共查询到19条相似文献,搜索用时 125 毫秒
1.
2.
以某厂300tRH真空精炼装置为研究原型,建立1∶6.5的水力模型对RH喷吹精炼工艺进行物理模拟。研究了喷吹位置、喷吹气量及驱动气体流量对循环流量和均混时间的影响。结果表明:不同喷吹气量、驱动气体流量条件下,获得大循环流量和短均混时间的最优喷吹位置不同。较小的喷吹气量(2.98~3.53m3/h)或者较小的驱动气体流量(0.93~1.02m3/h)时,宜采用低顶枪枪位(153.8mm)喷吹;喷吹气量大于3.91m3/h或者驱动气体流量大于1.12m3/h时,宜采用真空槽底部喷吹角度120°的侧喷嘴喷吹。顶枪与侧喷嘴复合喷吹有利于提高RH喷吹工艺的适应性及循环效率。 相似文献
3.
4.
5.
6.
7.
8.
用水模型对顶吹、中心小流量底吹及复合吹,在不同的气体流量下,用铝粉示踪法研究了熔池内的流谱,用频闪光照像法测定了涡环中的速度分布并由此计算循环流量.循环流量(Q_c)与顶吹流量(Q_T)和底吹流量(Q_B)间的关系为:Q_c=O.659Q_T+5.175Q_B-0.051 (Q_T)~2-4. 975(Q_B)~2-O.229Q_TQ_B.在试验的参数范围内,循环流量与顶吹气体流量之间为具有一极大值的曲线,循环流量与底吹气体流量之间为一条逐渐变缓的上升曲线,复合吹的循环流量小于单纯顶吹和底吹时的代数和,附加底吹所增加的循环流量随顶吹量的增大而减小. 相似文献
9.
RH-MFB真空精炼过程中循环流量的物理模拟研究 总被引:2,自引:0,他引:2
在120 t RH-MFB多功能真空精炼装置1∶5.45比例的水模型上,采用毕托管测定下降管内钢水流速,从而测定循环流量的方法,研究了真空循环精炼过程中钢液的环流特性.考察了该冶金反应器主要结构参数和工艺操作因素,包括插入管内径、驱动气体流量、驱动气体用喷嘴个数及其布置、驱动气体引入位置(气泡行程)、插入管浸入深度、钢水处理容量等对循环流量的影响关系.结果表明,循环流量随插入管内径、驱动气体流量、驱动气体用喷嘴个数、气泡行程、插入管浸入深度的增加而加大. 相似文献
10.
11.
《钢铁冶炼》2013,40(6):431-438
AbstractA numerical method has been employed to investigate the flow field and mixing characteristic in the Rheinsahl–Heraeus (RH) degasser with side–bottom blowing. The numerical results showed that stream flows in the up snorkel, the vacuum chamber, the down snorkel and the ladle form a large rectangular circulation zone in the RH degasser with side–bottom blowing, which can enhance the circulation flow rate effectively. For an RH with side–bottom blowing, when the included angle of the line between bottom blowing location and ladle centre and the line between two snorkels is zero, the circulation flow rate increases initially with increasing dimensionless distance between the bottom blowing location and the ladle centre and then decreases, while the mixing time increases with increasing dimensionless distance. On the other hand, when the dimensionless distance is 0·2, both the circulation flow rate and the mixing time decrease with the increasing included angle initially, reach their minimum value and then increase. The optimum values for the dimensionless distance and the included angle to achieve large circulation flow rate and small mixing time are 0·2 and π/4 in the present work. 相似文献
12.
13.
14.
为了提高RH精炼效率,缩短精炼时间。以某钢厂150 t RH真空精炼装置为原型,建立相似比为1∶4的水模型,研究底吹孔个数与底吹流量的影响。结果表明,实施底吹工艺后,RH循环流量和混匀时间相较无底吹时都有明显改善。相同底吹流量情况下,单孔底吹对循环流量提升效果明显优于双孔底吹工况,如当底吹流量为90 L/min时,单孔底吹工况相较于无底吹工况循环流量增加34%,而双孔底吹工况只增加13%。底吹流量小于90 L/min时,单孔底吹和双孔底吹工况下混匀时间相差不大。底吹流量大于90 L/min时,双孔底吹工况下混匀时间反而有所增加。建议生产现场采用单孔底吹工艺,如采用双孔底吹工艺时,底吹流量应小于90 L/min。 相似文献
15.
采用物理模拟方法对单管 RH 真空精炼过程流场的循环流动、混合特性等进行了研究,建立与 RH 真空精炼装置原型相似比为1∶5的水模型,研究了不同工艺参数对单管 RH 装置内钢液循环流动的影响。对比实验测量数据发现,增大吹氩量和浸渍管插入深度以及浸渍管有效横截面有利于提高循环流量,减小均混时间;在相同的实验条件下,椭圆形浸渍管 RH 比传统浸渍管 RH 的循环流量要大15%以上,单管 RH 的均混时间比传统RH 可以缩短20%;单管 RH 钢包底部吹氩位置位于距钢包中心0.4R(R 是钢包半径)处时,均混时间最短。 相似文献
16.
The three–dimensional flow field of molten steel in an 80–ton single snorkel vacuum refining furnace has been mathematically simulated to attain the optimal configuration and operation parameters, such as the bottom blowing Ar flow rate, the eccentric position of bottom blowing Ar port at ladle bottom, the single snorkel inner diameter, and the single snorkel immersion depth into molten steel. The mathematical simulation results show that a stable flow field of molten steel can be achieved in 70–second; meanwhile, the maximal circulation intensity of molten steel in the 80–ton single snorkel vacuum refining furnace can be found on a cross–section with y as 0 mm based on the middle of ladle bottom as circular point of the Cartesian space coordinate under the condition of injecting Ar gas on x coordinate considering the asymmetry of flow field for molten steel in the single snorkel vacuum refining furnace. The recommended parameters of the 80–ton single snorkel vacuum refining furnace with ideal circulation intensity as 970.1 kg/s are the bottom blowing Ar flow rate as 450–500 Nl/min, the eccentric position of bottom blowing Ar port as 250 mm, the single snorkel inner diameter as 1000 mm, and the single snorkel immersion depth as 500 mm. 相似文献
17.
18.