Program - Brookhaven National Laboratory
Program - Brookhaven National Laboratory
Program - Brookhaven National Laboratory
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transmuters, inclusive covariance data with respect to both the target nuclides and reactions are needed.<br />
To meet this requirement, the Japanese Evaluated Nuclear Data Library (JENDL-4.0) [1], released in<br />
2010, places much emphasis on the improvements of the covariance data; covariances for all reactions of<br />
almost all nuclides, as well as reaction parameters, were newly evaluated and/or revised based on available<br />
experimental data and theoretical calculations using the nuclear data evaluation codes. The objective of<br />
this study is to derive the reactor physics parameters with total uncertainty on ADS and FR with the use<br />
of the JENDL-4.0 cross-section and covariance data, and compare to the older one, JENDL-3.3. For ADS,<br />
the basic concept investigated in Japan Atomic Energy Agency (JAEA) [2] was adopted, namely the 800<br />
MWth lead-bismuth eutectic (LBE) cooled type ADS with nitride fuel (MA ratio: 63.7 wt%). For FR,<br />
we selected the 3,600 MWth sodium-cooled type FR with MOX fuel (MA ratio: 5.0 wt%) based on the<br />
concept investigated in the feasibility study in Japan [3]. As the reactor physics parameters, the criticality<br />
(keff ), coolant void reactivity, and Doppler reactivity was analyzed. Then, to identify the cause of the<br />
differences of the parameters between the two libraries, we analyezed differences by nuclies and reactions<br />
with the use of the sensitivity coefficients calculated by the sensitivity calculation code, SAGEP [4]. We<br />
also investigated nuclide- and reaction-wise uncertainties on the two reactors and compare the differences<br />
of the uncertainties between JENDL-4.0 and JENDL-3.3.<br />
[1] K. Shibata, O. Iwamoto, T. Nakagawa, et al., J. Nucl. Sci. and Technol., 48, 1, 1 (2011). [2] K.<br />
Nishihara, K. Iwanaga, K. Tsujimoto, et al., J. Nucl. Sci. and Technol., 45, 8, 812 (2008). [3] Japan<br />
Atomic Energy Agency, JAEA-Research 2006-042 (2006) [in Japanese]. [4] A. Hara, T. Takeda, and Y.<br />
Kikuchi, JAERI-M 84-065 (1984) [in Japanese].<br />
LC 4 4:40 PM<br />
Propagation of Neutron Cross Section, Fission Yield, and Decay Data Uncertainties in<br />
Depletion Calculations<br />
J. S. Martínez Gonzälez, L. Gallner, W. Zwermann, F. Puente-Espel, O. Cabellos, K. Velkov, A. Pautz<br />
Gesellschaft für Anlagen- und Reaktorsicherheit (GRS) mbH<br />
A complete reactor physics study requires not only the calculation of the values of interest but the assessment<br />
of their uncertainties arising from the nuclear data used. XSUSA represents a validated methodology<br />
to propagate cross-section uncertainties and analyze their impact on reactor analysis. However, until<br />
recently, it did not include the propagation of fission yields and decay constants uncertainties, relevant<br />
magnitudes for burn-up calculations and isotopic predictions. We describe in this paper a technique to<br />
propagate these fission yields and decay data uncertainties following the XSUSA procedure, that is, the<br />
generation, from the basic nuclear data, of varied libraries to be used by SCALE6.1 for reactor calculations.<br />
SCALE6.1 employs the ORIGEN-S module to perform depletion calculations. An automated process to<br />
vary the ORIGEN-S fission yields and decay input libraries according to the uncertainties found in the<br />
nuclear data files has been developed and applied to the ENDF/B-VII library. In order to study the impact<br />
of the uncertainties on depletion calculations, a light water reactor pin cell model as defined in the<br />
UAM Phase I Benchmark has been used. 1.000 depletion calculations were executed repeatedly using the<br />
different varied libraries. Various cases have been studied, perturbing (1) the fission yield libraries, (2) the<br />
decay libraries, (3) the neutron cross section libraries, and (4) all libraries simultaneously. This strategy<br />
helps us to shed light on the separate and combined effect of their uncertainties on the multiplication<br />
factors and isotopic content during the depletion cycle. It turns out that for the system under consideration,<br />
the multiplication factor uncertainty is dominated by the neutron cross section uncertainties. For<br />
certain isotopes, however, fission yield und decay data uncertainties may give significant contributions to<br />
the uncertainties of the respective concentrations.<br />
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