NACA0012低跨声速近地俯仰迟滞特性研究

Research on the hysteresis properties of a pitching NACA0012 airfoil under low transonic ground effect

  • 摘要: 针对电磁助推近地起飞过程中面临的俯仰振动问题,以NACA0012翼型为研究对象,提出了跨声速静态地面效应的分层依据,对比了各分层中的流动模态及气动特性,随后研究了地面效应、减缩频率对俯仰迟滞特性的影响,并分析了迟滞环形态、转向、饱满度变化的原因。结果表明,翼型下方流道收缩比与等熵极限的差值是对地面效应分层及判断流动模态的重要依据。含攻角影响下的跨声速静态地面效应可分为三个层次,依次是呈整体通流的第1层次、呈通流-壅塞交替的第2层次和呈完全壅塞的第3层次。与之相对应,其近地俯仰迟滞特性也呈现出层次性。在第1层地效中,由于地面效应相对较弱,因此迟滞特性与自由空间内相近。在第2层地效中,随着地面效应增强,壅塞效应使得振荡激波S2发生“驻定”或“驻定位置向后缘靠近”,分别导致了迟滞环缩小和整体平移。在第3层地效中,由于壅塞溢流加剧,振荡激波S1/S2在正攻角下差异较大,而在负功角下差异较小,使得迟滞环形态由椭圆状发展为“水滴状”,增大减缩频率能够使迟滞环重新转变为椭圆状。此外,不同层次内的俯仰迟滞特性也呈现出共性特征,如力矩迟滞环都是逆时针转向,升力迟滞环转向与曲线相位的正负变化保持一致,低频俯仰呈现准稳态,而高频俯仰却表现出强迟滞性。

     

    Abstract: This paper proposes a criterion for layering transonic static ground effects based on studying the pitch oscillation encountered in electromagnetic-assisted near-ground takeoff using the NACA0012 airfoil. The flow patterns and aerodynamic characteristics in each layer were analyzed first. Subsequently, the influence of ground effects and reduced frequencies on pitch hysteresis properties was studied, focusing on the mechanism of the variations of hysteresis loop shape, steering, and fullness. The results indicate that the difference between the contraction ratio of the flow channel under the airfoil and the isentropic limit is an important factor for layering ground effects and determining flow patterns. Under the influence of the angle of attack, the transonic static ground effects can be categorized into three layers, the first featuring unblocked flow, the second with alternating unblocked and choked flows, and the third characterized by completely choked flow. Correspondingly, the near-ground pitch hysteresis characteristics also exhibit a hierarchical pattern. In the first layer, the hysteresis properties resemble those in free space due to the relatively weak ground effect. In the second layer, as the ground effect strengthens, the oscillating shock wave S2 subjected to the blockage effects is either stationary or approaches the trailing edge, leading to a reduction and translation of the hysteresis loop, respectively. In the third layer, the intensified congestion and overflow result in significant differences between the oscillating shock waves S1 and S2 at positive angles of attack but less differences at negative angles of attack, transforming the hysteresis loop shape from elliptical to "water droplet". Increasing the reduction frequency can transform the hysteresis loop back into an elliptical shape. Moreover, pitch hysteresis characteristics in different layers share similarities, such as the counterclockwise rotation of the moment hysteresis loops, consistent direction changes in the lift hysteresis loop with the sign of the curve phase, quasi-steady state low-frequency pitching, and strong hysteresis at high-frequency.

     

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