Experiment and Simulation of plasma window

Transcription

1 Experiment and Simulation of plasma window Kun Zhu,Sheng Huang, Wang shaoze, Yuarong, Zhiyu Guo Physics school of Peking university Institute of Heavy Ion Physics UCANS2015

2 outline Ø Introduction Ø Plasma window test bench Ø Simulation of plasma window Ø conclusion

3 cathode what is plasma window Arc channel anode High pressure Plasm a Vacuum

4 Traditional solid window beam Solid window vacuum High pressure region Beryllium window Disadvantage: Thermal damage Radiation damage Increase energy loss and energy spread

5 Windowless target Windowless deuterium gas target Expensive differential pump system Complicated vacuum and mechanical system windowless hydrogen gas target for 7 Be(p,γ) reaction measurement

6 Why plasma window Ø needn t worry about thermal problem. Ø No radiation damage Ø Very thin equivalent thickness(~nm) Ø Effectively improve the performance of differential pump system

7 Non-vacuum electron beam welding Plasma window 9mA 25mA Electron beam current after exiting plasma window, Pure helium gas Aperture: 2.36mm Current: 45A Air boring and non-vacuum electron beam welding with a plasma window, Ady hershcovitch, Physics of plasma, 12(2005)

8 Deuterium gas target using plasma window Plasma window Deflector plate Differentially pumped gas chamber Beam Roots blower Turbo molecular pump 50kW power supply operating gas pressure is 0.5 bar for argon Diameter of plasma window: 5mm Performance of a plasma window for a high pressured differentially Pumped deuterium gas target for mono-energetic fast neutron Production-Preliminary results, A.De Beer, A. hershcovitch, et. al..nimb, 170(2000),

9 High ion current beam need larger plasma window Small diameter Plasma window(2-5mm) is successfully used for electron beam welding and gas target. If larger diameter plasma window is possible, It has some potential use for high current ion beam.

10 Plasma window test bench Vacuum gauge Plasma window Two stage pump Arc power supply

11 Plasma window Pressure measurement Spectrum diagnostic Water cooling Water outlet Copper plate Insulating pipe anode Three aperture: 3mm,6mm,10mm Cathode tip cathode

12 Plasma window sealing effect Inlet pressure(kpa) Outlet pressurek(pa) Gas flow(slm) discharge No discharge Operating current is 40A operating voltage is 58V this prove the plasma window s sealing effect!

13 Aperture:3mm Aperture:3mm Aperture:6mm Outlet pressure 60Pa Gas flow:1.6slm Length: 61mm

14 Measurement with spectrometer Schematic diagram of spectroscopy set up

15 Temperature of plasma

16 Experiment show that the plasma window can work. But the sealing ability decreased quickly when plasma window s aperture increase. It may consume much more energy

17 Simulation of plasma window Ø Use magneto-hydrodynamic model Ø Ansys fluent Ø Basic assumptions plasma is steady, continuous, axisymmetric and optically thin Plasma is in LTE state Swirling velocity is neglected

18 Configuration Input Material Geometry, Grid generation Boundary conditions Discretization Hydrodynami c governing equations Equation solver Radiation coefficients Gas transport coefficients Output

19 Govering equation Mass conservation equation Momentum conservation equation ( ρν z)+ (r ρν r)=0 z r r 1 P νz 1 νr νz ( ρν zν z)+ (r ρν zν r)=- +2 ( µ )+ [r µ ( + )]+jrb z r r z z z r r z r 1 P 2 νr νz νr νr ( ρν zν r)+ (r ρν rν r)=- + (r µ )+ [ µ ( + )]-2µ -j 2 zb z r r r r z r r r z r θ θ Energy conservation equation T 1 T jr + jz 5 T T ( ρν zct)+ p (r ρν rct)= p ( k )+ (r k )+ - qr+ kb(j z + j r )+B θ (jrvz- jv z r) z r r z z r r r σ 2e z r / z (σ φ/ z )+ /r r (rσ φ/ r )=0 Az 1 Az -( )+ )= µ 0 j z z r r r Ar 1 Ar -( )+ )= µ 0 j z z r r r z r

20 Boundary condition P u v T φ uv A AB: Inlet P = 52.5KPa / T = 300 φ / n = 0 A = 0 HI: Outlet P = 60 / T / n = 0 φ / n = 0 Ai / n= 0 AI: Axis P/ n = 0 u / n= 0 T / n = 0 φ / n = 0 A / n= 0 i CD: Cathode P/ n = 0 0 k T / n= h ( T 400) φ = 140 A / n= 0 EF: Anode P/ n = 0 0 k T / n= h ( T 400) φ = 0 A / n= 0 DE&FG: Wall P/ n = 0 0 T = 400 φ / n = 0 A / n= 0 BC&GH: Wall P/ n = 0 0 T = 300 φ / n = 0 A / n= 0 w w i i i i i i

21 Simulation domain r axis

22 Current Distribution Sheng huang, Kun Zhu, et al, Numerical Simulation Study on Fluid Dynamics of Plasma Window Using Argon, Physics of plasmas, 2013

23 Temperature Distribution

24 Pressure Distribution Pressure and velocity distribution along axis

25 Comparison of Experiment and Simulation results Inlet pressure: 51kPa Aperture : 3mm Length: 51mm Sheng huang, Kun Zhu, et al, Quantitative characterization of arc discharge as vacuum interface, Physics of plasmas, 2014

26 How to increase the aperture? Power is proportional to r 2, 10 times of 3mm plasma window Aperture:10mm Fixed Current:50A

27 Two stage construction 50A 50A

28 Conclusion Ø A test bench of plasma window is built. Small aperture plasma window experiment is done. Ø A simulation model is set up, the simulation result is agree with experiment result. It can be used for evaluating the performance of larger aperture plasma window Ø Large aperture will need very high power, So we design a new structure of two stage plasma windows with 10mm aperture, experiments have been done and the feasibility is proven

29 Future Ø Do plasma window experiments with deuterium gas Ø Improve the structure of plasma window Ø Use the simulation method to optimized the property of large diameter plasma window Ø Build two stage plasma window with large diameter if possible

30