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The cooling process of steel strips on an industry run‐out table (ROT) is simulated using an 1D model. In this model, the water bank information is not handled and the ROT directly consists of the jetlines. The simulation creates an advantage to study independently the spacing of jetlines on the cooling effect. In addition, a novel approach is used for time stepping in this study. First, five numbers of time steps are defined for different cooling zones and each number can be determined according to the accuracy requirement and the strip speed. Thus, the time step size is not constant and the total number of time steps can be reduced. Second, each time step is identified with a flag to indicate its belonging to the different zones. With this approach, tracking is not needed and none of the water cooling zones will be jumped over. The predicted coiling temperatures of 1D model simulations are in good agreement with the field measurements. 相似文献
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The solidification of low carbon (LC) steels on metallic substrates was investigated with a twin roll caster and a model mould. The substrate materials were steel, Ni, and two copper alloys, which are typical for the industrial construction of moulds. Heat flux density, heat transfer coefficient, growth rate, and cooling rate were evaluated. 相似文献
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热带钢超快速冷却条件下的对流换热系数研究 总被引:4,自引:0,他引:4
建立了热带钢超快速冷却过程的导热微分方程,采用有限差分方法计算了薄带钢实现超快速冷却(对于4 mm以下的薄带钢,冷却速率可达300℃/s)所需的带钢表面对流换热系数.同时,在实验室条件下采用厚度为20 mm的钢板进行了超快速冷却试验,得到了超快速冷却条件下的带钢表面对流换热系数与冷却水流量的关系.结果表明,在一定水流量范围内随着冷却水量的增加,带钢表面换热系数逐渐增加;采用所确定的换热系数对不同厚度钢板得到的温降曲线与实测值吻合较好,具有较高的精度. 相似文献
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为求解换热系数模型,以大量现场数据与热传递机制为基础,建立换热系数回归模型并使用ANSYS有限元软件对钢板冷却过程进行模拟,获取淬火过程中间数据。通过非线性回归算法对模型参数进行回归计算,最终取得整个淬火过程的换热系数公式。解决了现场无法测量淬火过程温度值,难以求解换热系数的难题。 相似文献
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Using a unique pilot facility a series of tests were conducted using three top jets to simulate the heat transfer that occurs during run‐out table (ROT) cooling. Steel samples instrumented with internal thermocouples were tested on this facility and the effect of top jet configuration (nozzle spacing of 40 to 115mm), and water flow rate (15 and 30 1/min) were quantified using moving plate samples. The multiple top jet work indicated that heat transfer across the plate width varies significantly and is high directly under the nozzle but decreases rapidly away from the nozzle in the interaction region. As cooling progresses a much larger wetted region occurs and more uniform cooling is experienced across the plate. Multiple jet cooling experiments have also confirmed that nozzle spacing does have an effect on heat transfer. This effect is predominate in the interaction region where closer nozzle spacing leads to enhanced and more uniform heat transfer in the lateral direction across the plate width away from the nozzle. As expected higher water flow rates led to higher heat transfer both under the nozzle and in the interaction region. 相似文献
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The heat transfer coefficient between spray water droplets and hot surface is measured in the laboratory. The effect of spray water flow rate, water pressure, spray distance of nozzle from the surface of strand, spray water temperature on the heat transfer is made a detail studied. And meanwhile, the effect of the strand surface FeO scale on the heat transfer is also investigated. According to the experimental results, the influence of above factors on the heat transfer coefficient has been discussed and a experience formula between the heat transfer coefficient and spray water flow rate is given out. 相似文献
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CSP和FTSC工艺结晶器的冷却结构及传热能力 总被引:1,自引:0,他引:1
结合实际生产数据,比较和分析了CSP及FTSC工艺结晶器的冷却结构及传热能力,结果表明,热流密度计算模型中,FTSC和CSP结晶器内传热区高度分别为1 200 mm和1 010 mm,相同工况下二者的传热能力相近;CSP结晶器采用42条凹型水道及20条内径11 mm的圆型水道进行组合冷却,FTSC结晶器采用72条内径14 mm的圆型水道进行冷却;弯月面处FTSC结晶器铜板热面温度高于银铜的再结晶温度,铜板将发生局部变形,这是造成镀层龟裂或铜板裂纹的主要原因。 相似文献
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在前人对单个液滴碰撞传热解析研究的基础上,通过实验与理论分析,建立了气-水喷雾冷却在膜态沸腾区的传热数学模型。采用此模型,可以在已知气-水喷嘴的冷态参数(流量密度、液滴粒径、液滴速度等)的情况下,模拟计算出该喷嘴的传热特性。计算结果与实验数据在可比的范围内基本吻合。 相似文献
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棒材穿水冷却温度场的仿真研究 总被引:1,自引:0,他引:1
针对棒材穿水冷却过程,采用有限元仿真软件ANSYS对其进行了温度场仿真,建立了棒材温度场预报模型。该模型的仿真结果与实测值相吻合,能够准确地预测棒材穿水冷却过程的温度分布,为棒材性能预报与优化控冷工艺提供依据。 相似文献
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以超高强度钢(UHSS)为对象,研究板坯连铸二冷设计。首先,基于凝固传热学基本理论,建立了二维板坯瞬态传热数学模型;其次,根据高温塑性实验曲线,结合二冷区冶金原则,确定二冷区各段终点的表面目标温度;最后,根据制定的铸坯表面目标温度,采用增量型PID算法调整二冷区各回路的水量。 相似文献
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基于热-黏弹塑性本构方程建立了大钢锭凝固时热-流-力耦合的3D有限元模型,并对8.5t钢锭浇注过程中不同位置处热流密度、气隙宽度和界面换热系数的变化规律进行了模拟分析。结果表明,钢水与钢锭模刚刚接触时的热流密度和换热系数最大,二者随后迅速下降,且角部区域的下降趋势略大于面部。凝固初期时热流密度和换热系数的最大值位置并非位于面部中心,而是在1/4宽度处;由于宽面对钢水静压力的抵抗作用小于窄面,其界面热流密度和换热系数也略大于窄面。凝固中后期时,换热系数的区域差异逐渐趋于不明显。同时,建立了基于凝固时间和界面温度的平均换热系数的反算模型。应用2个模型所求结果计算的钢锭和钢锭模温度变化与实测值及热-流-力耦合模型结果基本一致。进一步研究发现,界面换热系数随温度的变化规律可推广应用到3~30t钢锭的模拟研究中,计算结果与实际更为符合。 相似文献