主纵梁底板倾角对Π型叠合梁涡振特性影响和作用机理的试验研究

EXPERIMENTAL STUDY ON THE EFFECT AND MECHANISM OF THE BOTTOM PLATE TILT ANGLE OF THE MAIN LONGITUDINAL BEAM ON THE VORTEX-INDUCED VIBRATION CHARACTERISTICS OF THE Π-SHAPED COMPOSITE GIRDERS

  • 摘要: 作为典型的钝体断面,Π型叠合梁涡激振动问题特别突出,其主纵梁转角部位的旋涡脱落是诱发桥梁涡激共振的重要原因。为了研究主纵梁底板倾角对Π型叠合梁涡振特性影响和作用机理,通过节段模型静态测压与测振试验,比较研究了不同主纵梁底板倾角下Π型叠合梁涡振响应、平均和脉动风压系数特性。结果表明:在−5°和 0°攻角下,当主纵梁底板倾角为正时,涡振振幅会显著降低,特别当主纵梁底板倾角为20°时能完全抑制对应攻角下的竖弯和扭转涡激振动;主纵梁底板倾角的改变会使得气体流经上表面前缘分离后在中前部发生再附,且会造成主梁上、下表面脉动压力极值点的位置发生改变;主梁模型上、下表面脉动压力值较大,且下表面后部压力脉动变化剧烈,可能是造成主梁模型产生较大涡激振动的主要原因,并且,当脉动压力的主导频率更加分散时,涡激振动会变得更弱。

     

    Abstract: As a typical blunt-body section, the vortex-induced vibration (VIV) problem of Π-shaped composite girders is particularly prominent. The vortex shedding at the corner of the main longitudinal beam is an important cause of VIV in bridges. To study the effect and mechanism of the bottom plate tilt angle of the main longitudinal beam on the VIV characteristics of the Π-shaped composite girders, static pressure tests and vibration tests on a segmental model were conducted. The VIV responses and the average and fluctuating wind pressure coefficient characteristics of the Π-shaped composite beam under different bottom plate tilt angles of the main longitudinal beam were compared and analyzed. The results show that, under the attack angles of −5° and 0°, when the tilt angle of the main longitudinal beam's bottom plate is positive, the VIV amplitude significantly decreases. Especially when the tilt angle is 20°, it completely suppresses the vertical bending and torsional VIVs under the corresponding attack angles. The change in the bottom plate tilt angle causes the airflow to reattach in the middle and front part after the separation at the leading edge of the upper surface, and this also alters the location of the maximum fluctuating pressure on the upper and lower surfaces of the main beam. The larger fluctuating pressures on the upper and lower surfaces of the main beam model and the intense pressure fluctuations at the rear of the lower surface are likely the main reasons for the large VIVs of the main beam model. Additionally, when the dominant frequency of fluctuating pressures becomes more dispersed, the VIV weakens.

     

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