AAWSAP DIRD, Aneutronic Fusion Propulsion II, November 2010
DOW-UAP-D146 · page 27 of 36
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UNCLASSIFIED/ /FOR OFFICIAL tJ!H! 8HLY UI0/'20001 Pl; (18MI) "7..15 '"' ,,.,)- ST(ca 19731 COMPASS-D Cross s e ction ofpres e nt E U 0 -shape tokamaks compared to the JTE R project 0..0001 -1,.;....,,__,,.......,...,..i,......,__,_....,...11,-.....,,.....,.,..,,..i i k h ttttttnl 11 111t1 1l n 111tttd tttt !! !Ph t!tt1 ttt l H ttt't ■ 1 .. ., w ........, ,, tl ·0.1 ':LO ,oo 0 2 4 6 8 :A(MA} Major radius (m ) Figure 17. Progress in Tokomak Magnetic Confinement Fusion The issues of tokomaks as a potential source of fusion power are dramatized by the recent graphic (Figure 18) published in the American Nuclear Society's Fusion Energy Division Newsletter (Dec 2007) depicting the GE Next-Generation Boiling-Water Reactor (Economic Simplified BWR). The reactor, which costs about $3 billion, will produce enough thermal energy to generate 1.2 GWe (gigawatt electrical), . Its fuel rods will have to be replaced every 3 years. In an operating fusion tokamak reactor, the first wall and neutron absorbing and tritium breeding thermal blanket would have to be replaced every 5 years. Two orders of magnitude more volume and an extremely complex thermal transport system will be at a considerably greater cost and down time for the plant. With the recent and predicted escalation of fossil fuel costs, nuclear power has become economically competitive with coal and oil plants. It is clear that a tokamak power plant could not compete with the fission plant at current market energy prices. UNCLASSIFIED/ /EOA QFFI&IAl l:l!H! 9Ht'I" 22