Optimization of take-off rotation process considering tail striking dynamic limit angle
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摘要:
为防止擦机尾的发生,同时优化起飞抬轮过程,将抬轮过程中擦机尾角的变化考虑在内,建立计算飞机俯仰角、机尾离地高度等性能参数的抬轮阶段动力学模型。以波音737-800为例,探究抬轮速率变化对抬轮段距离的影响,对比擦机尾动态限制角和擦机尾固定限制角这2种抬轮方式的差异,分析动态限制角的优势。结果表明:大多数情况下,该机型最优抬轮速率范围为2.5~3.0 (°)/s。总体而言,相比于固定限制角,使用动态限制角的抬轮段距离减小约10%,从抬轮到离地的时间缩短约10%。对有关后机身长度和起落架高度的飞机设计提出建议,即后机身长度的选取与起落架高度应是相匹配的,选取比值约为5.0,若采用擦机尾动态限制角抬轮方式,比值应略微增大。研究结果可为飞行员提供抬轮操作参考,改善飞机的起飞性能,在防止擦机尾的同时,提高飞机载重。
Abstract:In order to prevent the occurrence of tail striking and optimize the take-off rotation process, this paper established a dynamic model of rotation to calculate the performance parameters such as pitch angle of the aircraft and tail ground clearance, taking into account the change of the tail striking angle during the rotation process. Using the Boeing 737-800 as an example, this study examined how the rotation rate affected the rotation distance, contrasted the tail striking dynamic limit angle with the tail striking fixed limit angle, and examined the benefits of the latter. The results show that in most cases, the optimal rotation rate ranges from 2.5 to 3.0 (°)/s. In comparison to the tail striking fixed limit angle, the rotation distance and lift-to-lift-off time are reduced by approximately 10% and 10%, respectively, with the tail striking dynamic limit angle. Finally, it is suggested that the ratio of the length of the rear fuselage to the length of the landing gear should be about 5.0, and that the ratio should be increased slightly if the tail striking dynamic limit angle is used. This study can provide pilots with a reference, improve the take-off performance of the aircraft, and increase the load of the aircraft while preventing tail striking.
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Key words:
- air transportation /
- take-off performance /
- tail striking /
- rotation rate /
- dynamic limit angle
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表 1 机型参数
Table 1. Aircraft parameters
飞机质量/kg 机翼面积/m2 标准抬轮速率/((°)·s−1) 后机身长度/m 起落架初始高度/cm 完全压缩后起落架高度/cm 压缩率/10−5(cm·N−1) 67 000 124.5 3 700 136 112 3 表 2 H=0 m,T=0 ℃, 不同抬轮速率下起飞性能参数变化
Table 2. H=0 m,T=0 ℃, variation of relevant parameters at different rotation speeds
距离抬轮
开始的时间/s$ \theta $/(°) $ {C}_{L} $ $ D $/N $ {F}_{\text{V}} $/N VR=
2.7 (°)/sVR=
3.1 (°)/sVR=
3.4 (°)/sVR=
2.7 (°)/sVR=
3.1 (°)/sVR=
3.4 (°)/sVR=
2.7 (°)/sVR=
3.1 (°)/sVR=
3.4 (°)/sVR=
2.7 (°)/sVR=
3.1 (°)/sVR=
3.4 (°)/s0 0 0 0 0.350 0.350 0.350 28371 28371 28371 0 0 0 0.5 1.35 1.55 1.70 0.519 0.544 0.563 29958 30259 30485 4551 5225 5731 1 2.70 3.10 3.40 0.677 0.721 0.754 32923 33644 34328 9099 10446 11456 1.5 4.05 4.65 5.10 0.825 0.888 0.936 36964 38309 39620 13643 15660 17171 2 5.40 6.20 6.80 0.967 1.051 1.114 41837 44646 46980 18179 20862 22872 2.5 6.75 7.75 8.50 1.109 1.214 1.290 48174 52972 56743 22704 26049 28552 3 8.10 9.04 9.04 1.250 1.344 1.344 56379 61535 61448 27217 30351 30351 表 3 不同标高、不同温度的离地参数
Table 3. Ground clearance parameters at different elevations and temperature
抬轮速率/((°)·s−1) 从抬轮到离地时间/s 速率×时间 $ H $=0 m,$ T $=0 ℃ $ H $= 1000 m, $ T $=15 ℃$ H $= 2000 m, $ T $=20℃$ H $=0 m, $ T $=0 ℃ $ H $= 1000 m, $ T $=15 ℃$ H $= 2000 m, $ T $=20 ℃2.3 3.91 8.98 2.4 3.80 9.11 2.5 3.56 3.81 8.91 9.51 2.6 3.46 3.83 9.01 9.95 2.7 3.27 3.38 3.85 8.83 9.13 10.39 2.8 3.18 3.35 3.87 8.90 9.38 10.82 2.9 3.09 3.37 3.88 8.96 9.77 11.26 3 3.03 3.38 3.90 9.08 10.15 11.70 3.1 2.99 3.40 3.91 9.28 10.53 12.12 3.2 3.00 3.41 9.60 10.91 3.3 3.01 3.42 9.93 11.28 3.4 3.02 10.26 -
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