AbstractAn understanding of the coarsening process of the large fission gas pores in the high burn-up structure (HBS) of irradiated UO2 fuel is very necessary for analyzing the safety and reliability of fuel rods in a reactor. A numerical model for the description of pore coarsening in the HBS based on the Ostwald ripening mechanism, which has successfully explained the coarsening process of precipitates in solids is developed. In this model, the fission gas atoms are treated as the special precipitates in the irradiated UO2 fuel matrix. The calculated results indicate that the significant pore coarsening and mean pore density decrease in the HBS occur upon surpassing a local burn-up of 100 GWd/tM. The capability of this model is successful...
The dimensional changes of a nuclear fuel in operation are strongly determined by two opposite effec...
We propose a model describing the HBS formation and the progressive intra-granular xenon depletion i...
A BWR design UO2 fuel irradiated to a burnup of 7.9% FIMA was selected for a careful calculational a...
AbstractAn understanding of the coarsening process of the large fission gas pores in the high burn-u...
In the periphery of UO2 fuel pellets, a restructuring of the fuel occurs, leading to the formation o...
AbstractA new methodology is introduced to analyse porosity data in the high burnup structure. Image...
In the present work the behavior of fuel pellets for LWR power reactors in the high burnup range (a...
The growth of the porosity in high-burnup fuel is of particular interest when considering the effect...
In the rim zone of UO2 nuclear fuel pellets, the combination of high burnup and low temperature driv...
AbstractVickers microhardness (HV0.1) and Young's modulus (E) measurements of LWR UO2 fuel at burn-u...
Vickers microhardness (HV0.1) and Young's modulus (E) measurements of LWR UO2 fuel at burn-up > 60 G...
The formation of the high burnup structure (HBS) is possibly the most significant example of the res...
During irradiation in a nuclear reactor, the fuel pellet experiences non-uniform fission density and...
Irradiation experience gained on fuel rods with burn-ups greater than 60 MWd/kgHM irradiated in the ...
The dimensional changes of a nuclear fuel in operation are strongly determined by two opposite effec...
We propose a model describing the HBS formation and the progressive intra-granular xenon depletion i...
A BWR design UO2 fuel irradiated to a burnup of 7.9% FIMA was selected for a careful calculational a...
AbstractAn understanding of the coarsening process of the large fission gas pores in the high burn-u...
In the periphery of UO2 fuel pellets, a restructuring of the fuel occurs, leading to the formation o...
AbstractA new methodology is introduced to analyse porosity data in the high burnup structure. Image...
In the present work the behavior of fuel pellets for LWR power reactors in the high burnup range (a...
The growth of the porosity in high-burnup fuel is of particular interest when considering the effect...
In the rim zone of UO2 nuclear fuel pellets, the combination of high burnup and low temperature driv...
AbstractVickers microhardness (HV0.1) and Young's modulus (E) measurements of LWR UO2 fuel at burn-u...
Vickers microhardness (HV0.1) and Young's modulus (E) measurements of LWR UO2 fuel at burn-up > 60 G...
The formation of the high burnup structure (HBS) is possibly the most significant example of the res...
During irradiation in a nuclear reactor, the fuel pellet experiences non-uniform fission density and...
Irradiation experience gained on fuel rods with burn-ups greater than 60 MWd/kgHM irradiated in the ...
The dimensional changes of a nuclear fuel in operation are strongly determined by two opposite effec...
We propose a model describing the HBS formation and the progressive intra-granular xenon depletion i...
A BWR design UO2 fuel irradiated to a burnup of 7.9% FIMA was selected for a careful calculational a...