Advanced-Fusion Neutron Source

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Presentation transcript:

Advanced-Fusion Neutron Source Workshop on Advanced Neutron Source and its Application 4-5 November, 2017 Aomori-city, Japan Advanced-Fusion Neutron Source Kentaro OCHIAI National Institutes for Quantum and Radiological Science and Technology (QST) Fusion Energy Research and Development Directorate Department of Fusion Reactor Materials Research Advanced Fusion Neutron Source Design Group

CONTENTS Background and objectives Advanced Fusion Neutron Source Requirement from DEMO fusion reactor design Necessity of early neutron source Present status of IFMIF/EVEDA Advanced Fusion Neutron Source A-FNS project based on IFMIF/EVEDA Site Basic parameters of A-FNS Schedule for A-FNS construction Issues for construction and operation Summary 1

・Diagnostic materials. Background and objectives Requirement from DEMO fusion reactor design Candidate material validation test by fusion neutron source irradiation is an essential issue for DEMO design and it should be done by the end of engineering design phase. Relation of DEMO design (JA) schedule and required irradiation data for materials 2015 2020 2025 2030 2035 DEMO Conceptual Design Engineering Design By 2035, main irradiation verification tests are required about, Blanket First data acquisition ・RAFM as FW First wall ・Blanket materials ・Divertor materials Divertor ・Diagnostic materials. We have to explore a possibility of early intense fusion neutron source construction. 2

Necessity of early neutron source DEMO reactor The DEMO reactor will finally exposed the structure materials up to around 80 dpa. As an initial data for the DEMO design, we think to need the irradiation up to 10 dpa/year at least. DT neutron source including ITER is quite not sufficient from the objectives. Fission reactor and spallation neutron sources will not be appropriate for the verification in the viewpoint of the ratio of He and dpa. Therefore, an fusion neutron source like a IFMIF should be operated around 2030 for the material irradiation. Contour map of helium production rate and displacement per atom (dpa) for fusion reactor and neutron source. We propose the complete achievement of irradiation examination with an advanced fusion neutron source facility ,A-FNS which is like a half intensity of IFMIF by 2035. 3

Present status of IFMIF/EVEDA From 2007, IFMIF/EVEDA has started to validate the construction of IFMIF on BA phase. IFMIF Intermediate Engineering Design Report(2014) Rokkasyo Oarai Linear IFMIF Prototype Accelerator (ongoing) EVEDA Lithium Test Loop (2014) High Flux Test Module (2015) To achieve 9 MeV(CW) operation Long-term stability of high speed liquid flow validated! Prototype manufactured, remote handling tested! We propose an A-FNS construction using by the IFMIF/EVEDA intellectual properties. 4

Advanced Fusion Neutron Source Advanced Fusion Neutron Source based on IFMIF/EVEDA From the viewpoint of the effective use, we will start to an conceptual design activity of an using by the IFMIF/EVEDA. Injector and RFQ+SRF SRF and Beam transport Test facility Related facility 58 60 18 15 11 Unit: meter Grand Accelerator facility L 160 x W 80 x H 25 Neutron point 9 IFMIF/EVEDA Post Irradiation Experiment Radio Active Processing Target handing system Cross sectional views of an A-FNS construction 5 Horizontal cross sectional view of A-FNS accelerator

Net volume for Irradiation Basic parameters of A-FNS Beam Particle Deuteron Energy 40 MeV Current 125 mA (CW) Foot print 200 x 50 mm2 Incident angle Normal Availability 33% at least Target Material lithium Liquid target (jet) Temp. 200 - 270 ℃ Velocity 10-15 m/s at target Schematic view of test cell (Ref. IFMIF design) Thickness 25 mm Net volume for Irradiation Window Free surface (no window) Neutron Intensity 6.8 x 1016 neutron/s 3cc at 25dpa/fpy (at back plate) 15cc at 20 dpa/fpy Average flux 6.0x 1014 n/cm2/s Neutron 80 mm 30cc at 15 dpa/fpy Helium P. R 3.12×102 appm/fpy 60cc at 10 dpa/fpy Displacement 24.7 dpa/fpy HePR/dpa 12.6 High Flux Test Module fpy: full power year Relation of irradiation volume and dpa/fpy (A-FNS)

Site of A-FNS The Pacific Ocean 245m Construction area of A-FNS 450m Rokkasho, Aomori Japan 245m Construction area of A-FNS 450m LIPAc building IFERC Site 110,083.72㎡ 6

Schedule for A-FNS construction 2015 2020 2025 2030 2035 DEMO Conceptual Design Engineering Design Neutron Source for irradiation First data acquisition First irradiation Conceptual design EDA phase Construction Operation Phase Pre-phase Construction decision Start commissioning 7

Issues for construction and operation Technical issues must be solved by 2025 based on the following items. Precise irradiation plans and their schedules Technical issues for plant safety and regulation Cost estimation for construction and operation As others Storage building Console area or building Achievement of LIPAc Extension of building Purification system of Li target Technical feedback from the LIPAc long operation Optimization of lithium target system Extension of SRF and beam line Optimization of HFTM Safety Remote handing for TA and TM Safety Remote handing from TC to PIE Designs of PIE, RIP and Li-HF We just start to verify the design and their development. 8

Another application proposal of A-FNS A-FNS should be also utilized like multi-purposes neutron source. Neutron beam station of A-FNS for material analysis ( it will be available to not only for general material analysises also fusion material micro-analysis) RI production module installation (ex. Mo-99) Pneumatic line to use the intense neutron field We just start to the investigations for the muti-purpose on A-FNS 9

Summary For fusion DEMO reactor design, we have started the design activity of an advanced fusion neutron source (A-FNS) facility. From the viewpoint of the effective use of IFMIF/EVEDA intellectual properties, as a candidate, first of all, we propose the extension type . A-FNS will be like a half size of IFMIF. The volume of irradiation will be narrow than half of IFMIF case. A-FNS should be operated around 2030 for the data acquisition and the availability have to be 33% at least. In case of the test facility, the hot area of remote handing will be most important issue. Especially, the exchange of Li-target assembly will be most serious action. For the construction of A-FNS, we will need to organize a consortium, not only QST, also institutes, universities and corporations. 10

Related presentations in ICFRM-18 11.6 17:00-19:00 6PT56 S.Kwon (QST, Japan) Investigation on A-FNS Neutron Spectrum Monitor System 11.7 16:40-18:40 7PT55 M. Nakamura (QST, Japan) Impact of the Beam Injection Momentum on the Free Surface of the Liquid Lithium Target of Advanced Fusion Neutron Source 11.8 16:40 - 18:40 8PT56 Investigation of Mo-99 Radioisotope Production by d-Li Neutron Source M. Ohta 11.9 16:00-18:00 9PT55 H. Kondo (QST, Japan) Experimental Study on Application of Large-Scale Cold Trap and Impurity Monitoring to Liquid Lithium for Intense Fusion Neutron Source

Conceptual view of A-FNS ECR ion injector RFQ SRF SRF MEBT BD BD Deuteron Energy (MeV) 5 9 14.5 26 40 HEBT Horizontal cross sectional view