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Influence of Shape of Cohesive Zone on Gas Flow and Permeability in the Blast Furnace Analyzed by DEM-CFD Model

机译:用DEM-CFD模型分析高炉内聚区形状对气体流量和渗透率的影响

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摘要

Maintaining gas permeability is an important issue to realize low coke rate operation of blast furnace. In present study, the melting behavior of the iron ore and the layer structure in low coke rate operation were introduced in to the DEM-CFD model, and then behaviors of gas and moving bed in the blast furnace were simulated. Influence of shape of cohesive zone in low coke rate operation was investigated, and the effect of coke slit in the cohesive zone on gas flow was demonstrated in the calculation result. Surface area of cohesive zone and intersection angle between the burden layers and cohesive zone will determine the activity of coke slit.
机译:维持透气性是实现高炉低焦炭运行的重要问题。在本研究中,将铁矿石的熔融行为和低焦炭运行中的层状结构引入到DEM-CFD模型中,然后模拟了高炉中煤气和移动床的行为。研究了低焦比运行时内聚区形状的影响,并在计算结果中证明了内聚区焦炭裂隙对气流的影响。粘聚区的表面积以及物料层与粘聚区之间的相交角将决定焦炭切缝的活性。

著录项

  • 来源
    《ISIJ international》 |2015年第6期|1232-1236|共5页
  • 作者单位

    Institute of Multidisciplinary Research for Advanced Materials (IMRAM), Tohoku University, 1-1, Katahira 2, Aoba-ku, Sendai, 980-8577 Japan;

    Institute of Multidisciplinary Research for Advanced Materials (IMRAM), Tohoku University, 1-1, Katahira 2, Aoba-ku, Sendai, 980-8577 Japan;

    Institute of Multidisciplinary Research for Advanced Materials (IMRAM), Tohoku University, 1-1, Katahira 2, Aoba-ku, Sendai, 980-8577 Japan;

    Faculty of Engineering, Hokkaido University, Kita 13, Nishi 8, Kita-ku Sapporo, 060-8628 Japan;

    Tohoku University, 1-1, Katahira 2, Aoba-ku, Sendai, 980-8577 Japan;

    Institute of Multidisciplinary Research for Advanced Materials (IMRAM), Tohoku University, 1-1, Katahira 2, Aoba-ku, Sendai, 980-8577 Japan;

  • 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

    blast furnace; numerical simulation; DEM-CFD model; cohesive zone; gas permeability;

    机译:高炉;数值模拟DEM-CFD模型;粘结区气体渗透率;
  • 入库时间 2022-08-17 23:59:06

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