东北大学学报(自然科学版)
東北大學學報(自然科學版)
동북대학학보(자연과학판)
JOURNAL OF NORTHEASTERN UNIVERSITY(NATURAL SCIENCE)
2015年
9期
1293-1296,1301
,共5页
周恒%游洋%罗志国%邹宗树
週恆%遊洋%囉誌國%鄒宗樹
주항%유양%라지국%추종수
COREX 竖炉%离散元法%流型%瞬态特性%法向应力
COREX 豎爐%離散元法%流型%瞬態特性%法嚮應力
COREX 수로%리산원법%류형%순태특성%법향응력
COREX shaft furnace%DEM(discrete element method)%flow pattern%transient features%normal stress
基于离散单元数值计算方法,建立 COREX 竖炉内物料颗粒尺度运动行为的数学模型,研究炉内物料运动流型及其瞬态特性,特别是颗粒的瞬态速度和瞬态应力分布.模拟结果表明:COREX 竖炉内存在三种类型的流动区域:活塞流区、准停滞区以及沟流区.炉内颗粒的瞬态速度分布表明炉内存在两种类型的速度波:装料过程引发的向下传播的速度波和底部排料引发的向上传播的速度波.COREX 竖炉内颗粒法向应力随时间的变化较小,竖炉底部导流锥顶部存在较强的应力区,而无导流锥竖炉底部中心存在较强应力区,沟流区的应力较弱.
基于離散單元數值計算方法,建立 COREX 豎爐內物料顆粒呎度運動行為的數學模型,研究爐內物料運動流型及其瞬態特性,特彆是顆粒的瞬態速度和瞬態應力分佈.模擬結果錶明:COREX 豎爐內存在三種類型的流動區域:活塞流區、準停滯區以及溝流區.爐內顆粒的瞬態速度分佈錶明爐內存在兩種類型的速度波:裝料過程引髮的嚮下傳播的速度波和底部排料引髮的嚮上傳播的速度波.COREX 豎爐內顆粒法嚮應力隨時間的變化較小,豎爐底部導流錐頂部存在較彊的應力區,而無導流錐豎爐底部中心存在較彊應力區,溝流區的應力較弱.
기우리산단원수치계산방법,건립 COREX 수로내물료과립척도운동행위적수학모형,연구로내물료운동류형급기순태특성,특별시과립적순태속도화순태응력분포.모의결과표명:COREX 수로내존재삼충류형적류동구역:활새류구、준정체구이급구류구.로내과립적순태속도분포표명로내존재량충류형적속도파:장료과정인발적향하전파적속도파화저부배료인발적향상전파적속도파.COREX 수로내과립법향응력수시간적변화교소,수로저부도류추정부존재교강적응력구,이무도류추수로저부중심존재교강응력구,구류구적응력교약.
A mathematical model based on discrete element method (DEM)was developed to investigate the behaviors of solid particulate motion in a COREX shaft furnace model from particle-scale view.The solid flow pattern and transient features of burden were simultaneously analyzed,especially the transient behavior of velocity and stress distribution were calculated.The results showed that the solid flow in COREX shaft furnace can be divided into three different flow regions:plug flow zone,quasi-stagnant zone and converging flow zone.The transient behavior of velocity distribution indicates that there are two types of velocity waves in the furnace.One is a downward wave caused by charging and the other is upward from bottom caused by discharging. The normal stress has a minor change with time.A high stress field exists on the top of the guiding cone,while for the furnace without guiding cone,the particles in the lower central zone present strong normal stress.On the contrary,the particles exhibit weak normal stresses in the converging flow zone.