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Program - Brookhaven National Laboratory

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ZPR-6/10 cores were applied as comparable core sets with blanket and reflector. The FCA X-1 and X-2<br />

cores were constructed at the Fast Critical Assembly (FCA) facility of JAEA for the mockup experiments<br />

of the Joyo Mk-II core. The FCA X-1 core was surrounded by depleted uranium blanket and the X-2<br />

core by sodium and stainless steel reflector while the compositions of the two cores were identical. The<br />

Joyo Mk-I and Mk-II cores were constructed at the experimental fast reactor Joyo of JAEA. The Joyo<br />

Mk-I core was surrounded by UO2 blanket and the Mk-II core by stainless steel reflector. The ZPR-3/53,<br />

-3/54 and ZPR-6/10 cores were constructed at the Zero Power Reactor (ZPR) critical assembly of ANL.<br />

The ZPR-3/53 was surrounded by depleted uranium blanket and the ZPR-3/54 by iron reflector while the<br />

compositions of the two cores were identical. The ZPR-6/10 was surrounded by stainless steel reflector<br />

and the core composition was different from those of ZPR-3/53 and -3/54. We analyzed reflector effects by<br />

comparing the ratio of calculation to experimental (C/E) values of keff between the cores with reflector and<br />

blanket, e.g. the FCA X-1 and X-2 cores. The keff calculations were performed by using the continuous<br />

energy Monte Carlo code MVP. Sensitivity analyses were also done to specify the source of keff difference<br />

among the nuclear data libraries. Sensitivity coefficients were obtained by diffusion calculations using a<br />

generalized perturbation code, SAGEP. In the benchmark test for the FCA cores by JENDL-4.0, there<br />

are no dependence of the C/E values between the FCA X-1 (depleted uranium blanket) and X-2 (stainless<br />

steel reflector) cores. On the contrary, by ENDF/B-VII.1, there appears a significant underestimation for<br />

the FCA X-2 core with reflector. From the sensitivity analysis, the different behaviors of the C/E values<br />

between JENDL-4.0 and ENDF/B-VII.1 are due to the discrepancies of µ-bar of Cr-52 and Na, the elastic<br />

scattering cross-section of Fe-57, Ni-60 and Al. This paper presents the results of the other cores and<br />

the JEFF-3.1.2. Finally, recommendations to nuclear-data study are summarized on the scattering-related<br />

data evaluation.<br />

PE 2 4:00 PM<br />

Analysis of the Neutronic Properties of the Prototype FBR Monju Based on Several<br />

Evaluated Nuclear Data Libraries<br />

W.F.G. van Rooijen, N. Yamano, Y. Shimazu<br />

Research Institute of Nuclear Engineering, University of Fukui<br />

In a recent study [1] an uncertainty analysis was presented for the criticality of the prototype FBR Monju<br />

using JENDL-4.0. In the course of the research for that paper, a considerable deviation was found for the<br />

reactivity as a function of which set of nuclear data was used. This deviation occurred in the analysis of<br />

Monju as well as in the analysis of benchmark experiments. In some cases, the deviation is larger than the<br />

expected error margins due to uncertainties in the nuclear data. The analyses of the neutronic properties<br />

of Monju published by JAEA were obtained using highly specific code systems using cross sections and<br />

covariance data that are specially adjusted for Monju, so in that sense it is not surprising that calculations<br />

with unadjusted data give different results. However, in general it would be desirable that evaluated nuclear<br />

data is of such a quality that adjustment for a specific application is not necessary. Besides, FBRs that are<br />

being designed for future applications, such as ASTRID (France) and JSFR (Japan) have design features<br />

for which no or very few experimental data are available. This means that a proper data adjustment<br />

is difficult or even impossible, and one may need (expensive) measurement campaigns to obtain enough<br />

experimental information to perform a proper data adjustment. To see how well modern nuclear data is<br />

capable of predicting the neutronic properties of an FBR, we are analyzing the prototype FBR Monju with<br />

the well-established ERANOS software. An automated system to generate cross sections and covariance<br />

data for ERANOS has been created. Monju was operated in 1994 / 1995 and 2010, and the 15-year<br />

shutdown period has caused considerable changes in the fuel composition (increase of Am-241). For the<br />

238

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