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PHASE-LAG-INDUCED FLUCTUATING LIFT FORCES ON TWO TANDEM BLUFF BODIES

机译:相位滞后诱导的两个串联虚张体的波动升力力

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A numerical simulation at a Reynolds number Re = 200 is conducted to find how flow-induced forces on two tandem circular cylinders is connected to the phase lag between vortex sheddings from the cylinders. The spacing ratio L~* (= L/D) is varied from 2 to 9, where L is the cylinder center-to-center spacing and D is the cylinder diameter. Here we mainly focus on fluctuating lift coefficient C_(Lf) of the upstream cylinder, vortex dynamics in the gap between cylinders, and phase lag Φ between the vortex sheddings from the two cylinders for L~* larger than the critical where the co-shedding flow prevails. Φ is indeed nonlinear function of L~*, Strouhal number (St) and convection velocity of vortices in the gap between the cylinders. We unearth that the upstream cylinder C_(Lf) is affected by both L~* and Φ. While the contribution of L~* to C_(Lf) diminishes rapidly with L~*, that of Φ makes the L~*-dependent C_(Lf) variation damped-sinusoidal, persisting in the L~* range examined. The inphase and antiphase flows respectively correspond to a local maximum and minimum C_(Lf). How C_(Lf) is correlated with L~* and Φ can be deduced as, C_(Lf) = Ae~(-αL~*) + Be~(-βL~*) sin(Φ + π/2) + C, where A, α, B, β and C are constants. The physics behind the damped-sinusoidal variation in C_(Lf) is discussed.
机译:进行雷诺数Re = 200的数值模拟,以找到两个串联圆柱上的流动引起的力与来自汽缸的涡流剪线之间的相位滞后。间距比L〜*(= L / D)从2到9变化,其中L是气缸中心到中心间距,D是圆柱体直径。在这里,我们主要关注上游圆筒的波动升力系数C_(LF),涡旋动力学在气缸之间的间隙中,以及来自两个气缸的涡旋剪线之间的涡流φ大于共同脱落的关键流动普遍存在。 φ确实是L〜*,Strouhal数(ST)的非线性函数和圆柱之间间隙中的涡流的对流速度。我们无法通过L〜*和φ的影响,上游气缸C_(LF)受到影响。虽然L〜*至C_(LF)的贡献随着L〜*迅速减少,而φ的φ使L〜* - 依赖性C_(LF)变化阻尼正弦,持续存在于L〜*范围内。同位和反相流分别对应于局部最大值和最小C_(LF)。 C_(LF)如何与L〜*,φ可以推导为,C_(LF)= AE〜(-αL〜*)+是〜(-βL〜*)SIN(φ+π/ 2)+ C. ,其中A,α,B,β和C是常数。讨论了C_(LF)的阻尼正弦变化背后的物理。

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