Published January 2018 | Version v1
Journal article

Burn-up characteristics and criticality effect of impurities in the graphite structure of a commercial-scale prismatic HTGR

  • 1. HTGR Hydrogen and Heat Application Research Center, Japan Atomic Energy Agency (JAEA), 4002 Narita-cho, Oarai-machi, Higashiibaraki-gun, Ibaraki 319-1395 (Japan)

Description

Highlights: • We evaluate the criticality effect of impurities in graphite block for HTGR by whole core burn-up calculations. • We confirm the boron equivalent can be also employed for burn-up calculations. • We conclude fine purified grade graphite IG-110 is not necessary from the viewpoint of criticality. - Abstract: This study investigates the burn-up characteristics and the criticality effect of impurities in the graphite structure of commercial-scale prismatic High Temperature Gas-cooled Reactor (HTGR), and thereby reconsiders the necessity of high-grade graphite material. In an HTGR, the core is filled with the graphite, and the impurities in the graphite have a non-negligible poison effect on the criticality. To account for the effect of the reflector blocks deployed adjacent to the fuel blocks, GTHTR300, commercial-scale HTGR, employed fine purified grade graphite material IG-110. Ideally, the fuel blocks should also employ IG-110; however, for economic purposes they are constructed from an un-purified grade graphite material IG-11. The poisoning effect of the impurity (which behaves like 10B burn-up and is expressed in boron equivalents) decreases exponentially and eventually saturates at 1% of the initial boron equivalent. However, the reactivity worth of the fuel and reflector blocks with 0.03 ppm boron equivalents (equivalent to 1% of IG-11) is negligible (i.e., k/kk′). Because the poisoning effect of the impurity mimics that of naturally occurring boron, it was evaluated in whole-core burn-up calculations with the impurities represented by naturally occurring boron. According to the results, the criticality of the commercial-scale HTGR is unaffected by the impurity levels (even in the un-purified grade IG-11) because the impurities burn cleanly until the End of Cycle (EOC). Therefore, the economy of electricity generation by HTGRs can be improved by using the un-purified grade IG-11 instead of the fine purified grade graphite IG-110.

Availability note (English)

Available from http://dx.doi.org/10.1016/j.nucengdes.2017.11.003

Additional details

Identifiers

DOI
10.1016/j.nucengdes.2017.11.003;
PII
S0029549317305071;

Publishing Information

Journal Title
Nuclear Engineering and Design
Journal Volume
326
Journal Page Range
p. 108-113
ISSN
0029-5493
CODEN
NEDEAU

Optional Information

Copyright
Copyright (c) 2017 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.