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Force and flow structures of a wing performing flapping motion at low Reynolds number

机译:在低雷诺数下执行拍打运动的机翼的力和流结构

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摘要

Aerodynamic force and flow structures of a wing performing a simplified flapping motion that emulates the wing motion of small insects in normal hovering flight are studied, using the method of numerically solving the Navier-Stokes equations. For a typical case (wing rotation-axis is at 0.25 chord position and wing rotation is symmetrical with respect to stroke reversal), large peaks inC L andC D are produced near the end of a stroke by the wing-rotation, but the wing-rotation also generates a vortical structure which induces strong downwash velocity, reducing the lift production in the early part of the following stroke; averaging over one flapping cycle,C L is 28% larger than the steady-state value and is about that needed to support the weight of a small insect. The timing of the wing-rotation at stroke reversal can change the size of the peaks inC L andC D and their averages; e.g. in the case of shifting the wing-rotation forward in time by 7.5% of a stroke period, the averageC L becomes 63% larger than the steady-state value, which is larger than that needed for weight supporting (and might provide extra force for control or maneuvers). When the rotation-axis is moved rearward to the middlechord position, the lift and drag peaks due to the wing-rotation become smaller, and in this case, the wing-rotation generates a vortical structure that tends to prevent the relative motion between positive and negative vorticities, also reducing the lift production in the early part of the following stroke, resulting in a smaller averageC L .
机译:使用数值求解Navier-Stokes方程的方法,研究了机翼的气动力和流动结构,该机翼执行了简化的扑翼运动,模仿了小昆虫在正常盘旋飞行中的机翼运动。在典型情况下(机翼旋转轴位于0.25弦位置,机翼旋转相对于冲程反转对称),在冲程接近终点时,C L 和C D 会出现较大的峰值。机翼旋转,但机翼旋转也会产生涡旋结构,从而引起强劲的下冲速度,从而在下一个行程的早期减少升力的产生;平均在一个扑动周期中,C L 比稳态值大28%,大约是支撑小昆虫重量所需的值。冲程反转时机翼旋转的时间会改变C L 和C D 的峰值大小及其平均值。例如在机翼旋转时间按冲程周期的7.5%向前移动的情况下,平均C L 比稳态值大63%,稳态值大于重量支撑所需的稳态值(并且可能为控制或操纵提供额外的力量)。当旋转轴向后移动到中弦位置时,由于机翼旋转而引起的升力和阻力峰值变小,在这种情况下,机翼旋转会产生涡旋结构,该结构倾向于防止正向和反向之间的相对运动。负涡度也降低了下一个中风早期的升力产生,导致平均C L 减小。

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  • 来源
    《Acta Mechanica》 |2001年第4期|35-48|共14页
  • 作者

    J. Tang; M. Sun;

  • 作者单位

    Institute of Fluid Mechanics Beijing University of Aeronautics Astronautics;

    Institute of Fluid Mechanics Beijing University of Aeronautics Astronautics;

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  • 正文语种 eng
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