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BUBBLE SIZE EFFECTS ON DISPERSED PHASE MOTION IN VERTICAL BUBBLY PIPE FLOW

机译:垂直泡沫管流动分散相运动的泡沫尺寸效应

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Three-dimensional measurements of bubble size, and velocity are presented along with the associated statistics for dilute bubbly flow in a vertical pipe. These measurements were obtained through a combination of precise index-of-refraction matching and a stereoscopic high-speed imaging system. An image-processing algorithm has been developed and used to extract instantaneous bubble size, shape, velocity and trajectory information and statistics corrected for magnification errors (maximum of 2%). The experiments have been conducted at a Reynolds of 14,600 in vertical pipe-flow and a volumetric gas flow ratio of 0.29%. Bubble sizes ranged from sub millimeter to several millimeters. The results indicate that bubbles less than approximately 20 wall units with very low ratios of rise-velocity-to-liquid-average-velocity occupy the full breadth of the test section, while bubbles in the range between 20 and 60 wall units with ratios of rise-velocity-to-liquid-average-velocity greater than 0.5 are efficiently trapped by the wall and are almost exclusively found in the inner wall region (y~+<30). Bubbles larger than 60 wall units with ratios of rise-velocity-to-liquid-average-velocity less than 0.5 are found throughout the pipe cross-section although with a strong preference to the wall neighborhood. This bubble behavior is put in perspective considering four mechanisms of bubble migration: (a) turbulent dispersion due to near-wall large scale structure, (b) inviscid transverse forces (Magnus), (c) viscous transverse forces (Saffman), and (d) unsteady transverse forces because of vortex shedding and bubble shape deformation.
机译:与垂直管中的稀释气泡流动的相关统计,呈现出气泡尺寸的三维测量和速度。通过精确的折射率匹配和立体高速成像系统的组合获得这些测量。已经开发了一种图像处理算法并用于提取瞬时气泡尺寸,形状,速度和轨迹信息和校正校正的统计信息(最大值为2%)。实验已经在垂直管道流动的14,600的曲回处进行,体积气体流量比为0.29%。泡沫尺寸范围从亚毫米到几毫米。结果表明,小于大约20个壁单元的气泡,具有非常低的上升 - 速度 - 液体 - 平均速度的速度,占据了试验部分的完整宽度,而20至60个壁单元之间的气泡具有比率壁的升高到液体平均速度大于0.5,壁是有效捕获的,并且几乎专门发现在内壁区域(Y〜+ <30)中。在整个管道横截面中发现了大于60个壁单元的泡沫,具有小于0.5的升高到液体平均速度小于0.5的比例。考虑到泡沫迁移的四种机制:(a)由于近壁大规模结构,(b)粘性横向力(MAGNU),(c)粘性横向力(Saffman),(a)湍流色散的透视图d)由于涡旋脱落和气泡形状变形而不稳定的横向力。

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