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Thermodynamic mixing properties of the UO2-HfO2 solid solution: Density functional theory and Monte Carlo simulations

机译:UO2-HfO2固溶体的热力学混合性质:密度泛函理论和蒙特卡洛模拟

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摘要

HfO2 is a neutron absorber and has been mechanically mixed with UO2 in nuclear fuel in order to control the core power distribution. During nuclear fission, the temperature at the center of the fuel pellet can reach above 1300 K, where hafnium may substitute uranium and form the binary solid solution of UO2-HfO2. UO2 adopts the cubic fluorite structure, but HfO2 can occur in monoclinic, tetragonal, and cubic structures. The distribution of Hf and U ions in the UO2-HfO2 binary and its atomic structure influence the thermal conductivity and melting point of the fuel. However, experimental data on the UO2-HfO2 binary are limited. Therefore, the enthalpies of mixing of the UO2-HfO2 binary with three different structures were calculated in this study using density functional theory and subsequent Monte Carlo simulations. The free energy of mixing was obtained from thermodynamic integration of the enthalpy of mixing over temperature. From the DG of mixing, a phase diagram of the binary was obtained. The calculated UO2-HfO2 binary forms extensive solid solution across the entire compositional range, but there are a variety of possible exsolution phenomena associated with the different HfO2 polymorphs. As the structure of the HfO2 end member adopts lower symmetry and becomes less similar to cubic UO2, the miscibility gap of the phase diagram expands, accompanied by an increase in cell volume by 7-10% as the structure transforms from cubic to monoclinic. Close to the UO2 end member, which is relevant to the nuclear fuel, the isometric uranium-rich solid solutions exsolve as the fuel cools, and there is a tendency to form the monoclinic hafnium-rich phase in the matrix of the isometric, uranium-rich solid solution phase. (C) 2015 Elsevier B.V. All rights reserved.
机译:HfO2是一种中子吸收剂,已经与UO2机械混合在核燃料中,以控制堆芯功率分配。在核裂变期间,燃料芯块中心的温度可以达到1300 K以上,其中where可以替代铀并形成UO2-HfO2的二元固溶体。 UO2采用立方萤石结构,但HfO2可以单斜晶,四方晶和立方结构出现。 Hf和U离子在UO2-HfO2二元体中的分布及其原子结构会影响燃料的导热率和熔点。但是,有关UO2-HfO2二进制文件的实验数据有限。因此,在本研究中,使用密度泛函理论和随后的蒙特卡洛模拟,计算了UO2-HfO2二元与三种不同结构的混合焓。混合的自由能由混合焓随温度的热力学积分获得。从混合的DG中,获得二元相图。计算得出的UO2-HfO2二元化合物在整个组成范围内形成了广泛的固溶体,但是与不同的HfO2多晶型物相关的各种可能的析出现象。当HfO2末端成员的结构采用较低的对称性并变得与立方UO2相似时,相图的可混溶间隙扩大,并且随着结构从立方转变为单斜晶,细胞体积增加7-10%。在与核燃料相关的UO2末端构件附近,等轴测富铀固溶体在燃料冷却时溶解,并且有在等轴测铀铀基体中形成单斜晶ha富集相的趋势。富固溶相。 (C)2015 Elsevier B.V.保留所有权利。

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