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ORNL-5388 - the Molten Salt Energy Technologies Web Site

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4-31<br />

a significant increase in burnup over <strong>the</strong> current design would require mechanical design<br />

modifications.<br />

The <strong>the</strong>rmal efficiency can be improved by increasing <strong>the</strong> coolant pressure. This<br />

would require stronger pressure tubes and thus penalize <strong>the</strong> neutron economy. The use of<br />

enriched fueling could result in a higher power peaking factor, which would require a re-<br />

duced linear power rating, unless an improved fuel management scheme is developed to re-<br />

duce <strong>the</strong> power peaking factor.<br />

Scoping calculations have been performed to address possible design modifications<br />

for CANDU fuel cycles o<strong>the</strong>r than natural ~ranium,”~ and detailed design tradeoff and<br />

optimization studies associated with <strong>the</strong> enriched fuel cycles in CANDUs are being carried<br />

out by Combustion Engineering as a part of <strong>the</strong> NASAP program. In <strong>the</strong> study reported here,<br />

in which only <strong>the</strong> relative performance of <strong>the</strong> denatured 233U cycle is addressed, <strong>the</strong> currentgeneration<br />

1200-MWe CANDU .fuel design presented in Table 4.3-1 was assumed for all except<br />

<strong>the</strong> natural-uranium-fueled reactor. A discharge burnup of 16,000 MWD/T (which is believed<br />

to be achievable with <strong>the</strong> current design) and <strong>the</strong> on-line refueling capability were also<br />

assumed.<br />

The fuel utilization characteristics for various fuel cycle options, including <strong>the</strong><br />

denatured 233U cycle option, were analyzed at Argonne National Laboratory5 and <strong>the</strong> results<br />

are sumnarized in Table 4.3-2. Some observations are as follows:<br />

1. Natural-Uranium Once-Through Cycle: In <strong>the</strong> reference natural uranium cycle,<br />

<strong>the</strong> 30-yr U308 requirement is about 4,700 ST/GWe, which is approximately 20% less than<br />

<strong>the</strong> requirement for <strong>the</strong> LWR once-through cycle. Even though <strong>the</strong> fissile plutonium<br />

concentration in <strong>the</strong> spent fuel is low (4.27%).<br />

discharged annually is twice that from <strong>the</strong> LWR.<br />

<strong>the</strong> total quantity of fissile plutonium<br />

2. Slightly-Enriched-Uranium Once-through Cycle: With slightly-enriched uranium<br />

(1% 235U), a 16,000-MWD/T burnup can be achieved and <strong>the</strong> U308 consumption is reduced by<br />

25% from <strong>the</strong> natural-uranium cycle. As shown in Fig. 4.3-1, <strong>the</strong> optimum enrichment is<br />

in <strong>the</strong> area of 1.2%, which corresponds to a burnup of about 20,000 MWD/T.<br />

3. Pu/U, Pu Recycle: In this option, <strong>the</strong> natural uranium fuel is “topped” with<br />

0.3% fissile plutonium. A discharge burnup of 16,000 MWD/T can be achieved and <strong>the</strong> plu-<br />

tonium content in <strong>the</strong> discharge is sufficient to keep <strong>the</strong> system going with only <strong>the</strong><br />

natural-uranium makeup. The U308 requirement is reduced to about one half of that for<br />

<strong>the</strong> natural-uranium cycle. (Smaller plutonium toppings decrease <strong>the</strong> burnup and make <strong>the</strong><br />

system a net plutonium producer; larger toppings increase <strong>the</strong> burnup and make <strong>the</strong> system<br />

a net plutonium burner.)

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