Design Integration of the LHD-type Energy Reactor FFHR2 towards Demo

Transcription

1 Design Integration of the LHD-type Energy Reactor FFHR2 towards Demo A. Sagara 1, S. Imagawa 1, Y. Kozaki 1, O. Mitarai 2, T. Tanaka 1, T. Watanabe 1, N. Yanagi 1, T. Goto 1, H. Tamura 1, K. Takahata 1, S. Masuzaki 1, M. Shoji 1, M. Kobayashi 1, K. Nishimura 1, T. Muroga 1, T. Nagasaka 1, M. Kondo 1, A.Nishimura 1, H. Igami 1, H. Chikaraishi 1, S. Yamada 1, T. Mito 1, N. Nakajima 1, S. Fukada 3, H. Hashizume 4, Y. Wu 5, Y. Igitkhanov 6, O. Motojima 1 and FFHR design group 1 National Institute for Fusion Science, Toki, Gifu, Japan 2 Tokai University, Kumamoto, Japan 3 Kyushu University, Fukuoka, Japan 4 Tohoku University, Sendai, Japan 5 Institute of Plasma Physics, Chinese Academy of Sciences, Hefei, China. 6 Max-Planck Planck-Institut für Plasmaphysik,, IPP-EURATOM Ass., Greifswald, Germany Invited in 18 th ITC 2008 Dec.9-12, 2008 at Toki, Japan. FFHR2m2 3GWth 5 Tesla 30,000 ton ton 1/ 25

2 FFHR design collaborations Confinement scaling H.Yamada, Miyazawa Helical core plasma K.Yamazaki Magnetic structure T.Morisaki, Yanagi SC magnet & supprt S.Imagawa T.Mito Takahata, Yamada, Tamura, Virtual Reality tool N.Mizuguchi Power supply H.Chikaraishi External heating O.Kaneko, Igami LHD Ignition access & heat flux O.Mitarai (Kyusyu Tokai Univ.) SC magnet & support Heating FFHR design / Sytem Integration / Replacement A.Sagara Protection wall Ph =0.2 M W / m 2 Pn =1.5 M W / m 2 Nd =4 50 dp a/3 0y 14MeV neutron Core surface heat flux Plasma In-vessel Component s Divertor pumping Fueling Sakamoto Divertor pumping S.Masuzaki, Kobayashi Fusion Research Network Fusion Eng.R.C. Fueling Thermofluid Structural Materials Purifier Pump Thermofluid MHD S.Satake (Tokyo Univ. Sci.) Advanced first wall T.N orimatsu (Osaka Univ.) Blanket material system T.Muroga, T.Nagasaka, M.Kondo Self-cooled T b ree der TB R lo cal > 1. 2 Be Tank Liquid / Gas HX Radi ati on s h ield r educ tio n > 5 or der s Thermal shield high temp. T-dise nga ge r Chemistry Blanket shie ld ing materials. Vacuu m vessel & T boundary SC magnet 20 C Pum p T s torage Turbine Safety & Cost Tritium Thermofluid system K.Yuki, H.Hashizume (Tohoku Univ.) Advanced thermofluid T.Kunugi (Kyoto Univ.) Neutronics T.Tanaka, A.Sagara Mag. material system A.Nishimura, Y.Hishinuma Blanket system T.Terai (Univ. of Tokyo) Safety T.U da Cost evaluation Y. Kozaki T-disengager system S.Fukada, M.Nishikawa (Kyusyu Univ.) Heat exchanger & gas turbine system A.Shimizu (Kyusyu Univ.) April 10, 2008, A.Sagara Int. Collaboration TITAN : USA (ORNL, INL, UCLA, UCSD) CUP : China (SWIP, ASIPP) Int. Network Program : EU (IPP), Russia, Ukraine, Korea (KAERI) 2/ 25

3 3/ 25 Role of Design Study to Helical Demo-Reactor based on LHD Project FFHR design with R&D s

4 Two main features in FFHR (1) Quasi-force free γ optimization on continuous helical winding to reduce the magnetic hoop force (Force Free Helical Reactor: FFHR) large maintenance ports to expand the blanket space γ = m l a c R J x B surf = 0, when ϑ = 45 deg. 2 1 LHD R ax =3.6m, B q =100%, Φ = 0 γ=1.33 γ=1.18 γ=tanθ Z (m) R (m) (2) Self-cooled liquid Flibe (BeF 2 -LiF) blanket low MHD pressure loss low reactivity with air low pressure operation low tritium solubility 4/

