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过程工程学报 ›› 2023, Vol. 23 ›› Issue (10): 1411-1420.DOI: 10.12034/j.issn.1009-606X.223040

• 研究论文 • 上一篇    下一篇

自吸射流搅拌桨液-液非均相混合特性分析

张静, 袁佳新, 李宏业, 张成松, 龚斌*   

  1. 沈阳化工大学机械与动力工程学院,辽宁 沈阳 110142
  • 收稿日期:2023-02-16 修回日期:2023-03-23 出版日期:2023-10-28 发布日期:2023-10-30
  • 通讯作者: 龚斌 gbsyhgdx@163.com
  • 基金资助:
    辽宁省应用基础研究计划项目;辽宁省教育厅自然科学基础项目

Liquid-liquid heterogeneous mixing characteristics of self-priming jet impeller

Jing ZHANG,  Jiaxin YUAN,  Hongye LI,  Chengsong ZHANG,  Bin GONG*   

  1. School of Mechanical and Power Engineering, Shenyang University of Chemical Technology, Shenyang, Liaoning 110142, China
  • Received:2023-02-16 Revised:2023-03-23 Online:2023-10-28 Published:2023-10-30
  • Contact: Bin GONG gbsyhgdx@163.com

摘要: 自吸射流搅拌槽作为新型搅拌装置在非均相强化混合过程中具有潜在的工程应用前景。以水为连续相,油为分散相,运用数值模拟和实验研究了自吸射流搅拌槽内液-液非均相混合过程及强化非均相混合过程的影响因素。结果表明,搅拌转速及分散相相含率对液-液非均相自吸射流轴线上无量纲速度影响较小。自吸射流管倾角β对搅拌槽内流场和分散相分布的影响显著,β<0°时,不利于油水非均相在搅拌槽内径向混合;β=0°时,搅拌槽内无自吸和射流现象,不利于轴向混合;β>0°时,搅拌桨上部产生自吸流,下部产生射流,高油相相含率流体被自吸射流管吸入,向下以射流方式进入低油相相含率流体,有效提高了搅拌槽底部湍流动能,强化了油水非均相混合过程。

关键词: 自吸射流, 非均相, 搅拌桨, 计算流体力学, 混合

Abstract: As a new type of stirred device, the self-priming jet stirred tank has potential engineering application value in heterogeneous mixing enhanced process. The engineering design and industrial application of self-priming jet stirred tank were restricted by the insufficient research on the mixing characteristics. In this study, the liquid-liquid heterogeneous mixing process in self-priming jet stirred tank was investigated using numerical simulation and experiment. Water and oil were set as continuous phase and dispersed phase, respectively. Realizable k-ε turbulence model and Eulerian-Eulerian multiphase flow model were used to numerically simulate the liquid-liquid heterogeneous flow field in the self-priming jet stirred tank. The enhanced mass transfer mechanism of the self-priming jet impeller was investigated. The results showed that the dimensionless velocity on the axis of self-priming jet pipe was less affected by the stirring speed and the dispersed phase holdup. However, the single-phase flow without oil phase had lower velocity inside the self-priming jet pipe and higher velocity outside the pipe. The flow field and dispersed phase distribution in the stirred tank were significantly influenced by the inclination angle β of self-priming jet pipe. When β<0°, the self-priming flow was formed at lower end of the pipe and the jet was formed at upper end of the pipe, which was unfavourable to the radial mixing of oil and water in the stirred tank. When β=0°, the fluid velocity in pipe was close to the impeller speed, and there was no self-priming and jet flow. The impeller only produced the stirring function, which was not good to axial mixing. When β>0°, the self-priming flow was formed at upper end of the pipe and the jet was formed at lower end of the pipe. The high oil phase fluid was sucked by the self-priming jet pipe, and was jetted downward into the low oil phase fluid. The oil phase moved upward by buoyancy. For the self-priming jet impeller with β>0°, the turbulent kinetic energy at the bottom of stirred tank was effectively increased. β>0° was beneficial to eliminate the flow inhomogeneity and oil-water heterogeneous mixing process was enhanced. When β=30°, the fluid region, which dimensionless phase fraction was 0.95~1.05, accounted for 81.88% of the stirred tank volume, and the oil phase distribution was more uniform along the axial and radial directions.

Key words: self-priming jet, Heterogeneous, agitator blade, computational fluid dynamics, mixing