东北大学学报(自然科学版) ›› 2013, Vol. 34 ›› Issue (11): 1589-1592.DOI: 10.12068/j.issn.1005-3026.2013.11.017

• 材料与冶金 • 上一篇    下一篇

非对称两流中间包内流体流动的对称化

雷洪1,毕乾2,罗智恒2,赵岩2   

  1. (1东北大学材料电磁过程研究教育部重点实验室,辽宁沈阳110819;2东北大学材料与冶金学院,辽宁沈阳110819)
  • 发布日期:2013-07-09
  • 通讯作者: 雷洪
  • 作者简介:雷洪(1973-),男,湖北武汉人,东北大学教授.
  • 基金资助:
    中央高校基本科研业务费专项资金资助项目(N100409007).

The Symmetic Fluid Flow in an Asymmetic TwoStrand Tundish〓

LEI Hong1, BI Qian2, LUO Zhiheng2, ZHAO Yan2   

  1. 1. Key Laboratory of Electromagnetic Processing of Materials, Ministry of Education, Northeastern University, Shenyang 110819, China; 2. School of Materials & Metallurgy, Northeastern University, Shenyang 110819, China.
  • Published:2013-07-09
  • Contact: LEI Hong
  • About author:-
  • Supported by:
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摘要: 采用数值模拟和水模型实验相结合的方法研究了不同控流方案下非对称两流中间包内流体流动行为,并将优化方案进行了工业实验.实验结果表明:采用经典组合方法计算各流的死区时,出现负死区现象,因此采用平均停留时间作为评价参数;原方案中靠近长水口侧出口的平均停留时间为194s,水口两流之间的平均停留时间之差为97s,两流之间钢液温度差为5℃.利用非对称长方形湍流控制器可以实现钢液在湍流控制器出口处流量的非对称分布.采用非对称长方形湍流控制器和多孔挡墙后,近长水口侧出口的平均停留时间为211s,水口两流之间的平均停留时间之差为34s,两流之间钢液温度差为3℃.

关键词: 非对称中间包, 准对称化, 非对称湍流控制器, RTD曲线, 平均停留时间

Abstract: Mathematical simulations and water modeling experiments were applied to study the fluid flow in an asymmetric twostrand tundish under different flow controlling devices, and the optimized configuration was used in the industrial continuous caster. The experimental results showed that the negative dead volume fraction appeared if the classic combined method was applied to calculate the dead volume fraction for each strand, so the mean residence time was chosen as the key parameter. In the former tundish, the mean residence time at the strand near the ladle shroud was 194 seconds, the difference of the mean residence time between two strands was 97 seconds, and the difference of the temperature between two strands was 5℃. The asymmetric distribution of the flow rate of the molten steel was realized using the asymmetric rectangle turbulence inhibitor at the exit of it. Because of the asymmetry of the turbulence inhibitor, the flow rate of the molten steel was asymmetrical at the exit of the turbulence inhibitor. In the optimized tundish with asymmetric rectangle turbulence inhibitor and multihole baffle the mean residence time at the strand near the ladle shroud was 211 seconds, the difference of the mean residence time between two strands was 34 seconds, and the difference of the temperature between two strands was 3℃.

Key words: asymmetric tundish, quasisymmetry, asymmetric turbulence inhibitors, residence time distribution curves, mean residence time

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