欢迎访问《金属矿山》杂志官方网站,今天是 分享到:
×

扫码分享

金属矿山 ›› 2022, Vol. 51 ›› Issue (03): 171-176.

• 机电与自动化 • 上一篇    下一篇

基于DPM的悬浮磁化焙烧主炉气固流动传热数值模拟

蔡玉节1孙永升1,2,3高鹏1,2,3张琦1唐志东1   

  1. 1.东北大学资源与土木工程学院,辽宁 沈阳110819;2.东北大学轧制技术及连轧自动化国家重点实验室,辽宁 沈阳110819;3.难采选铁矿资源高效开发利用技术国家地方联合工程研究中心,辽宁 沈阳110819
  • 出版日期:2022-03-15 发布日期:2022-04-02
  • 基金资助:
    国家自然科学基金项目(编号:51734005)

Numerical Simulation of Gas-solid Flow and Heat Transfer in Main Furnace of Suspension Magnetization Roasting Based on DPM

CAI Yujie1SUN Yongsheng1,2,3 GAO Peng1,2,3ZHANG Qi1TANG Zhidong1   

  1. 1.School of Resources and Civil Engineering,Northeastern University,Shenyang 110819,China;2.State Key Laboratory of Rolling and Automation,Northeastern University,Shenyang 110819,China;3.National-local Joint Engineering Research Center of High-efficient Exploitation Technology for Refractory Iron Ore Resources,Shenyang 110819,China
  • Online:2022-03-15 Published:2022-04-02

摘要: 为探明悬浮磁化焙烧主炉内气相温度场分布、颗粒流动特性以及颗粒升温速率等信息,基于CFD理论,对悬浮磁化焙烧主炉内稀相气固流动以及传热进行三维数值模拟计算。文中气相计算采用欧拉方法,固相计算采用Discrete Phase Model(DPM),并考虑气固两相之间的相互作用。结果表明,悬浮磁化焙烧主炉温度在径向呈现炉心温度高、近壁温度低的分布特征,在轴向逐渐趋于均匀。矿石颗粒进入主炉后,在气流的拖曳作用下迅速上升,1.0 s时颗粒可到达主炉顶部,1.2 s时颗粒在顶部弯管处出现逃逸现象;颗粒进入主炉后,自身温度迅速上升达到峰值。由于颗粒相和气相不断进行热量交换,在主炉上部低温区域,颗粒温度有所降低。颗粒在主炉内停留时间呈现“早出峰、长拖尾”的分布特征,其中95%以上的颗粒在1.2~3.6 s内完成逃逸。

关键词: 气固两相流, 温度场, 停留时间, 颗粒温度

Abstract: In order to ascertain the distribution of gas phase temperature field,particle flow characteristics,particle residence time,particle heating rate in the main furnace of suspension magnetization roasting,three-dimensional numerical simulation of gas-solid flow and heat transfer in the main furnace of suspension magnetization roasting was carried out by utilizing Euler method for gas phase calculation and Discrete Phase Model for particle calculation.The gas-solid interaction is also considered in the calculation.The result showed that the temperature in the center of the furnace is high,and low temperature is distributed near the furnace wall.Additionally,the temperature distribution in the furnace gradually tends to be uniform along the height direction of the main furnace.After the particles enter the main furnace,the particles rise rapidly under the drag of the air flow.The particles reach the top of the main furnace in 1.0 s,and the particles begin to escape at the outlet of the top elbow at 1.2 s.After the particles enter the main furnace,the temperature rises to peak rapidly.Due to the continuous energy exchange between the particle phase and the gas phase,the particle temperature decreases when the particles reach the upper low temperature zone of the main furnace.The particle residence time present “early peak,long tail”,more than 95% of the particles escape within 1.2~3.6 s.

Key words: gas solid two phase flow, temperature field, residence time, particle temperature