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120 t钢包底吹氩过程中气泡行为的数值模拟研究

Numerical simulation study on bubble behavior during bottom blowing argon for 120 t ladle

  • 摘要: 钢包底吹氩过程中气泡的尺寸分布直接影响精炼效果,本文通过建立耦合气泡碰撞与聚合模型的流体体积法-离散相(VOF-DPM)混合数值模型来系统描述渣-金界面动态和大量离散气泡的运动与演化行为。通过水模型试验验证了模型的准确性,进而系统模拟分析了120 t钢包底吹流量、吹气位置及双孔夹角3个关键工艺参数对气泡尺寸分布与渣眼形态的影响规律。结果表明,增大底吹流量会显著促进气泡聚合和渣眼扩张,流量从 80 L/min 增加至400 L/min,气泡平均直径增大 30.1%;改变底吹位置可优化流场结构,底吹位置从 0.1r(r为钢包底部半径)移至 0.7r,气泡平均直径先减 16.4% 后增14.3%,渣眼面积先减小后增大;在0.3r附近能获得更细小弥散的气泡群;调整双孔夹角能调控2股气泡流的相互作用,双孔夹角从 45°增加至180°,气泡平均直径先减 9.8% 后增 7.8%,渣眼面积先减小后增大,且钢包顶部气泡尺寸变化更显著。

     

    Abstract: Bubble size distribution during ladle bottom argon-blowing directly affects the refining performance. A hybrid VOF-DPM numerical model coupled with bubble collision and coalescence models is established to systematically describe the dynamics of slag-metal interface as well as the motion and evolution behaviours of numerous discrete bubbles. The accuracy of the model is validated by water-model experiments. Further, systematic simulation and analysis are performed to investigate the influences of three key process parameters, namely bottom-blowing flow rate, blowing position and double-hole included angle, on bubble size distribution and slag eye morphology for a 120 t ladle. The results show that bubble coalescence and slag-eye expansion are significantly promoted with the increase of bottom-blowing flow rate. When the flow rate rises from 80 to 400 L/min, the average bubble diameter is increased by 30.1%. The flow-field structure can be optimised by varying the bottom-blowing position. As the bottom-blowing position is shifted from 0.1r(r denotes the ladle bottom radius) to 0.7r, the average bubble diameter is first reduced by 16.4% and then increased by 14.3%, and the slag-eye area is decreased first and increased afterwards. Finer and more dispersed bubble groups are obtained near 0.3r. The interaction between two bubble plumes can be regulated by adjusting the double-hole included angle. As the double-hole included angle increases from 45° to 180°, the average bubble diameter is first reduced by 9.8% and then increased by 7.8%, the slag-eye area decreases first and increases subsequently, and more remarkable variations of bubble size are observed at the ladle top.

     

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