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Numerical Investigation of Ultra-High Lift Coefficient Co-Flow Jet Wing Without Flaps

机译:超高升力系数融流喷射机翼的数值研究,没有襟翼

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Recent advances in 2D Co-Flow Jet (CFJ) flow control airfoil has achieved the super-lift coefficient that exceeds theoretical lift coefficient limit [1]. The super lift coefficient of the 3D finite-span CFJ wing has not yet been investigated. To understand the aerodynamic performance of the finite-span CFJ wing, numerical simulations were conducted at high angles of attack for the takeoff/landing conditions in this paper. This paper applies the Super-Lift 2D CFJ airfoil to 3D finite span wings to investigate the flapless wing performance and the capability of ultra-high lift coefficient generation for takeoff and landing performance. The 3D wings with aspect ratio of 20, 10 and 5 are studied. The Reynolds averaged Navier-Stokcs equations (RANS) are solved with the Spalart-Allmaras (S-A) turbulence model. The fifth-order WENO scheme is used to reconstruct the iuviscid fluxes and a fourth-order central differencing scheme is used to reconstruct the viscous fluxes. The simulations are performed at .Vlarh number of 0.063 and Reynolds number of 3.03 x 10~6. The CFJ wing is generated by the CFJ6421-SST01C-SUC053-INJ009 airfoil, which is designed for the super-lift coefficient. The aspect ratio of CFJ wing of 20, 10, and 5 is studied. The simulations are conducted at the AoA of 25°, 45°, and 70° with the CFJ jet momentum coefficient C_μ of 0.15, 0.2, 0.25 and 0.3. The maximum lift coefficient of C_l = 7.81 is achieved at AoA = 70°, C_μ=0.3 , and aspect ratio of 20. The lift coefficient of CFJ wing is reduced compared to that, of a 2D airfoil, while the drag is increased due to lift induced wingtip vortex. The Oswald efficiency of 3D CFJ wing is much higher than that of the conventional wing with no flow control. It indicates that the penalty of induced drag for 3D CFJ wing is small with decreased aspect ratio even though very high lift coefficient is obtained.
机译:最近的2D共流式喷射(CFJ)流量控制翼型的进展已经实现了超过理论提升系数限制的超级升力系数[1]。尚未研究3D有限跨度CFJ机翼的超级升力系数。要了解有限跨度CFJ机翼的空气动力学性能,本文在起飞/着陆条件的高角度下进行数值模拟。本文将超级升降机2D CFJ翼型应用于3D有限跨度翅膀,以研究飞行和降落性能超高升力系数的浮动机翼性能和能力。研究了具有20,10和5的宽高比的3D翼。随着Spalart-Allmaras(S-A)湍流模型,恢复雷诺瓦斯平均求解了Navier-Stokcs方程(RAN)。第五阶WENO方案用于重建IUVISCID助熔剂,并使用四阶中央差异方案来重建粘性助焊剂。模拟在0.063和雷诺数3.03×10〜6的雷诺数。 CFJ机翼由CFJ6421-SST01C-SUC053-INJ009翼型产生,该翼型设计用于超升力系数。研究了20,10和5的CFJ翼的纵横比。该模拟在25°,45°和70°的AOA下进行,CFJ喷射动量系数C_μ为0.15,0.2,0.25和0.3。 C_L = 7.81的最大提升系数在AOA = 70°,C_μ= 0.3和宽高比为20.与该翼型相比,CFJ机翼的升力系数减小,而2D翼型的升降系数减小,而拖动则增加提升诱导翼状涡旋。 3D CFJ翼的oswald效率远高于传统机翼,没有流量控制。它表明,即使获得了非常高的升力系数,宽度率下降的诱导杆的触控较小。

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