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Christmas Light
’Twas the night before Christmas when all through the house
No electrons were flowing through even my mouse.
All devices were plugged by the chimney with care
With the hope that St. Nikola Tesla would share.
Alvin Radkowsky, Z. Shayer
Nuclear Technology | Volume 80 | Number 2 | February 1988 | Pages 190-215
Technical Paper | Advanced Light Water Reactor / Fission Reactor | doi.org/10.13182/NT88-A34045
Articles are hosted by Taylor and Francis Online.
The view has long been held that breeding in light water cores is possible only with the thorium cycle, at a rate slightly above the break-even point. If we utilize the uranium-plutonium cycle (plutonium fuel with 238U fertile material), we find that in a typical light water spectrum the value of η (number of neutrons emitted per neutron absorbed) for 239Pu, the principal plutonium isotope in standard light water reactor (LWR) spent fuel, is <2, which is the minimum value necessary for break-even in fissile fuel content. The reason for the low yield of fission neutrons from 239Pu absorption is that nearly one-third of the time 239Pu does not fission but instead forms 240Pu, a relatively nonfissile isotope. However, in studying the effect of neutron absorption by 240Pu and then by the subsequent 241Pu, which is highly fissionable with a large value of η, it is found that a net neutron gain is obtained. This, combined with the neutrons obtained from 239Pu fission and the fast effect (238U fissions), yields sufficient neutrons for a high gain breeding potential. Unfortunately, in a conventional LWR with plutonium fuel, we cannot run long enough to produce neutron absorption in 240Pu and in the resultant 241Pu because the 240Pu forms too quickly and its absorption is so high that it rapidly depletes the initial core reactivity. In the present concept, this difficulty has been overcome by a novel method of fuel management, which assumes the availability of rapid fuel reprocessing. In the design concept presented, two seed-blanket cores are utilized, a prebreeder and a breeder. The prebreeder core is fueled with plutonium obtained from standard LWR spent fuel and generates plutonium with a high isotopic content of 240Pu and 241Pu, which is used to fuel the breeder core. The initial fissile fuel for a 950-MW(electric) prebreeder is between 3000 and 4000 kg. Assuming the availability of rapid fuel reprocessing and refabrication, overall breeding of well over 10%/6 yr is feasible. The time between core refuelings is >1 yr, rather than once every 3 months as required in the case of liquid-metal fast breeder reactors, so that the fuel inventories are substantially reduced for our system. Thermal-hydraulic analysis indicates that each of the two seed-blanket cores can fit into a standard pressurized water reactor pressure vessel and meet safety requirements. Major advantages of the concept are continued utilization of present LWR plants and strong negative void coefficients for the core. It is anticipated that at equilibrium conditions, when plutonium for the prebreeder and breeder cores is recycled into standard LWRs, there will be a further gain in breeding.