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RRFM 2009 Transactions - European Nuclear Society

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small in a plate having a low fission rate and, hence, typically a low temperature. These<br />

observations suggest that Si accumulation in the ILs occurs primarily during a heating process of<br />

the fabrication stage and additionally by fission enhanced diffusion when the fission rate is high.<br />

It is fortunate that the Si diffusion is fast in a plate with a high fission rate and therefore high<br />

temperature in which the effectiveness of Si addition is needed the most.<br />

The IL thicknesses observed in R2R040 and other plates with 2wt% or more Si addition is small,<br />

smaller than in U 3 Si 2 /Al at the same condition. This remarkable effectiveness of Si addition is<br />

similar to the test results by Ugajin [12], although he added Mo in U 3 Si 2 . Ugajin observed that<br />

U 3 Si 2 +0.5wt%Mo/Al dispersion grew thinner ILs than U 3 Si 2 /Al dispersion. This observation and<br />

the present result show that Si has a superior effectiveness when combined with Mo.<br />

As discussed earlier, no porosity was observed in the ILs in plates with the addition of 2wt% or<br />

more Si to a burnup close to 90%. This stability improvement by the presence of Si in the IL was<br />

theorized by Ryu [13]. Ryu showed that the enthalpy of formation of IL decreases, or becomes a<br />

larger negative number, when Si is added to the IL. The average bond strength typically<br />

increases with decreasing enthalpy of formation, by which the viscosity of the IL increases to<br />

better retain fission gas.<br />

However, as the IL thickness increases, Si deficiency eventually will occur in the IL. Then, the IL<br />

growth rate increases and pores may form in the ILs as observed in R2R088 and R6R018 from<br />

the RERTR-9B. In order to estimate the minimum as-fabrication Si content to avoid the Si<br />

deficiency, we assume the following: (1) Fuel particles have a uniform size (~90 μm) and<br />

distribution in the meat. (2) Thermal diffusion during fabrication reaches equilibrium. (3) For<br />

conservative results, fission enhanced diffusion is neglected. (4) By analogy to UAl 3 [14], the<br />

minimum Si concentration is 5at% in the IL. (5) The amount of Si diffused into the ILs is equal to<br />

the amount in the ILs.<br />

Figure 4 shows the estimated Si contents in ILs for two IL thicknesses that have as-fabrication Si<br />

content of 2% in the Matrix. As shown in Fig. 4(b), the estimated Si content in ILs is slightly<br />

higher for the high U-loading cases than the minimum Si content. This overprediction suggests<br />

that some of the assumptions for the model may be unrealistic. The inhomogeneity of fuel<br />

particle size and distribution seems to be the most sensitive assumption.<br />

1.0<br />

10<br />

1.0<br />

10<br />

IL volume fraction<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

8<br />

6<br />

4<br />

2<br />

Si content in IL (%)<br />

IL volume fraction<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

8<br />

6<br />

4<br />

2<br />

Si content in IL (%)<br />

0.0<br />

0<br />

5 6 7 8 9<br />

U-loading (gU/cm 3 )<br />

0.0<br />

0<br />

5 6 7 8 9<br />

U-loading (gU/cm 3 )<br />

(a) IL = 5 μm and 2% as-fabrication Si in Al (b) IL = 9 μm and 2% as-fabrication Si in Al<br />

Fig. 4 Estimated Si content in IL for Al-2wt% as-fabrication Si for typical RERTR test<br />

condition. The broken lines indicate the minimum Si content in the IL necessary for<br />

the Si addition to be effective.<br />

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