Current Status of CADS:

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1 Current Status of CADS: New kind of the coolant for subcritical core and the target research Zhan, WenLong Xu, HuShan Yang, Lei Institute of modern physics, Chinese academy of sciences CW-316LSS

2 RFQ: pulsed beam Venus 2 R&D projects of CIAE,CAS

3 MW

4 Power Source coupler ECR Beam monitor RFQ Prototype of proton accelerator test (ECR+LEBT+RFQ) for CADS

S-HWR Electromagnetic field contours Superconducting

15 Epk/Eacc 5.96 4.8 Bpk/Eacc 12.18 6.1 G=Rs Q0(Ω) 32.

5 S-HWR Electromagnetic field contours Superconducting cavity parameters f(mhz) β Epk/Eacc Bpk/Eacc G=Rs Q0(Ω) R/Q Q0(4.4K, 4.52E8 7.25E8 Rs=71.4nΩ) Uacc(MV) Epeak(MV/m) Bpeak(mT) Pdiss(W) (4.4K, Rs=71.4nΩ) T-HWR Electromagnetic field contours Freq./MHz Uacc. Max /MV Emax /MV/m Bmax /mt R/Q / Vertical measurement results

0kW 1kW 6kW 10kW 20kW details The outer conductor was designed to be

while the inner conductor was cooled by water.

mode limited by the RF source available.

3kW 6 hrs 2013-6-4 9:55 23:47 ~2.90kW 12.

6 0kW 1kW 6kW 10kW 20kW details The outer conductor was designed to be cooled by helium gas through the spiral grooves around the outer surface while the inner conductor was cooled by water. The coupler has passed a RF power of 20kW in continuous travelling wave mode limited by the RF source available. Spiral grooves Date Start time Stop time Pf1 max Elapsed time/hrs :50 20:00 ~212W 5.3 hrs :25 16:30 ~738W 7 hrs :10 17:17 ~Peak 1.3kW 6 hrs :55 23:47 ~2.90kW 12.3hrs :10 22:32 ~5kW 12 hrs :13 21:56 ~9.42kW 8 hrs window-up windowdown :07 20:50 ~10.6kW 10hrs :13 18:00 ~20.0kW 8.6 hrs Total conditioning time : 63~69 hrs

7 Ready for VT.

8 Design parameters frequency(mhz) intensity(ma) 10 Input energy(mev) 3 Output energy(mev) 6 S-HWR number 6 HWR Heat Leakage(W) 10 Coupler cooled load(g/s) 0.024

9 :ECRIS+LEBT+RFQ+MEBT+CM6

Tasks of IMPCAS Injector II ECR LEBT RFQ 162.5MHz MEBT1 SC-HWR SC-CH 162.

1 MeV MEBT2 10MeV Spoke021 325MHz 28 cavities Spoke040 325MHz 72 cavities Elliptical 063

2 MeV 34 MeV 178 MeV 367 MeV 1500 MeV ECR LEBT RFQ 325.

10 Tasks of IMPCAS Injector II ECR LEBT RFQ 162.5MHz MEBT1 SC-HWR SC-CH 162.5MHz Tasks of IHEP 35 kev 2.1 MeV MEBT2 10MeV Spoke MHz 28 cavities Spoke MHz 72 cavities Elliptical MHz 28 cavities Elliptical MHz 85 cavities HEBT Target 35 kev 3.2 MeV 34 MeV 178 MeV 367 MeV 1500 MeV ECR LEBT RFQ 325.0MHz MEBT1 Spoke 325MHz Main Linac Injector I IHEP and IMPCAS co-work on the accelerator. Final project has two identical injectors. Two designs of injector is due to technical uncertainty at very low energy segment.

