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Modeling of Slag Eye Area in Argon Stirred Ladles

机译:搅拌钢包渣眼区域的建模

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摘要

Slag eye area in an axi-symmetrical water model of an argon stirred ladle has been measured through video photography as a function of gas flow rates, liquid depth, slag layer thickness and different types of upper phase liquid. It is shown that in addition to the principal operating parameters (i.e., gas flow rate, liquid depth and amount of slag), physical properties of the overlying liquid, particularly kinematic viscosity and density exert considerable influence on slag eye formation. Based on our experimental observation, it is shown that existing correlations do not constitute a sufficiently reliable basis for prediction of slag eye area in steelmaking ladles. Accordingly, a new correlation for slag eye area has been formulated through dimensional analysis embodying a large set of experimental data, derived from different combinations of bulk and upper phase liquids. Polynomial regression indicates that dimensionless slag eye area can be expressed in terms of Froude number, (U_P~2/gH), density ratio, (R_L/Δp), and Reynolds number, (HU_p/v_s), via: (A_(es)/hH)=3.25(u_p~2/gH)~(1.28)(P_L/Δp)~(0.55)(V_s/HU_p)~(-0.05) in which, A_(es) is the eye area, H is the slag layer thickness, h is the bulk liquid depth and U_P is the average plume rise velocity. Experimental data reported by many investigators on aqueous as well as industrial scale ladle gas stirred ladles systems were subsequently applied to demonstrate the adequacy and appropriateness of the proposed correlation. Possible extrapolation of the correlation to eccentric gas injection and melt covered with a thick slag layer, which are more typical of ladle metallurgy steelmaking, is also examined.
机译:已经通过视频摄影测量了氩搅拌钢包的轴对称水模型中的渣眼面积与气体流速,液体深度,渣层厚度和不同类型的上相液体的关系。结果表明,除了主要的操作参数(即气体流速,液体深度和炉渣量)外,上覆液体的物理性质,特别是运动粘度和密度对炉渣的形成也有很大的影响。根据我们的实验观察结果表明,现有的相关性不足以预测炼钢钢包的渣眼面积。因此,通过尺寸分析已体现了炉渣眼面积的新相关性,该尺寸分析体现了大量的实验数据,这些数据是从散装和上相液体的不同组合得出的。多项式回归表明无量纲渣眼面积可以通过以下公式表示:弗洛德数(U_P〜2 / gH),密度比(R_L /Δp)和雷诺数(HU_p / v_s),可通过以下方式表示: )/ hH)= 3.25(u_p〜2 / gH)〜(1.28)(P_L /Δp)〜(0.55)(V_s / HU_p)〜(-0.05)其中,A_(es)是眼睛区域,H是渣层的厚度,h是散装液体的深度,U_P是平均羽流上升速度。随后,许多研究人员报告了在水和工业规模钢包气搅拌钢包系统上的实验数据,以证明所提出的相关性的充分性和适当性。还研究了与钢包冶金炼钢中较典型的偏心气体注入和被厚渣层覆盖的熔体的相关性的可能推断。

著录项

  • 来源
    《ISIJ international》 |2010年第11期|p.1622-1631|共10页
  • 作者单位

    Formerly Department of Materials Science and Engineering, Indian Institute of Technology Kanpur, 208016 India. Now at Research Engineer, JSW Steel Limited, Torangallu, Bellary, Karnataka, India;

    Department of Materials Science and Engineering, Indian Institute of Technology Kanpur, 208016 India;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    argon stirred ladle; ladle homogenization; slag eye area; water modelling; measurements and correlations;

    机译:氩气搅拌钢包钢包均质化渣眼区域水模型;测量和相关;

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