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A mean field theory for diffusion in a dilute multi-component alloy: a new model for the effect of solutes on self-diffusion

机译:稀释多组分合金中扩散的平均场理论:溶质对自扩散影响的新模型

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A new extension of the self-consistent mean field (SCMF) theory is developed to describe diffusion in dilute alloys, special attention being paid to the problem of self-diffusion in the presence of solute atoms. We start from a microscopic model of the atom-vacancy exchange frequency including nearest neighbour (nm) interactions and derive kinetic equations from a Master equation. The non-equilibrium distribution function is expressed through time-dependent effective interactions. Their range of interaction is controlling the level of description of the paths of a vacancy after a first exchange. In contrast to the previous diffusion models devoted to concentrated alloys, the present formulation makes appear into the final result several exchange frequencies associated to a given atom depending on the chemical species of the atoms nearby. A first approximation restricted to nn effective interactions yields analytical expressions of the transport coefficients of a face centered cubic dilute binary alloy. The phenomenological coefficients are equivalent to the ones obtained using the five-frequency model within the first shell approximation. A new expression of the self-diffusion coefficient is proposed and compared to Monte Carlo (MC) simulations using the same atomic diffusion model. The SCMF theory reproduces the main tendencies of the MC simulations, in particular within the random alloy region where the recent five-frequency model was not satisfying. The limitations and future improvements of the SCMF approach are easily related to the range of the effective interactions considered.
机译:自洽平均场(SCMF)理论的新扩展被开发来描述稀合金中的扩散,尤其要注意溶质原子存在下的自扩散问题。我们从原子-空位交换频率的微观模型(包括最近的邻居(nm)相互作用)开始,并从Master方程中得出动力学方程。非平衡分布函数通过与时间有关的有效相互作用来表示。它们的交互作用范围控制着第一次交换后空缺路径描述的水平。与先前致力于浓缩合金的扩散模型相反,本公式根据最终原子的化学种类,在最终结果中出现了与给定原子相关的几种交换频率。限于nn有效相互作用的一阶近似值可得出面心立方稀二元合金的传输系数的解析表达式。现象学系数等于在第一层近似中使用五频模型获得的现象系数。提出了一种自扩散系数的新表达式,并将其与使用相同原子扩散模型的蒙特卡洛(MC)仿真进行了比较。 SCMF理论再现了MC模拟的主要趋势,特别是在最近的五频模型不令人满意的随机合金区域内。 SCMF方法的局限性和未来的改进很容易与所考虑的有效交互作用的范围有关。

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