Computing eigenvalue sensitivity coefficients to nuclear data based on the CLUTCH method with RMC code. (February 2016)

• Record Type: Journal Article
• Authors: Qiu, Yishu; She, Ding; Tang, Xiao; Wang, Kan; Liang, Jingang
• Is Part Of: Annals of nuclear energy. Volume 88(2016:Feb.)
• Page Start: 237
• Page End: 251
• Publication Date: 2016-02
• Subjects: Monte Carlo -- Sensitivity analysis -- Nuclear data -- F-CLUTCH -- RMC; Nuclear energy -- Periodicals; Nuclear engineering -- Periodicals; 621.4805
• DOI: 10.1016/j.anucene.2015.11.007
• Languages: English
• ISSNs: 0306-4549

Abstract

Highlights: A new algorithm is proposed to reduce memory consumption for sensitivity analysis. The fission matrix method is used to generate adjoint fission source distributions. Sensitivity analysis is performed on a detailed 3D full-core benchmark with RMC. Abstract: Recently, there is a need to develop advanced methods of computing eigenvalue sensitivity coefficients to nuclear data in the continuous-energy Monte Carlo codes. One of these methods is the iterated fission probability (IFP) method, which is adopted by most of Monte Carlo codes of having the capabilities of computing sensitivity coefficients, including the Reactor Monte Carlo code RMC. Though it is accurate theoretically, the IFP method faces the challenge of huge memory consumption. Therefore, it may sometimes produce poor sensitivity coefficients since the number of particles in each active cycle is not sufficient enough due to the limitation of computer memory capacity. In this work, two algorithms of the Contribution-Linked eigenvalue sensitivity/Uncertainty estimation via Tracklength importance CHaracterization (CLUTCH) method, namely, the collision-event-based algorithm (C-CLUTCH) which is also implemented in SCALE and the fission-event-based algorithm (F-CLUTCH) which is put forward in this work, are investigated and implemented in RMC to reduce memory requirements for computing eigenvalue sensitivity coefficients. While the C-CLUTCH algorithm requires to store concerning reaction rates of every collision, the F-CLUTCH algorithm only stores concerning reaction rates of every fission point. In addition, the fission matrix method is put forward to generate the adjoint fission source distribution for the CLUTCH method to compute sensitivity coefficients. These newly proposed approaches implemented in RMC code are verified by a SF96 lattice model and the MIT BEAVRS benchmark problem. The numerical results indicate the accuracy of the F-CLUTCH algorithm is the same as the C-CLUTCH algorithm while the F-CLUTCH algorithm requires less memory and has higher computational efficiency.