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Direct resolution of differential pressure fluctuations to characterize multi-scale dynamics in a gas fluidized bed

机译:直接解决压差波动的问题,以表征气体流化床中的多尺度动力学

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A direct resolution approach was proposed to decompose differential pressure signals from a gas fluidized bed into macro- and super-imposing components, which were further subjected to structure density function analysis (SDF analysis) to study dynamics of multi-scale structures in flow. Direct resolution performed well in extracting feature information of multi-scale structures, especially macro- and meso-scale structures whose dynamic behaviors majorly affected hydrodynamics in bed, from measured differential pressure fluctuations. With the assistance of Gaussian fitting and Kolmogorov-Smirnov test, SDF analysis divided the probability distribution of multiple structures with respect to their amplitude scale r into four feature regions (Regions B-I, B-II, B-III and Region A). Parameter K-SDF derived from slope of Region B-II quantified frequency of various meso-scale structures in flow, and well followed the tendency of flow patterns transition after being normalized by bubble (slug) rising velocity U-b(sl). Frequency of macro scale structures in slugging flow depended greatly on rising velocity of slugs, so SDFmacro increased with increased fluidization velocity. Developed turbulent flow had a high SDFmacro exceeded 0.8 Hz due to the fast passage and split/integration of large voids. Structures localized in Region A mainly represented noise from measurements, other measurable micro-scale disturbances in single phases or phase-interfaces, and had an occurring frequency increased with increase of fluidization velocity. (C) 2016 Elsevier Ltd. All rights reserved.
机译:提出了一种直接解析方法,将来自气体流化床的压差信号分解为宏叠加分量和叠加叠加分量,然后进一步对其进行结构密度函数分析(SDF分析),以研究流动中多尺度结构的动力学。直接分辨率在从测量的压差波动中提取动态结构主要影响床层流体动力学的多尺度结构(尤其是宏观和中尺度结构)的特征信息时表现良好。借助高斯拟合和Kolmogorov-Smirnov检验,SDF分析将多个结构相对于其振幅标度r的概率分布分为四个特征区域(区域B-I,B-II,B-III和区域A)。从区域B-II的斜率得出的参数K-SDF量化了流中各种中尺度结构的频率,并且在通过气泡(弹头)上升速度U-b(sl)归一化之后很好地遵循了流型转变的趋势。团状流中宏观结构的频率很大程度上取决于团状体的上升速度,因此SDFmacro随着流化速度的增加而增加。由于大空隙的快速通过和分裂/整合,发达的湍流具有超过0.8 Hz的高SDFmacro。区域A中的结构主要表示来自测量的噪声,单相或相界面中的其他可测量的微尺度扰动,并且其发生频率随流化速度的增加而增加。 (C)2016 Elsevier Ltd.保留所有权利。

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