11 heat exchanger core arrangement reactor roof pressure vessel refueling system reactor components parameters core barrel diameter m 4.38 height m 6.4 reactor vessel diameter m 4.72 height m 7.22 reactor roof outer diameter m 4.4 Inter diameter m 2.88

CFD simulation results coolant channel the passive

of a natural circulation loop parameters Power(MW)

9 Coolant inlet/outlet temperature ( ) 260/390

12 CFD simulation results coolant channel the passive residual heat removal (PRHR) system CFD Simulation of a natural circulation loop parameters Power(MW) 10 Average linear power density (kw/m) 3.9 Coolant inlet/outlet temperature ( ) 260/390 Height of cycle(m) 2 Average velocity of coolant(m/s) 0.17 Flow rate(kg/s) fuel rod clad tube temperature( ) 462 Fuel rod temperature ( ) 660 core flow distribution

13 refueling system 3D model engineering structure analysis shielding design

14 Stress Distribution temperature Distribution velocity Distribution Temperature Near the Window Velocity Near the Window Grid:>6*10^7 Physical Design Parameters Neutron Yield Diameter of Beam Beam Energy Beam Current LBE average velocity LBE max velocity Window Thickness Temp. Difference of Heat Exchanger Max velocity of cold fluid Wall Thickness of Heat Exchanger Flux of Gas inject Width of Lacuna 3.2 n/p 8cm 250MeV 2mA 0.21~0.49m/s 1.29m/s 2mm 90K 1.52m/s 1.75cm 5L/s 7cm

16 MAX Temperature: 800 o C MAX Velocity: 10m/s

18 Coolant: Liquid Heavy Metal and Gas

19 Density (kg m -3 ) Volume Specific heat (J ml 1 K 1 ) Thermal conductivity (W m 1 K 1 ) Lead / LBE He / / (4MPa) 35.3 / Corrosion Large / Large Small Erosion Large / Large Middle (high velocity) Radioactivity & toxicity Large / Huge Small

20 Lead/LBE Cooling Fast Reactor IAEA Nuclear Power (NENP) Technical Meeting, Gas Cooling Fast Reactor

Q: How to avoid the weak points of Gas Cooling

can increase the specific heat; High pressure

21 Q: How to avoid the weak points of Gas Cooling Fast Reactor and keep the strong points. A: Granular + Helium (Low pressure) for the coolant? can increase the specific heat; High pressure From the fluidized bed to the dense granular flow The kinds of the solid grains can be considered

22 Coolant Water ~4 Na ~1 LBE ~1.6 Molten Salt ~4 Helium SiC Granular ~1.4 Volume specific heat (J/ml K) ~0.03(4Mpa) Coolant SiC granular LiZrO 3 granular Steel granular Helium 0.15 Ƙ (W/m K) d (mm) ~120 ~0.16 ~ Ƙ eff (20 ) (W/m K) Solid Ƙ(W/m K) Gas d(mm) Time(s) h(w/m 2 K) SiO2 1.7 Air 1 10 ~100-~200 Ceramic 0.5 H2(1000,1 0bar) Al 217 He short 1500 Glass 0.93 Air 1 60& 1 60 & 290 Helium ~100 Convective heat transfer coefficient

23 Low pressure inter-fluid (He) High thermal inertia The grains can be optimized for Fast spectrum Low radio-toxicity Small erosion and chemical toxicity For example: SiC grains and SiC Hexagonal prism

24 Pressure vessel MOX UO 2 /ThO 2 Fuel rod Graphite reflector 1 m 2.4m B 4 C neutron Shield reactor core Diameter of SiC granular: ~0.5 mm Helium pressure: 0.1 MPa Fuel assembly 19.6 cm Coolant channel 1.5cm

25 Density of Power in vertical distribution Density of Power distribution The neutron spectrum Burning calculation

26 0.6 m/s Dense granular flow by gravity driven Heat transfer by granular flow

27 High of the fuel rod:100 cm High of the :70 cm Thermal Power:100 MW Fuel:(Pu x Am 1-x )O 1.88 Theoretical density of fuel: g/cm 3 Density of power:34w/cm 3 K eff =0.95(BOL) Proton beam: 1GeV@4.3mA(BOL) Diameter of SiC granular: ~0.5 mm Helium pressure: 0.1 MPa

>X00 μ A/cm^2 Liquid target Porosint target: Packed beds (rod, ball, etc), increasing

28 Average Beam intensity: <10 μ A/cm^2 Average Beam intensity : <20 μ A/cm^2 Solid target: rotating target can enlarge relatively the beam spot Average Beam intensity :?>X00 μ A/cm^2 Liquid target Porosint target: Packed beds (rod, ball, etc), increasing coolant contact surface.? : tens of MW target for ATW Average Beam intensity : <30 μ A/cm^2 rotating moving target

Gas Dust Filter 6. Gas Heat Exchanger 7.

