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4:1矩形柱绕流的风攻角和雷诺数效应

THE EFFECTS OF ANGLE OF ATTACK AND REYNOLDS NUMBER ON THE FLOW AROUND A 4:1 RECTANGULAR CYLINDER

  • 摘要: 以宽高比为4:1的矩形柱为对象, 采用大涡模拟(LES)方法, 在风攻角α = 0° ~ 12°、雷诺数Re = 100 ~ 120000范围内, 研究了风攻角α和雷诺数Re联合作用对矩形柱的表面风压、气动力和Strouhal数等气动性能的影响规律, 探究了绕流场流态和转捩点位置的演变过程. 结果表明, 随着风攻角的增加, 平均阻力系数逐渐增大, 脉动升力系数先增大后减小, 而Strouhal数的变化较为复杂; 气动力系数在100 ≤ Re ≤ 1000之间变化剧烈, 而在1000 < Re12000之间则变化较小. 随着风攻角和雷诺数的增加, 矩形柱上壁面会依次呈现“后角分离”、“分离再附”和“前角分离” 3种流态, 下壁面则表现为“后角分离”和“分离再附”两种流态, 流态的变化伴随表面风压、气动力和Strouhal数的突变. 随着雷诺数的增大, 矩形柱绕流场会出现层流、尾流转捩和剪切层转捩等流动现象, 而风攻角会影响发生流动转捩的临界雷诺数; 当Re = 100, 所有攻角的矩形柱绕流均为层流; 当Re = 250, 随着风攻角的增加, 流动依次出现层流涡脱、尾流转捩和剪切层转捩; 当Re = 500, α = 0°时流场发生尾流转捩, 而当α ≥ 3°时则均为剪切层转捩; 当Re ≥ 1000, 所有攻角均发生剪切层转捩现象.

     

    Abstract: This study investigates the aerodynamic performance of a rectangular cylinder with an aspect ratio of 4:1 using the large eddy simulation (LES) method. Within the ranges of angle of attack (α = 0° ~ 12°) and Reynolds number (Re = 100 ~ 120 000). The effects of both parameters on surface pressure, aerodynamic forces, and Strouhal number are systematically examined, together with the evolution of flow patterns and the position of flow transition. The results show that with the increase of the angle of attack, the mean drag coefficient gradually increases, while the fluctuating lift coefficient first increases and then decreases, and the Strouhal number exhibits a complex and irregular variation. When 100 ≤ Re ≤ 1000, the influence of the Reynolds number on aerodynamic force coefficients is pronounced; when 1000 < Re120000, the aerodynamic force coefficient is relatively stable and less sensitive to Re. As angle of attack and Reynolds number increase, the upper-side flow successively exhibits three distinct regimes “trailing-edge separation” “separation–reattachment” and “leading-dege separation”, while the lower-side flow exhibits two regimes, namely “trailing-edge separation” and “separation–reattachment.” The regime transitions are closely associated with abrupt variations in pressure coefficient, aerodynamic force coefficients and Strouhal number. As the Reynolds number increases, the flow around the rectangular cylinder progresses through laminar, wake-transition, and shear-layer-transition regimes, while the angle of attack influences the critical Reynolds number of flow transition. When Re = 100, the flow remains laminar for all angles of attack; when Re = 250, increasing the angle of attack causes the flow to evolve sequentially from laminar vortex shedding to wake transition and then to shear layer transition; when Re = 500, wake transition occurs at α = 0°, whereas shear-layer transition dominates for α ≥ 3°; when Re ≥ 1000, shear-layer transition prevail at all angles of attack.

     

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