5 5/ Presentation outline 1. Blanket and divertor space Design windows and cost Nuclear shield on SC coils Reactor size optimization New ignition regime Design parameters 2. SC magnet and supports 3. Blanket system integration 4. Concluding remarks Magnetic field B 0 (T) ITER Ap~ FFHR2 Ap ~ 8 γ =1.15 ARIES-CS Ap~ FFHR2m1 Ap ~ 8 γ =1.15 outer shift 1995 FFHR1(l=3) Ap ~ 10 γ =1 optimum? FFHR2m2 LHD Ap ~ 6 Ap ~ 6 γ =1.25? inner shift Coil major radius R c (m)

6 6/ (a) Issues on blanket and divertor space (b) To To remove the the interference between the the first first walls walls and and the the ergodic layers layers surrounding the the last last closed closed flux flux surface, helical helical x-point x divertor (HXD) (HXD) has has been been proposed. Helical X-point Divertor (HXD) T. Morisaki et al., FED 81 (2006) However For For α-heating efficiency over over 90%, 90%, the the importance of of the the ergodic layers layers has has been been found found by by collisionless orbits orbits simulation of of 3.52MeV alpha alpha particles. By T. Watanabe

7 By T. Watanabe 7/ 25 21

8 Fast neutron flux (>0.1MeV) (n/cm 2 /s) 1. Reduction of the inboard shielding thickness using WC JLF JLF-1 (70vol.%) +B 4 C (30vol.%) B 4 C WC Plasma Breeding layer [Flibe+Be] (32cm) Radiation shield (60 cm) Three candidates are proposed to increase blanket space > 1.1 m (Magnet) Radial position(cm) 25cm thinner 2. Improvement of the symmetry of magnetic surfaces by increasing the current density at the inboard side of the helical coils by splitting the helical coils. N. Yanagi et al., in this conference. FFHR-2S Type-I ICRF antenna R c = 15.0 m, a c = 3.0 m, γ = 1.0 B axis = 6 T, a p = 1.5 m, W = GJ Smaller size and higher field with γ = 1 (reduction of total mass) K. Saito et al., in this conference. 8/ 25

9 P f (GW), TCC (G$), B o (T) J = 25 ~ 33 A/mm 2 Γ n = 1.3 ~ 1.5 MW/m 2 B 0 TCC (total capital cost) P f (fusion output) FFHR Coil major radius R c (m) Three candidates are proposed to increase blanket space > 1.1 m Enlargement of of reactor size Neutron wall loading should be kept at < 2 MW/m 2 blanket space > 1 m W g (magnetic energy) COE FFHR2m1 FFHR2m Wg (GJ), COE (mil/kwh) A. Sagara et al., in ISFNT-8, FED 83 (2008) R p =16m (R c =17.3m) is selected. (simple expansion of LHD gives too large R c.) Thermal insulation for SC magnet (Includes SOL and V/V) 9/ 25

10 10 / 25 Presentation outline 1. Blanket and divertor space Design windows and cost Nuclear shield on SC coils Reactor size optimization New ignition regime Design parameters 2. SC magnet and supports 3. Blanket system integration 4. Concluding remarks

11 Design windows and cost W GJ (β 4%, Pf 3GW) Y. Kozaki et al., in this conference. β=5%, γ = 1.20, j=26a/mm 2 are selected W GJ (β 5%, Pf 4GW) 100 Pf3GW 3GW 90 COE (mill/kwh) COE GW 80 4G W 4.75GW HF<= Rp m Rp m Rp m The design windows limited with Δd 1.1m, H f 1.16, W<160GJ, depending on γ and β. H f =1.16 means the 1.2 times value achieved in LHD experiment. j=26a/mm 2 is premised. The COEs of helical reactors, which depend on Rp, γ and β, show the bottom as the result of the trade-off between the Cmag and Cbs, i.e., B0 versus plasma volume. 11 / 25

12 12 / 25 Issues on nuclear shield on SC coils Discrete Pumping with Semi-closed Shield (DPSS) has been proposed A. Sagara et al., in ISFNT-8, FED 83 (2008) Acceptable level achieved Cover rate > 90% Fast neutron < 1E22 n/m 2 in 30 years Max. nuclear heating < 0.2 mw/cm 3 Total nuclear heating ~ 40 kw Cryogenics power ~ 12 MW (1% of P f ) 3D design with DPSS

