• Infrared and Laser Engineering
  • Vol. 49, Issue 9, 20200556 (2020)
Jianguo He1、2、3, Ming Li4, Zeqiang Mo1、2、3, Jinduo Wang1、2, Jin Yu1、2、*, Shoujun Dai1、2, Yanzhong Chen1, Wenqi Ge1, Yang Liu1、3, and Lianwen Fan5
Author Affiliations
  • 1Aerospace Information Research Institute, Chinese Academy of Sciences, Beijing 100094, China
  • 2University of the Chinese Academy of Sciences, Beijing 100049, China
  • 3Key Laboratory of Computational Optical Imaging Technology, Chinese Academy of Sciences, Beijing 100094, China
  • 4Xi'an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi'an 710119, China
  • 5Technology and Engineering Center for Space Utilization, Chinese Academy of Sciences, Beijing 100094, China
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    DOI: 10.3788/IRLA20200556 Cite this Article
    Jianguo He, Ming Li, Zeqiang Mo, Jinduo Wang, Jin Yu, Shoujun Dai, Yanzhong Chen, Wenqi Ge, Yang Liu, Lianwen Fan. Longitudinal forced convection heat transfer for high power slab laser media[J]. Infrared and Laser Engineering, 2020, 49(9): 20200556 Copy Citation Text show less
    Side-faces even pumping and cooling schematic for slab amplifer
    Fig. 1. Side-faces even pumping and cooling schematic for slab amplifer
    Schematic diagrams of cooling configuration. (a) Cavity forced convection; (b) Conduction through micro-channel heat sink; (c) Longitudinal forced convection
    Fig. 2. Schematic diagrams of cooling configuration. (a) Cavity forced convection; (b) Conduction through micro-channel heat sink; (c) Longitudinal forced convection
    Temperature contour on the x-z center cross section of laser slab. (a) Cavity forced convective configuration; (b) Micro-channel conductive configuration; (c) Longitudinal forced convective configuration
    Fig. 3. Temperature contour on the x-z center cross section of laser slab. (a) Cavity forced convective configuration; (b) Micro-channel conductive configuration; (c) Longitudinal forced convective configuration
    Different parameters of longitudinal forced convective configuration vs the inlet flow rate, insert figure is temperature variance varying with the inlet flow rate
    Fig. 4. Different parameters of longitudinal forced convective configuration vs the inlet flow rate, insert figure is temperature variance varying with the inlet flow rate
    Relationships of the different parameter differences vs inlet flow about fully developed and developing flow
    Fig. 5. Relationships of the different parameter differences vs inlet flow about fully developed and developing flow
    Simulation result of convective heat transfer coefficient vs x axis at the slab surface
    Fig. 6. Simulation result of convective heat transfer coefficient vs x axis at the slab surface
    Effection of the surface roughness on performance of cooling system
    Fig. 7. Effection of the surface roughness on performance of cooling system
    Crystal end faces temperature in investigation with laser amplifier working in longitudinal forced convection- infrared thermal imager (up) and simulation results (down)
    Fig. 8. Crystal end faces temperature in investigation with laser amplifier working in longitudinal forced convection- infrared thermal imager (up) and simulation results (down)
    Cooling configurationFlow rate/ L·min−1Max static pressure/ MPa Max flow velocity/ m·s−1Max temperature/ ℃ Average temperature/℃ Temperature variance
    Cavity forced convection40.000.3113.7232.2323.553.78
    Micro-channel conduction0.60 (one side)0.875.9532.3029.002.05
    Longitudinal forced convection20.00 (one side)0.2211.3326.122.690.95
    Table 1.

    Simulation results of several cooling configurations

    几种冷却方案的模拟结果

    ParameterValue
    Thermal power/W8509009601 020
    Measurement/℃34.636.338.640.1
    Simulation/ ℃33.5134.3836.4438.17
    Table 2.

    Crystal end faces temperature in investigation with laser amplifier working in longitudinal forced convection

    纵向强制对流冷却方案中实验用激光放大器工作状态晶体端面温度

    Jianguo He, Ming Li, Zeqiang Mo, Jinduo Wang, Jin Yu, Shoujun Dai, Yanzhong Chen, Wenqi Ge, Yang Liu, Lianwen Fan. Longitudinal forced convection heat transfer for high power slab laser media[J]. Infrared and Laser Engineering, 2020, 49(9): 20200556
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