Nonproliferation Role of 231Pa and 232U from a Fusion Breeder for the Thorium Molten Salt Reactor
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Nonproliferation role of 231Pa and 232U from a fusion breeder for the thorium molten salt reactor Ralph Moir! ! Vallecitos Molten Salt Research! 607 E. Vallecitos Rd., Livermore,! CA 94550 USA! [email protected]! www.ralphmoir.com/! ! Thorium Energy Alliance 2014 Conference (TEAC6) May 29, 2014, Chicago! ! ! Incentives for molten salt reactors are so great that one" asks why the reactor has not already been developed? 5/13/14 Abstract" !Initial and makeup 233U fuel for a thorium molten salt reactor can be produced in a fusion breeder with 2.4% 232U that will make this fuel “self-protected” by its strong gamma radiation according to IAEA standards. 232U significantly contributes towards nonproliferation of nuclear weapons use. Fusion technology even early in its development towards a commercial power plant nevertheless can produce 233U by neutron capture in 232Th and simultaneously produce both 231Pa and 232U in a neutron reaction having a 6 MeV threshold making fusion’s 14 MeV neutrons uniquely well suited for this purpose. The 231Pa can make 232U by neutron capture in the fusion breeder in large enough quantity to make the simultaneously produced 233U self protected with 2.4% 232U. Excess 231Pa can be extracted and exported to fission reactors where by neutron capture 232U is made in situ for nonproliferation purposes. When the fission reactor’s conversion ratio of fertile to fissile approaches unity (breeding or isobreeding) its fissile 233U is produced internally with too little 232U nonproliferant made to satisfy the 2.4% rule because fission’s neutrons are below the 6 MeV threshold. In this case, as the conversion ratio approaches unity, 231Pa is supplied so that the production of 232U by neutron capture in 231Pa keeps 232U/233U=2.4%. ! ! In the long term, producing 233U by fusion breeding avoids the need for isotope enrichment facilities to be greatly expanded thus contributing to nonproliferation. In the short term, before fusion bred 231Pa, 232U and 233U become available, the required fissile material can come from enriched 235U with enough 238U to be denatured for nonproliferation or can come from plutonium from spent fuel.! Key words: molten salt reactor, thorium, fusion breeder, 231Pa, 232U, 233U nonproliferation! 5/13/14 2 Nonproliferation strategy #1 § The Denatured Molten Salt Reactor (DMSR) dilutes 233U and 235U with enough 238U to be below weapons grade.! § 233U/U<13%! § 235U/U<20%! § Also safeguards and emphasize openness and transparency! Recommendation to MSR developers:! Initially go for DMSR! 5/13/14 3 With denaturing 238U builds up and Th drops off. With 233U from fusion 232Th would not drop off and 238U would not build up. 120,000! ! 232 100,000! Th! Th inventory! 80,000! 235U 20%! 233U! U238inventory! DMSR! 60,000! Inventory, kg Inventory, U238 inventory! makeup! Fusion makeup! 40,000! Th inventory! 20,000! 238U! 0! 0! 5! 10! 15! 20! 25! 30! t, years! DMSR=ORNL/TM-7207! 4 5/13/14 With denaturing 233U and 235U reach steady values in about 3 y. DMSR-235U startup & makeup! 4,000! ! U235inventory! U233inventory! 3,000! Pu239inventory! 233 2,000! U! 1,000! 235 Fissile inventory, kg inventory, Fissile U! 239Pu! 0! 0! 5! 10! 15! 20! 25! 30! Time, y! 5/13/14 5 Nonproliferation strategy #2 2nd Gen MSR § Spike the fissile 233U with fusion produced 2.4% 232U, a strong gamma and heat generator making the material undesirable for weapons.! § Employ safeguards and emphasize openness and transparency! Recommendation to MSR developers: Generate a market for 233U, 232U and 231Pa! Recommendation to fusion developers: Design a fusion breeder for 233U, 232U and 231Pa! 5/13/14 6 The reaction paths that lead to 232U with % for each route for the (Li/MS, Be/MS) blankets •(0.3%, 0.1%)! •(0.03%, 0.01%)! •(16%, •(84%,98%)! 2%)! 233U is produced in the following reaction ! 232 233 233 " 233 " 5/13/14 n+ Th! Th! Pa + e ! U + e 7 231Pa and 232U are produced in the following reactions 232 233 233 •1 ! n+ Th! Th! Pa + e" n+ 233Pa ! 