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Deep Fission to break ground this week
With about seven months left in the race to bring DOE-authorized test reactors on line by July 4, 2026, via the Reactor Pilot Program, Deep Fission has announced that it will break ground on its associated project on December 9 in Parsons, Kansas. It’s one of many companies in the program that has made significant headway in recent months.
C. J. Hah, T. J. Downar
Nuclear Science and Engineering | Volume 121 | Number 3 | December 1995 | Pages 405-415
Technical Paper | doi.org/10.13182/NSE95-A24143
Articles are hosted by Taylor and Francis Online.
The application of nodal equivalence theory (NET) in multigroup diffusion theory has required the use of “discontinuity factors” (DFs) to account for the homogenization errors that are inherent in all coarse-mesh nodal methods. Traditionally, DFs have been applied directly to the nodal matrix equations as multipliers to the group constants. For most problems of practical interest, the application of DFs has not led to the divergence of the iterative methods used to solve the discretized nodal equations. However, because of the large discontinuity factors resulting from the steep flux gradients in the modular high-temperature gas reactor, the inner and upscatter iterations failed to converge, motivating an investigation into alternative methods for applying NET. In this work, the augmented source method (ASM) for applying NET to the nodal expansion method is introduced. External surface sources at a node boundary are introduced to account for the homogenization errors thereby preserving the original matrix properties for which convergence of iterative methods is guaranteed. The ASM produced converged solutions for any magnitude of DFs and reproduced the reference solution when the augmented sources were constructed from the reference quantities. The application of the ASM to the core depletion calculation demonstrated the use of various approximations for the augmented source. An augmented source, which was constant during the burnup cycle, resulted in an improved solution in which the eigenvalue error was reduced by a factor of 6 compared with the nodal solution without DFs.