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Phase-field modeling of microstructural pattern formation during directional solidification of peritectic alloys without morphological instability

机译:微观结构模式形成的相场模拟   没有形态学的包晶合金的定向凝固   不稳定

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摘要

During the directional solidification of peritectic alloys, two stable solidphases (parent and peritectic) grow competitively into a metastable liquidphase of larger impurity content than either solid phase. When the parent orboth solid phases are morphologically unstable, i.e., for a small temperaturegradient/growth rate ratio ($G/v_p$), one solid phase usually outgrows andcovers the other phase, leading to a cellular-dendritic array structure closelyanalogous to the one formed during monophase solidification of a dilute binaryalloy. In contrast, when $G/v_p$ is large enough for both phases to bemorphologically stable, the formation of the microstructurebecomes controlledby a subtle interplay between the nucleation and growth of the two solidphases. The structures that have been observed in this regime (in small sampleswhere convection effect are suppressed) include alternate layers (bands) of theparent and peritectic phases perpendicular to the growth direction, which areformed by alternate nucleation and lateral spreading of one phase onto theother as proposed in a recent model [R. Trivedi, Metall. Mater. Trans. A 26, 1(1995)], as well as partially filled bands (islands), where the peritecticphase does not fully cover the parent phase which grows continuously. Wedevelop a phase-field model of peritectic solidification that incorporatesnucleation processes in order to explore the formation of these structures.Simulations of this model shed light on the morphology transition from islandsto bands, the dynamics of spreading of the peritectic phase on the parent phasefollowing nucleation, which turns out to be characterized by a remarkablyconstant acceleration, and the types of growth morphology that one might expectto observe in large samples under purely diffusive growth conditions.
机译:在包晶合金的定向凝固过程中,两个稳定的固相(母相和包晶)竞争性地生长成杂质含量高于任一固相的亚稳态液相。当母体固相或固相固相在形态上不稳定时,即,对于较小的温度梯度/生长速率比($ G / v_p $),一个固相通常会长出并覆盖另一固相,从而导致与该固相相似的细胞树突状阵列结构在稀二元合金的单相凝固过程中形成。相反,当$ G / v_p $足够大以使两个相在形态上都稳定时,微结构的形成将受到两个固相的成核和生长之间微妙的相互作用的控制。在这种情况下观察到的结构(在对流效应被抑制的小样本中)包括垂直于生长方向的母相和包晶相的交替层(带),这些层是通过将一相交替成核和横向扩展到另一相而形成的在最近的模型中[R.特里维第(Metall)。母校反式A 26,1(1995)],以及部分充满的带(岛),其中包晶相没有完全覆盖连续生长的母相。为了探索这些结构的形成,我们开发了包晶层凝固的相场模型,以探索这些结构的形成。该模型的仿真揭示了从孤岛到能带的形态转变,成核后包晶相在母相上的扩散动力学,事实证明,它具有明显恒定的加速特性,并且在纯扩散性生长条件下,人们可能会在大型样品中观察到这种生长形态。

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