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Program - Brookhaven National Laboratory

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Uncertainty Assessment for fast Reactors Based on Nuclear Data Adjustment<br />

T. Ivanova, E. Ivanov, F. Ecrabet<br />

Institut de Radioprotection et de Surete Nucleaire<br />

For the purpose of safety assessment, IRSN studies issues of use of high-accurate codes and methods for fast<br />

reactor simulation and uncertainty study. The unbiased Monte Carlo methods (MCNP code and SCALE<br />

sequences) are used together with deterministic methods (ERANOS code) for computation of fast system<br />

neutronics parameters. The cross-section adjustment technique has been recently implemented in the<br />

IRSN’s in-house BERING validation tool in order to establish values for the robust biases and uncertainties<br />

in these parameters. The adjustment technique is used for consolidation of a prior set of integral parameters<br />

measured in benchmark experiments and a corresponding set of calculated parameters obtained with<br />

mentioned computational codes. A better understanding of the performance of the adjustment methodology<br />

is needed in order to improve the confidence concerning its validity and applicability for uncertainty<br />

assessment. The benchmark exercise, established by the OECD/NEA Working Party on International<br />

Nuclear Data Evaluation Co-operation (WPEC) Subgroup 33, offers a very good opportunity to learn the<br />

drawbacks and advantages of the adjustment and to test BERING performance. The benchmark exercise<br />

has been proposed with the aim to test different methods of nuclear data adjustment and different sets of<br />

covariance data, so as to reduce the design uncertainties of a particular type of sodium-cooled fast reactor.<br />

The exercise uses a single, limited set of integral experiments and measurements, which include Keff for<br />

Jezebel, Jezebel- 240 Pu, Flattop- 240 Pu, ZPR6-7, ZPR6-7 with high 240 Pu content, ZPPR-9 and Joyo MK-1;<br />

reaction rates for Jezebel, Flattop- 240 Pu, ZPR6-7 and ZPPR-9; and sodium void effects for ZPPR-9. The<br />

final results are tested on a model of the Advanced Fast Burner Reactor (ABR) with plutonium oxide fuel<br />

and a model of the Fast Breeder Reactor (FBR) core. Every participant to the benchmark is supposed<br />

to use the same integral experiment values and uncertainties, but their own calculated values, sensitivity<br />

coefficients, and adjustment method. Own or same initial cross sections and nuclear data covariances can<br />

be used depending on step of the exercise. The full paper will present IRSN’s results of the benchmark<br />

exercise generated using different sets of input data: integral parameters and sensitivity coefficients computed<br />

by the deterministic ERANOS code and the Monte Carlo and deterministic SCALE6.0 sequences;<br />

ENDF/B-VI.8 and ENDF/B-VII cross-section data; COMMARA 2.0 and TENDL-2011 covariances; with<br />

and without integral correlations provided by JAEA. The outcomes of BERING will be analyzed and<br />

compared in order to demonstrate whether the results of the adjustment converge when using different<br />

input cross-section covariances. The impact of different calculation methods’ approximation bias will also<br />

be shown.<br />

OB 4 2:40 PM<br />

New JEFF-3.2 Sodium Neutron Induced Cross-Sections Evaluation for Neutron Fast<br />

Reactors Applications: from 0 to 20 MeV<br />

P. Archier, G. Noguère, C. De Saint Jean<br />

CEA, DEN, DER, SPRC, LEPh, Cadarache, F-13108 Saint-Paul-lez-Durance, France<br />

A.J.M. Plompen, C. Rouki<br />

JRC-IRMM, Retieseweg, 2440 Geel, Belgium<br />

The current JEFF-3.1.1 sodium evaluation shows large discrepancies with the microscopic measurements<br />

available on the EXFOR database. Furthermore, no cross-sections covariance matrices are available in this<br />

file, which are of interest for fast reactor applications. In the framework of the ASTRID project (French<br />

sodium fast reactor), a new sodium evaluation, from 0 to 20 MeV, have been carried out using the CONRAD<br />

code. This file contains both re-evaluated nuclear data and covariances and is divided in two energy<br />

207

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