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Lightnin静态混合器内气泡分散流体动力学特性实验研究
引用本文:禹言芳,刘桓辰,孟辉波,刘励图,李毓,吴剑华. Lightnin静态混合器内气泡分散流体动力学特性实验研究[J]. 化工学报, 2022, 73(8): 3565-3575. DOI: 10.11949/0438-1157.20220313
作者姓名:禹言芳  刘桓辰  孟辉波  刘励图  李毓  吴剑华
作者单位:沈阳化工大学机械与动力工程学院,辽宁沈阳110142;沈阳化工大学辽宁省高效化工混合技术重点实验室,辽宁沈阳110142
基金项目:辽宁特聘教授计划项目(辽教函[2018]35号);国家自然科学基金项目(21476142);辽宁省教育厅高等学校基本科研项目重点项目(LJKZ0429);辽宁省“百千万人才工程”人选项目(201892151);辽宁省自然科学基金项目(2022-MS-0310);沈阳市中青年科技创新人才计划项目(RC200032)
摘    要:以Lightnin静态混合器(LSM)内水-空气气液两相体系为研究对象,在连续相水表观速度UL=0.071~0.127 m/s和离散相空气表观速度UG=0.007~0.042 m/s的条件下,研究内径100 mm的LSM内气液两相湍流流动阻力与气泡分散水动力学行为。使用分辨率为1920×1080的高速相机Revealer-2F04M采集混合器内不同轴向窗口的气泡群演化过程。结果表明:当UL<0.085 m/s和UG=0.025~0.042 m/s时,LSM内的流型为泡状流。随着气泡群流经混合元件数的增加,气泡群的Sauter平均直径d32逐渐减小。当液体表观速度UL≤0.085 m/s时,Sauter平均直径d32随气体表观速度的增加先减小后增大;UG =0.028 m/s时d32达到局部最小值,53%的气泡直径dB/D0在0.02~0.05范围内。Sauter平均直径、内径与无量纲停留时间τ之间的关系满足d32/D0=0.031τ-0.14We-0.41。平均气含率α的增大显著增加了单位体积内气泡数量密度,加剧气泡与元件表面碰撞频率,增大旋涡二次流强度,导致摩擦系数显著降低;采用Lockhart-Martinelli方法对实验数据回归,得到气液两相流压降预测常数C的关联式:C=5.26×105UG-0.91/Re0.74

关 键 词:静态混合器  气液两相  Sauter平均直径  气含率  压降
收稿时间:2022-03-02

Experimental investigation of turbulent dispersion and hydrodynamic behavior of bubble in Lightnin static mixer
Yanfang YU,Huanchen LIU,Huibo MENG,Litu LIU,Yu LI,Jianhua WU. Experimental investigation of turbulent dispersion and hydrodynamic behavior of bubble in Lightnin static mixer[J]. Journal of Chemical Industry and Engineering(China), 2022, 73(8): 3565-3575. DOI: 10.11949/0438-1157.20220313
Authors:Yanfang YU  Huanchen LIU  Huibo MENG  Litu LIU  Yu LI  Jianhua WU
Affiliation:1.School of Mechanical and Power Engineering, Shenyang University of Chemical Technology, Shenyang 110142, Liaoning, China;2.Liaoning Key Laboratory of Chemical Technology for Efficient Mixing, Shenyang University of Chemical Technology, Shenyang 110142, Liaoning, China
Abstract:The gas-liquid two-phase bubbly flow in a Lightnin static mixer (LSM) with a diameter of 100 mm and an aspect ratio of 1.0 was investigated. The turbulent dispersion and hydrodynamic behavior of bubble groups was focused under the conditions of liquid phase superficial velocity UL=0.071—0.127 m/s and gas phase superficial velocity UG=0.007—0.042 m/s. The evolution of bubble populations in different axial windows in the mixer was collected by using a high-speed camera Revealer-2F04M with a resolution of 1920×1080. The results show that the flow pattern in the LSM is in bubbly flow at the superficial velocity of continuous phase UL no more than 0.085 m/s and UG=0.025—0.042 m/s. The Sauter mean diameter d32 of bubble groups gradually decreased with the increase of axial mixing length. With the given liquid flow superficial velocity UL≤0.085 m/s, the Sauter mean diameter d32 firstly decreased and then increased with the increase of gas flow superficial velocity. The local minimum of d32 was obtained at UG=0.028 m/s and 53% of the dB/D0 is in the range of 0.02—0.05. The relationship among Sauter mean diameter, the inner diameter and the non-dimensional residence time satisfies the correlation d32/D0=0.031τ-0.14We-0.41. As the gas superficial velocity increases, the density function of the number of bubbles per unit volume increases significantly. The probability of bubble collided with the surfaces of the element is enhanced which increases the intensity of the vortex secondary flow and leads to a significant decrease in the friction coefficient. By fitting the pressure drop of two-phase flow, the empirical correlation prediction formula C=5.26×105UG-0.91/Re0.74 was obtained.
Keywords:static mixer  gas-liquid flow  Sauter mean diameter  gas holdup  pressure drop  
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