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RRFM 2009 Transactions - European Nuclear Society

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Fig. 4. A compacted and sintered lump for the mixed powder by passing through multi-stack of sieves<br />

Part 1<br />

Part 2 Part 3<br />

Part 4<br />

Part 4<br />

Part 5<br />

Part 6<br />

Part 5<br />

Part 7<br />

Part 8<br />

Part 9<br />

Part 6<br />

Transverse section<br />

Vertical Section<br />

Fig. 5 Cross section of pressure-sintered sample<br />

Fig. 6. Cross section of a fuel meat fabricated by 5 times of extrusions in the KOMO-3 and KOMO-4.<br />

Fig. 6 represents a typical large U-Mo particle dispersion in the fuel meat fabricated by 5 extrusions in<br />

the KOMO-4. From the observation there is not much difference from the dispersion point of view for<br />

the two photos.<br />

The results in table 1 are density measurements for the 9 obtained parts. The variations of the 9<br />

measured values are less than 6 %. The limit of the U-235 homogeneity for the fuel meat rod of the<br />

HANARO fuel is +/- 8.5 %. The dispersion degree of the mixed powder is considered to be acceptable.<br />

When the mixed powder is extruded, it is expected that the homogeneity of the extruded fuel meat rod<br />

would be improved. The target volume fraction of the U-Mo powder for this dispersion experiment was<br />

30 %. The theoretical density of the above fraction is estimated to be about 6.99 g/cc. The average<br />

value of the measured densities for the sintered sample is 6.59 g/cc, which corresponds to 94.3% of<br />

the theoretical density. When compared to the density of the plate fuel fabricated by a rolling, the<br />

density obtained by the pressure-sintering is considered to be appropriate for forming the fuel meat.<br />

392 of 455

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