固体中相互扩散和离子电导率中的空风因子和曼宁因子

I. Belova, G. Murch
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引用次数: 0

摘要

在结晶固体中,在合金中的化学相互扩散、离子电导率和辐射损伤退火等过程中,不可避免地会存在空位的净通量。在大多数情况下,当不同种类的原子在一个空位的净通量内具有不同的空位跳跃率时,就会出现空位风效应的现象。这种效应最早是在20世纪60年代由已故的约翰·曼宁博士发现的。这是一种微妙的现象,由于在驱动力中相对于两种或两种以上漂移原子的空位平衡浓度的局部重新分布而产生。这种效应体现在各种“空风因子”(其中一些现在有时被称为曼宁因子)中,这些因子通常来自非零的非对角线Onsager现象输运系数和示踪相关因子的非单位值。本文对其效果进行了回顾和讨论。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The Vacancy-Wind Factor and the Manning Factor Occurring in Interdiffusion and Ionic Conductivity in Solids
In crystalline solids, during such processes as chemical interdiffusion in alloys, ionic conductivity and the annealing out of radiation damage there will inevitably be a net flux of vacancies. In most cases, when different species of atoms have different jump rates with vacancies within a net flux of vacancies, the phenomenon of the vacancy-wind effect will occur. This effect was first discovered in the 1960s by the late Dr John Manning. It is a subtle phenomenon that comes about because of the local redistribution of the equilibrium concentration of vacancies with respect to two or more species of drifting atoms in a driving force. The effect is captured in various ‘vacancy-wind factors’ (some of which are now sometimes called Manning factors) which formally arise from non-zero off-diagonal Onsager phenomenological transport coefficients and non-unity values of the tracer correlation factors. In this paper, the effect is reviewed and discussed.
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