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PLENTIFUL ENERGY

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like breeding, does increase such damage. But three- or four-year residence times<br />

for fuel are perfectly satisfactory, and in fact are typical for all power reactors.<br />

14.5 Considerations for Burner vs. Breeder<br />

There have been suggestions that higher actinides created in other reactors<br />

should be destroyed by irradiation in reactors with a fast neutron spectrum.<br />

Certainly at present, when plutonium stocks from LWRs are building up<br />

worldwide, and some weapons plutonium stocks having been declared surplus, a<br />

case can be made for reactor configurations that burn more of these actinide<br />

elements than they create. The IFR core can be designed as a burner or breeder of<br />

fissile isotopes, or indeed of all actinides. All are fissionable in the IFR neutron<br />

spectrum. If the core shown in Figure 14-5 is surrounded by reflector assemblies<br />

(steel components that tend to reflect neutrons back into the core, thus conserving<br />

neutrons), the core itself will not breed enough to break even in fissile conversion,<br />

and the core becomes a net burner of fissile isotopes and total actinides. If the<br />

reflector assemblies are replaced by blanket assemblies of depleted uranium,<br />

leakage neutrons are captured by the uranium and produce plutonium that can later<br />

be harvested by pyroprocessing and used to manufacture new fuel pins. If adequate<br />

blankets are provided (including axial as well as radial), the breeding ratio (the ratio<br />

of fissile production to fissile destruction) can substantially exceed unity. Selfsufficiency<br />

only, a breeding ratio of unity, indeed any burner or breeder<br />

configuration desired, is easily achieved by such blanket adjustments during<br />

planned refueling outages at any time during the reactor‘s lifetime.<br />

As a rule of thumb, an LWR operating for thirty years generates enough<br />

actinides to start up an IFR. The LWRs currently operating worldwide, a capacity<br />

of about 375 GWe, operating for a sixty-year lifetime, will have generated<br />

sufficient actinides to start up about 750 GWe IFRs. Even if only a fraction of the<br />

LWR spent fuel is reprocessed, a large number of IFRs can be built without the<br />

need yet to breed. The penalty of such breeding is only that blanket assemblies will<br />

have to be processed, which can mean more heavy metal throughput than for the<br />

core fuel itself. If reflectors are installed, this cost can be avoided until such time as<br />

breeding is required.<br />

There are two figures of merit that have been put forward for designers<br />

concentrating their attention on actinide burning instead of breeding. [13] Clearly<br />

there is incentive to burn actinides in IFRs. Where burning actinides instead of<br />

replacing them by normal breeding has been emphasized, the net actinide<br />

destruction rate in terms of kg/GWe-yr is used as a figure of merit. This emphasizes<br />

non-fertile fueling (little or no uranium in the fuel), and even non-reactor options<br />

such as accelerator-driven subcritical systems emerge as possible optimum<br />

strategies.<br />

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