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In-Vessel Tritium Inventory in Fusion DEMO Plant at JAERI Hirofumi Nakamura and JAERI-DEMO design team Japan Atomic Energy Research Institute(JAERI) Japan-US.

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Presentation on theme: "In-Vessel Tritium Inventory in Fusion DEMO Plant at JAERI Hirofumi Nakamura and JAERI-DEMO design team Japan Atomic Energy Research Institute(JAERI) Japan-US."— Presentation transcript:

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2 In-Vessel Tritium Inventory in Fusion DEMO Plant at JAERI Hirofumi Nakamura and JAERI-DEMO design team Japan Atomic Energy Research Institute(JAERI) Japan-US Workshop on Fusion Power Plants and Related Advanced Technologies with participation of EU January 11-13, 2005 at Tokyo, JAPAN

3 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 2 Tritium Issues in Fusion Power Plant Tritium inventory in fusion power plant relates - Tritium inventory control (Accountancy of T production and consumption, Waste management) - Source term for safety assessment (Accidental and normal T release) - Design basis of tritium processing plant (Water detritiation system of cooling system, T removal method from materials) Knowledge on tritium inventory is essential to safety and economical design of the fusion power plant

4 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 3 Objective and Outline OBJECTIVE -To estimate in-vessel tritium inventory in the Fusion DEMO reactor designed by JAERI -To clarify critical tritium issue on inventory reduction or on tritium inventory control in DEMO OUTLINE - Clarification of difference of specification concerning T inventory issues between DEMO and ITER - Evaluation of T inventory in DEMO  analytical method  analytical conditions  analytical results - Characterization of feature of T inventory issues in DEMO

5 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 4 Difference of basic specification between DEMO and ITER on T issues Basic parameters ITERDEMO Fusion power0.5 GW3 GW(1 GWe) OperationPulse operationSteady operation (75%/year) Coolant temp.Low (<450K)High (600~700K) T consumption~17 gT/day~450 gT/day T productionnegligible~500 g/day(TBR=1.1) Site T inventory~3 kgT<3 kgT PFCW/Be/CFC/CuW/F82H StructureSS316/WaterF82H/Water BLKvariousSolid breeder /Water Reactor operation Fuel cycle Material selection

6 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 5 T Inventory in ITER and DEMO ITERDEMO T in T plant~1 kgTSame with ITER T in PFC~1 kgT (0.35 kgT) Mainly in Co-deposition layer How much amount of T? Mainly ? T in coolant<2 gT (mainly from Be FW) T concentration <<10 Ci/L* How much amount of T? Where from mainly? (There is rough estimation from BLK region) T in BLKTBD (Maybe negligible)How much amount of T? (There is rough estimation) Key issue on T inventory Only the co-deposition of carbon and tritium is a critical problem in ITER. What is the critical issue on T inventory in DEMO? *Based on the safety handling experience of tritiated water in CANDU reactor. Evaluation of Tritium inventory in DEMO

7 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 6 Evaluation method Tritium inventory evaluation - Classified the DEMO into several in-vessel components - One dimensional analysis for simplification - Combined tritium transport and thermal transport analysis for one-dimensional analytical system (TMAP5 code) Tritium transport  :density, C p :heat capacity, T:temp.,  :thermal conductivity, S h :Heat source C(x,t):T concentration, S:T source J:diffusion flux, γ:decay constant D eff :Effective diffusivity, Q*:heat of transport t, Thermal transport To solve tritium inventory using above analytical system - Operational conditions (heat load, particle load,etc.) - Tritium transport properties (Diffusivity, Solubility etc.) are necessary

8 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 7 Classified In vessel components in DEMO for T inventory analysis VV DIV/FW BLK In-vessel component in DEMO DEMO components were classified into - PFC Divertor (DIV), First wall(FW) - Blanket(BLK) - Structure material (VV) - Coolant

9 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 8 Detail of classified in-vessel components in DEMO FW DIV VV FW and BLK Coolant T inventory in coolant is evaluated by permeation from the components W armor F82H Cooling tube Thermal and particle load Cooling Tube 1st Breeding Layer Coolant manifold 1st Multiplier Layer Third Breeder Layer 2nd Breeder Layer 2nd Multiplier Layer Third Multiplier Layer BLK Thermal and particle load W F82H W 1.5mm t

10 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 9 Operating conditions of the in- vessel components of DEMO DIV Thermal load (heat flux/Temp.) Particle Load PFCcoolantFluxRange DEMO7/12734733x10 23 2.5nm FW Thermal load (heat flux/Temp.) Particle Load PFCcoolantFluxRange DEMO0.6/7736033x10 21 2.5nm Unit of parameters Heat flux: MW/m 2 /s, Temp.: K, Flux:DT/m 2 /s VV Thermal load (heat flux/Temp.) Particle Load Inner surfacecoolantT Pressure DEMO0/3333331 Pa BLK Thermal load (heat flux/Temp.) Particle Load Cooling tubecoolantT Pressure DEMO633~653 1Pa (H 2, T=1%) DIVFWVVBLK cooling tube* Area/material200 m 2 W/F82H700 m 2 W/F82H~800 m 2 F82H8000 m 2 glass/F82H Surface area and base materials of in-vessel components in DEMO * Y.Kosaku et al., Fusion Sci. Technol.,41 958 (2002)

