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強制流動對Mg–9%Al合金定向凝固組織演化的模擬研究

Simulation of forced flow on the evolution of directional solidification microstructure of Mg–9%Al alloy

  • 摘要: 基于歐拉多相流技術與元胞自動機方法構建了鎂合金凝固組織預測模型,研究了無流動、x方向流動和y方向流動三種條件下Mg–9%Al合金定向凝固過程中的成分和組織演化過程. 研究結果表明,無流動作用時鎂合金枝晶呈現互為60°夾角生長,并在凝固后期出現與一次枝晶呈60°夾角二次枝晶形貌,凝固組織具有密排六方(HCP)晶體結構特征,驗證了該模型的可靠性. 由于x方向的流動作用下,與無流動結果相比較,迎流方向枝晶生長較快并出現發達的二次枝晶形貌,研究表明由于枝晶前端排出的溶質受流動影響被運輸到枝晶后端區域,從而使前端區域具有更大的過冷度,提升了凝固驅動力. 由于y方向流動的存在,枝晶呈現不對稱生長,其中部分枝晶生長方向偏轉約3°,研究表明迎流枝晶前沿的溶質被運輸并富集在其他枝晶生長區域,最終使其發生了生長偏轉;進一步分析枝晶生長前沿的流場和成分分布信息發現,枝晶生長過程中流動引起的 \boldsymbolu_\mathrml\nablac_\textl 值在固液界面處的不對稱分布是導致枝晶生長發生偏轉的主要原因.

     

    Abstract: In this paper, a solidification model of magnesium alloy based on the Eulerian multiphase flow technique and cellular automata method is proposed to investigate the evolutions of aluminum concentration and solidification microstructure during the directional solidification of magnesium alloy with 9% (mass fraction) aluminum concentration under three types of boundary conditions, i.e., no flow, forced flow in the x-direction, and forced flow in the y-direction. The numerical simulations reveal that the dendrites of magnesium alloy grow at an angle of 60° to each other for the no-flow condition. In addition, secondary dendrites are also found in the late period of solidification, which grow at an angle of 60° to the primary dendrites. Both characteristics of primary dendrites and secondary dendrites demonstrate that the simulated solidification microstructure has a characteristic of crystal solidification with the hexagonal closed-packed structure, which confirms the reliability of the model. For the condition of forced flow in the x-direction, the main difference between this case and the no-flow condition is that the dendrites grow faster along the direction of the melt flow. Moreover, the characteristics of well-developed secondary dendrites are also found in the late solidification period for this condition. The main reason for current solidification phenomena is that the rejected solute in the vicinity of liquid–solid interface is transported along the melt flow during the solidification and accumulates in the rear of the dendrites. The decrease in aluminum concentration due to the melt flow in the area of dendritic tips will increase the supercooling, which finally advances the dendrite growth. Conversely, for the condition of forced flow in the y-direction, asymmetric growths of dendrites appear, and the preferred orientation for some dendrites has deflected about 3° compared with the no-flow condition. The numerical simulations indicate that the rejected solute is transported along the melt flow from one side of the dendrite to another side due to the forced flow in the y-direction, which results in the asymmetric distribution of aluminum concentration and the forming asymmetric characteristics of dendrites. Meanwhile, \boldsymbolu_\textl\nabla c_1 represents the formation mechanism of the asymmetric morphology of dendrites. The results show that it promotes solidification when \boldsymbolu_\textl\nabla c_1 > 0 and suppresses the dendrite growth when it is negative. The \boldsymbolu_\textl\nabla c_1 in the vicinity of the liquid–solid interface is seen as asymmetric distribution due to the forced flow in the y-direction during the solidification, which finally results in the deflection of the dendrite growth.

     

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