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核工程计算物理实验室 Nuclear Engineering Computational Physics 2015-9-17 The Neutronics Studies of Fusion Fission Hybrid Power Reactor Youqi Zheng Ph. D Nuclear Engineering Computational Physics Lab. Xi’an Jiaotong University
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2 Contents Background Fusion Source and Blanket Design Neutronics Design and Sensitivity Analysis Conclusions
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3 NOW2018 2030 2050 3 A long way for the pure fusion energy, but A short way for the application of fusion source Background(1/3) It is well recognized that the fusion fission hybrid power reactor is an important early use of fusion source
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4 After 2000 1991-2000 1986-1990 1980-1985 4 Background(2/3) R&D of hybrid reactor in China Re-evaluation for Producing Energy, Breeding and Transmutation R&D of Hybrid Power Reactor (National Magnetic Confinement Fusion Science Program, 2010)
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Background(3/3) The target—A hybrid power reactor 1000MWe Power Output for 5 years Tritium self-sustaining considering 5% loss Applying the existing fission technology as much as possible Sufficient energy multiplication of blanket for different fusion power The first step Determining the outline of reactor Determining the candidate fuel Evaluating the feasibility 5
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6 Contents Background Fusion Source and Blanket Design Neutronics Design and Sensitivity Analysis Conclusions
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The referred fusion reactor Citing from the works on FDS-I by ASIPP ( under the cooperation in National Magnetic Confinement Fusion Science Program ) 7 Fusion Source and Blanket Design (1/4) ParametersReference Value Major radius/m4 Minor radius/m1 Aspect ratio4 Plasma elongation1.78 Triangularity0.4
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Fusion Source and Blanket Design (2/4) Preliminary evaluation of water cooling blanket 8 200mm is required for the FW based on the press analysis (Referring: for a PWR vessel 43mm is required, but the practical one is >200mm) For the fuel pins and pressurized water coolant with 15.5MPa
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Fusion Source and Blanket Design (3/4) The modular-type pressure tube blanket 9
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Fusion Source and Blanket Design (4/4) The simplified evaluation model 10
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11 Contents Background Fusion Source and Blanket Design Neutronics Design and Sensitivity Analysis Conclusions
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Neutronics Design and Sensitivity Analysis (1/4) Energy multiplication requirements of the fission blanket 12 For the 50MW fusion power Keff >0.9 For the 100~200MW fusion power Keff~0.8 For the 500MW fusion power Keff~0.6
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Neutronics Design and Sensitivity Analysis (2/4) Keff varying in the lifetime of different fuels 13 Reprocessed fuel for high energy multiplication Spent fuel for middle energy multiplication Natural uranium fuel for low energy multiplication
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High energy multiplication blanket 14 Neutronics Design and Sensitivity Analysis (3/4) 14.3%w/o Pu Moderator-fuel ratio 1.0 Gd 2 O 3 0.85%w/o 4.5%w/o Pu More plutonium content Flattened burn-up process Burnable poison is another choice
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Low energy multiplication blanket Higher fusion power and released blanket performance 15 Neutronics Design and Sensitivity Analysis (4/4) Moderator-fuel ratio 0.5 Modified blanket Moderator-fuel ratio 1.0 The same blanket
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16 Contents Background Fusion Source and Blanket Design Neutronics Design and Sensitivity Analysis Conclusions
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The reprocessed fuel containing existing plutonium from PWRs makes the hybrid power reactor feasible in the coming future Progress of fusion technology may encourage the more easier fuels like the natural uranium fuel and directly burning the spent fuel from PWRs Advanced work can and should be boosted based on the analysis 17 Conclusions (1/2)
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Discussions High energy multiplication Fuel support of the reactors –~40tons plutonium will be loaded every 5 years Control of the reactors –90 times multiplication down to 60 times Low energy multiplication For the natural uranium fuel, the required small moderator- fuel ratio is very difficult to achieve for the pressure tubes For the spent fuel, the fuel processing before loading 18 Conclusions (2/2)
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19 eutronics valuation omprehensive ackage ovelty ndeavor ooperation ersist Thank you ! Welcome to: http://necp.xjtu.edu.cn
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