Evaluation and optimization of tritium breeding, shielding and nuclear heating performances of the helium cooled solid breeder blanket for CFETR

Abstract Chinese Fusion Engineering Test Reactor (CFETR) is a new test tokamak device being designed in China aimed to bridge gaps between ITER and DEMO. As one of the candidate tritium breeding blankets, a conceptual design scheme of the helium cooled solid breeder blanket has been proposed and a series of preliminary analyses have been carried out to access the performances. However, both the required global tritium breeding ratio for CFETR not less than 1.2 and its poor working conditions under intense radiation need further thorough neutronics analyses and optimizations during the design phase. In this work, first, three-dimensional neutronics model of CFETR was built, and the neutron wall loading and global TBR were obtained. The nuclear and thermal calculation results were automatically coupled, which could make the neutronics calculation results more accurate and guaranteed they could always satisfy the corresponding thermal limits during the whole process. Then, the tritium breeding and shielding performances of both the outboard and inboard equatorial blanket modules were optimized for the comprehensive optimal schemes. The influences of Be/W armors on the shielding performance and TBR were also investigated. Finally, the nuclear heating rates and the neutron flux densities in different components were calculated based on the obtained comprehensive optimal scheme. In this paper, the neutronics analyses and optimizations verified that the optimized conceptual design could well meet the tritium self-sufficiency and neutron shielding requirements, and this could provide a valuable reference for the further thermal-hydraulic analysis and structural optimization of the CFETR helium cooled solid breeder blanket.

[1]  Wenxi Tian,et al.  Numerical research on the neutronic/thermal-hydraulic/mechanical coupling characteristics of the optimized helium cooled solid breeder blanket for CFETR , 2017 .

[2]  S. Tosti,et al.  Behaviour of hydrogenated lead–lithium alloy , 2017 .

[3]  Chia-Chieh Shen,et al.  Passivation and reactivation of Ti25V35Cr40 hydrides by cycling with impure hydrogen gas , 2015 .

[4]  Wenxi Tian,et al.  Development of a MCNP–ORIGEN burn-up calculation code system and its accuracy assessment , 2014 .

[5]  Zhongliang Lv,et al.  Preliminary neutronics design and analysis of helium cooled solid breeder blanket for CFETR , 2015 .

[6]  William R. Martin,et al.  Pseudo material construct for coupled neutronic-thermal-hydraulic analysis of VHTGR , 2005 .

[7]  Xiaokang Zhang,et al.  Nuclear-thermal-coupled optimization code for the fusion breeding blanket conceptual design , 2016 .

[8]  Zhongliang Lv,et al.  Thermal-mechanical analysis of the first wall for CFETR helium cooled solid breeder blanket , 2015 .

[9]  Lorenzo V. Boccaccini,et al.  Preliminary steady state and transient thermal analysis of the new HCPB blanket for EU DEMO reactor , 2016 .

[10]  Lorenzo V. Boccaccini,et al.  Preliminary structural analysis of the new HCPB blanket for EU DEMO reactor , 2016 .

[11]  M. Ghoranneviss,et al.  RETRACTED: Feedback controller input design for ignition of deuterium–tritium in NSTX tokamak , 2016 .

[12]  Yuntao Song,et al.  Thermal hydraulic analysis of the HECLIC blanket breeder unit for CFETR , 2015 .

[13]  Wenxi Tian,et al.  Preliminary accident analysis of Loss of Off-Site Power and In-Box LOCA for the CFETR helium cooled solid breeder blanket , 2017 .

[14]  R. Aymar,et al.  Overview of ITER-FEAT - The future international burning plasma experiment , 2001 .

[15]  Hacı Mehmet Şahin,et al.  Investigation of tritium breeding ratio using different coolant material in a fusion–fission hybrid reactor , 2016 .

[16]  Zhongliang Lv,et al.  Preliminary structural design and thermo-mechanical analysis of helium cooled solid breeder blanket for Chinese Fusion Engineering Test Reactor , 2015 .

[17]  H. Petersen,et al.  The properties of helium: Density, specific heats, viscosity, and thermal conductivity at pressures from 1 to 100 bar and from room temperature to about 1800 K , 1970 .

[19]  T. Tang,et al.  Preparation technique and alloying effect of aluminide coatings as tritium permeation barriers: A review , 2015 .

[20]  Guangming Zhou,et al.  Conceptual design and analysis of the helium cooled solid breeder blanket for CFETR , 2015 .

[21]  Rosaria Villari,et al.  Tokamak D-T neutron source models for different plasma physics confinement modes , 2012 .

[22]  S. Zheng,et al.  Tritium self-sufficiency of HCPB blanket modules for DEMO considering time-varying neutron flux spectra and material compositions , 2013 .

[23]  Zaixin Li,et al.  Neutronics study on HCCB blanket for CFETR , 2017 .

[24]  Qingwei Yang,et al.  Overview of the present progress and activities on the CFETR , 2017 .

[25]  J. F. Briesmeister MCNP-A General Monte Carlo N-Particle Transport Code , 1993 .

[26]  Yu.A. Sokolov,et al.  ITER conceptual design , 1991 .