13 a PC = 8.2 m, HC : MA, OV : MA, IV : MA 13 / 25 Reactor size optimization of FFHR2m2 Vacuum Magnetic Surface R p R b R c inner shifted (equivalent to Rax=3.6m in LHD), γ = 1.20, α = +0.1 R p =16m, R c =17.3m, B 0 =4.84T, j=26a/mm 2, W mag =167.7GJ expanded PC position Type A

14 Reactor size optimization of FFHR2m2 Vacuum Magnetic Surface R p R b R c inner shifted (equivalent to Rax=3.6m in LHD), γ = 1.20, α = +0.1 R p =16m, R c =17.3m, B 0 =4.84T, j=26a/mm 2, W mag =149.1GJ moved PC position Type B HC : MA, OV : MA, IV : MA 14 / 25

15 Reactor size optimization of FFHR2m2 Vacuum Magnetic Surface inner shifted (equivalent to Rax=3.6m in LHD), γ = 1.20, α = +0.1 R p =15.5m, R c =16.7m, B 0 =4.90T, j=25a/mm 2, W mag =135.6GJ WC shield at inboard PC position Type B B HC : MA, OV : MA, IV : MA 15 / 25

16 16 / 25 Presentation outline 1. Blanket and divertor space Design windows and cost Nuclear shield on SC coils Reactor size optimization New ignition regime Design parameters 2. SC magnet and supports 3. Blanket system integration 4. Concluding remarks

17 17 / 25 New control method in a thermally unstable ignition regime O. Mitarai et al., in this conference. Proportional-Integration Integration-Derivative (PID) control The error of the fusion power with an opposite sign of e(p f )= - (P fo -P f ) can stabilize the thermal instability through fueling. S DT (t)=0 if S DT (t)<0 O. Mitarai al. Plasma and Fusion Research, Rapid Communications, 2, 021 (2007). τ α */τ E =3 ~ 5 τ p */τ E =2 ~ 8 But, effectively reduced due to burning

18 Design parameters Design parameters LHD FFHR2 FFHR2m1FFHR2m2 SDC Polarity l Field periods m Coil pitch parameter γ Coil major Radius R c m Coil minor radius a c m Plasma major radius R p m Plasma radius <a p > m Plasma volume Vp m Blanket space Δ m Magnetic field B 0 T Max. field on coils B max T Coil current density j MA/m Magnetic energy GJ Fusion power P F GW Neutron wall load Γ n MW/m External heating powep ext MW α heating efficiency η α Density lim.improvement H factor of ISS Effective ion charge Z eff Electron density n e (0) 10^19 m Temperature T i (0) kev Plasma beta <β> % Plasma conduction lo P L MW Diverter heat load Γ div MW/m Total capital cost G$(2003) COE mill/kwh Stored Energy, W/WHC only a PC to 0.95R c Z OV =Z IV Z OV /R c =3.8/14 Z OV /R c =4.5/14 Z OV /R c =5/14 a PC to R c 0.7 γ=1.20, R p /R c =3.6/3.9 a IV =a OV, R IV <R c -a c B leak (2.5 R c ) < 0.5 mt (a PC -a c )/R c Type A LHD Type B Z IV (R IV ) increase. In SDC, divertor heat load is drastically reduced (~1/4). 18 / 25

19 19 / Presentation outline 1. Blanket and divertor space Design windows and cost Nuclear shield on SC coils Reactor size optimization New ignition regime Design parameters 2. SC magnet and supports 3. Blanket system integration 4. Concluding remarks

20 S. Imagawa et al., in this conference.cc Base design of CICC magnet system Nuclear heating (mw/cm 3 ) Nuclear heating in FFHR2m Neutron+Gamma Gamma 5 times Radial position (cm) By T. Tanaka Max. cooling path is 500 m for the nuclear heat of 1 mw/cm 3. This value is 5 times larger on the FFHR magnets. Gamma-ray heating is dominant. 20 / 25

