中间雷诺数下质量分布对圆柱形粒子下落的影响

B. Angle, M. Rau, M. Byron
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引用次数: 3

摘要

在自然沉降中,许多感兴趣的颗粒既大又非球形。一些常见的颗粒类型(如自然产生的聚集体)没有均匀的质量分布。因此,质量中心和浮力中心不在同一位置,导致更复杂的沉降动力学。在这里,我们研究了自由下落圆柱体的方向和终端速度,其中质量分布要么是恒定的(均匀密度,UD),要么是二部的,沿着长度的一半经历阶跃函数(化合物密度,CD)。圆柱体的长径比相对较低(1 < AR < 4),并且在中间雷诺数(100数量级)下降。这些圆柱体最初是水平的,在一个高大的六角形静水箱的顶部释放出来,由高速摄像机拍摄。两台低速摄像机同时捕捉到1)整个气缸轨迹和2)着陆位置。我们记录了每个圆柱体的最终速度、下落方向和着陆点。结果表明均匀密度圆柱体与复合密度圆柱体的沉降特性有显著差异。AR = 1的UD圆柱体最初是沿侧面落下的,而AR = 1的CD圆柱体是垂直落下的。然而,这两种情况下均表现出下降时柱体方向的振荡。当AR = 2和AR = 4时,UD圆柱体的侧壁一致,圆柱体轴向振荡最小。AR = 2的CD圆柱体有两种不同的落模。在模式1中,圆柱体在开始绕垂直轴振荡之前从其初始方向旋转90°。在模态2中,圆柱体方向保持恒定,与水平面有一个小角度。在CD AR = 4圆柱体中也观察到这种模式,它们以恒定的(倾斜的)取向角下落,并在下落时水平移动。所有CD圆柱体的着陆点都偏向于目标的一侧,即圆柱体密度较大的一端最初朝向的位置,而UD圆柱体则均匀分布在罐中心周围。一般来说,垂直投影面积最小的圆柱体下落时的终端速度最大;然而,控制取向的机制尚不清楚。我们的研究结果对预测自然粒子的沉降行为具有重要意义,并为进一步研究湍流等复杂流动中的粒子沉降奠定了基础。考虑到我们在静水中的结果,质心和体积中心之间的偏移产生的浮力扭矩之间的相互作用可能会强烈影响湍流中的粒子运动。
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Effect of Mass Distribution on Falling Cylindrical Particles at Intermediate Reynolds Numbers
In natural sedimentation, many particles of interest are both large and nonspherical. Some common particle types (e.g. naturally occurring aggregates) do not have a uniform mass distribution. As a result, the centers of mass and buoyancy are not co-located, leading to more complex settling dynamics. Here we investigated the orientation and terminal velocity of freely falling cylinders, in which the mass distribution was either constant (uniform-density, UD) or bipartite, undergoing a step function halfway along the length (compound-density, CD). Cylinders had relatively low aspect ratios (1 < AR < 4), and fell at intermediate Reynolds numbers (of order 100). The cylinders, initially horizontal, were released at the top of a tall hexagonal still-water tank, and imaged by a high-speed camera. Two low-speed cameras simultaneously captured 1) full cylinder trajectory and 2) landing position. We recorded the terminal velocity, fall orientation, and landing site of each cylinder. Results showed significant differences in the settling characteristics of uniform- vs. compound-density cylinders. UD cylinders of AR = 1 fell broadside initially, whereas AR = 1 CD cylinders fell vertically. However, both cases showed oscillation in cylinder orientation upon descent. UD cylinders with AR = 2 and AR = 4 consistently fell broadside, with minimal cylinder axis oscillation. CD cylinders with AR = 2 fell with two different modes. In mode 1, cylinders rotated 90° from their initial orientation before beginning to oscillate about the vertical axis. In mode 2, cylinder orientation remained constant at a slight angle from the horizontal. This mode was also observed in the CD AR = 4 cylinders, which fell at a constant (tilted) orientation angle and moved horizontally as they fell. The landing sites for all CD cylinders were biased toward the side of the target where the denser end of the cylinder was initially oriented, whereas UD cylinders landed in a uniform distribution around the tank center. In general, cylinders with the smallest vertical projected area fell with the greatest terminal velocity; however, the mechanisms controlling orientation remain unclear. Our results have important implications for predicting the settling behavior of naturally-occurring particles, and lay the groundwork for further study of particles settling in complex flows such as turbulence. Given our results in still water, the interplay between the buoyant torques created by the offset between the center of mass and center of volume are likely to strongly impact particle motion in turbulence.
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