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Furnace gas flow distribution estimation method of blast furnace, furnace gas flow of blast furnace distribution estimation apparatus and blast furnace gas flow distribution estimation program of

机译:高炉炉煤气分布估算方法,高炉煤气分布估算装置的煤气流量和高炉煤气分布估算程序

摘要

PROBLEM TO BE SOLVED: To estimate the distribution of in-furnace gas flow in a furnace gas flowing in the furnace top part, on the basis of the measured values of the gas temperature in the furnace top part, the raw material height in a blast furnace and the total gas flowing amount of the in-furnace gas without directly measuring the flowing amount of the in-furnace gas in the furnace top part.;SOLUTION: An apparatus 34 for estimating the distribution of gas flow estimates the gas distribution of the in-furnace gas flow flowing at the plurality of gas measuring points respectively, on the basis of the measured values of the gas temperatures TGM measured at the plurality of gas-measuring points in the furnace top part 14, the raw material height RMN measured at the plurality of height measuring points and the total gas flowing amount GTL of the in-furnace gas flowing in the furnace top part 14. By this method, the necessity of directly measuring the flowing gas amount or the flowing speed of the in-furnace gas G in the furnace top part 14 with gas flowing sensors, such as flowing amount meter and flowing speed meter having some problems from the view points of maintenance and durability, is eliminated.;COPYRIGHT: (C)2010,JPO&INPIT
机译:解决的问题:根据炉顶部的气体温度测量值,高炉中的原料高度,估算在炉顶部流动的炉内气体的炉内气流分布炉和炉内气体的总气体流量,而不直接测量炉顶部内炉内气体的流量。解决方案:用于估计气流分布的装置34估算炉内气体的分布。基于在炉顶部14中的多个气体测量点处测量的气体温度T GM 的测量值,分别在多个气体测量点处流动的炉内气流然后,在多个高度测量点处测量的原料高度R MN 和在炉顶部14中流动的炉内气体的总气体流量G TL 通过这种方法,直接测量浮点数的必要性从维护和耐用性的角度来看,消除了带有气体流量传感器(例如流量计和流速计)的炉顶气体14在炉顶部14中的尾气量或炉内气体G的流动速度。版权:(C)2010,日本特许厅和INPIT

著录项

  • 公开/公告号JP5387066B2

    专利类型

  • 公开/公告日2014-01-15

    原文格式PDF

  • 申请/专利权人 JFEスチール株式会社;

    申请/专利号JP20090056499

  • 发明设计人 津田 和呂;島本 拓幸;

    申请日2009-03-10

  • 分类号C21B5;C21B7/24;G01N25/18;

  • 国家 JP

  • 入库时间 2022-08-21 16:14:01

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