class='kwd-title'>Keywords: Microsegregation, So'/> Modeling diffusion-governed solidification of ternary alloys – Part 2: Macroscopic transport phenomena and macrosegregation
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Modeling diffusion-governed solidification of ternary alloys – Part 2: Macroscopic transport phenomena and macrosegregation

机译:三元合金扩散控制的凝固建模–第2部分:宏观传输现象和宏观偏析

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摘要

class="kwd-title">Keywords: Microsegregation, Solidification, Macrosegregation, Ternary alloy, Steel ingot class="head no_bottom_margin" id="ab015title">AbstractPart 1 of this two-part investigation presented a multiphase solidification model incorporating the finite diffusion kinetics and ternary phase diagram with the macroscopic transport phenomena (Wu et al., 2013). In Part 2, the importance of proper treatment of the finite diffusion kinetics in the calculation of macrosegregation is addressed. Calculations for a two-dimensional (2D) square casting (50 × 50 mm2) of Fe–0.45 wt.%C–1.06 wt.%Mn considering thermo-solutal convection and crystal sedimentation are performed. The modeling result indicates that the infinite liquid mixing kinetics as assumed by classical models (e.g., the Gulliver–Scheil or lever rule), which cannot properly consider the solute enrichment of the interdendritic or inter-granular melt at the early stage of solidification, might lead to an erroneous estimation of the macrosegregation. To confirm this statement, further theoretical and experimental evaluations are desired. The pattern and intensity of the flow and crystal sedimentation are dependent on the crystal morphologies (columnar or equiaxed); hence, the potential error of the calculated macrosegregation caused by the assumed growth kinetics depends on the crystal morphology. Finally, an illustrative simulation of an engineering 2.45-ton steel ingot is performed, and the results are compared with experimental results. This example demonstrates the model applicability for engineering castings regarding both the calculation efficiency and functionality.
机译:<!-fig ft0-> <!-fig @ position =“ anchor” mode =文章f4-> <!-fig mode =“ anchred” f5-> <!-fig / graphic | fig / alternatives / graphic mode =“ anchored” m1-> class =“ kwd-title”>关键字:微偏析,凝固,宏观偏析,三元合金,钢锭 class =“ head no_bottom_margin” id = “ ab015title“>摘要这项由两部分组成的研究的第1部分介绍了一个多相凝固模型,该模型将有限扩散动力学和三元相图与宏观输运现象结合在一起(Wu等人,2013)。在第2部分中,讨论了在宏观偏析计算中适当处理有限扩散动力学的重要性。考虑到热溶质对流和晶体沉降,对Fe–0.45 wt。%C–1.06 wt。%Mn的二维(2D)方形铸件(50×50 mm 2 )进行了计算。模拟结果表明,经典模型(例如,Gulliver-Scheil或杠杆法则)所假定的无限液体混合动力学可能无法适当考虑凝固初期的枝晶间或粒间熔体的溶质富集。导致对宏分离的错误估计。为了证实这一说法,需要进一步的理论和实验评估。流动的形式和强度以及晶体的沉积取决于晶体的形态(柱状或等轴状)。因此,由假定的生长动力学引起的所计算的宏观偏析的潜在误差取决于晶体形态。最后,对工程2.45吨钢锭进行了说明性仿真,并将结果与​​实验结果进行了比较。该示例说明了在计算效率和功能性方面对工程铸件的模型适用性。

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