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1.
根据宝#连铸机中间包的实际操作工艺参数,在中间包结构内部加装吹气装置,进行了气-液两相的流动和传热耦合的数值模拟.模拟研究结果表明,底吹气可以显著改善中间包内钢水的流动特征,增加钢水流动的轨迹,延长钢水在中间包内的停留时间,提高中间包内钢水的混合程度;在坝堰中间加装吹气装置有助于均匀整个中间包内钢水的速度,减少中间包的死区体积分率,得到更好的冶金效果.  相似文献   

2.
模拟研究了中间包上使用狭缝式透气砖条件下,连铸中间包内气体体积分布和流场.结果表明,狭缝宽度和气体流量对气幕挡墙的形成影响显著;气体流量约为10 m3/h时,中间包内钢液的流动特性较好.  相似文献   

3.
采用CFD软件Fluent对漩流中间包内的流场进行了数值模拟,分析了漩流中间包内的流场特征,以及漩流室的加入,中间包内的流动形态.模拟结果表明,由于漩流室的加入使湍动能耗散主要集中在漩流室内部,有利于夹杂物的聚合长大;漩流室的加入可改善钢液的流动状态,利于夹杂物的上浮。由于入口位置的非对称布置,造成了漩流中间包内的流场在入口区呈明显的非对称分布,这些结果为进一步优化漩流中间包内漩流室的位置和中间包挡墙参数提供了理论依据.  相似文献   

4.
采用FLUENT软件对中天钢铁集团公司七流连铸中间包内型流场进行数值模拟,研究速度矢量、湍动能和流体迹线分布规律,分析中间包内有无C型挡墙加入的流场特征.模拟结果表明,加入C型挡墙使中间包的湍动能主要集中在入口区域,利于延长包内各流的平均停留时间,减小死区体积分数,包内各流流动更加均匀,有利于钢液温度和成份的均匀.  相似文献   

5.
六流小方坯连铸中间包内型优化设计水模研究   总被引:5,自引:1,他引:4  
通过水力学模型试验,研究了中间包内的流场和流动分布。研究表明:现场中间包内型结构欠合理。试验通过在中间包模型内加设V型档墙,并调整挡墙上开孔的数量、大小、倾角和位置来控制流体流动的方式,从而使流场得以改善,满足生产实际要求,保证了连铸机的正常操作和铸坯质量。  相似文献   

6.
广钢高效连铸改造的中间包内型优化   总被引:2,自引:0,他引:2  
广钢连铸中间包采用三流和入流非对称布置的结构,生产中钢水流动不稳定,温度不均匀,为改变这种状况,有必要对中间包进行结构改造。在中间包冷态和热态水模型上,安装纵向局部挡墙和带导流孔“V”型挡墙,研究中间包内钢水流动和温度分布情况。模拟试验结果表明:“V”形挡墙能显著改善钢水的流动,使各流钢水平均停留时间趋于均衡,温度差减少,中间包内死区减少。此外,作者还给出了推荐的中间包改造方案。  相似文献   

7.
采用FLUENT软件对板坯连铸中间包内的流场和浓度场进行数值模拟,分析中间包内有无挡墙以及挡墙参数变化引起中间包内流场、浓度场的变化情况。模拟结果表明,湍流控制器与挡墙的优化配合使中间包内钢液的平均停留时间由502 s延长至573 s,死区体积分数由29.7%降为14.4%,优化挡墙与挡坝参数有利于钢液温度和成份的均匀,及夹杂物的上浮去除。  相似文献   

8.
根据相似原理,利用水模拟钢液流动来研究中间包内流场的流动状况,通过调节中间包内挡墙位置及其开孔大小来改善和优化中间包内的流场。对比计算机采集的RTD数据及用墨汁作为示踪剂的照片寻求出最优化方案。得出经过改进的中间包各流平均停留时间增加50-90s,死区体积由25%~30%降低到14%~19%,活塞流的体积比从8%~13%增加到26%-27%,优化了中间包内的流场。  相似文献   

9.
连铸中间包内流场与温度场的数值模拟   总被引:2,自引:0,他引:2  
针对国内某钢厂中间包,利用CFD软件FLUENT研究该中间包内传输现象,计算挡墙对中间包流场和温度分布的影响,结果表明设置合适的中间包挡墙,能明显改善中间包内的流场和温度场.  相似文献   

