Reactor physics ideas for large scale utilization of thorium in gas cooled reactors
- 1. Light Water Reactors Physics Section, Bhabha Atomic Research Centre, A-5/15, Central Complex, Mumbai, Maharashtra 400085 (India)
- 2. Department of Nuclear Engineering, Tokai University, Kanagawa 259-1292 (Japan)
Description
The physics principles for maximizing the fertile to fissile conversion were used in developing reactor concepts for large scale utilization of thorium in thermal and fast reactors (Jagannathan & Pal, 2006; Jagannathan et al., 2008). It is recognized that these principles are very well suited for 'He' gas cooled reactors with graphite moderator since both helium gas coolant and the graphite moderator have low neutron absorption characteristics and thus gives better neutron economy. In this paper, these ideas are applied to the High Temperature Test Reactor (HTTR) core of Japan to assess its advantage over the present day gas cooled reactors. HTTR is helium cooled and graphite moderated system. Significant amount of thorium has been loaded in the HTTR core with some minimal changes in the existing core design. The modified design is called HTTR-M core.In the HTTR-M core, the fuel is changed from enriched UO2 fuel to Pu in ThO2 fuel. The locations of boron type burnable poison rods within each fuel assembly of HTTR are replaced by one cycle irradiated thoria rods. Also, the B4C type control assembly around the HTTR core is replaced by fresh seedless thorium assembly. The fertile thoria assembly are scattered uniformly in the HTTR-M core. The equilibrium core of HTTR-M shows very small burnup reactivity swing. The core excess reactivity is ∼18 mk at BOC and reduces to 1 mk at 660 days. It is interesting to note that this small reactivity change is intrinsically achieved by the choice of seed and fertile dimensions and their contents without the use of burnable poison rods or mechanical control rods which are used in HTTR core. The burnup reactivity swing in the latter after using burnable poison is ∼100 mk. The fissile seed inventory ratio (FIR) in a fuel cycle is 0.90 as compared with 0.717 of HTTR core. Since 233U is a better fissile nuclide with highest 'η' value in thermal range, the above conversion ratio can be regarded as quite good.
Availability note (English)
Available from http://dx.doi.org/10.1016/j.pnucene.2011.05.028Additional details
Identifiers
- DOI
- 10.1016/j.pnucene.2011.05.028;
- PII
- S0149197011001168;
Publishing Information
- Journal Title
- Progress in Nuclear Energy
- Journal Volume
- 53
- Journal Issue
- 7
- Journal Page Range
- p. 814-819
- ISSN
- 0149-1970
INIS
- Country of Publication
- United Kingdom
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 51010868
- Subject category
- S21: SPECIFIC NUCLEAR REACTORS AND ASSOCIATED PLANTS;
- Descriptors DEI
- BORON; BORON CARBIDES; BURNABLE POISONS; BURNUP; CONTROL ELEMENTS; FUEL ASSEMBLIES; FUEL CYCLE; GRAPHITE; HELIUM; HTTR REACTOR; JAPAN; NEUTRON FLUX; PLUTONIUM; REACTOR PHYSICS; THORIUM; THORIUM OXIDES; URANIUM 233; URANIUM DIOXIDE
- Descriptors DEC
- ACTINIDE COMPOUNDS; ACTINIDE NUCLEI; ACTINIDES; ALPHA DECAY RADIOISOTOPES; ASIA; BORON COMPOUNDS; CARBIDES; CARBON; CARBON COMPOUNDS; CHALCOGENIDES; DEVELOPED COUNTRIES; ELEMENTS; ENRICHED URANIUM REACTORS; EVEN-ODD NUCLEI; EXPERIMENTAL REACTORS; FLUIDS; GAS COOLED REACTORS; GASES; GRAPHITE MODERATED REACTORS; HEAVY ION DECAY RADIOISOTOPES; HEAVY NUCLEI; HELIUM COOLED REACTORS; HTGR TYPE REACTORS; ISOTOPES; MATERIALS; METALS; MINERALS; NEON 24 DECAY RADIOISOTOPES; NEUTRON ABSORBERS; NONMETALS; NUCLEAR POISONS; NUCLEI; OXIDES; OXYGEN COMPOUNDS; PHYSICS; RADIATION FLUX; RADIOISOTOPES; RARE GASES; REACTOR COMPONENTS; REACTOR MATERIALS; REACTORS; RESEARCH AND TEST REACTORS; SEMIMETALS; SPONTANEOUS FISSION RADIOISOTOPES; THORIUM COMPOUNDS; TRANSURANIUM ELEMENTS; URANIUM COMPOUNDS; URANIUM ISOTOPES; URANIUM OXIDES; YEARS LIVING RADIOISOTOPES
Optional Information
- Notes
- Copyright © 2011 Elsevier Ltd. All rights reserved.