Acta Aeronautica et Astronautica Sinica ›› 2023, Vol. 44 ›› Issue (21): 528665-528665.doi: 10.7527/S1000-6893.2023.28665
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Yongjie ZHANG1, Bo CUI1(), Mingzhen WANG2, Chuzhe ZHANG2, Linyin LUO3, Xiangming CHEN4, Xiaochuan LIU4
Received:
2023-03-08
Revised:
2023-05-06
Accepted:
2023-06-19
Online:
2023-11-15
Published:
2023-06-21
Contact:
Bo CUI
E-mail:cuibo0112@mail.nwpu.edu.cn
Supported by:
CLC Number:
Yongjie ZHANG, Bo CUI, Mingzhen WANG, Chuzhe ZHANG, Linyin LUO, Xiangming CHEN, Xiaochuan LIU. Research progress of amphibious aircraft water landing test and theoretical analysis methods[J]. Acta Aeronautica et Astronautica Sinica, 2023, 44(21): 528665-528665.
Table 1
Some typical water landing tests
结构尺度 | 文献 | 水面状态 | 模型设计 | 释放设备形式 | 入水速度/( | 入水角度 | 结构响应 |
---|---|---|---|---|---|---|---|
材料 | Battley等[ | 直径3.5 m,水深1.5 m的圆柱形水池 | 复合材料三明治结构板 | SSTS系统 | 0.5~6 | 10°~40° | 入水时龙骨处应变先增大,后保持恒定;舷处应变在板件入水时并未增加,在板件入水一半时迅速上升。 |
Huera-Huarrte等[ | 40 m×1.09 m×0.61 m的水池 | 复合夹芯板 | SITS系统 | 3.38~5.17 | 0.3°~25° | 当板件与水面开始接触,总力迅速增加,直到板件被彻底淹没,此时总力达到最大值。 | |
Battley和Allen[ | 直径1.4 m水深3.5 m的圆柱形水池 | 复合夹芯板 | SSTS系统 | 1~8 | 0°~40° | 面板柔韧性对总力有影响,特别是低刚度面板具有较高的峰值力。 | |
Hassoon等[ | 3 m×2 m×2 m的水池 | 复合夹芯板 | 伺服坠撞系统 | 4~10 | 垂直入水,斜升角10° | 损坏首先出现在夹紧区域的面板末端,并向中心扩展。中心剪切损伤导致弯曲强度降低,并增加沿界面的法向应力和剪切应力, | |
Hassoon等[ | 3 m×2 m×2 m的水池 | 复合夹芯板 | 伺服坠撞系统 | 4~10 | 垂直入水,斜升角10° | 弹性板比刚性板的峰值载荷更大,弹性板具有显著的动态噪声问题。 | |
组件 | Xie等[ | 150 m×7.5 m×3.5 m的水池 | 复合材料船体截面 | 自由下落系统 | 2.01~3.42 | 垂直入水 | 船体截面入水瞬间应力达到最大值,速度显著降低,之后速度出现高频振荡。 |
部件 | Lin和Shieh[ | 20 m×0.8 m×0.6 m的波浪水池 | 平底船体 | 自由下落系统 | 0.44~1.98 | 由圆筒安装角度确定 | 当平底接触水面时,水花会在平底周围飞溅出来。同时,气泡在边缘附近形成。 |
Yettou等[ | 30 m×2 m×1 m的水池 | 楔形体结构 | 自由下落系统 | 4.43~5.05 | 垂直入水,斜升角为15°~35° | 两种不同的下降高度的楔形体在撞击水面时,楔形体速度均在撞击后迅速减小,两条曲线趋向于融合成一条单一的曲线。 | |
Panciroli等[ | 0.8 m×0.32 m ×0.32 m的水池 | 曲面楔形体结构 | 自由下落系统 | 2.21~4.43 | 垂直入水 | 在结构入水过程中,运动物体的动能很大一部分会转化为自由液面抬升所产生的势能以及自由面飞溅的动能部分。 | |
Anghileri等[ | 直径8 m、深1.1 m的水池 | 楔形体 | 自由下落系统 | 4.3~8.6 | 垂直入水 | 在冲击减速和压力方面的试验的可重复性证实了测试和收集数据的可靠性。 | |
褚林塘等[ | 平静水面 | 楔形体 | 自由下落系统 | 3~4 | 垂直入水 | 楔形体着水冲击载荷大小与楔形体重量及入水速度正相关,带舭弯的楔形体模型相较无舭弯模型对速度及重量变化更加敏感。 | |
唐彬彬等[ | 510 m×6.5 m×5 m的水池 | 单船身模型 | 拖曳水池试验 | 0.17~0.75倍离水速度 | 纵倾角5°和4.3° | 增加鳍式浮筒安装高度改善水面滑行稳定性,减小了水面滑行中水阻力。 | |
Fisher[ | 平静水面 | 加装水橇结构的飞机 | 滑轨弹射 | 36.6~49.2 | 2°~10° | 水橇可在多种入水姿态下显著降低飞机入水冲击时所受的压力。 | |
高霄鹏等[ | 平静水面 | 加装水橇结构的飞机 | 拖曳水池试验 | 垂向速度0.7,有水平速度 | 6° | 船身中部先触水,随后艏部与水接触受到冲击力迅速抬起,机身脱离水面一小段距离,随后落下。 | |
整机 | 王明振等[ | 平静水面 | 某型水陆两栖飞机缩比模型 | 拖行后释放 | 模型垂向速度1,有水平速度 | 5°~7° | 模型姿态出现先小幅低头后大幅抬头的趋势。 |
黄淼等[ | 平静水面 | 某型水陆两栖飞机缩比模型 | 拖曳水池试验 | 离水速度 | 平均为4.93° | 飞机滑行起飞过程中,随速度增加参与滑水的船体面积减小,水阻力减小 | |
焦俊等[ | 开阔自然水域,未测浪高 | 框架结构,复合材料蒙皮 | 自由飞 | 与实机对应 | 7° | 着水瞬间出现较大压力,着水滑行阶段因水上跳跃而出现二次峰值。 | |
Guo等[ | 开阔水域 | 某型水陆两栖飞机缩比模型 | 自主起飞 | 2~14 | 未提及 | 随着模型速度的增加,水体逐渐与断阶分离,在断阶后面形成充满空气的空腔。 |
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