东北大学学报（自然科学版）

东北大学学报(自然科学版) ›› 2012, Vol. 33 ›› Issue (9): 1303-1306+1318.DOI: -

• 论著 • 上一篇    下一篇

底吹冰铜吹炼炉中气-液流动状况的数学模拟

邵品;张廷安;刘燕;王东兴;   

  1. 东北大学材料与冶金学院;
  • 收稿日期:2013-06-19 修回日期:2013-06-19 出版日期:2012-09-15 发布日期:2013-04-04
  • 通讯作者: -
  • 作者简介:-
  • 基金资助:
    国家自然科学基金资助项目(50934005,51074047);;

Numerical simulation of gas-liquid flow behavior in a copper matte bottom-blowing converter

Shao, Pin (1); Zhang, Ting-An (1); Liu, Yan (1); Wang, Dong-Xing (1)   

  1. (1) School of Materials and Metallurgy, Northeastern University, Shenyang 110819, China
  • Received:2013-06-19 Revised:2013-06-19 Online:2012-09-15 Published:2013-04-04
  • Contact: Zhang, T.-A.
  • About author:-
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摘要： 采用Eulerian-Eulerian模型描述了底吹冰铜吹炼炉内气液两相流行为,在模拟结果与实测结果一致的基础上,对双喷嘴在不同喷气角度下熔池内的气液两相流行为及气体含量进行模拟计算与比较.结果表明:随着喷吹角度的增大,喷溅情况相应有所减弱,在14°对喷角度下的喷溅现象最为严重.随着双喷嘴对喷角度的增大,射流轴线横向穿透距离增大,湍动能的分布区域也相应增大,气泡在容器中停留时间增加.但当夹角超过一定范围后,继续增大角度会使喷嘴口距离液面垂直距离减小,气泡在熔池中的停留时间反而减小,其中28°对喷角度下,熔池中的气体体积分数最大,而且湍动能分布范围最广.

关键词: 底吹, 冰铜吹炼, 两相流, 欧拉-欧拉模型, 数值模拟

Abstract: The gas-liquid two-phase flow behavior in the copper matte bottom-blowing converter was described with the Euler-Euler model, and the simulation results are consistent with the measured results. On this basis, the gas-liquid two-phase flow behavior and the gas volume at different jet angles with double nozzles were described. The results showed that the splash decreases with the increasing of jet angles with double nozzles. When the jet angle is 14 degrees, the splash is the most serious. The transverse penetration distance of gas-liquid jet trajectory and the distribution area of turbulent kinetic energy increase with the increasing of jet angles, and the residence time of the gas phase in the pool increases. However, after the jet angle exceeds a certain range, the vertical distance from the jet nozzle to the liquid surface decreases when the jet angle continues to increase. Then the residence time of gas phase in the pool is shortened. When the jet angle is 28 degrees, the gas volume fraction is the highest and distribution of the turbulent kinetic energy is the largest.

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