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[1] D. Jacquet and M. Morjean, Prog. Part. and Nucl. Phys. 63 (2009) 155 [2] P. Grangé, L. Jun-Qing<br />

and H.A. Weidenmuller, Phys. Rev. C 27 (1983) 2063<br />

Session RC Covariances<br />

Friday March 8, 2013<br />

Room: Empire East at 10:30 AM<br />

RC 1 10:30 AM<br />

Applications of Nuclear Data Covariances to Criticality Safety and Spent Fuel<br />

Characterization<br />

M. L. Williams, G. Ilas, W. J. Marshall, B. T. Rearden<br />

Oak Ridge <strong>National</strong> Lab<br />

During the last several years much advancement has been made in providing nuclear data covariances<br />

for nuclear technology applications. These advancements include new covariance evaluations released in<br />

ENDF/B-VII.1 [1] for many important nuclides, as well as more approximate “low fidelity” uncertainty<br />

data [2] for nuclides without covariance evaluations in ENDF/B nuclear data files. Using these resources,<br />

a comprehensive library of covariance data [3] has been developed for the SCALE code system. [4] This<br />

covariance library – along with the sensitivity/uncertainty (S/U) computation methods in SCALE – allow<br />

realistic uncertainty analysis of diverse types of applications. [5] Previously, most uncertainty analysis with<br />

SCALE has focused on determining uncertainties in the multiplication factor (keff) for criticality safety<br />

applications. The SCALE S/U methodology was recently used in a comprehensive study to compute<br />

eigenvalue uncertainties for a large number of critical experiments. [6] In this paper we compare results<br />

obtained from uncertainty analysis using the SCALE nuclear data covariances, and the actual distribution<br />

of the computed benchmark multiplication factors. SCALE uncertainty analysis for critical eigenvalues is<br />

based on first order perturbation, which is a very efficient technique for determining the uncertainty in a<br />

single response (keff) for a fixed invariant system. At present this perturbation approach cannot be applied<br />

to burnup calculations where a large number of responses are of interest, and where the composition of<br />

the system (i.e., reactor) varies as a function of time due to non-linear interactions between the neutron<br />

flux and nuclide fields. A new method based on statistical sampling [7] has recently been developed for<br />

SCALE. When combined with a comprehensive covariance library, the statistical sampling method allows<br />

uncertainty analysis to be performed for reactor burnup calculations to obtain uncertainties in spent<br />

fuel responses, which are important for burned fuel transportation, on-site storage, and disposition. [8]<br />

Computed uncertainties are presented for time-dependent responses such as actinide and fission isotopics,<br />

decay heat, and decay activity, which depend on uncertainties in the nuclear data of many fission products<br />

and actinides.<br />

[1] M. B. Chadwick, et al “ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections,<br />

Covariances, Fission Product Yields and Decay Data,” Nuclear Data Sheets 112, 12, 2887-2996 (December<br />

2011). [2] R. C. Little, et al., “Low-fidelity Covariance Project” Nuclear Data Sheets 109, 2828 (2008).<br />

[3] M. L. Williams and B. T. Rearden “Sensitivity/Uncertainty Analysis Capabilities and New Covariance<br />

Data Libraries in SCALE” Nuclear Data Sheets 109, 12, 2796-2800 (December 2008). [4] “SCALE: A<br />

Comprehensive Modeling and Simulation Suite for Nuclear Safety Analysis and Design,” ORNL/TM-<br />

2005/39, Version 6.1, Oak Ridge <strong>National</strong> <strong>Laboratory</strong>, Oak Ridge, Tennessee (June 2011). [5] B. T.<br />

Rearden, M. L. Williams, M. A. Jessee, D. E. Mueller, D. A. Wiarda. “Sensitivity and Uncertainty<br />

Analysis Capabilities in SCALE” Nuclear Technology 174, 236-288 (May 2011) [6] W. J. Marshall and<br />

B. T. Rearden, Criticality Safety Validation of SCALE 6.1, ORNL/TM-2011/450, Oak Ridge <strong>National</strong><br />

251

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