Abstract
Keywords
Introduction
Theory and method
Framework and code development
Numerical results and analysis
Conclusions
Declaration of Competing Interest
Acknowledgments
References
Abstract
The fusion-reactor blanket is very important, as it is responsible for the tritium self-sustaining, energy gain, and radiation shielding. Due to the complex structure, large geometry size and inhomogeneous neutron-flux distribution, the Monte-Carlo method is widely used for the neutronics analysis of fusion-reactor blanket, but it takes a large amount of computational time for acceptable simulation results. The deterministic code is the better choice for the fusion-reactor blanket. The geometry capability and accuracy limitation are the most important issues for the deterministic code to simulate the fusionreactor blanket. Therefore, the newly deterministic code named NECP-FISH has been developed for the fusion-reactor blanket, in which the spherical harmonic function and finite element method were applied. Moreover, the open-source platform SALOME has been applied to generate the complex geometry as pre-process of NECP-FISH. As code verification, NECP-FISH has been applied to simulate the Breeding Unit of HCCB-DEMO, using Monte-Carlo code to provide the reference results. It can be observed that the simulation results of the tritium breeding ratio (TBR), neutron flux and heat release rate provided by NECP-FISH are agreed well with corresponding values by the Monte-Carlo code.
Introduction
The fusion-reactor blanket is very important, as it is responsible for the tritium self-sustaining, energy gain, and radiation shielding. However, the geometry of the fusion-reactor blanket is very complicated, as there are many irregular structures applied in the blanket. Therefore, the Monte-Carlo method has been widely applied to perform the neutronics analysis of the fusion-reactor blanket, because of its advantage in powerful capability for complex geometry. As improvement in geometry modeling, the Monte-Carlo codes McCad (Große et al., 2013) and MCAM (Wu, 2009) have been updated to automatically generate the input card based on the CAD files of fusion-reactor blanket. However, large amount of particles are required for the Monte-Carlo code to simulate the fusionreactor blanket, which takes a long computational time. Therefore, the deterministic method is another choice for the modeling and simulation of the fusion-reactor blanket.