COMPLETE DOCUMENT (1862 kb) - OECD Nuclear Energy Agency
COMPLETE DOCUMENT (1862 kb) - OECD Nuclear Energy Agency
COMPLETE DOCUMENT (1862 kb) - OECD Nuclear Energy Agency
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2.2 Target and fuel fabrication technology<br />
2.2.1 Fuels for homogeneous recycling<br />
2.2.1.1 Fabrication of fuel including neptunium<br />
237 Np and particularly its daughter 233 Pa have a considerable γemission requiring appropriate<br />
shielding in the powder blending section of the fabrication plant. In the remainder of the fuel plant, the<br />
effect is very small and can be neglected.<br />
In principle, neptunium could be mixed with the standard UO 2 fuel of current PWR cores.<br />
However, the reference 235 U enrichment should be significantly increased, which is seen as a major<br />
penalty [54].<br />
It is more advisable to mix NpO 2 with the usual MOX fuel (U, Pu)O 2 . This has been done<br />
already for irradiation in fast reactors: first of all for the SUPERFACT experiment in Phénix, the fuel<br />
of which was manufactured by ITU Karlsruhe, and more recently in view of the NACRE experiment in<br />
Superphénix, the fuel of which was fabricated, with 2% Np, at the CFCA plant of Cogéma Cadarache.<br />
In a MOX fuel factory, with respect to the pure PuO 2 reference case, the presence of NpO 2<br />
does not affect the α and neutron emission but increases the γsource, due to 233 Pa (the daughter of<br />
237 Np). The powder blending glove box should be protected by some 2 mm-thick Pb layers, to keep the<br />
external dose rates unchanged [55].<br />
In case of a multiple recycling of 237 Np, 238 Pu is progressively built-up, and this additional<br />
source of neutrons (mostly from (α,n) reaction) and of heat affects further re-processing and<br />
refabrication steps. Np should therefore be irradiated preferably in fast reactors with a lower capture to<br />
fission ratio and consequently reduce 238 Pu yield from irradiation. On the other hand, a multiple recycle<br />
of 237 Np in fast reactors also increases the tiny 236 Pu fraction, and the radioactive chain<br />
236 Pu - 232 U - 208 Tl brings a further emission of high-energy γ-rays, so that the 2 mm-thick Pb layer<br />
quoted above would become about 5 mm.<br />
As a conclusion, Np recycling affects fuel refabrication in a UO 2 factory substantially but a<br />
MOX factory to a limited extent, so that the present MOX plants can afford it without major<br />
modification.<br />
2.2.1.2 Fabrication of MOX fuel containing americium for LWR<br />
For the implications of recycling, both plutonium and americium as MOX fuel in light water<br />
reactors have been considered, with reference to the current (PuO 2 -UO 2 ) fabrication of MOX fuel.<br />
Recycling of plutonium and americium simultaneously in LWRs<br />
It is assumed that not only plutonium, but also americium can be recovered from spent fuel<br />
reprocessing, and recycled in the form of MOX fuel (Pu+Am) in the same PWR under the same<br />
conditions. A recovery yield of 99.5% for Pu and 98% for Am has been assumed.<br />
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