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ORNL-5388 - the Molten Salt Energy Technologies Web Site

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2-7<br />

denatured reactors or by energy-center reactors.<br />

provided a source of 233U for initial loading and makeup requirements, as well as a means<br />

for disposing of <strong>the</strong> non-recyclable (in <strong>the</strong> dispersed reactors) plutonium. The significant<br />

point of such a system is that no plutonium-containing fresh fuel circulates outside <strong>the</strong><br />

energy center. The plutonium contained in <strong>the</strong> spent fuel is returned to <strong>the</strong> center for<br />

ultimate destruction.<br />

The dispersed reactors in turn are<br />

DENATURED FUEL ASSEMBLIES (NO Pu)<br />

oRI?L-Iwc 77-1041<br />

~KEUP ,y38<br />

ENERGY<br />

(U-233, U-238, T~-232) OXIDE<br />

I<br />

/CENTER<br />

[ BOUNDARY<br />

DISPERSED REACTORS<br />

-1 LWR<br />

IRRADIATED<br />

FUEL<br />

, SPENT FUEL t~<br />

rn<br />

FABRICATION PU<br />

- TH<br />

Pu TO U-233<br />

TRANSMUTER<br />

I<br />

TERM I NAL<br />

STORAGE<br />

IRRADIATED<br />

FUEL<br />

Fig. 2.2-1. Schematic Fuel Flow for Symbiotic System Consisting of an<br />

<strong>Energy</strong> Center and Dispersed Reactors Operating on Denatured 233U Fuel.<br />

One obvious concern regarding such a coupled system is <strong>the</strong> amount of power produced<br />

by <strong>the</strong> dispersed systems relative to that produced in <strong>the</strong> energy center reactors.<br />

power ratio,* defined a5 dispersed power generated relative to centralized power, can be<br />

viewed as a parameter characterizing <strong>the</strong> practicality of <strong>the</strong> system.<br />

ratio depends on <strong>the</strong> characteristics of <strong>the</strong> reactors actually utilized for <strong>the</strong> various<br />

components and is considered in detail later in this report, certain generic statements<br />

can be made. In a mature "safeguarded" plutonium cycle, <strong>the</strong> ratio would be zero since<br />

all reactors would, of necessity, be located in energy centers. In <strong>the</strong> current open-ended<br />

LEU cycles, this ratio is essentially infinite since current nuclear generating capacity<br />

is dispersed via "naturally denatured" <strong>the</strong>rmal systems. The denatured 233U cycle will fall<br />

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* A1 so called ''energy support ratio."<br />

The<br />

While <strong>the</strong> power<br />

.

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