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ORNL-5388 - the Molten Salt Energy Technologies Web Site

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4-54<br />

4.6. ALTERNATE FAST REACTORS<br />

4.6.1. Advanced Oxide-Fueled LMFBRs<br />

T. J. Burns<br />

Oak Ridge National Laboratory<br />

One method of improving <strong>the</strong> breeding performance of <strong>the</strong> LMFBRs discussed in <strong>the</strong><br />

previous section is to increase <strong>the</strong> core fertile loadings. Typically, this goal is<br />

accomplished by one of two means: redesign of <strong>the</strong> pins to accommodate larger pellet<br />

diameters or <strong>the</strong> use of a heterogeneous design (i.e., intermixed core and blanket<br />

assemblies). To maintain consistency with <strong>the</strong> "classical" designs considered in <strong>the</strong><br />

previous section, using <strong>the</strong> same fuel elements for both concepts, <strong>the</strong> latter option was<br />

i<br />

pursued to assess <strong>the</strong> impact of possible redesign options. Table 4.6-1 summarizes some<br />

preliminary results from calculations for a heterogeneous reactor core model consisting<br />

of alternating concentric fissile and fertile annuli (primed cases) and compares <strong>the</strong>m<br />

with results from calculations for corresponding homogeneous cores (unprimed cases).<br />

As <strong>the</strong> data in Table 4.6-1 indicate, <strong>the</strong> heterogeneous conffquration results in a<br />

significant increase in <strong>the</strong> overall breeding ratio relative to <strong>the</strong> corresponding homo- .<br />

geneous calculation. The heterogeneous reactors also require a much greater fissile<br />

loading for criticality due to <strong>the</strong> increase in <strong>the</strong> core fertile loading. However, <strong>the</strong><br />

increase in <strong>the</strong> breeding gain more than compensates for <strong>the</strong> increased fissile requirements,<br />

resulting in an overall improvement in <strong>the</strong> fissile doubling time. On <strong>the</strong> o<strong>the</strong>r hand,<br />

because of <strong>the</strong> high fissile loading requirements, it appears that a heterogeneous model for<br />

<strong>the</strong> denatured cases with 12% enrichment (cases 6 or 7 of <strong>the</strong> previous section) is unfeasible;<br />

<strong>the</strong>refore, an enrichment of 120% was considered as <strong>the</strong> minimum for <strong>the</strong> denatured heterogeneous<br />

configuration.<br />

While <strong>the</strong> denatured heterogeneous configurations result in an increase in <strong>the</strong><br />

overall breeding ratio, it is significant that <strong>the</strong> 233U component of <strong>the</strong> breedinq ratio<br />

also improves. Figure 4.6-1 depicts <strong>the</strong> breeding ratio components for both <strong>the</strong> homogeneous<br />

and heterogeneous denatured configurations.<br />

as <strong>the</strong> upper limit.) As Fig. 4.6-1 indicates, <strong>the</strong> heterogeneous confiaurations are<br />

clearly superior from <strong>the</strong> standpoint of 233U self-sufficiency (i.e. , requirinq less<br />

makeup requirements). Moreover, if enrichments in <strong>the</strong> range of 304: - 40% are allowed,<br />

it appears possible for a denatured heterogeneous reactor to produce enough 233U to<br />

satisfy its own equilibrium cycle fuel requirements. Production reactors would <strong>the</strong>refore<br />

be required only to supply <strong>the</strong> initial inventory plus <strong>the</strong> additional makeup consumed<br />

before <strong>the</strong> equilibrium cycle is reached.<br />

(Aaain , <strong>the</strong> 233U/Th LMFBR is included

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