Author/Authors :
Y. Boulaich، نويسنده , , Y. and El Bardouni، نويسنده , , T. and Erradi، نويسنده , , L. and Chakir، نويسنده , , E. and Boukhal، نويسنده , , H. and Nacir، نويسنده , , B. and El Younoussi، نويسنده , , C. and El Bakkari، نويسنده , , B. and Merroun، نويسنده , , O. and Zoubair، نويسنده , , M.، نويسنده ,
Abstract :
In the present work, we analyze the CREOLE experiment on the reactivity temperature coefficient (RTC) by using the three-dimensional continuous energy code (MCNP5) and the last updated nuclear data evaluations. This experiment performed in the EOLE critical facility located at CEA/Cadarache, was mainly dedicated to the RTC studies for both UO2 and UO2–PuO2 PWR type lattices covering the whole temperature range from 20 °C to 300 °C. We have developed an accurate 3D model of the EOLE reactor by using the MCNP5 Monte Carlo code which guarantees a high level of fidelity in the description of different configurations at various temperatures taking into account their consequence on neutron cross section data and all thermal expansion effects. In this case, the remaining error between calculation and experiment will be awarded mainly to uncertainties on nuclear data. Our own cross section library was constructed by using NJOY99.259 code with point-wise nuclear data based on ENDF-BVII, JEFF3.1 and JENDL3.3 evaluation files. The MCNP model was validated through the axial and radial fission rate measurements at room and hot temperatures. Calculation-experiment discrepancies of the RTC were analyzed and the results have shown that the JENDL3.3 and JEFF3.1 evaluations give the most consistent values; the discrepancy is less than 0.23 pcm/°C. Whereas, when using ENDF-BVII evaluation for UOX configuration, this discrepancy reaches a value of 0.63 pcm/°C. In order to specify the source of this relatively large discrepancy in the case of ENDF-BVII nuclear data evaluation, the keff discrepancy between ENDF-BVII and JENDL3.3 was decomposed by using sensitivity and uncertainty analysis technique. The thermal energy range of 238U(n,γ) absorption cross section was found to contribute to the major part of the observed keff discrepancy between ENDFB-VII and JENDL3.3 evaluations.
