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NON-ISOTHERMAL OR NON-ISOBARIC KINETIC MODELLING OF THE REDUCTION OF U_3O_8 INTO UO_2 BY HYDROGEN

机译:氢还原U_3O_8到UO_2的非等温或非等温动力学模型

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摘要

A method for the kinetic modelling of non-isothermal and / or non-isobaric successive reactions in powders is presented, and illustrated with the reduction of U_3O_8 into UO_2 by hydrogen. This transformation involves two intermediate compounds, U_3C_(8-x) and U_4O_9. The principle of the method was based on the kinetic modelling of the three reactions by means of the rate equations dα_i/dt=φ_i(T,P)E_i(α), for i=1 to 3, with φ_i(T, P), in mol.m~(-2).s~(-1), and E_i, in m~2.mol~(-1). A mechanism involving several elementary steps (interface, diffusion) was proposed for each reaction; then, the determination of the rate-limiting step, due the study of the influence of the hydrogen partial pressure, gave the expressions of the functions φ_i(T, P) and E_i. Moreover, it was taken into account a particle size distribution for the theoretical expression of the rates. The resulting theoretical rate was obtained by means of a linear combination of the rates dα_i/dt, and successfully compared to the experiments performed in non-isothermal or non-isobaric conditions.
机译:提出了一种用于粉末中非等温和/或非等压连续反应动力学模型的方法,并通过氢气将U_3O_8还原为UO_2进行了说明。此转换涉及两个中间化合物U_3C_(8-x)和U_4O_9。该方法的原理基于三个反应的动力学建模,其中速率方程为dα_i/ dt =φ_i(T,P)E_i(α),对于i = 1到3,其中φ_i(T,P) ,以mol.m〜(-2).s〜(-1)表示,E_i,以m〜2.mol〜(-1)表示。对于每个反应,提出了一种涉及几个基本步骤(界面,扩散)的机理。然后,通过研究氢分压的影响,确定限速步骤,给出了函数φ_i(T,P)和E_i的表达式。此外,对于速率的理论表达,考虑了粒度分布。通过比率dα_i/ dt的线性组合获得了理论值,并成功地与非等温或非等压条件下进行的实验进行了比较。

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