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dc.contributor.authorSONODA T.en_GB
dc.contributor.authorKAMEYAMA T.en_GB
dc.contributor.authorSASAHARA A.en_GB
dc.contributor.authorKITAJIMA S.en_GB
dc.contributor.authorNAUCHI Y.en_GB
dc.contributor.authorKINOSHITA M.en_GB
dc.contributor.authorRONDINELLA VINCENZOen_GB
dc.contributor.authorWISS THIERRYen_GB
dc.contributor.authorHIERNAUT JEAN-POLen_GB
dc.contributor.authorPAPAIOANNOU DIMITRIOSen_GB
dc.contributor.authorSHEINDLIN M.en_GB
dc.contributor.authorSTAICU DRAGOSen_GB
dc.date.accessioned2010-02-25T14:52:44Z-
dc.date.available2007-10-16en_GB
dc.date.available2010-02-25T14:52:44Z-
dc.date.created2007-10-16en_GB
dc.date.issued2007en_GB
dc.date.submitted2007-10-16en_GB
dc.identifier.citationProceedings of the 2007 International LWR Fuel Performance Meeting / Top Fuel p. 340- 346 / paper 1026en_GB
dc.identifier.urihttp://publications.jrc.ec.europa.eu/repository/handle/JRC40841-
dc.description.abstractAt the peripheral region of high burnup fuel pellets, a crystallographic re-structuring is observed, commonly called the rim structure, which is characterized by the existence of highly dense small sub-grains, whose size is approximately 100 nm, and the accumulation of small pores with average size around 1 µm. This restructuring can influence the fuel performance including, e.g. fission gas release behaviour, temperature, hardness and density. In order to clarify the threshold burnup and temperature of rim structure formation and fuel performances of LWR UO2 fuels and gadolinia-doped ((U,Gd)O2) fuels whose usage is increasing for higher burnup in LWR, several post irradiation examinations such as scanning electron microscope (SEM) /transmission electron microscope (TEM) observation, density measurements, hot cell annealing and thermal diffusivity measurements are done. By SEM and TEM observations, it is clarified that the microstructure evolution and the burnup and temperature threshold of rim structure formation of (U,Gd)O2 fuels is not different from that of UO2 fuels. The density change of UO2 and (U,Gd)O2 fuels is almost similar, and the irradiation temperature does not affect the density change significantly. Fission gas release behaviour can be classified by the existence of rim structure, and the release behaviour between UO2 and (U, Gd)O2 fuels is almost same.en_GB
dc.description.sponsorshipJRC.E.4-Nuclear fuelsen_GB
dc.format.mediumCD-ROMen_GB
dc.languageENGen_GB
dc.publisherOmnipressen_GB
dc.relation.ispartofseriesJRC40841en_GB
dc.titleClarification of Rim Structure Effects on Properties and Behaviour of LWR UO2 Fuels and Gadolinia Doped Fuelsen_GB
dc.typeArticles in periodicals and booksen_GB
JRC Directorate:Nuclear Safety and Security

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