考虑近距离海洋下垫面影响的对称风机翼型静气动特性

Static aerodynamic characteristics of symmetrical wind turbine airfoils considering the influence of near-ocean underlying surface

  • 摘要: 为探究海洋下垫面对近海面静态风机翼型气动特性的干扰机理,以NACA 0012对称翼型为研究对象,采用流体体积分数模型构建风浪-翼型耦合场,结合翼型升力系数时频特征和表面流场,分析不同风浪参数、翼型与静水面相对距离下的静气动特征,揭示近距离海洋下垫面对大攻角静态翼型气动特征的干扰机理。研究发现:海洋下垫面通过附加攻角β间接影响近海面翼型气动特性,与风场相比,风浪场中翼型的静态失速攻角减小,其减小量取决附加攻角平均值;海洋下垫面对翼型各流动阶段均存在干扰,但显著抑制了大攻角翼型涡的发展,导致前缘漂移涡与尾缘脱落涡发展的机制存在差异,前者是由海洋下垫面干扰引起的长周期高强度漂移现象,后者是由大攻角翼型自身的流动分离特性主导,表现为短周期低强度脱落,且风浪场翼型尾涡脱落频率均小于风场翼型的涡脱频率(0.537 Hz);翼型距静水面30 m时,海洋下垫面的干扰效应显著减弱,出现独立的尾缘涡脱落频率0.43 Hz,且涡形态更复杂。本文研究对提高大型浮式风机安全性能具有一定的借鉴意义。

     

    Abstract: This paper presents a numerical investigation of the effects of the ocean underlying surface (OUS) on the static aerodynamic characteristics of a symmetric airfoil ‌NACA 0012‌ near the sea surface utilizing the ‌Volume of Fluid (VOF)‌ model. The interference of OUS on the static aerodynamic characteristics of ‌NACA 0012‌ is studied thoroughly by examining the time-frequency characteristics of lift coefficients and flow field characteristics under different ‌wind-wave environments‌. Results show that the interference exerted by OUS originates from the additional ‌angle of attack (AoA)‌. ‌Root mean square (RMS)‌ values of the airfoil lift coefficients and the additional ‌AoA‌ exhibit a similar variation trend with wave height and wind speed. The airfoil’s static stall ‌AoA‌ in the ‌wind-wave field‌ is smaller than in the wind field, with the decrement depending on the average value of the additional ‌AoA‌. The interference of OUS persists throughout all flow stages of the airfoil, but it only significantly suppresses the development of airfoil vortices at high ‌AoA‌, leading to different development mechanisms of leading edge drift vortices and trailing edge shedding vortices. The former is a long-period (‌4.5 s wave period‌), high-intensity drift disturbed by OUS, while the latter is a short-period, low-intensity shedding induced by the flow separation around the high-‌AoA‌ airfoil itself. Notably, the shedding frequency of the trailing edge vortices in the wind wave field is lower than that in the wind field by 0.537 Hz. When the airfoil is positioned 30 meters above the ‌still water surface‌, an independent trailing edge vortex shedding frequency of 0.43 Hz appears, accompanied by a more ‌complex‌ vortex shape. The findings of this study will shed light on improving the safety performance of large floating wind turbines.

     

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