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凹/凸处理后平板绕流特性的数值模拟研究

NUMERICAL SIMULATION STUDY ON THE FLOW CHARACTERISTICS AROUND FLAT PLATES WITH CONCAVE/CONVEX TREATMENT

  • 摘要: 采用数值模拟方法,在雷诺数("Re=ρ" "U" _"0" "D/?" ,其中"ρ" 为流体密度,"U" _"0" 为来流速度,D为平板特征长度,"?" 为流体的动力粘度)为26400时,研究了18组不同凹/凸程度平板的绕流特性,分析了凹/凸平板的平均阻力系数("C" _"D,mean" )、脉动升力系数("C" _"L,rms" )和斯托罗哈数(Strouhal number,用St表示)随凹/凸程度变化的规律,从壁面压力和流场角度剖析了气动特性变化的机理。结果表明:对矩形平板两侧纵边进行凹/凸处理可改变其流场与气动力特性。凸处理时,随着平板上凸程度的增加,其平均阻力系数逐渐减小,脉动升力系数呈先减小后增大再减小的趋势,斯托罗哈数呈逐渐增大趋势,凸处理后平板的平均阻力系数与脉动升力系数均小于矩形平板的基准数值,当上凸高度与矩形宽度之比(H*/D)为0.15时,凸平板的脉动升力系数最小,约为0.005,相较于矩形平板降幅达99.2%,几乎完全抑制了升力脉动。凹处理时,随着平板下凹程度的增加,其平均阻力系数与脉动升力系数均呈现先增大再减小的趋势,但斯托罗哈数未出现明显变化,凹处理后平板的平均阻力系数与脉动升力系数均大于矩形平板的对应值,平均阻力系数在下凹高度与矩形宽度之比为0.25时达到峰值1.278,涨幅达20.2%;凹平板的脉动升力系数在凹进高度与矩形宽度之比为0.35时达到峰值1.273,涨幅达102%。

     

    Abstract: The flow characteristics around 18 different flat plates with varying degrees of surface roughness were studied at a Reynolds number (The Reynolds number (Re) is defined as "Re=ρ" "U" _"0" "D/?" , where "ρ" represents the fluid density, "U" _"0" denotes the approach velocity of the fluid, D is the characteristic dimension of the flat plate, and "?" signifies the dynamic viscosity of the fluid) of 26,400 using numerical simulation methods. The study analyzed how the average drag coefficient("C" _"D,mean" ), fluctuating lift coefficient("C" _"L,rms" ), and Strouhal number (St) of both convex and concave plates varied with the degree of convexity and concavity. Additionally, the aerodynamic mechanisms behind these variations were examined from the perspectives of wall pressure and flow field. The results show that altering the longitudinal edges of a rectangular plate with either convex or concave modifications can change its flow field and aerodynamic characteristics. When convex modifications are applied, as the degree of convexity on the plate increases, the average drag coefficient gradually decreases, while the fluctuating lift coefficient initially decreases, then increases, and finally decreases again. The Strouhal number shows a gradual increase. After convex modification, both the average drag coefficient and the fluctuating lift coefficient of the plate are lower than the baseline values of the rectangular plate. When the ratio of the protrusion height to the plate width (H*/D) is 0.15, the fluctuating lift coefficient of the convex plate reaches its minimum value of approximately 0.005, representing a 99.2% reduction compared to the rectangular plate and nearly completely suppressing lift fluctuations. When concave modifications are applied, as the degree of concavity on the plate increases, both the average drag coefficient and the fluctuating lift coefficient initially increase and then decrease. However, the Strouhal number does not show significant changes. After concave modification, both the average drag coefficient and the fluctuating lift coefficient of the plate are higher than the corresponding values for the rectangular plate. The average drag coefficient peaks at 1.278 when the ratio of concave height to plate width is 0.25, representing a 20.2% increase. The fluctuating lift coefficient peaks at 1.273 when the ratio of concave height to plate width is 0.35, showing a 102% increase.

     

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