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ORNL-5388 - the Molten Salt Energy Technologies Web Site

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trons in <strong>the</strong> Zircaloy cladding and <strong>the</strong> coolant of conventional PWRs (~4% of all<br />

neutron absorptions in PWRs result from hydrogen absorption).<br />

2. Low 233Pa burnout due to <strong>the</strong> low (7-8 W/cm3) power density.<br />

The combination of low power density and large core heat capacity associated with<br />

<strong>the</strong> graphite moderator and <strong>the</strong> ceramic fuel largely mitigate <strong>the</strong> consequences of HTGR loss-<br />

of-coolant accidents. Loss of cooling does not lead to severe conditions nearly as quickly<br />

as in conventional LWRs or FBRs since <strong>the</strong> heat capacity of <strong>the</strong> core is maintained, <strong>the</strong>re-<br />

fore allowing considerable time to initiate actions designed to provide auxiliary core cooling.<br />

The HTGR offers a near-term potential for realization of tmproved U308 utilization.<br />

The 330-MWe Fort St. Vrain plant has been under start-up for several years with a current<br />

licensed power level of 70% and <strong>the</strong> plant has operated at <strong>the</strong> 70% power level for limited<br />

periods. A data collection program is providing feedback on problem areas that are becoming<br />

apparent during this start-up period and will serve as <strong>the</strong> basis for improvements in <strong>the</strong><br />

comsercial plant design.<br />

An advantage of <strong>the</strong> HTGR steam cycle is that its commercialization could lead to<br />

later commercialization of advanced gas-cooled systems based on <strong>the</strong> HTGR technology. These<br />

include <strong>the</strong> HTGR gas turbine system which has a high <strong>the</strong>rmal efficiency of 45 to 50% and<br />

<strong>the</strong> VHTR (Very High Temperature Reactor) system for high-temperature process heat appl i-ca-<br />

tion.<br />

Mass balance calculations have been performed by General Atomic for several a1 ternate<br />

HTGR fuel cycles,l and some additional calculations carried out at <strong>ORNL</strong> have verified certain<br />

GA results.2 Their results for <strong>the</strong> following fuel cycles are presented here:<br />

Dispersible Resource-Based Fuels<br />

1. LEU, no recycle.<br />

a.<br />

b.<br />

Carbon/uranium ratio (C/U) = 350.<br />

C/U = 400, optimized for no recycle.<br />

2. MEU/Th (20% 235U/U mixed with 232Th), C/Th = 650, no recycle.<br />

3. MEU/Th (20% 235U/U), C/Th = 306 for initial core, C/Th = 400 for reload segments,<br />

23311 recycle.<br />

Dispersible Denatured Fuel<br />

4. MEU/Th (15% 233U/U), C/Th = 274/300 (initial core/reload segments), optimized<br />

for uranium recycle (23% t 2351)).<br />

<strong>Energy</strong>-Center-Constrai ned Fuel<br />

5. Pu/Th, C/Th = 650 (batch-loaded core).<br />

Reference Fuels<br />

6. HEU(235U)/Th, C/Th = 214/238 (initial core/reload segments), no recycle.<br />

7. HEU(233U)/Th, C/Th = 150, high-gain design, uranium recycle.<br />

8. HEU(235U)/Th, C/Th = 180/180 (initial core/reload segments), uranium recycle<br />

(from ref. 3).

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