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Numerical Simulation for Effect of Inlet Cooling Rate on Fluid Flow and Temperature Distribution in Tundish

QU Tian-peng , LIU Cheng-jun , JIANG Mao-fa

钢铁研究学报(英文版)

The fluid flow in tundish is a non-isothermal process and the temperature variation of stream from teeming ladle dominates the fluid flow and thermal distribution in tundish. A numerical model was established to investigate the effect of inlet cooling rate on fluid flow and temperature distribution in tundish based on a FTSC (Flexible Thin Slab Casting) tundish. The inlet cooling rate varies from 0.5 to 0.25 ℃/min. Under the present calculation conditions, the following conclusions were made. When the stream temperature from teeming ladle drops seriously (for inlet cooling rate of 0.5 ℃/min), there is a “backward flow” at the coming end of casting. The horizontal flow along the free surface turns to flow along the bottom of tundish. The bottom flow shortens the fluid flow route in tundish and deteriorates the removal effect of nonmetallic inclusions from molten steel. Nevertheless, when the inlet cooling rate decreases to 0.25 ℃/min, the horizontal flow is sustained during the whole casting period. The present research provides theoretical directions for temperature control in teeming ladle and continuous casting tundish during production of advanced steels.

关键词: tundish , thermal distribution , unsteady , numerical simulation

Modeling of an Impinging Oxygen Jet on Molten Bath Surface in 150 t EAF

HE Chun-lai , ZHU Rong , DONG Kai , QIU Yong-quan , SUN Kai-ming

钢铁研究学报(英文版)

A transient three-dimensional mathematical model has been developed to analyze the three-phase flow in a 150 t EAF (electric arc furnace) using oxygen. VOF (multiphase volume of fluid) method is used to simulate the behaviors of molten steel and slag. Numerical simulation was conducted to clarify the transient phenomena of oxygen impingement on molten bath. When oxygen jet impinges on the surface of molten bath, the slag layer is broken and the penetrated cavity in molten steel is created. Simultaneously, the wave is formed at the surface of uncovered steel on which the slag layer is pushed away by jet. The result of numerical simulations shows that the area and velocity of uncovered steel created by impingement, jet penetration depth change from 0.10 m2, 0.0125 m/s, 3.58 cm to 0.72 m2, 0.1445 m/s, 11.21 cm, when the flow rate of an oxygen lance varies from 500 to 2000 m3/h. The results have been validated against water model experiments. More specially, the relation between the penetration depth and oxygen flow rate predicted by numerical simulation has been found to agree well with that concluded by water model.

关键词: electric arc furnace , three-phase flow , numerical simulation

二辊斜轧延伸大口径P92厚壁管分层缺陷倾向性研究

尹元德,,李胜祗,康永林,王鹏展,王向东,李国涛

钢铁

为研究不同轧辊转速、送进角、轧辊入口锥角等工艺参数对大口径厚壁P92钢管二辊斜轧延伸过程分层缺陷形成倾向性的影响,借助于商用有限元软件MSC.SuperForm,对不同工艺条件下大口径厚壁P92钢管二辊斜轧延伸过程进行了三维热力耦合模拟;采用Oyane韧性断裂准则分析了轧件损伤场及钢管分层缺陷的倾向性。研究结果表明:钢管内表邻近顶头接触区存在破裂高危带,轧件最大损伤特征值随轧辊转速的降低、送进角和轧辊入口锥角的增大而减小,发生分层缺陷的倾向性降低。此研究为揭示钢管分层缺陷形成机制,确定缺陷发生的敏感工况,制定防止或减轻分层缺陷的有效措施提供科学依据。

关键词: 大口径P92厚壁管 , two-roll rotary elongating , technological parameter , lamination defect , numerical simulation

两种不同强塑性薄钢板抗弹性能的试验和数值模拟

肖红亮,时捷,曹文全,雍岐龙,董瀚

钢铁

利用51B式7.62mm手枪弹对不同强度和塑性的薄钢板进行枪击试验,采用ANSYS/LS-DYNA软件对试验过程进行数值模拟,对试验和数值模拟过程的钢板破坏形貌、背凸高度、残余弹丸长度等宏观形貌进行比较。结合抗弹过程中弹丸和钢板消耗的能量,分析了强度和塑性对钢板抗弹性能的影响。结果表明:尽管两种钢板的抗拉强度和断后伸长率差异较大,但其抗51B式7.62mm手枪弹性能相当。试验和数值模拟结果吻合较好,模拟方法能够正确地反映弹丸冲击靶板过程。因较高强度钢板使弹丸变形消耗的能量大于较低强度钢板,塑性较好钢板本身变形消耗的能量大于较低塑性钢板,从而解释了两种钢板抗弹性能相当的试验结果。

关键词: 薄钢板 , 51B type 7.62mm pistol bullet , energy absorption , numerical simulation

侧孔长水口两流非对称中间包流场优化

赵岩,雷洪,周骏,,陈海耿,孙中强,邢国成

钢铁

中间包流体流动直接影响连铸坯的质量,为了缩小非对称中间包两流之间的流动差异,利用水模型和数值模拟方法,研究了侧孔长水口中间包流体流动特性。研究结果表明:直通型长水口、圆形湍流控制器和单挡墙结构中间包两出口流体差异较大,侧孔长水口和多孔挡墙结构中间包两流之间平均停留时间差异是直通型长水口中间包的3/4,且近长水口侧出口的平均停留时间延长7.7%。

关键词: 非对称中间包 , shroud with side-hole , average residue time , water model , numerical simulation

宽度变化对板坯连铸结晶器流场影响的数值模拟

唐德池,冯捷,李永林,朱立新

钢铁

运用fluent 6.3对板坯连铸结晶器进行数值计算,研究结晶器宽度对流场的影响。结果表明:对于230mm厚结晶器,随结晶器宽度增加,其液面的最大水平流速减小,但减小的幅度趋缓,液面最大垂直速度和冲击点处速度逐渐减小;宽度分别为1400、1600和2150mm时,液面水平流速达到最大时分别为距离窄边460、540和750m处,冲击点位置分别距离液面0.37、0.40和0.46m,冲击点的速度分别为5.2、4.4和2.5cm/s。

关键词: 结晶器 , flow field , numerical simulation

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