2n + 232Pa!232U + e" Fast n 232Th 233Th 233Pa e" 233U e" •2 ! + ! ! + ! + n+ 233U ! 2n+ 232U Fast 232 231 231 " •3 ! n+ Th ! 2n+ Th! Pa + e Fast n+ 231Pa!232Pa!232U + e" 5/13/14 8 Fusion is unique for producing 231Pa & 232U" Threshold cross-sections ! !Fusion ! for producing 232U ! 100% neutrons > 6 MeV)! N(E) fission spectra! ! ! N(E) fusion spectra/5! 0.4! 2.5! Th232 n,2n! ! !Fission ! Pa233 n,2n! 2.0! 0.3! U233 n,2n! 1.5! 3% neutrons > 6 MeV).! 0.2! 1.0! 0.1! 0.5! (n,2n) cross section, barns (n,2n) cross section, 0! 0.0! Fission and fusion neutron spectra Fission and fusion 0! 5! 10! 15! 20! Neutron energy, MeV! 5/13/14 9 231Pa and 232U are produced in a fusion blanket of Li followed by a Li Th molten thorium molten salt. salt kg PR = 4.318 F ! Pfusion (MW ) MWfusion ! y 231 § Fn,2n = 0.0246 Pa 32,800 y half-life 233 233 § Fn, g = 0.515 Pa 27.0 d half-life, decays to U 5/13/14 10 Revenues from 231Pa and 232U at assumed value per gram 231 kg Pa $82, 000 231 PR = 0.1062 Pfusion (MW ) " Pnuclear (MW ) for $1000 / g of Pa MWfusion ! y MWnuclear ! y 233 kg Pa $130, 000 233 = 2.224 Pfusion (MW ) " Pfusion (MW ) for $60 / g of U MWfusion ! y MWfusion ! y 233 kg Pa $103, 000 233 = 1.72 Pnuclear (MW ) " Pnuclear (MW ) for $60 / g of U MWnuclear ! y MWnuclear ! y 1 GWe; Pnuclear/Pfusion=1.3! 5/13/14 11 Revenues from electricity and isotopes 0.48! Q! 4.8! 48! ! 0.2! 0.2! 50 $/MWeh! ! ! Breeding! revenues! 0.1! DC=0,BDC=0.5! 0.1! ! Electrical! DC=BDC=0.5! 0.1 $/Wnuc y! revenues! ! 0! Breeding revenues! 0! $/Wnuclear-year M=2.1! no DC! Annual revenues/nuclear power revenues/nuclear Annual -0.1! -0.1! 1! 10! 100! MQ! Q=fusion power/input power= Gain! 5/13/14 12 Cost for isotopes depends on electricity sales/purchases (Q) 1000! ! 50 $/MWeh! etadc=0.0 100! Pa sales 231 1.25 $/Wnuclear! 10! 1.5 $/Wnuclear! U, $/g no 2.0 $/Wnuclear! 233 1! 0.1! 1! 10! 100! Q! Q=fusion power/input power= Gain! 5/13/14 13 The value of 233U can be corrected for the 231Pa sales. 150! 233U=150 $/g without 231Pa sales ! 100! U, $/g U, 233 100 $/g 50! Value of Value 50 $/g 0! 0! 1000! 2000! 3000! Value of 231Pa, $/g! 5/13/14 14 Supply 233U + 2.4% 232U to MSR for startup and makeup fissile For conversion ratio (CR)>0.75! 232U/233U falls below 2.4%! 0.1! 0.08! ! U 0.06! 233 U/ 0.04! 232 IAEA "self protected"! 0.02! by 2.6 MeV gamma rays! 0! 0! 0.2! 0.4! 0.6! 0.8! 1! Conversion ratio, CR! 5/13/14 15 For CR>0.75 supply 231Pa to MSR as well as 233U. Then 232U/233U # 2.4% for any CR.! 0.1! 7! 6! 0.08! 5! 231Pa ! 0.06! 4! 232U/233U! kg/y! 0.04! 3! 232U/233U! 2! 0.02! 231Pa/y! 1! 0! 0! 0! 0.5! 1! Conversion ratio, CR! 1 GWe! 5/13/14 16 For startup on 239Pu (or 235U), 239Pu is replaced~2 y with 233U without 232U 1500! 233U! inventory, inventory, 1000! 233U, CR=0.75! ! Pu 0.9! kg 239 1! 500! 239Pu! Pu239! U and U and 0! 233 0! 1! 2! 3! Time, y! Assume 1500 kg/1 GWe! 5/13/14 17 For startup on 239Pu or 235U an initial supply of 232U and 231Pa is needed. 232U/233U builds up to 2.4% 15 years starting with 231Pa=25.5 kg.! 0.04! 232 40! ! U! 232U, kg! 0.03! 232U/233U! 30! 0.02! 20! CR=0.75! 232U/233U 0.9! 0.01! 1! 10! self-protection! U232, CR=0.8! 0! 0! 0! 5! 10! 15! 20! Time, y! 35 kg 232U initially would keep 232U/233U $ 2.4%! Otherwise we have a problem.! 5/13/14 18 6840 kg/y 233U is extracted by fluorination and 150 kg/y 231Pa by reductive extraction 3000 MW fusion! 5/13/14 19 Conclusions Nonproliferation strategy #1 First generation MSR should use denatured uranium (235U/U<0.2)! Also safeguards and emphasize openness and transparency! ! 5/13/14 20 Nonproliferation strategy #2 2nd gen MSR when fusion is available § Spike the fissile 233U with fusion produced 2.4% 232U, a strong gamma and heat generator making the material undesirable for weapons.! § Employ safeguards and emphasize openness and transparency! Recommendation to MSR developers: Generate a market for 233U, 232U and 231Pa! Recommendation to fusion developers: design a fusion breeder for 233U, 232U and 231Pa! See my website for details 5/13/14 ! 21 .