29 Granular flow by gravity Proton Beam 1. Target Body 2.Heat Exchanger 3. Solid horizontal Transport & Dreg Filter 4. Gas- Solid Separator 5. Gas Dust Filter 6. Gas Heat Exchanger 7.Gas Blower 8.Gas Pipes 9.Gas-Solid Mixer 10. Solid Lifter

30 Mass parallel Simulation: Contact mechanism + MD + MC transport K20GPU 2500ALU Number of particles: 0.5 M

Temperature distribution (10MW=1GeV@10mA) Fraction of volume distribution Maximum erosion

31 Temperature distribution Fraction of volume distribution Maximum erosion estimation distribution Temperature distribution neutronics Fraction of volume vs. time

Countercurrent water corrugated plate heat

particles since the force of gravity under the

upward flow of the cooling water absorbs the

Heat exchanger principle and main structure

32 Countercurrent water corrugated plate heat exchanger to be cooled beryllium alloy particles since the force of gravity under the direction of flow, and the corrugated plate upward flow of the cooling water absorbs the heat carrying particles derived. Heat exchanger principle and main structure parameters Heat exchanger 2.5 kw Flow rate 200 kg/s Granular outlet temperature ~200 Granular <1000 The cooling water inlet temperature 20 Cooling water outlet temperature 80

chain, thus allowing delivery of high temperature materials (material temperature

33 NE series hoist suitable for conveying the powder, granular and small block of non-abrasive and abrasive materials small, because the traction hoist is a ring chain, thus allowing delivery of high temperature materials (material temperature does not exceed 250 ). General transport height up to 40 meters, TG type up to 80 meters

中子总产额 (n/p) 中子总产额 ( n / p ) 23.9550 23.9500 23.9450 23.9400 23.9350 23.9300 23.9250 23.9200 23.

08E-5-4.62E-6-9.24E-6 +1.29E-4 SiC RT 300 500 800 1000 min 30 20 20 20 20 Specific wear rate mm 3 /Nm -3.56E-7-2.

34 中子总产额 (n/p) 中子总产额 ( n / p ) Re 所占百分比 (%) RT W min Specific wear ratemm 3 /Nm -4.92E E E E E-4 SiC RT min Specific wear rate mm 3 /Nm -3.56E E E E-7 In the RT-1000 temperature range, W granular, polycrystalline sintered SiC is excellent in wear resistance, wear amount of <1mm.

Solid target: Thermal stress Radiation damage Shock waves Cooling Lubrication Liquid target: Corrosion Cavitation Shock waves splashing Radiochemistry parameters Granular material Structure material

35 Solid target: Thermal stress Radiation damage Shock waves Cooling Lubrication Liquid target: Corrosion Cavitation Shock waves splashing Radiochemistry parameters Granular material Structure material Granular size Inlet temperature of granular Outlet temperature of granular Proton beam Intensity of beam Diameter of beam spot Average velocity of granular flow Tungsten/Tungsten alloy TZM/SiC 10±5mm 250 C 550 C 1GeV@10mA=10MW >100 μ A/cm^2 10cm ~0.9m/s Dense granular flow target have chance to increase power and using for ATW

(GPU) Radiation transport computation in

36 (GPU) Radiation transport computation in stochastic granular and neutronic analysis, etc. Granular flow and fluid flow simulations and thermal-hydraulic analysis. 2010/11: rank 1 in TOP500; Now rank 8. Grains:~250 M;MD + Contact mechanic. 512GPU, 512*448= ALU; parallel efficiency: ~38%.

37 Thank you!

KIPT ACCELERATOR DRIVEN SYSTEM DESIGN AND PERFORMANCE

KIPT ACCELERATOR DRIVEN SYSTEM DESIGN AND PERFORMANCE Yousry Gohar 1, Igor Bolshinsky 2, Ivan Karnaukhov 3 1 Argonne National Laboratory, USA 2 Idaho National Laboratory, USA 3 Kharkov Institute of Physics