Solubility of fission products (FPs) in spent nuclear fuels is a key issue in understanding their performance. In this study, a detailed density functional theory study on solubility of La, Nd, Zr and Mo in uranium dioxide (UO2) and triuranium octoxide (U3O8) was carried out. The most favorable sites of La, Nd, Zr and Mo were calculated by analyzing the solution energies of these four FP elements in UO2 and U3O8. Thermodynamic properties of FPs doping in UO2 as well as in U3O8 were determined from 0 K to 2000 K. The results reveal that the effect of FPs on thermodynamic properties of U3O8 is slightly larger than that of UO2 due to the presence of an oxygen vacancy in FP-doped U3O8. On this basis, the solubility of La, Nd, Zr and Mo in UO2 and U3O8 was predicted, showing a good agreement with available experiments. Subsequently, the difference in solubility behaviors was studied through electronic properties. The simulation results indicate that the solubility of La, Nd, Zr and Mo in U3O8 is much lower than that in UO2. Therefore, an idea to separate FPs from spent nuclear fuel is using mutual transformations between FP-doped UO2 and FP-doped U3O8 under different temperatures, which is a promising way to promote the development of nuclear fuel cycles.
Alloy 800H is currently used as structural material in light-water cooled nuclear reactors, and it is also considered as candidate materials for various advanced reactor designs. Under operation, the exposure of alloy 800H to neutron irradiation results in the formation of helium (He), mainly from Ni by the transmutation reaction (n, α). In this work, we present a molecular dynamics (MD) simulation study of the behavior and effects of He on the microstructure and mechanical properties of alloy 800H. Our results show that the population of clusters made of 5 to 9 He atoms is nearly constant throughout the simulation time (10 ns), while the population of larger clusters increases as the simulation time increases. The growth of clusters is controlled by either the dissociation and diffusion of smaller clusters towards nearby larger clusters or the merging of larger clusters initially located nearby to each other. A significant accumulation of He is observed at the grain boundaries (GB), while a depletion zone is found at the neighboring regions. As a result, the density of He cluster is significantly higher at the GBs as compared to the intra-granular regions. The nucleation and growth of He clusters also results in the formation of Frenkel pairs (FP), whose associated self-interstitial atoms (SIA) agglomerate into interstitial clusters in the alloy 800H matrix. As a consequence, dislocation segments, mostly of the Shockley type, are generated in the microstructure, and often located next to He clusters. The combination of the aforementioned defect structures and the high density of He clusters at the GBs results in a substantial degradation of the mechanical properties of alloy 800H single crystal and bicrystals.