• High Power Laser and Particle Beams
  • Vol. 34, Issue 1, 011008 (2022)
Peng Hu, Jianzhu Zhang, and Feizhou Zhang*
Author Affiliations
  • Institute of Applied Physics and Computational Mathematics, Beijing 100088, China
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    DOI: 10.11884/HPLPB202234.210296 Cite this Article
    Peng Hu, Jianzhu Zhang, Feizhou Zhang. Modeling and analysis of inner thermal effects in high energy laser system[J]. High Power Laser and Particle Beams, 2022, 34(1): 011008 Copy Citation Text show less
    Thermal aberrations of Si reflector of different absorptivity
    Fig. 1. Thermal aberrations of Si reflector of different absorptivity
    Thermal aberrations of reflection and transmission for SiO2 and Al2O3
    Fig. 2. Thermal aberrations of reflection and transmission for SiO2 and Al2O3
    Thermal diffusion of different materials vs time
    Fig. 3. Thermal diffusion of different materials vs time
    Distribution of thermal aberration of SiO2 under uniform and non-uniform laser irradiation
    Fig. 4. Distribution of thermal aberration of SiO2 under uniform and non-uniform laser irradiation
    RMS of thermal aberration under uniform and non-uniform laser spot irradiation as a function of time
    Fig. 5. RMS of thermal aberration under uniform and non-uniform laser spot irradiation as a function of time
    Sketch of a horizontal closed tube
    Fig. 6. Sketch of a horizontal closed tube
    Thermal aberrations in a closed horizontal tube
    Fig. 7. Thermal aberrations in a closed horizontal tube
    Temperature distribution of media gas at different time
    Fig. 8. Temperature distribution of media gas at different time
    Thermal aberrations of media gas under different pressure
    Fig. 9. Thermal aberrations of media gas under different pressure
    Thermal aberrations of gas of different ε
    Fig. 10. Thermal aberrations of gas of different ε
    Component interface of laser source
    Fig. 11. Component interface of laser source
    Component interface of reflector
    Fig. 12. Component interface of reflector
    Component interface of media gas
    Fig. 13. Component interface of media gas
    Component of analysis for wavefront and laser in far-field
    Fig. 14. Component of analysis for wavefront and laser in far-field
    Sketch of inner thermal effect simulation in Easylaser
    Fig. 15. Sketch of inner thermal effect simulation in Easylaser
    Complementary effect of thermal aberration between optical components and media gas
    Fig. 16. Complementary effect of thermal aberration between optical components and media gas
    Laser distribution in far-field
    Fig. 17. Laser distribution in far-field
    Characters of laser propagation in far-field
    Fig. 18. Characters of laser propagation in far-field
    materialdensity/(kg·m−3)heat capacity/(J·K−1·kg−1)thermal conductivity/(W·m−1·K−1)Young’s modulus/GPaPoisson ratiothermal expansion/K−1thermal optic coefficient/K−1
    Si23296951531900.264.68×10−6
    Al2O33980761.5243790.277.8×10−61.15×10−5
    SiO222007531.4730.170.42×10−61.10×10−5
    Table 1. Physical values of the glasses
    density/(kg·m−3)specific heat capacity/ (J·K−1·kg−1)thermal conductivity/(W·m−1·K−1)dynamic viscosity/(μPa·s)refractive index
    1.250610430.02617.91.0002793
    Table 2. Physical values of the N2
    Peng Hu, Jianzhu Zhang, Feizhou Zhang. Modeling and analysis of inner thermal effects in high energy laser system[J]. High Power Laser and Particle Beams, 2022, 34(1): 011008
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