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Molten fuel nuclear reactor with neutron reflecting coolant

專利號
US10867710B2
公開日期
2020-12-15
申請人
TerraPower, LLC(US WA Bellevue)
發(fā)明人
Anselmo T. Cisneros, Jr.; Charles Gregory Freeman; Kevin Kramer; Jeffery F. Latkowski
IPC分類
G21C7/28; G21C3/54; G21C1/02; G21C7/22; G21C1/22; G21C15/28; G21C1/32; G21C7/27; G21C11/06; G21C15/02
技術領域
neutron,reflector,reactor,fuel,neutrons,in,core,flowing,material,molten
地域: WA WA Bellevue

摘要

Configurations of molten fuel salt reactors are described that utilize neutron-reflecting coolants or a combination of primary salt coolants and secondary neutron-reflecting coolants. Further configurations are described that circulate liquid neutron-reflecting material around a reactor core to control the neutronics of the reactor. Furthermore, configurations which use the circulating neutron-reflecting material to actively cool the containment vessel are also described. A further configuration is described that utilizes a core barrel between a reactor core volume of molten fuel salt and a reflector volume, in which the reflector volume contains a plurality of individual reflector elements separated by an interstitial space filled with molten fuel salt.

說明書

A plot line 204 shows reactivity over time for a fast MSR with a static graphite moderator configuration, wherein the moderating neutron reflector assembly tends to provision the reactor core with thermalized neutrons. On the plot line 204, reactivity begins around time T0 at a relatively higher level than plot line 202 due in part to thermalization caused by the graphite moderator increasing the probability of fission. Plot line 204 may drop significantly near time T0 due to thermal spectrum multiplication adjacent to the graphite reflector. Reactivity may then gradually reduce over time in a generally linear manner as the thermal neutrons burn fissile fuel in the reactor core. The plot line 204 is similar to plot line 202 in the respect that neither plot line reaches or maintains a maximized burn rate achievable within the reactor core. The plot line 204 does not reach the reactor's maximum burn rate because there are not enough fast neutrons to maintain a breeding rate high enough to support the burn rate as time progresses though the period T0-T5. In the plot lines 202 and 204, the burn rate is not optimized over the time period T0-T5. Instead, each plot has a period of relatively higher burn rate and a period of relatively lower burn rate over the course of the graph.

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