Abstract

The internal blown flap was numerically simulated. Firstly, a parameterization method was developed, which can properly describe the shape of the internal blown flap according to such geometrical parameters as flap chord length, flap deflection, height of blowing slot and its position. Then the reliability of the numerical simulation was validated through comparing the pressure distribution of the CC020-010EJ fundamental generic circulation control airfoil with the computational results and available experiment results. The effects of the geometrical parameters on the aerodynamic performance of the internal blown flap was investigated. The investigation results show that the lift coefficient increases with the increase of flap chord length and flap deflection angle and with the decrease of height of blowing slot and its front position. Lastly, a method of optimal design of the geometrical parameters of the internal blown flap was developed. The design variables include flap chord length, flap deflection, height of blowing slot and its position. The optimal design is based on maximum lift coefficient, the angle of attack of 5 degrees and the design constraint of stall angle of attack of less than 9 degrees. The optimization results show that the optimal design method can apparently raise the lift coefficient of an internal blown flap up to 1.7.

Highlights

  • A parameterization method was developed, which can properly describe the shape of the internal blown flap according to such geometrical parameters as flap chord length, flap deflection, height of blowing slot and its position

  • The reliability of the numerical simulation was validated through comparing the pressure distribution of the CC020⁃010EJ fundamental generic circulation con⁃ trol airfoil with the computational results and available experiment results

  • The investigation results show that the lift coefficient increases with the increase of flap chord length and flap deflection angle and with the decrease of height of blowing slot and its front position

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Summary

Introduction

不变。 吹气缝高度分别为 3,5,7 mm。 图 12a) 为 3 个构型的升力特性对比。 随着吹气缝高度的增大, 升力系数逐渐减小。 吹气缝高度从 3 ~ 7 mm,升力 系数减小了 1.3 左右。 吹气缝高度变化对失速迎角 的影响较大,失速迎角从 9°减小到 3°。 为了保证失 图 15b) 为 1°迎角压力分布对比。 可以看出,吹 气缝位置的变化对主翼压力分布的影响很小。 图 1) 内吹式襟翼参数化方法能够根据几何参数 准确全面地描述内吹式襟翼的气动外形; 2) 内吹式襟翼失速是由主翼尾迹在襟翼上表 面堆积形成的低能量气流随着迎角增大范围逐渐扩 大、流速进一步降低导致的; 3) 襟翼弦长和吹气缝位置对于失速迎角影响 较小,襟翼偏角和吹气缝高度对失速迎角影响较大。 襟翼偏角主要改变了逆压梯度,造成气流能量消耗 的不同,从而影响襟翼上表面的低能量区,继而影响 失速迎角。 吹气缝高度主要改变了吹出气流的速 度,也就是改变了吹气注入的能量,造成襟翼上表面 低能量区的变化,从而改变失速迎角; 4) 襟翼弦长从 20%Cfoil 到 30%Cfoil ,升力系数增 大了 0.5 左右;襟翼偏角从 50°增大到 70°,升力系数 增大了 1.3 左右;吹气缝高度从 3 mm 增大到 7 mm, 升力系数减小了 1.2 左右;吹气缝位置从 0°增大到 20°,升力系数减小了 0.1 左右; 5) 在一定范围内,襟翼弦长、偏角、吹气缝高 度、位置对升力系数影响程度不同。 襟翼偏角和吹 气缝高度对升力系数的影响较大,襟翼弦长的影响 次之,吹气缝位置的影响最小; 6) 内吹式襟翼的优化设计中,襟翼弦长增大了 将近 10%Cfoil ,襟翼偏角增大了 1°,吹气缝位置前移 了 9.8°,接近主翼后缘位置,吹气缝高度几乎不变。 襟翼头部峰值增大,对主翼产生的上洗增强,最终翼 型的升力系数增大了约 1.7。

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