The FuTure oF nuclear Fuel cycle - MIT Energy Initiative
The FuTure oF nuclear Fuel cycle - MIT Energy Initiative
The FuTure oF nuclear Fuel cycle - MIT Energy Initiative
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As expected, the breeder installed capacity will over time become greater than that of the<br />
other FR options, and those in turn will reach a larger capacity than LWRs-MOX. Table 6.5<br />
shows the installed capacity of each technology for the once through fuel <strong>cycle</strong> and the four<br />
main scenarios in 2050 and 2100 for the three cases of growth rates. It is clear that only in<br />
the slow growth scenario would the capacity of fast reactors dominate the <strong>nuclear</strong> energy<br />
supply system by the end of century. In the higher growth scenarios, the LWR will continue<br />
to play a major role, providing more than 50% of the <strong>nuclear</strong> capacity even at the end of the<br />
century. This is a result of the traditional assumption that to startup FRs only TRU from<br />
LWR spent fuel and FR spent fuel can be used. For a high growth rate, it takes many more<br />
LWRs to produce the plutonium needed for startup of the fast reactors.<br />
Table 6.5 Installed LWR for the OTC, and Advanced Reactor<br />
Capacities in the Alternative Schemes in 2050 and 2100 (in GWe)<br />
GroWth rate <strong>Fuel</strong> CyCle by 2050 by 2100<br />
lWr-oTc 166 269<br />
1%<br />
MoX 41 32<br />
Fr* 20;22; 20 234; 236; 234<br />
lWr-oTc 250 859<br />
2.5%<br />
MoX 41 91<br />
Fr* 20; 23; 21 259; 345; 391<br />
lWr-oTc 376 1,001**<br />
4.0%<br />
MoX 41 117<br />
Fr* 20; 23; 21 400; 521; 540<br />
*results for cr=0.75, 1.00 and 1.23<br />
** <strong>The</strong> maximum allowed capacity per assumptions in this analysis, reached in 2088<br />
However, it is noticeable that in the base growth case and high growth case, the penetration<br />
of a breeder fast reactor at 2100 is close to that of the self-sustaining fast reactor, and both<br />
have a significantly higher installed capacity than that of the fast burner. At first glance this<br />
appears strange, since the added fissile production in the case of the breeder should enable<br />
added FR capacity. However, the fact that the initial core of the breeder reactor requires<br />
more fissile material explains the close penetration rate of the FR with unity conversion<br />
factor and that of a breeder over this period. <strong>The</strong> burner and self-sustaining fast reactors<br />
minimize the presence of excess fertile material (blankets), whereas the higher breeding<br />
ratio reactor needs such blankets. Thus, it needs more fissile loading to compensate for<br />
neutron absorption in the blanket.<br />
Reprocessing plants<br />
Figure 6.7 shows the development of the thermal reprocessing capacities in the various fuel<br />
<strong>cycle</strong> schemes, for the 2.5% growth case. Recall that the unit capacity is 1000 tHM/year and<br />
that thermal reprocessing is introduced in 2025 in the MOX scenario vs. 2035 in the FR<br />
scenarios. Each facility is assumed to operate for 40 years before being retired. <strong>The</strong> need<br />
for thermal recycling capacity is nearly the same for all schemes until 2070, with somewhat<br />
larger capacity needed for the case of a fast burner. However, after 2070, the need for thermal<br />
recycling capacity in the case of MOX goes well above the FR cases, due to the exhaustion<br />
of the spent fuel in interim storage, and the presence of fissile fuel from reprocessing<br />
fast reactor fuel in the FR cases.<br />
82 <strong>MIT</strong> STudy on <strong>The</strong> <strong>FuTure</strong> <strong>oF</strong> <strong>nuclear</strong> <strong>Fuel</strong> <strong>cycle</strong>