Impact of weight percent gadolinium and the number of its fuel rods on the neutronic and safety parameters
Creators
- 1. Department of Industrial Physics, Ebonyi State University, P.M.B. 053, Abakaliki (Nigeria)
- 2. Department of Physics, University of Malaya, 50603, Kuala Lumpur (Malaysia)
- 3. Centre for Applied Physics and Radiation Technologies, School of Engineering and Technology, Sunway University, 47500, Bandar Sunway, Selangor Darul Ehsan (Malaysia)
- 4. Nuclear and Reactor Physics Section, Nuclear Technology Center, Technical Support Division, Malaysian Nuclear Agency, Bangi, 43000, Kajang, Selangor (Malaysia)
- 5. Department of Physics, Faculty of Engineering and Physical Sciences, University of Surrey, Guildford, GU2 7XH (United Kingdom)
Description
Highlights: • The reactivity swing-peak decreases with gadolinium weight percent. • Reactivity swing curve increases with increasing number of gadolinium fuel rods. • Large gadolinium weight percent impacts negatively on FTC. • Large gadolinium weight percent impacts positively on MTC. • Gadolinium is not economically viable at and above 12 w/o. Control of neutron multiplication in a nuclear reactor is fundamental in achieving stable reactor power. The present study has sought to determine the impact of gadolinium weight percent (w/o) in respect of the number of fuel rods on the neutronic and safety parameters of (Th, U)O2 fuel in a Westinghouse small modular reactor. The MCNPX 2.7 integrated with CINDER90 fuel depletion code was used. The results show that the k-infinite and reactivity swing peak decrease with increasing gadolinium weight percent, with the highest and lowest k-infinite recorded in the fuel assembly containing zero (0) and 12 w/o, respectively. The largest and lowest reactivity swing curve occurs in the fuel assembly with 3.6 and 12 w/o at ~15 and ~35 GWd/THM, respectively. It shows that the impact of gadolinium w/o and the number of fuel rods on k-infinite follow similar trend. Conversely, the reactivity swing curve is observed to flatten with increasing gadolinium w/o but increases with increase in the number of gadolinium burnable absorber fuel rods. These phenomenological variations suggest that flat reactivity swing and power control can be achieved within 9.2–12 w/o gadolinium although not without economic penalty on fuel utilisation.
Availability note (English)
Available from http://dx.doi.org/10.1016/j.radphyschem.2021.109686Additional details
Identifiers
- DOI
- 10.1016/j.radphyschem.2021.109686;
- PII
- S0969806X21003364;
Publishing Information
- Journal Title
- Radiation Physics and Chemistry (1993)
- Journal Volume
- 188
- Journal Page Range
- vp.
- ISSN
- 0969-806X
- CODEN
- RPCHDM
INIS
- Country of Publication
- United Kingdom
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 54050171
- Subject category
- S21: SPECIFIC NUCLEAR REACTORS AND ASSOCIATED PLANTS; S11: NUCLEAR FUEL CYCLE AND FUEL MATERIALS;
- Descriptors DEI
- FUEL ASSEMBLIES; FUEL RODS; GADOLINIUM; NEUTRON TRANSPORT; NUCLEAR FUELS; NUCLEAR INDUSTRY; REACTIVITY; SMALL MODULAR REACTORS; THORIUM
- Descriptors DEC
- ACTINIDES; ELEMENTS; ENERGY SOURCES; FUEL ELEMENTS; FUELS; INDUSTRY; MATERIALS; METALS; NEUTRAL-PARTICLE TRANSPORT; RADIATION TRANSPORT; RARE EARTHS; REACTOR COMPONENTS; REACTOR MATERIALS; REACTORS
Optional Information
- Copyright
- Copyright (c) 2021 Elsevier Ltd. All rights reserved.