21 Indirect-cooled cooled helical coil system (alternative for CICC) with quench protection by by internal dumping SS316 SS316 Stress analysis inside of the coil H. Tamura et al., in this conference.cc Indirect Cooling Circumferential strain distribution Cross-sectional structure of the helical coil Quench protection by internal dumping K. Takahata et al., ITC-17. Quench back with a secondary circuit to increase a decay time constant > t=20 s to reduce a transient voltage V max =10 kv to avoid a serious hot spot < 150 K Hoop stress distribution Confirmed to be within the permissible range. 21 / 25

22 22 / 25 LHD-type support post for FFHR By H. Tamura Gravity per support = 16,000 ton / 30 legs ~ 530 ton. Thermal contraction < max. 55 mm Total heat load to 4K ~ 0.34 kw ( 1/20 of stainless steel post) (Carbon Fiber Reinforcement Plastic)

23 Wide maintenance ports 23 / 25

24 Confinement scaling H.Yamada, Miyazawa Helical core plasma K.Yamazaki Magnetic structure T.Morisaki, Yanagi SC magnet & supprt S.Imagawa T.Mito Takahata, Yamada, Tamura, Virtual Reality tool N.Mizuguchi Power supply H.Chikaraishi External heating O.Kaneko, Igami Blanket system integration by broad R&D collaboration activities LHD Ignition access & heat flux O.Mitarai (Kyusyu Tokai Univ.) SC magnet & support Heating Fueling Sakamoto Divertor pumping S.Masuzaki, Kobayashi MHD on Flibe FFHR design / Sytem Integration / Replacement A.Sag ara Protection wall 2 Ph =0.2 M W / m Pn =1.5 M W / m 2 Nd =4 50 dp a/3 0y 14MeV neutron Core surface heat flux Plasma In-vessel Component s Divertor pumping Fusion Research Network Fusion Eng.R.C. Fueling Thermofluid Structural Materials Purifier Pump Thermofluid MHD S.Satake (Tokyo Univ. Sci.) Advanced first wall T.N orimatsu (Osaka Univ.) Blanket material system T.Muroga, T.N agasaka, M.Kondo S elf - cool ed T bree der TB R lo cal > 1. 2 Be Tan k Liquid / Gas HX Radi ati on sh ield reduc tio n > 5 orders Thermal shield high temp. T-d ise nga ge r Chemistry Blanket shie ld ing materials. Vacuu m vessel & T b oun dar y SC magnet 20 C Pum p T s torag e Turbine Safety & Cost Tritium Thermofluid system K.Yuki, H.Hashizume (Tohoku Univ.) Advanced thermofluid T.Kunugi (Kyoto Univ.) TNT Loop : 600 C Neutronics T.Tanaka, A.Sagara Mag. material system A.Nishimura, Y. Hishinuma Blanket system T.Terai (Univ. of Tokyo) Safety T.Uda Cost evaluation Y. Kozaki T-disengager system S.Fukada, M.Nishikawa (Kyusyu Univ.) Heat exchanger & gas turbine system A.Shimizu (Kyusyu Univ.) Closed He gas turbine April 10, 2008, A.Sagara cycle with three-stage compression/expansion T or h T en Tn Tl 550 C 450 C 30 C Permeation window system Tritium molar fraction in Flibe [-] Tritium leak ferrite-steel permeation window T=843K, Q T =190g -T /day, W Flibe =2.3m 3 /s Fluid film diffusion controlling Fluid-film diffusion + permeation Permeation controlling Large apparatus Permeation window Permeation area [m 2 area [m] 2 ]( α=1, t=1mm) Tritium partial pressure [Pa] 24 / 25

25 25 / 25 Concluding remarks 1. Helical reactor is superior in steady state operation and Reduced neutron wall loading < 2MW/m 2 with long-life blanket concept, High density operation with reduced heat load on divertor. 2. On the 3D design, a simply defined blanket shape can be compatible with the ergodized magnetic layer which is essential on both of divertor and α-heating. 3. This simple methodology on LHD-type reactors can be used for design optimization towards DEMO, which is economically comparable to Tokamak. 4. The design parameters of FFHR2m2 have been totally improved, where a new ignition regime at SDC is an innovative alternative. 5. The large scale SC magnet system and their support posts are conceptually feasible. 6. Large R&D progress has been made on blanket and magnet materials. 7. The next key work is to realize the DPSS divertor concept compatible with replacement scenario and neutronics issues on TBR and nuclear shielding for SC magnets.