11 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 10 T Transport properties of in- vessel components materials TungstenF82H Effective Diffusion coefficient (m 2 /s) 6.74×10 -8 exp(-0.73eV/kT) *1 10times larger in plasma facing region *2 1.07×10 -7 exp(-0.15eV/kT) /(1+2.9x10 -8 exp(0.58eV/kT) *5 10times larger in plasma facing region *2 Solubility (atoms/m 3 /√Pa) 1.83×10 24 exp(-1.04eV/kT) *3 6.21×10 23 exp(-0.28eV/kT) *5 Recombination coefficient (m 4 /s) 7.1×10 -18 exp(-0.81eV/kT) *4 9.4×10 -26 exp(-0.12eV/kT) *6 *1 H. Nakamura et al., JNM 297(2001)285, *2 H. Nakamura et al., JNM 313-316 (2003) 675 *3 R. Frauenfelder, J. Vac. Sci. Technol. 6 388 (1969), *4 R. A. Anderl et al., Fusion Technol. 21 745 (1992)., *5 E. Serra et al., JNM 245 (1997) 108, *6 M. Enoeda et al., JAERI-tech 2001-078, * Irradiation effect was not considered in this evaluation

12 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 11 Analytical result (1) Transient T inventory in DEMO operation - Tritium inventory in the components and permeation into the coolant will reach at saturation level and steady state within one year operation of DEMO, respectively, while permeation in ITER will not reach steady state even after 3 years operation* - Tritium inventory and permeation in DEMO is quite faster to reach steady state than the ITER case due to steady state operation, higher operation temp. and ferritic steel (F82H) structure. Time evolution of tritium inventory in the components and coolant during DEMO operation (except BLK). DIV:1  m W coating on the cooling tube FW: 1mm W coating *H. Nakamura et al., JAERI-Research 2003-024 (2003). and JNM 329-333 (2004) 183 ON OFF

13 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 12 Analytical result (2) T inventory in in-vessel components DIVFWBLKVV ~1.5gT~0.3gT~1.2 gT* (Li 2 O case) ~mgT Tritium inventory in the components at saturation level (Those results didn’t include neutron irradiation effect) - Tritium in the components mainly exists in the DIV (armor region) and BLK. - Total T inventory in the in- vessel components is ~gT. It is negligible smaller than ITER case(1.2kgT) due to carbon free PFC in DEMO. * M. Enoeda et al., Nuclear Fusion, 43 1837 (2003) Breakdown of T inventory in materials for DIV and FW Tritium inventory in the components will not be a critical issue in DEMO

14 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 13 Analytical result (3) T inventory in coolant(1) - T inventory in coolant strongly depends on the permeation reduction effect of coatings on components surface. -Current design of DEMO FW: W coating (~mm) is necessary for the reduction of erosion of ferritic steel BLK: 100 or more PRF is expected by the glassy coating on the cooling tubes** - In current design of DEMO, T in the coolant is mainly attributed to permeation from BLK region. Annual T inventory increase in the coolant from PFC (DIV and FW) and BLK for various permeation reduction barrier PRF:Permeation Reduction Factor W armor: W armor thickness on FW * Y.Kosaku et al., Fusion Sci. Technol.,41 958 (2002) ** M. Enoeda et al., JAERI-tech 2001-078 (By Nakamichi) *

15 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 14 Analytical result (3) T inventory in coolant(2) - Without permeation barrier, annual T inventory increase in the coolant will be tens kgT/y. -Water detritiation system (WDS) can not recover such amount of tritium from cooling water even in the R&D target for DEMO. -It means tritium will run out within one month operation of DEMO. -It is not acceptable !! -At least PRF=100 is required to maintain the T concentration in the coolant below 10 Ci/L/year (within R&D target of WDS capacity) Tritium permeation reduction is a critical issue in a viewpoint of the tritium inventory control at DEMO * Annual T inventory increase in the coolant from PFC (DIV and FW) and BLK for various permeation reduction barrier

16 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 15 Analytical result (4) T Inventory in ITER and DEMO ITERDEMO T in PFC ~1.2 kgT Mainly in Co-deposition ~1.5 gT Mainly in W armor of DIV T in coolant <2 gT (20 years) mainly from Be FW ~tens kgT/y (worst case) <200 gT/y (target value) T in BLK TBD (Maybe negligible) ~1.2 gT Mainly in the breeder In ITER, - Only the co-deposition issue is a critical issue In DEMO -Tritium inventory in the component (PFC and BLK) will be negligible, since there are no carbon materials. - Tritium inventory in the coolant will be a critical issue without permeation reduction method.

17 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 16 Uncertainties and Further analysis We could identify the critical issue on T inventory in DEMO. There are still uncertainties, however. Uncertainties - T transport properties in the permeation reduction coating materials (Key issue for PRF in BLK region) - Neutron irradiation effect on T transport properties in the DEMO components materials (Durability of coating and inventory enhancement) -T transport mechanism at the interface between cooling tube and coolant Further analysis - Further evaluation in BLK region -Evaluation of tritium migration into the secondary coolant -Modification of evaluation with resolved uncertainties

18 H. Nakamura, Japan-US WS on Fusion Power Plant in participant of EU, 2005,Jan.11-13 17 Summary - In-vessel tritium inventory in the JAERI-DEMO has been evaluated under the current design and operational conditions - Based on the obtained results, the feature of tritium inventory in DEMO has been characterized by comparing with that in ITER -Analytical results indicated that tritium inventory in in-vessel components will be negligible in DEMO. However, the tritium inventory in the coolant in DEMO is much greater than that in ITER. - Establishment of tritium permeation reduction technique into the coolant is a critical issue in a viewpoint of tritium inventory control.

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