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U-shaped fairings suppress vortex-induced vibrations for cylinders in cross-flow

机译:U形整流罩抑制了横流中气缸引起的涡流引起的振动

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摘要

We employ three-dimensional direct and large-eddy numerical simulations of the vibrations and flow past cylinders fitted with free-to-rotate U-shaped fairings placed in a cross-flow at Reynolds number 100 ⩽ Re ⩽ 10,000. Such fairings are nearly neutrally buoyant devices fitted along the axis of long circular risers to suppress vortex-induced vibrations (VIVs). We consider three different geometric configurations: a homogeneous fairing, and two configurations (denoted A and AB) involving a gap between adjacent segments. For the latter two cases, we investigate the effect of the gap on the hydrodynamic force coefficients and the translational and rotational motions of the system. For all configurations, as the Reynolds number increases beyond 500, both the lift and drag coefficients decrease. Compared to a plain cylinder, a homogeneous fairing system (no gaps) can help reduce the drag force coefficient by 15 % for reduced velocity U* = 4.65, while a type A gap system can reduce the drag force coefficient by almost 50 % for reduced velocity U* = 3.5, 4.65, 6, and, correspondingly, the vibration response of the combined system, as well as the fairing rotation amplitude, are substantially reduced. For a homogeneous fairing, the cross-flow amplitude is reduced by about 80 %, whereas for fairings with a gap longer than half a cylinder diameter, VIVs are completely eliminated, resulting in additional reduction in the drag coefficient. We have related such VIV suppression or elimination to the features of the wake flow structure. We find that a gap causes the generation of strong streamwise vorticity in the gap region that interferes destructively with the vorticity generated by the fairings, hence disorganizing the formation of coherent spanwise cortical patterns. We provide visualization of the incoherent wake flow that leads to total elimination of the vibration and rotation of the fairing–cylinder system. Finally, we investigate the effect of the friction coefficient between cylinder and fairing. The effect overall is small, even when the friction coefficients of adjacent segments are different. In some cases the equilibrium positions of the fairings are rotated by a small angle on either side of the centreline, in a symmetry-breaking bifurcation, which depends strongly on Reynolds number.
机译:我们对通过圆柱体的振动和流动进行了三维直接和大涡流数值模拟,圆柱体装有自由旋转的U形整流罩,以雷诺数100⩽Re 10,000横流放置。这种整流罩是沿着长圆形立管的轴线安装的几乎中性的浮力装置,可抑制涡流引起的振动(VIV)。我们考虑了三种不同的几何构型:均质的整流罩,以及涉及相邻线段之间的间隙的两种构型(表示为A和AB)。对于后两种情况,我们研究了间隙对流体力学力系数以及系统的平移和旋转运动的影响。对于所有配置,随着雷诺数增加到500以上,升力和阻力系数都会减小。与普通气缸相比,均质的整流罩系统(无间隙)可将阻力系数降低15%,以降低速度U * = 4.65,而A型间隙系统可将阻力系数降低近50%,以降低速度速度U * = 3.5、4.65、6,并且相应地,组合系统的振动响应以及整流罩旋转幅度被大大减小。对于均匀的整流罩,错流幅度降低了约80%,而对于间隙大于圆柱直径一半的整流罩,VIV被完全消除,导致阻力系数进一步降低。我们已经将这种VIV抑制或消除与尾流结构的特征相关联。我们发现间隙会在间隙区域中产生强烈的沿流涡流,从而对整流罩产生的涡流产生破坏性干扰,从而破坏了连贯的展向皮质模式的形成。我们提供不相干尾流的可视化,从而完全消除了整流罩-圆柱系统的振动和旋转。最后,我们研究了气缸与整流罩之间的摩擦系数的影响。即使相邻节段的摩擦系数不同,总体效果也很小。在某些情况下,整流罩的平衡位置会在对称线的分叉处在中心线的两侧旋转小角度,这在很大程度上取决于雷诺数。

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