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Coke behavior with H_(2)O in a hydrogen-enriched blast furnace:A review
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作者 Feng Zhou Daosheng Peng +5 位作者 Kejiang Li alberto n.conejo Haotian Liao Zixin Xiong Dongtao Li Jianliang Zhang 《International Journal of Minerals,Metallurgy and Materials》 SCIE EI CAS CSCD 2024年第5期959-976,共18页
Hydrogen-enriched blast furnace ironmaking has become an essential route to reduce CO_(2)emissions in the ironmaking process.However,hydrogen-enriched reduction produces large amounts of H_(2)O,which places new demand... Hydrogen-enriched blast furnace ironmaking has become an essential route to reduce CO_(2)emissions in the ironmaking process.However,hydrogen-enriched reduction produces large amounts of H_(2)O,which places new demands on coke quality in a blast furnace.In a hydrogen-rich blast furnace,the presence of H_(2)O promotes the solution loss reaction.This result improves the reactivity of coke,which is 20%-30%higher in a pure H_(2)O atmosphere than in a pure CO_(2)atmosphere.The activation energy range is 110-300 kJ/mol between coke and CO_(2)and 80-170 kJ/mol between coke and H_(2)O.CO_(2)and H_(2)O are shown to have different effects on coke degradation mechanisms.This review provides a comprehensive overview of the effect of H_(2)O on the structure and properties of coke.By exploring the interactions between H_(2)O and coke,several unresolved issues in the field requiring further research were identified.This review aims to provide valuable insights into coke behavior in hydrogen-rich environments and promote the further development of hydrogen-rich blast furnace ironmaking processes. 展开更多
关键词 hydrogen ironmaking coke behavior blast furnace GASIFICATION microstructure kinetics
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吹气孔直径对钢包模型内流动的影响 被引量:5
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作者 赵根安 张立峰 +3 位作者 alberto n.conejo 段豪剑 周海忱 董佳鹏 《中国冶金》 CAS 北大核心 2020年第12期22-27,共6页
采用相似比为1∶10的水模型研究了钢包底吹氩系统中吹气孔直径对钢液流动的影响,通过测量钢包中心面的速度场,得到流体流动随吹气孔直径的变化规律。研究结果表明,吹气孔直径在1~3 mm范围内,随吹气孔直径增加,气柱、液面和包壁附近的流... 采用相似比为1∶10的水模型研究了钢包底吹氩系统中吹气孔直径对钢液流动的影响,通过测量钢包中心面的速度场,得到流体流动随吹气孔直径的变化规律。研究结果表明,吹气孔直径在1~3 mm范围内,随吹气孔直径增加,气柱、液面和包壁附近的流体速度减小,整个钢包内速度场分布更均匀。随吹气孔直径增加,涡心坐标从(0.12,0.12)向(0.12,0.10)和(0.12,0.09)变化,涡心向上移动,横向移动不明显。随着吹气孔直径的增加,底部产生的气泡直径变大,混匀时间有所减小。 展开更多
关键词 钢包 水模型 底吹氩 流体流动 吹气孔
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