JAEA-Conf 2011-002 - 日本原子力研究開発機構
JAEA-Conf 2011-002 - 日本原子力研究開発機構
JAEA-Conf 2011-002 - 日本原子力研究開発機構
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JENDL-3.3 showed better applicability to the HTTR criticality calculations than the other<br />
libraries as mentioned above, but still overestimated the keff values by 0.5-1.1%k.<br />
Overestimating the keff values, the calculation result of the loaded number of the fuel columns<br />
achieving the first criticality did not agree with the experimental results. These problems has<br />
not been resolved until today, despite our efforts of the refinement such as the description of the<br />
core geometry and the concentration of the components. Meanwhile, the neutron capture cross<br />
section of carbon at 0.0253eV stored in each nuclear data library had not been revised for a long<br />
time. Thus we proposed this cross section should be revised based on the latest measurement<br />
data, and also predicted that the problem of overestimating the keff values will be resolved by<br />
revising the cross section to be about 10% larger than that of JENDL-3.3.<br />
In May 2010, the latest JENDL: JENDL-4.0[2], was released by <strong>JAEA</strong>. In JENDL-4.0, our<br />
proposal and prediction were applied, and the neutron capture cross section of carbon at<br />
0.0253eV was revised based on the latest measurement data[3]. Accordingly the problem of<br />
overestimating the keff values in the HTTR criticality calculations was expected to be improved.<br />
This paper describes the investigation of the applicability of JENDL-4.0 to the HTTR criticality<br />
calculations.<br />
2. Calculations for HTTR critical approach with JENDL-4.0<br />
2.1 Objective and method<br />
The objective of this study is to investigate the applicability of JENDL-4.0 to the HTTR<br />
criticality calculations. The investigation was performed by comparing (a)The loaded number of<br />
fuel columns achieving the first criticality, and (b)Excess reactivity of the fully loaded core,<br />
between the experimental results and the calculation results with several nuclear data libraries,<br />
which are JENDL-4.0, previous JENDL: JENDL-3.3, the latest ENDF: ENDF/B-VII.0, and the<br />
latest JEFF: JEFF-3.1. Additionally, identification of nuclides which have large effects on the<br />
difference of the following issues among the libraries was studied.<br />
2.2 HTTR critical approach<br />
<strong>JAEA</strong>-<strong>Conf</strong> <strong>2011</strong>-<strong>002</strong><br />
(1) HTTR<br />
The HTTR is a graphite-moderated and helium gas-cooled block-type HTGR, situated at<br />
<strong>JAEA</strong>-Oarai Resarch and Development Center. It has 30MW thermal power and its outlet<br />
coolant temperature, which can be used for nuclear heat utilization, is 850C in rated power<br />
operation. Additionally, the HTTR can also be operated in high temperature test operation<br />
mode, with which its outlet coolant temperature is 950C.<br />
Figure 1 shows radial and bird-eye views of the HTTR core. The core is constructed by<br />
stacking four kinds of hexagonal blocks, which are fuel blocks, control rod guide blocks,<br />
replaceable reflector blocks and irradiation blocks (for irradiation test), and is surrounded by<br />
permanent reflectors made of graphite. All these hexagonal blocks are made of high-purity<br />
graphite, and are the same in across flats (36cm) and height (58cm). Fuel region in the core is<br />
composed of 30 fuel columns, in which five fuel blocks are stacked.