The neutronic characteristics of (Th- 233 U)O 2 , (Th- 233 U)C, and (Th- 233 U)N have been compared in small long-life pressurized water reactors (PWRs). Neutronic calculations were carried out at 300 MW th , 400 MW th , and 500 MW th with two cladding types: zircaloy-4 and ZIRLO (Zr low oxygen). They were performed using the Standard Reactor Analysis Code (SRAC) and JENDL-4.0 nuclide data, dividing the reactor core into three fuel zones with varying 233 U enrichment levels, ranging from 3% to 9% and fluctuating by 1%, employing the PIJ module at the fuel cell level and the CITATION module at the reactor core level. In addition, 231 Pa was added as burnable poison (BP). The (Th- 233 U)N fuel demonstrated superior criticality compared to the other fuel types, as it consistently achieves critical conditions throughout the reactor’s operating cycle with excess reactivity <1.00% dk/k for several fuel configurations at the 300 MW th and 400 MW th power levels. Moreover, the (Th- 233 U)N and (Th- 233 U)C fuels exhibited similar and flatter power density distribution patterns compared to the (Th- 233 U)O 2 fuel. The power peaking factor (PPF) value was relatively higher for (Th- 233 U)O 2 fuel than the other two fuels. The (Th- 233 U)N fuel exhibited the most negative Doppler coefficient, followed by (Th- 233 U)C and (Th- 233 U)O 2 fuels. Analysis of burnup levels revealed that the (Th- 233 U)O 2 fuel achieved significantly higher burnup than the other two fuels.
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Lapanporo et al. (2024) studied this question.
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