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Aeroelastic Analysis of Hypersonic Aircraft Wing

Dan Xie1,*, Shihao Zhang1, Zijun Yi1

1 Northwestern Polytechnical University, Xi’an, 710072, China

* Corresponding Author: Dan Xie. Email: email

The International Conference on Computational & Experimental Engineering and Sciences 2023, 26(1), 1-1. https://doi.org/10.32604/icces.2023.010490

Abstract

Considering the high cost of numerical simulation for aeroelastic coupling analysis, it is difficult to directly apply it to engineering. In this paper, the typical swept trapezoidal wing of hypersonic aircraft [1] is simplified to a cantilever trapezoidal plate [2]. Based on semi-analytical method [3], including von Karman plate theory to consider the structural geometric nonlinearity, third-order piston theory to calculate quasi steady aerodynamic force, and Rayleigh-Ritz method to characterize the displacement as a mode superposition form, the aeroelastic equation of the swept trapezoidal wing is established, and the fourthorder Runge Kutta numerical integration is used to solve the aeroelastic response, realizing the rapid prediction of the stability boundary. Furthermore, by changing the geometric parameters of the swept trapezoidal wing, including sweep angle, taper ratio and aspect ratio, the effects of wing geometry parameters on aeroelastic response characteristics and flutter critical dynamic pressure are studied.

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Cite This Article

APA Style
Xie, D., Zhang, S., Zijun Yi, (2023). Aeroelastic analysis of hypersonic aircraft wing. The International Conference on Computational & Experimental Engineering and Sciences, 26(1), 1-1. https://doi.org/10.32604/icces.2023.010490
Vancouver Style
Xie D, Zhang S, Zijun Yi . Aeroelastic analysis of hypersonic aircraft wing. Int Conf Comput Exp Eng Sciences . 2023;26(1):1-1 https://doi.org/10.32604/icces.2023.010490
IEEE Style
D. Xie, S. Zhang, and Zijun Yi "Aeroelastic Analysis of Hypersonic Aircraft Wing," Int. Conf. Comput. Exp. Eng. Sciences , vol. 26, no. 1, pp. 1-1. 2023. https://doi.org/10.32604/icces.2023.010490



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