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Transitory behavior of a finite span synthetic jet

机译:有限跨度合成射流的瞬态行为

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The transitory behavior of a finite span synthetic jet, following the onset of a (pulse) input signal, was investigated and characterized using hot-wire anemometry and particle image velocimetry techniques. Measurements were performed in two planes: along the centerline of the synthetic jet slit (x-z plane) and across the jet slit (x-y plane) with varying stroke lengths and Reynolds numbers. The synthetic jet parameter matrix included actuation frequencies (f(act)) of 300 and 917 Hz, stroke lengths from 16 to 50 times the slit width, and Reynolds numbers (based on the averaged orifice velocity) between 85 and 364. The transitory evolution of the synthetic jet consists of four stages: (1) in the x-y plane, the lead vortex pair advects downstream without spreading in the cross-stream direction while in the x-z plane, two vortices with opposite senses are formed (one on each end of the slit edge); (2) the vortex pair in the x-y plane moves in the cross-stream and streamwise directions, while the edge-vortices in the x-z plane move downstream and towards the center of the jet to form an array of vorticity concentrations of opposite sense; (3) accumulation of consecutive vortex pairs in the x-y plane, while in the x-z plane, consecutive pairs of the edge vortices propagate downstream and merge with the previous vortices, resulting in a three-dimensional vortex line; and (4) the combined leading vortex pair (in the x-y plane) detaches and moves downstream while the main jet penetrates through the leading vortex pair. During this time period the vortex lines (in the x-z plane) have a higher velocity in the center than the sides. Similar transitory behavior was observed for different stroke lengths, where as the stroke length increases the transient time decreases. Moreover, the spanwise vorticity concentrations lose their coherence as the stroke length increases. (c) 2007 American Institute of Physics.
机译:使用热线风速仪和粒子图像测速技术研究了有限跨距合成射流在(脉冲)输入信号出现后的瞬态行为并进行了表征。在两个平面上进行测量:沿着合成射流狭缝的中心线(x-z平面)和横跨射流狭缝(x-y平面),具有不同的行程长度和雷诺数。合成射流参数矩阵包括300和917 Hz的致动频率(f(act)),行程宽度为缝隙宽度的16至50倍以及雷诺数(基于平均孔速)在85至364之间。的合成射流由四个阶段组成:(1)在xy平面上,铅涡流向下游平流而没有在横流方向上扩散,而在xz平面上,形成了两个具有相反方向的涡流(在每个方向上狭缝边缘); (2)x-y平面中的涡流沿横流和水流方向移动,而x-z平面中的边缘涡流向下游并向射流中心移动,从而形成一系列相反方向的涡度集中度; (3)x-y平面中连续涡旋对的积累,而在x-z平面中,边缘涡旋的连续对向下游传播并与先前的涡流合并,从而形成三维涡旋线; (4)当主射流穿过前涡流对时,组合的前涡流对(在x-y平面内)分离并向下游移动。在这段时间内,涡流线(在x-z平面上)在中心的速度高于侧面的速度。对于不同的冲程长度,观察到了类似的瞬态行为,其中,随着冲程长度的增加,瞬态时间减少。此外,随着冲程长度的增加,翼展方向的涡度浓度会失去其连贯性。 (c)2007年美国物理研究所。

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