10.
基于数理模拟,对五流大方坯连铸中间包内钢水流动特性及温度场进行了研究.物理模拟结果表明:采用湍流控制器可明显延长钢水的响应时间和停留时间,采用梯形围墙有利于钢水在各流间合理分配,在2#、4#流水口下游设置挡坝,能够进一步改善中间包内钢水的流动特性.当采用稳流器+梯形围墙+挡坝的控流方式时,各流的流动特征参数一致,死区体积在25.0%以下,平均停留时间达15 min以上;数值模拟结果表明,采用本研究开发的控流方式,中间包内钢水温度分布合理,包内钢水最大温差在10℃以内,各流间出口钢水温差为2~3℃,有利于发挥中间包的冶金效果,保证连铸生产顺行和铸坯质量.  相似文献   

11.
Fluid flow characteristics in a four-strand tundish with gas blowing were studied by water modeling experiments.It is found that gas blowing can greatly improve the flow characteristics in the tundish with a turbulence inhibitor.It dramatically increases the peak concentration time,and greatly decreases the dead volume,and reduces the minimum residence time.The gas blowing location,gas flow rate,and porous plug area greatly influence the flow characteristics in the tundish;the gas blowing location near t...  相似文献   

12.
The metallurgical effect of a round tundish used to cast heavy steel ingots in machine works at present was evaluated through water modeling experiments.The flow control devices of the improved oval tundish,which was used instead of the round tundish,had been optimized.The results show that the residence time of the round tundish is short,its inclusion removal efficiency is too low,and it has more dead zones and an unreasonable flow field.Compared with the round tundish,the improved oval tundish with the optimized weir and dam has a better effect:its minimum residence time is prolonged by 38.1 s,the average residence time is prolonged by 233.4 s,its dead volume fraction decreases from 26% to 15%,and the ratio of plug volume fraction to dead volume fraction increases from 0.54 to 1.27.The inclusion removal efficiency also increases by 17.5%.  相似文献   

13.
Fluid Flow in Tundish Due to Different Type Arrangement of Weir and Dam   总被引:2,自引:1,他引:2  
Tundish is an important metallurgical reactor in the continuous casting process,In order to control the fluid flow in tundish and thus take full advantage of the residence time available for the removal of inclusions from molten steel,the effect of weir and dam on the fluid flow has been studied in a water model based on the characteristic number Froude and Reynold number similarity criteria.The residence time distribution curves of the flow were measured by SG800,The optimum arrangement of dam and weir and the nonstationary flow in tundish were discussed.The results show that the comnbination of weir and dam is benefit for the flow pattern in tundish,weir can prevent the upper recirculating flow.dam can cut off the bottom flow and turn to upwards,it is advantageous to separate the nometallic inclusions.Furthermore,it is importnat to exceed the critical depth of bath during exchange ladles,not only for the inclusion floatation but also for avoiding tundish slag drainage earlier.  相似文献   

14.
The behavior of fluid flow and particle motion in a 6-strand bloom caster tundish was investigated by a water model and numerical simulation. Compared with a device without flow control, the tundish with flow control has an important effect on the fluid flow pattern and inclusion removal. It is revealed that by non-isothermal process, which is real production condition, the fluid flow in tundish shows a strong buoyancy pattern, which drives particles to move upwards. The particle removal was quantitatively studied by mathematical and physical simulations.  相似文献   

15.
以某钢厂230t钢包为研究对象。通过实验水模型对现场生产过程的模拟,研究底吹透气元件的布置方式和吹氩流量对搅拌效果和夹杂物去除率的影响。结果表明.双透气元件吹氩优于单透气元件吹氩搅拌效果,0.6R-γ双透气元件布置方式最佳,混匀时间随吹气量和透气元件夹角的增大而减少;夹杂物的去除率取决于吹氩量和吹氩时间,在0.2~0.8L/min吹气量下,处理时间为0~4min时夹杂物去除效果最好,5~8min时可去除大部分夹杂物,24min左右可去除所有夹杂物。  相似文献   

