• High Power Laser and Particle Beams
  • Vol. 35, Issue 6, 065005 (2023)
Miao Qu1、2 and Sha Yan2、*
Author Affiliations
  • 1China Institute of Nuclear Industry Strategy, Beijing 100048, China
  • 2Institute of Heavy Ion Physics, Peking University, Beijing 100871, China
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    DOI: 10.11884/HPLPB202335.220182 Cite this Article
    Miao Qu, Sha Yan. Correction method for pulse energy density of compression plasma flows[J]. High Power Laser and Particle Beams, 2023, 35(6): 065005 Copy Citation Text show less
    Compact magnetoplasma compressor and compression plasma flow
    Fig. 1. Compact magnetoplasma compressor and compression plasma flow
    Surface morphology of tungsten under CPF single pulse irradiation with nominal energy density of 0.3 MJ/m2 (pulse width 0.1 ms)
    Fig. 2. Surface morphology of tungsten under CPF single pulse irradiation with nominal energy density of 0.3 MJ/m2 (pulse width 0.1 ms)
    Variation of surface temperature with time under different pulse energy densities (pulse width 0.1 ms) calculated by Comsol
    Fig. 3. Variation of surface temperature with time under different pulse energy densities (pulse width 0.1 ms) calculated by Comsol
    Schematic diagram of energy input and dissipation without boiling and ablation
    Fig. 4. Schematic diagram of energy input and dissipation without boiling and ablation
    Schematic diagram of energy input and dissipation with vaporization or ablation
    Fig. 5. Schematic diagram of energy input and dissipation with vaporization or ablation
    Energy density correction method for vaporization process
    Fig. 6. Energy density correction method for vaporization process
    Temperature dependence of thermal conductivity of W
    Fig. 7. Temperature dependence of thermal conductivity of W
    Time dependence of temperature distribution in depth direction of tungsten irradiated by CPF single pulse (pulse width 0.1 ms) with input energy density of 1.2 MJ/m2
    Fig. 8. Time dependence of temperature distribution in depth direction of tungsten irradiated by CPF single pulse (pulse width 0.1 ms) with input energy density of 1.2 MJ/m2
    Variation of the calculated surface degeneration with the input energy density
    Fig. 9. Variation of the calculated surface degeneration with the input energy density
    Variation of mass loss with nominal energy density in experiment
    Fig. 10. Variation of mass loss with nominal energy density in experiment
    Degenerative length under different energy densities from Table 2 and Table 3
    Fig. 11. Degenerative length under different energy densities from Table 2 and Table 3
    Schematic diagram of result evaluation of energy density correction
    Fig. 12. Schematic diagram of result evaluation of energy density correction
    parametervalue
    specific heat capacity of solid state/(J·kg−1·K−1) 144
    specific heat capacity of liquid state/(J·kg−1·K−1) 200
    solid density/(kg·m−3) 19 350
    liquid density/(kg·m−3) 17 600
    thermal conductivity/(W·m−1·K−1) variation with temperature
    melting point Tm/K 3 683.15
    boiling point Tb/K 5 933.15
    latent Heat LS-L/(kJ·kg−1) 187
    latent Heat LL-G/(kJ·kg−1) 4 009
    Table 1. Parameters of tungsten materials
    $ \varepsilon $/(MJ/m2) $ \Delta x $/μm
    0.700.00
    0.750.19
    0.800.58
    0.951.94
    1.002.52
    1.052.94
    1.153.98
    1.204.51
    Table 2. Calculated surface degeneration under different input energy densities
    $ {\varepsilon _n} $/(MJ/m2) $ \Delta m $/mg $ \Delta x' $/μm
    0.302.801.28
    0.404.452.04
    0.506.102.80
    0.9513.546.20
    1.0014.366.58
    1.0515.196.96
    1.1516.847.72
    1.2017.678.10
    Table 3. Surface degeneration corresponding to mass loss in the experiment
    $ {\varepsilon _n} $/(MJ/m2) $ \varepsilon $/(MJ/m2)
    0.30.87
    0.40.95
    0.51.03
    0.951.39
    1.051.46
    1.151.54
    1.201.58
    Table 4. Correction results of nominal average energy densities
    Miao Qu, Sha Yan. Correction method for pulse energy density of compression plasma flows[J]. High Power Laser and Particle Beams, 2023, 35(6): 065005
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