移动孤立波的风场特性及对薄平板抖振响应的影响

WIND FIELD CHARACTERISTICS OF MOVING SOLITARY WAVE AND ITS EFFECTS ON BUFFETING RESPONSE OF THIN PLATES

  • 摘要: 为研究极端风浪环境下风浪之间的相互作用对跨海桥梁抖振响应影响,基于CDRFG方法生成LES入口紊流,以薄平板为研究对象,采用移动孤立波模拟极端波浪,分析了不同净空高度下有孤立波与无孤立波对薄平板的绕流场、气动力以及抖振响应的影响,并结合理论方法等手段探究了其影响机理。结果表明:孤立波会对2.5倍波高范围的风速以及4.5倍波高范围的湍流强度有明显的遮蔽效应,使风速变小、湍流强度增加。当孤立波在薄平板上游移动时,波峰位置处产生的旋涡脱落会改变薄平板周围的流场和脉动能量分布,此时薄平板气动力的主导频率相对无孤立波时有明显改变;同时薄平板振动幅值显著增大,振动能量主要集中于薄平板自振频率附近,且净空高度越低,上述现象越明显。当孤立波移动到薄平板下游时,不同净空高度下薄平板周围的旋涡尺度较小、能量较低,薄平板气动力的主导频率与无孤立波时较一致;此时薄平板横向位移由于薄平板扭转角达到峰值而继续增大,但随着孤立波远离薄平板,各方向的振动幅值均逐渐下降。

     

    Abstract: To study the effects of the interaction between the wind and wave on the buffeting response of coastal bridges in extreme wind and wave environments, the CDRFG method was used to generate the inlet turbulence of the LES. A thin plate was taken as the research object, and a moving solitary wave was used to simulate the extreme wave. Then, the effects of presence or absence of the solitary wave on the flow field, on aerodynamic forces, and on buffeting response of the thin plate were analyzed at different clearance heights. Also, the impact mechanisms were explored through theoretical methods and other means. The results indicate that the solitary wave has significant shielding effects on wind speeds and turbulence intensities in the range of 2.5 times and 4.5 times the wave height, respectively, resulting in a decrease in wind speeds and an increase in turbulence intensities. When the solitary wave propagates upstream along the thin flat plate, the vortex shedding generated at the peak position of the solitary wave will change the flow field and fluctuating energy distribution around the thin plate, and the dominant frequencies of the aerodynamic forces of the thin plate are significantly changed, compared with those with the absence of the solitary wave. At the same time, vibration amplitudes of the thin plate increase significantly, and the vibration energy is mainly concentrated near the natural frequencies of the thin plate. The lower the clearance height, the more obvious the above phenomena. When the solitary wave propagates downstream along the thin plate, the vortex scales around the thin plate at different clearance heights are smaller and the energy is lower, and the dominant frequencies of the aerodynamic forces of the thin plate are consistent with those without the solitary wave. At this point, the lateral displacement of the thin plate continues to increase due to the peak torsional angle of the thin plate reaching the peak value, but as the solitary wave moves far from the thin plate, the vibration amplitudes in all directions gradually decrease.

     

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