/m
    盘高/m 缝高/m 带高/m 单幅
    带宽/m
    伞绳
    长度/m
    0.813 0.057 0.296 0.034 0.098 0.077 1.328
    下载: 导出CSV

    表  2  研究算例

    Table  2.   Research examples

    马赫数 收口比/%
    1.8 10,15,25,30,35,40
    2.2 10,15,25,30,35,40
    2.6 10,15,25,30,35,40
    下载: 导出CSV

    表  3  材料属性

    Table  3.   Material property

    结构名称 密度/(kg·m−3) 弹性模量/Pa 泊松比
    伞衣 538 4.3×108 0.14
    纬向加强带 1194 1.5×1010
    伞绳 468 1.5×1010
    收口绳 800 5×109
    下载: 导出CSV

    表  4  仿真使用来流条件

    Table  4.   Freestream condition for simulation

    马赫数来流速度/(m·s−1)静压/Pa密度/(kg·m−3)温度/K
    1.8429.13330.560.00744231.28
    2.2524.50330.560.00744231.28
    2.6619.85330.560.00744231.28
    下载: 导出CSV

    表  5  阻力系数对比

    Table  5.   Comparison of drag coefficients

    马赫数 阻力系数 误差/%
    试验结果 数值模拟结果
    2.0 0.21344 0.19464 8.81
    2.5 0.21484 0.19662 8.48
    下载: 导出CSV
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出版历程
  • 收稿日期:  2023-12-13
  • 录用日期:  2024-03-27
  • 网络出版日期:  2024-04-03
  • 整期出版日期:  2026-03-31

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