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Breaking ground on a new approach to construction
The drive to Kairos Power’s reactor demonstration site in Oak Ridge, Tenn., is not only scenic—it’s historic. Nearly 85 years ago, roughly 30,000 construction workers transformed orchards and farmland into a key Manhattan Project site. Depending on your route, you may pass by one of the three gatehouses that were once military checkpoints controlling access to Atomic Energy Commission production facilities.
J. D. Stewart
Nuclear Science and Engineering | Volume 25 | Number 3 | July 1966 | Pages 266-274
Technical Paper | doi.org/10.13182/NSE66-A17834
Articles are hosted by Taylor and Francis Online.
Two equally valid systems of definitions are given for the neutron diffusion parameters of a reactor lattice: cell-average and cell-surface. In defining the cell-average parameters, we imagine a macroscopic flux distribution to be fixed in space while the lattice is translated with respect to it. In defining the cell-surface parameters, we work in terms of fluxes and currents on the surface of a cell having the fissile material at its center. Parameters from both systems have been used before; but until recently we have lacked complete clarity of definition and the realization that there are two valid systems of parameters that should not be mixed in the one calculation. The early formula, L2 is equal to the summation over all values of i of fiLi2, is for a cell-average thermal diffusion area; L2 = (outleakage)/B2 (absorption), applied to a cell with the fissile material at the center, is a cell-surface diffusion area and is less than the summation over all values of i of fiLi2 by ≈(lattice spacing)2/24.