ORNL-5388 - the Molten Salt Energy Technologies Web Site
ORNL-5388 - the Molten Salt Energy Technologies Web Site
ORNL-5388 - the Molten Salt Energy Technologies Web Site
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8-4<br />
Table B-6. Reprocessing, Shipping, and Waste Storage Costs for Various Reactor Types<br />
Reactor<br />
Type<br />
LWR<br />
SSCR<br />
HWR<br />
HTGR<br />
FBR<br />
Costs ($/kg HM)<br />
Reprocessing Costs Spent Fuel Waste Shipping Waste Storage Total Costs<br />
Over First Decade9 ShiPP’S9 costs costs Over First Decade<br />
costs After IntroductionC<br />
225 (1991) * 150 (2001) 15 10 45 295 (1991) + 220 (2001)<br />
225 (1991) * 150 (2001) 15 10 45 295 (1991) + 220 (2001)<br />
225 (1995) + 150 (2005) 10 5 15 255 (1995) + 180 (2005)<br />
800 (1995) + 400 (2005) 85 35 65 985 (1995) + 585 (2005)<br />
500 (2001) + 200 (2011) 80 50 115 745 (2001) + 445 (2011)<br />
aFissile storage costs after reprocessing = f2/g-yr for ‘’’0 and fissile plutonium.<br />
bTotal costs for throwaway cycle are spent fuel shipplng costs plus $100/kg HM.<br />
‘50% uncertainty on total costs for all reactor types.<br />
is deployed, <strong>the</strong> tails composition would decrease continuously from 0.0020 to 0.0010 between<br />
<strong>the</strong> years 1980 and 2000 as <strong>the</strong> installed capacity of <strong>the</strong> advanced technology increased, and<br />
<strong>the</strong> cost of a unit of separative work would decrease to approximately 60% of that of <strong>the</strong><br />
gaseous diffusion process. It was also assumed that <strong>the</strong> tails composition would fur<strong>the</strong>r<br />
decrease from 0.0010 to 0.0005 between <strong>the</strong> years 2001 and 2030 due to improvements in<br />
technology, while <strong>the</strong> cost of a unit of enrichment would remain constant during this period.<br />
The tails composition and enrichment cost were assumed to remain constant <strong>the</strong>reafter.<br />
The capacity factors of a plant throughout its 30-yr lifetime are shown in Table B-9.<br />
The capacity factor increases from 60% to 72% during <strong>the</strong> first 3 yr of operation and remains<br />
at 72% during <strong>the</strong> subsequent 14 yr. It <strong>the</strong>n decreases continuously as <strong>the</strong> forced outage<br />
rate increases and as <strong>the</strong> plant is shifted from a base-load unit to an intermediate-load unit.<br />
The long-term real cost of money to <strong>the</strong> electric utility industry is shown in Table 6-10.<br />
These costs were developed by analyzing <strong>the</strong> deflated cost of debt and equity to <strong>the</strong> industry<br />
over <strong>the</strong> past 30 yr. The long-term deflated cost of debt has been 2.5%/yr and <strong>the</strong> long-term<br />
deflated cost of equity has been 7.0%/yr.<br />
Assuming <strong>the</strong> industry to be funded at approximately<br />
55% debt and 45% equity, <strong>the</strong> long-term real money cost is approximately 4.5%/yr.<br />
The combined effects of capital , fuel fabrication, and reprocessing (or permanent<br />
disposal) cost uncertainties on <strong>the</strong> levelized total power costs for individual reactor and<br />
fuel cycle options are shown in Fig. B-1. These costs represent typical nonfuel components<br />
whose uncertainties are easily quantified. Figures 6-2a and B-2b show <strong>the</strong> relationship of<br />
total power costs to <strong>the</strong> U& price for four reactors on <strong>the</strong> throwaway fuel cycle.<br />
sensitivity of <strong>the</strong> total power costs to <strong>the</strong> U308 price was analyzed first by assuming that<br />
<strong>the</strong> price remained constant over <strong>the</strong> 30-yr life of <strong>the</strong> reactor, and second by assuming that<br />
<strong>the</strong> price increases in relation to <strong>the</strong> rate of consumption (see Fig. 8-3). Thus, <strong>the</strong> total<br />
power costs in Fig. B-2b are given for a reactor starting up with <strong>the</strong> U308 price shown on<br />
The<br />
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c<br />
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