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Modelling mixed columnar-equiaxed solidification with melt convection and grain sedimentation - Part I: Model description

机译:具有熔体对流和颗粒沉降的混合柱状均等凝固模型-第一部分:模型描述

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摘要

Part I of this two-part investigation presents a volume-averaging multiphase solidification model that accounts for mixed columnar-equiaxed solidification, non-dendritic and dendritic crystal growth, nucleation of equiaxed grains, columnar primary dendrite tip tracking, melt flow, sedimentation of equiaxed crystals, and their influence on macrostructure and macrosegregation. Five distinct thermodynamic phases (phase regions) are defined: solid dendrites in equiaxed grains, the interdendritic melt between equiaxed dendrites, solid dendrites in columnar trunks, the interdendritic melt between trunk dendrites, and the extradendritic melt. These five phase regions are quantified by their volume fractions and characterized by their solute concentrations. The five phase regions are grouped into three hydrodynamic phases: equiaxed grains consisting of solid dendrites and interdendritic melt, columnar trunks consisting of solid dendrites and interdendritic melt, and extradendritic melt. The extradendritic melt is separated from the interdendritic melt with a grain envelope, whose profile connects the primary, secondary or tertiary dendrite tips to form a 'natural' enclosure of the equiaxed grains or columnar trunks. The envelope is further simplified as a volume-equivalent sphere for equiaxed grains, or as volume-equivalent cylinder for columnar trunks by use of morphological shape factors. Expansion of the envelopes during solidification is determined by dendrite growth kinetics, using the Kurz-Giovanola-Trivedi model for growth of columnar primary dendrite tips and the Lipton-Glicksman-Kurz model for growth of columnar secondary dendrite tips (radial growth of the columnar trunk) and equiaxed primary dendrite tips. The solidification of the interdendritic melt is driven by the supersaturation of the interdendritic melt and governed by the diffusion in the interdendritic melt region. Illustrative process simulations and model verifications are presented in Part II.
机译:这个由两部分组成的研究的第一部分介绍了一个体积平均的多相凝固模型,该模型说明了混合的柱状均等凝固,非树枝状和树枝状晶体的生长,等轴晶粒的成核,柱状初生枝晶尖端跟踪,熔体流动,等轴沉积晶体及其对宏观结构和宏观偏析的影响。定义了五个不同的热力学相(相区域):等轴晶状体中的固态树突,等轴晶状体之间的树突间熔体,柱状主干中的固体树突,主干树突状体之间的树突间熔体和树突外熔体。这五个相区通过其体积分数进行定量,并通过其溶质浓度进行表征。五个相区分为三个流体动力学相:等轴晶粒由固态树枝状晶体和枝晶间熔体组成,柱状主干由固态树枝状晶体和枝晶间熔体组成,以及枝晶外熔体。树突外熔体通过晶粒包膜与树突间熔体分离,其轮廓连接一次,二次或三次枝晶尖端,形成等轴晶粒或柱状主干的“天然”外壳。通过使用形态学形状因子,将包络进一步简化为等轴晶粒的体积等效球体,或圆柱状躯干的体积等效圆柱体。凝固过程中包膜的膨胀由枝晶生长动力学决定,使用Kurz-Giovanola-Trivedi模型用于柱状初级枝晶尖端的生长,使用Lipton-Glicksman-Kurz模型用于柱状次级枝晶尖端的生长(柱状主干的径向生长) )和等轴初级枝晶尖端。枝晶间熔体的凝固是由枝晶间熔体的过饱和驱动的,并且由枝晶间熔体区域中的扩散决定。第二部分介绍了说明性的过程仿真和模型验证。

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