The main benefit above is not so much the energy difference but the much smaller quantity required to reach critical mass, aka you can make an efficient core at a smaller size.
Quote from: Rei on 11/15/2016 09:48 amThe main benefit above is not so much the energy difference but the much smaller quantity required to reach critical mass, aka you can make an efficient core at a smaller size. Not much weight benefit to be had there. You need less than 8Kg of HEU to achieve critical mass in a reactor.
I believe you're thinking of bombs, including reflectors, compression and the like. My reading says that the bare sphere critical mass of 100% 235U is ~50kg, vs. ~10kg for 100% 239Pu. Practical reactor geometries lead you to significantly worse than the bare sphere minimum before neutron reflection comes into play. Neutron reflector effectiveness is proportional to thickness, wherein mass for a constant thickness reflector grows proportional to the core radius squared. Hence my comments about scaledown.
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