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Launching into tomorrow: NRIC guides new era of research and deployment
In June 2025, the Department of Energy announced the Reactor Pilot Program, an authorization pathway that allowed reactor developers to partner with the DOE to get first-of-a-kind (FOAK) reactors built and tested. Soon after, the DOE rolled out a complementary Fuel Line Pilot Program, which aimed to fast-track fuel projects. In all, 20 projects were accepted into the new programs.
Yukio Ishiguro, Keisuke Okumura
Nuclear Technology | Volume 84 | Number 3 | March 1989 | Pages 331-343
Technical Paper | Probabilistic Safety Assessment and Risk Management / Fission Reactor | doi.org/10.13182/NT89-A34217
Articles are hosted by Taylor and Francis Online.
A new concept is proposed for a high conversion light water reactor (HCL WR) that achieves both high conversion and high burnup while maintaining a negative void reactivity coefficient. This HCLWR has a flat “pancake” core with thick axial blankets. By using the flat core, a potential problem of HCLWRs, the positive void reactivity coefficient, can be reduced by neutron leakage, and a fuel assembly of very tight lattice pitch can be used. The leakage neutrons are utilized in the axial blankets to enhance the conversion ratio. With the axial blankets, the core shows a small value for the axial power peaking factor, and the plutonium enrichment can be largely reduced by the neutron reflection, including the fast fission due to 238U, compared with the bare core. Moreover, upgraded burnup characteristics can be obtained by the accumulation of fissile plutonium in the blankets. The flat core with the blankets can be applied to a small- or intermediate-scale light water reactor. The analysis combines a cell burnup calculation and a one-dimensional burnup calculation based on the diffusion method. The evaluation method of the void coefficient is validated for the flat core with axial blankets under practical, controlled conditions. Moreover, the accuracy of the present method is validated for the transport effect on the major physics parameters of interest by using the one-dimensional transport code ANISN and the Monte Carlo code VIM.