球形颗粒表面成核转变动力学及晶界成核转变新模型

N. V. Alekseechkin
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引用次数: 3

摘要

在适用于该问题的Kolmogorov方法框架下,推导了非等温和等温表面有成核的球形粒子的转换体积分数方程。确定了控制转化动力学的特征参数;后者的研究特别强调了Avrami指数的时间行为。结果表明,在特征参数较大时,表面成核相变与体形成核相变在性质上存在差异,这是由于在相变的早期,在表面本身完全转变之后出现了一维径向生长的新相。这种效应也表现在粒径分布的粒子系综和晶界成核转变中。数值计算采用研磨获得的颗粒固有的对数正态分布,并显示在时间上拉伸相同颗粒系综的体积分数和avrami指数依赖关系。提出了一种新的晶界成核变换模型,用以替代随机平面的Cahn模型;它是基于大小分布的球形粒子的集合,具有生长的核跨越晶界的可能性。这一过程的动力学与单个粒子的动力学一样,是由相同的特征参数控制的,并且在质量上不同于卡恩模型。特别是,在大块金属玻璃结晶的实验曲线上观察到,在较大的控制参数值处,对数体积分数图以特征弯曲结束。这一特性连同图的整体形式直接表明了金属玻璃的晶粒(多团簇)结构和团簇间边界的成核。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Kinetics of the Surface-Nucleated Transformation of Spherical Particles and New Model for Grain-Boundary Nucleated Transformations
Equations for the transformed volume fraction of a spherical particle with nucleation on its surface, both nonisothermal and isothermal, are derived in the framework of Kolmogorov method adapted for this problem. Characteristic parameters governing the transformation kinetics are determined; the latter is studied with particular emphasis on the Avrami exponent temporal behavior. It is shown that the surface-nucleated transformation qualitatively differs from the bulk-nucleated one at large values of the characteristic parameters due to the one-dimensional radial growth of the new phase occurring after the complete transformation of the surface itself at the early stage of the process. This effect also manifests itself in the considered ensemble of size-distributed particles and in the grain-boundary nucleated transformations. The logarithmic normal distribution inherent for the particles obtained by grinding is employed for numerical calculations and shown to stretch temporally the volume-fraction and Avrami-exponent dependences for the ensemble of identical particles. A new model for grain-boundary nucleated transformations alternative to the Cahn model of random planes is offered; it is based on the ensemble of size-distributed spherical particles with the possibility for a growing nucleus to cross grain boundaries. The kinetics of this process is shown to be governed by the same characteristic parameter, as for a single particle, and qualitatively differs from the Cahn-model one. In particular, the logarithmic volume-fraction plot at large values of the governing parameter ends by a characteristic bend observed on experimental curves for the crystallization of bulk metallic glasses. This peculiarity together with the form of the plot as a whole directly indicates to the grain (polycluster) structure of metallic glasses and nucleation at intercluster boundaries.
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