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2.67 L板式表面张力贮箱设计及抗扰动性能仿真

李光昱 戴炜 黄天麒 赖堂豪 吴宗谕

李光昱, 戴炜, 黄天麒, 赖堂豪, 吴宗谕. 2.67 L板式表面张力贮箱设计及抗扰动性能仿真[J]. 空间科学学报, 2025, 45(2): 458-467. doi: 10.11728/cjss2025.02.2024-0134
引用本文: 李光昱, 戴炜, 黄天麒, 赖堂豪, 吴宗谕. 2.67 L板式表面张力贮箱设计及抗扰动性能仿真[J]. 空间科学学报, 2025, 45(2): 458-467. doi: 10.11728/cjss2025.02.2024-0134
LI Guangyu, DAI Wei, HUANG Tianqi, LAI Tanghao, WU Zongyu. Design and Sloshing Suppression Simulation of 2.67 L Vane-type Surface Tension Tank (in Chinese). Chinese Journal of Space Science, 2025, 45(2): 458-467 doi: 10.11728/cjss2025.02.2024-0134
Citation: LI Guangyu, DAI Wei, HUANG Tianqi, LAI Tanghao, WU Zongyu. Design and Sloshing Suppression Simulation of 2.67 L Vane-type Surface Tension Tank (in Chinese). Chinese Journal of Space Science, 2025, 45(2): 458-467 doi: 10.11728/cjss2025.02.2024-0134

2.67 L板式表面张力贮箱设计及抗扰动性能仿真

doi: 10.11728/cjss2025.02.2024-0134 cstr: 32142.14.cjss.2024-0134
基金项目: 国家自然科学基金项目(52105290, 62373276)资助
详细信息
    作者简介:
    • 李光昱 男, 1988年6月出生于江西省赣州市, 现为南昌航空大学航空宇航学院讲师, 主要研究方向为微重力流体力学、卫星在轨加注技术等. E-mail: lgynudt@sina.com
    通讯作者:
    • 吴宗谕 男, 1991年3月出生于河南省周口市, 现为国防科技大学空天科学学院副教授, 主要研究方向为微重力流体力学、卫星在轨服务技术等. E-mail: wuzongyu@nudt.edu.cn
  • 中图分类号: V432

Design and Sloshing Suppression Simulation of 2.67 L Vane-type Surface Tension Tank

  • 摘要: 板式表面张力贮箱因结构简单、性能良好被广泛应用于各类卫星平台. 本文针对微小卫星平台, 设计了一个2.67 L板式表面张力贮箱及其推进剂管理装置, 介绍了贮箱壳体、蓄液器、导流板和气泡筛网等主要部件的设计过程. 根据平板间的蓄流原理完成了贮箱蓄液器的设计, 得到不同加速度扰动情况下的蓄液体积; 基于内角自流理论对导流板进行几何设计并确定了内外导流板数量; 对气泡筛网进行了选型, 复核了典型工况下气泡筛网泡破点的有效性; 通过CFD仿真, 分析了贮箱在不同填充率、不同加速度扰动情况下的质心变化. 仿真结果表明, 当该贮箱受到10–3g量级加速度扰动时, 贮箱内推进剂质心变化小于10–2 m, 证明本文所设计的2.67 L板式表面张力贮箱具有较强的抗扰动特性.

     

  • 图  1  贮箱壳体(a)及其推进剂管理装置(b)

    Figure  1.  Tank shell (a) and its propellant management device (b)

    图  2  蓄液器工作原理

    Figure  2.  Working principle of propellant reservoir

    图  3  内外导流板贮箱截面

    Figure  3.  Cross section of inner and outer vanes

    图  4  内导流板内角

    Figure  4.  Interior corner created by inner vanes

    图  5  50%充液量受扰动时的液面

    Figure  5.  Surface of the liquid under 50% filling rate

    图  6  90%充液量受扰动时的液面

    Figure  6.  Surface of the liquid under 90% filling rate

    图  7  50%充液量时的质心变化

    Figure  7.  Centroid change under 50% filling rate

    图  8  90%充液量时的质心变化

    Figure  8.  Centroid change under 90% filling rate

    图  9  80%充液量时通过xy平面的质量流率及质心偏移

    Figure  9.  Mass flow rate and centroid change under 80% filling rate in xy plane

    表  1  钛合金材料部分力学性能

    Table  1.   Partial mechanical properties of titanium alloy

    材料牌号屈服强度$ \sigma_{0.2} $/MPa抗拉强度$ \sigma_{\mathrm{b}} $/MPa
    TC4≥870925~1150
    TA1≥250370~530
    下载: 导出CSV

    表  2  无水肼化物特性

    Table  2.   Characteristics of hydrazine

    密度/
    (kg·m–3)
    黏度/
    (mPa·s)
    表面张力/
    (N·m–1)
    接触角/(º)
    10080.9710.06985
    下载: 导出CSV

    表  3  蓄液器的蓄液能力

    Table  3.   Liquid storage capacity of propellant reservoir

    扰动量级/ g0.010.0050.001
    蓄液能力/ mL74.687.4102.6
    下载: 导出CSV

    表  4  仿真工况

    Table  4.   Conditions for simulation

    序号 充液率/(%) 扰动大小/ (m·s–2) 扰动持续时间/s
    1 50 无扰动 4
    2 50 ax=–0.014 4
    3 50 ax=–0.00141 4
    4 50 az=–0.00141 4
    5 50 az=–0.0141 4
    6 80 ax=–0.00141 8.8
    7 90 无扰动 1
    8 90 ax=–0.014 1
    9 90 ax=–0.00141 1
    10 90 az=–0.00141 1
    11 90 az=–0.0141 1
    下载: 导出CSV
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  • 收稿日期:  2024-10-22
  • 修回日期:  2024-12-10
  • 网络出版日期:  2025-01-15

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