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STUDY ON THE RELATION BETWEEN SIDE RATIOS OF RECTANGULAR CROSS SECTIONS AND SECONDARY VORTICES AT TRAILING EDGE IN MOTION-INDUCED VORTEX EXCITATION

机译:运动诱发涡激激励中矩形截面的边比与尾端二次涡关系的研究

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According to the results of conventional wind tunnel tests on rectangular cross sections with side ratios of B/D=2-8 (B: along-wind length (m), D: cross-wind length (m)), motion-induced vortex excitation was confirmed. The generation of motion-induced vortex excitation is considered to be caused by the unification of separated vortices from the leading edge and secondary vortices at the trailing edge [1]. Spring-supported test for B/D=1.18 was conducted in a closed circuit wind tunnel (cross section: 1.8 m high×0.9 m wide) at Kyushu Institute of Technology. Vibrations were confirmed in the neighborhoods of reduced wind speeds Vr=V/fD=2 and Vr=8 (V: wind speed (m/s), f: natural frequency (Hz)). Because the reduced wind speed in motion-induced vortex excitation is calculated as Vr=1.67×B/D=l.67×1.18=2.0 [1], vibrations around Vr=2 were considered to be motion-induced vortex excitation. According to the smoke flow visualization result for B/D=1.18 which was carried out by the authors, no secondary vortices at the trailing edge were formed, although separated vortices from the leading edge were formed at the time of oscillation at the onset wind speed of motion-induced vortex excitation, where aerodynamic vibrations considered to be motion-induced vortex excitation were confirmed. It was suggested that motion-induced vortex excitation might possibly occur in the range of low wind speeds, even in the case of side ratios where secondary vortices at trailing edge were not confirmed.
机译:根据常规风洞试验的结果,矩形截面的边比为B / D = 2-8(B:沿风向长度(m),D:沿风向长度(m)),运动引起的涡流激发被确认。运动引起的涡旋激励的产生被认为是由于从前缘分离的涡旋和在后缘的次级涡旋统一造成的[1]。 B / D = 1.18的弹簧支撑试验是在九州技术学院的封闭式风洞(横截面:1.8 m高×0.9 m宽)中进行的。在降低的风速Vr = V / fD = 2和Vr = 8(V:风速(m / s),f:自然频率(Hz))附近确认振动。因为在运动引起的涡旋激励中降低的风速被计算为Vr = 1.67×B / D = 1.67×1.18 = 2.0 [1],所以将Vr = 2附近的振动视为运动引起的涡旋激励。根据作者针对B / D = 1.18进行的烟流可视化结果,尽管在起始风速振荡时与前缘形成了分离的涡流,但在后缘没有形成次级涡流。运动引起的涡流激励的原理,其中空气动力学振动被认为是运动引起的涡流激励。建议在低风速范围内可能发生运动引起的涡旋激励,即使在边比没有确定后缘的二次涡旋的情况下也是如此。

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