风向对串列双锥形方柱气动力特性和流场的影响

EFFECTS OF WIND DIRECTION ON AERODYNAMIC CHARACTERISTICS AND FLOW FIELD OF TWO TANDEM TAPERED SQUARE CYLINDERS

  • 摘要: 为深入了解风向对串列双锥形方柱气动力特性和流场的影响,开展了雷诺数Re = 2×103,间距比G/D = 4(G为柱心间距,D为方柱边长)的串列双锥形方柱绕流三维大涡模拟(Large Eddy Simulation, LES)研究。全面分析了风向(α = 0°~45°)和锥度化措施(ξ = 0%,5%)对串列双方柱流场形态、气动力和风压分布的影响,从流场角度揭示了气动力变化原因和柱体间干扰机理,建立了风向与气动力系数间的数学关系式。结果表明:根据风向角可将不同锥度下(ξ =0%,5%)中等间距比(G/D = 4)双方柱绕流划分为前角分离(α = 0°)、分离泡(α = 5°, 10°, 15°)和附着流(α = 30°, 45°)流动状态。双方柱平均气动力系数、脉动气动力系数和漩涡脱落频率在流态转变位置处(α = 5°, 15°)会发生突变,在α = 5°处的突变程度更强,且存在最大的脉动特性和漩涡脱落强度,但具有最小的漩涡脱落频率。前角分离流态和分离泡流态下剪切层和尾流漩涡分别会再附和撞击下游方柱表面,附着流流态下柱体间表现出偏向流特点,这是气动力随风向发生变化的根本原因。锥度化措施还会导致剪切层宽度变窄,漩涡脱落的一致性和脉动性显著减弱,进而降低双方柱气动力系数、表面风压强度和漩涡脱落能量,提升漩涡脱落频率。

     

    Abstract: To further understand the effect of wind direction on the aerodynamic forces and flow fields of two tandem tapered square cylinders, three-dimensional (3D) large eddy simulations (LESs) of the flow around the two cylinders with a spacing ratio G/D = 4 (G is the cylinder center-to-center distance and D is the cylinder width) are conducted at Reynolds number (Re) = 2×103. The influence of the wind directions (α = 0°~45°) and tapered modifications (ξ = 0% and 5%) on flow regime, aerodynamic force coefficient and wind pressure distribution are comprehensively analyzed. The flow field is also investigated to reveal the variation and interference mechanism of the aerodynamic forces, then the mathematical relationship between the wind directions and the aerodynamic force coefficients is established. The results indicate that the flow structures can be divided into three flow regimes based on the wind direction: leading-edge separation (α = 0°), separation-bubble (α = 5°, 10°, and 15°) and attached-flow (α = 30° and 45°) regimes. There is an abrupt change in the mean and fluctuating force coefficients, as well as vortex shedding frequency of the two cylinders when the flow regime is transformed. The maximums of the fluctuating force coefficients and the vortex shedding intensity occur at α = 5°, while the vortex shedding frequency is the smallest. The shear layer and the wake vortex reattach on the surface of the downstream cylinder when the flow structures are in the leading-edge separation flow regime. The flow structures exhibit a skew feature in the attached-flow regime, which resulting in the variation in the aerodynamic forces with the wind direction. Meanwhile, the mean and fluctuating force coefficients, wind pressure coefficients, and vortex shedding intensity all decrease with the increase in taper ratio, however the vortex shedding frequency increases. It may be attributed to the narrower shear layer and the weaker periodicity and consistency of the vortex shedding.

     

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