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

机译:两个串联Bluff机构上的相位滞后引起的波动力

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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 Φcan 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:进行了雷诺数Re = 200的数值模拟,以发现两个串联圆柱体上的流致力如何与圆柱体涡流脱落之间的相位滞后联系起来。间距比L〜*(= L / D)在2到9之间变化,其中L是圆柱体中心距,D是圆柱体直径。在这里,我们主要关注上游汽缸的升力系数C_(Lf)的波动,汽缸之间间隙中的涡旋动力学以及两个汽缸的涡流脱落之间的相位滞后Φ(对于L〜*大于共同脱落的临界值)流占上风。 Φ确实是L〜*,斯特劳哈尔数(St)和圆柱体之间间隙中的涡流对流速度的非线性函数。我们发现上游气缸C_(Lf)受L〜*和Φ的影响。虽然L〜*对C_(Lf)的贡献随着L〜*迅速减少,但Φ的贡献使依赖L〜*的C_(Lf)变化衰减正弦曲线,并保持在所检查的L〜*范围内。同相和反相流动分别对应于局部最大值和最小值C_(Lf)。 C_(Lf)与L〜*和Φ的关系可以推导为C_(Lf)= Ae〜(-αL〜*)+ Be〜(-βL〜*)sin(Φ+π/ 2)+ C,其中A,α,B,β和C是常数。讨论了C_(Lf)中阻尼正弦变化背后的物理学。

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