16.
Numerical simulation on inclusion transport in continuous casting mold   总被引:3,自引:0,他引:3  
Turbulent flow, the transpor't of inclusions and bubbles, and inclusion removal by fluid flow, transport and by bubble flotation in the strand of the continuous slab caster are investigated using computational models, and validated through comparison with plant measurements of inclusions. Steady 3-D flow of steel in the liquid pool in the mold and upper strand is simulated with a finitedifference computational model using the standard k-εturbulence rondel. Trajectories of inclusions and bubhles tire calculated by integrating each local velocity, considering its drag and buoyancy forces, A "random walk" model is used to incorporate the effect of turbulent fluctuations on the particle motion. The attachment probability of inclusions on a bubble surface is investigated based on fundamental fluid flow simulations, incorporating the turbulent inclusion trajectory and sliding time of each individual inclusion along the bubble surface as a function of particle and bubble size. The chunge in inclusion distribution due to removal by bubble transport in the mold is calculated based on the computed attachment probability of inclusions on each bubble and the computed path length of the bubbles. The results indicate that 6%-10% inclusions are removed by fluid flow transport. 10% by bubble flotation, and 4% by entrapment to the submerged entry nozzle (SEN) walls. Smaller bubbles and larger inclusions have larger attachment probabilities. Smaller bubbles are more efficient for inclusion removal by bubble flotation, so Inng as they are not entrapped in the solidifying shell A larger gas flow rate favors inclusion removal by bubble flotation. The optimum bubble size should be 2-4mm.  相似文献   

17.
针对CSP中间包内冶金过程,建立中间包内钢水流场、温度场、夹杂物运动的数学模型,对不同挡墙和挡坝的5种组合方案的中间包钢水,从流动、传热和去夹杂能力等方面进行分析。结果表明:不同挡墙和挡坝的组合方案中,方案5效果最佳,其结构合理,钢液停留时间有效延长,利于夹杂物的上浮;没有明显的低温区域,中间包出口与入口的温差为5℃;对50μm的夹杂物能去除98.4%,对40μm的夹杂物去除率达到92.3%。  相似文献   

18.
精炼过程中进行钢包吹氩是一种去除钢中夹杂,提升其洁净度的重要手段。为快速且低成本地捕获最佳吹氩流量,通过流体分析软件FLUENT对钢包偏心底吹氩过程进行数值模拟。结果表明:在合适的吹气量下,气流会随着吹气时间的延长,在钢液中形成一个闭合的循环区域;吹气量从10 Nm3/h增大到30 Nm3/h,气流的平均动能和平均速度显著增大,死区比例则从21%下降到6%;当吹气量超过临界值30 Nm3/h时,进一步加大吹气量,死区比例趋于稳定,氩气利用率降低;吹气量为30 Nm3/h时达到最佳吹气量,此时钢液中的流体能够获得较大的平均湍动能和平均速度,且钢液中死区比例也达到最小,钢液获得较大的搅拌强度和搅拌区域。  相似文献   

19.
以某钢厂180t钢包为原型,进行超声波改善钢包熔池搅拌效果的冷态模拟实验。通过记录pH计示数变化研究底吹气体搅拌均混时间及超声波搅拌均混时间。实验结果表明,在底吹空气水模实验中,当吹气位置在距离中心为0.33R,流量为0.1m3/h时,底吹气体搅拌所需的均混时间最短为50s;超声波水模实验中,当波源伸入钢包的中心液面下25cm处,输出功率1.8kw,均混时间最短为35s;在超声波和底吹气体联合实验中。当吹气位置在距离中心为0.33R,流量为0.1m^3/h,波源伸入钢包的中心液面下25cm处,输出功率1.8kw时,均混时间最短为48s;可以看出超声波可明显缩短钢包均混时间,改善钢包精炼动力学条件。  相似文献   

20.
Fine bubbles will create when the inert gas is introduced to the high rapid steel stream within the shroud nozzle between ladle and tundish. The collision and attachment among the bubbles and fine inclusions will promote the floatation efficiency of inclusions in the tundish. The behaviors of the bubbles, such as the dispersion in shroud, coalescence and floatation in tundish, are studied. The results show that the maximum sizes of the bubbles in the water and steel flow within the shroud in the length of 1.2 m are 0.70-1.44 mm and 1.53-3.16 mm respectively when the flow rates are 0.006-0.016 m3/s; the terminal velocities of fine bubbles in the water and molten steel within the tundish are 0.02-0.2 and 0.05-0.6 m/s.  相似文献   

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