现代防御技术 ›› 2024, Vol. 52 ›› Issue (5): 40-50.DOI: 10.3969/j.issn.1009-086x.2024.05.006
收稿日期:2023-10-26
修回日期:2023-11-29
出版日期:2024-10-28
发布日期:2024-11-01
作者简介:唐伟强(1978-),男,广西梧州人。副教授,博士,研究方向为飞行器动力学与控制。
基金资助:Weiqiang TANG, Chengchao JIA, Wenke SHI, Tianpeng XU
Received:2023-10-26
Revised:2023-11-29
Online:2024-10-28
Published:2024-11-01
摘要:
针对高超声速飞行器不确定性问题,提出了一种自抗扰控制与积分滑模控制结合的跟踪策略。通过对高超声速飞行器模型的分析,将其转变为速度子系统和高度子系统,其中速度子系统是典型的一阶系统,高度子系统则由高度环、航迹角环、俯仰角环组成。采用跟踪微分器安排系统的过渡过程,使用扩张状态观测器对系统总扰动进行估计。设计积分滑模控制律代替自抗扰控制中的非线性状态误差反馈控制律。结果表明所设计的跟踪控制策略对不确定性具有很强的鲁棒性,与传统滑模自抗扰控制相比,其在调节时间、跟踪精度和控制信号平滑性方面更有优势。
中图分类号:
唐伟强, 甲成超, 石文科, 许天鹏. 高超声速飞行器积分滑模自抗扰控制研究[J]. 现代防御技术, 2024, 52(5): 40-50.
Weiqiang TANG, Chengchao JIA, Wenke SHI, Tianpeng XU. Research on Integral Sliding Mode Active Disturbance Rejection Control for Hypersonic Vehicles[J]. Modern Defense Technology, 2024, 52(5): 40-50.
| 参数 | 值 | 参数 | 值 | 参数 | 值 |
|---|---|---|---|---|---|
| 0.5 | 0.78 | ||||
| 0.25 | 0.05 | 1 | |||
| 0.001 | 8 | 10 | |||
| 0.01 |
表1 传统滑模自抗扰控制器参数
Table 1 Parameters of traditional sliding mode active disturbance rejection controller
| 参数 | 值 | 参数 | 值 | 参数 | 值 |
|---|---|---|---|---|---|
| 0.5 | 0.78 | ||||
| 0.25 | 0.05 | 1 | |||
| 0.001 | 8 | 10 | |||
| 0.01 |
| 参数 | 值 | 参数 | 值 | 参数 | 值 |
|---|---|---|---|---|---|
| 3 | 200 | 0.05 | |||
| 10 | 400 | 0.05 | |||
| 10 | 600 | 8 | |||
| 10 | 0.5 | 2 | |||
| 0.001 | 0.5 | 10 | |||
| 0.001 | 0.5 | 3 | |||
| 0.001 | 0.5 | 0.000 6 | |||
| 0.001 | 0.5 | 10 | |||
| 400 | 0.5 | 16 | |||
| 800 | 0.05 | 64 | |||
| 8 000 | 0.05 | 2 | |||
| 200 | 0.05 | 100 | |||
| 800 | 0.25 | 0.02 |
表2 积分滑模自抗扰控制器参数
Table 2 Parameters of integral sliding mode active disturbance rejection controller
| 参数 | 值 | 参数 | 值 | 参数 | 值 |
|---|---|---|---|---|---|
| 3 | 200 | 0.05 | |||
| 10 | 400 | 0.05 | |||
| 10 | 600 | 8 | |||
| 10 | 0.5 | 2 | |||
| 0.001 | 0.5 | 10 | |||
| 0.001 | 0.5 | 3 | |||
| 0.001 | 0.5 | 0.000 6 | |||
| 0.001 | 0.5 | 10 | |||
| 400 | 0.5 | 16 | |||
| 800 | 0.05 | 64 | |||
| 8 000 | 0.05 | 2 | |||
| 200 | 0.05 | 100 | |||
| 800 | 0.25 | 0.02 |
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