Laser & Optoelectronics Progress, Volume. 60, Issue 21, 2116001(2023)

Effect of Asymmetry in Cooling on Residual Temperature Field of an N41-Type Neodymium Glass Main Amplifier Slab

Jixi Xu1,2, Xin Wang1, Jingping Tang1, Wei Chen1、*, Shubin Chen1, and Lili Hu1
Author Affiliations
  • 1Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
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    Figures & Tables(8)
    Model of Nd-glass main amplifier slab. Nd-glass plate has dimension of 786 mm×436 mm×40 mm, whose four edges are bonded with 12 mm thick edge-cladding glass by epoxy glue, and origin of coordinates is located at geometric center
    Temperature distribution in xy section (z=0) of N41-type Nd-glass main amplifier slab at different time after pumping. Heat transfer coefficient of Nd-glass surface is 2.5 W/(m2·K). (a)‒(e) Heat transfer coefficient of edge-cladding of Nd-glass is 2.5 W/(m2·K); (f)‒(j) heat transfer coefficient of edge-cladding of Nd-glass is 30 W/(m2·K)
    Temperature field distribution of N41-type Nd-glass main amplifier slab at thermal recovery state under asymmetric cooling at xy profile with z=0. Heat transfer coefficient of Nd-glass surface is 2.5 W/(m2·K). (a) Up side is 2 W/(m2·K), bottom side is 3 W/(m2·K), and left and right sides linearly transit from 2 to 3 W/(m2·K); (b) up side is 4 W/(m2.K), bottom side is 6 W/(m2·K), and left and right sides linearly transit from 4 to 6 W/(m2·K); (c) up side is 12 W/(m2·K), bottom side is 18 W/(m2·K), and left and right sides linearly transit from 12 to 18 W/(m2·K); (d) up side is 20 W/m2K, bottom side is 30 W/m2K, and left and right sides linearly transit from 20 to 30 W/(m2·K)
    (a) Average temperature rise and (b) temperature difference between upper-corner point and down-corner point of N41-type Nd-glass main amplifier slab under unsymmetrical edge cooling conditions
    Relationship between (a) slab-equilibration time and (b) self-equilibration time of N41-type Nd-glass main amplifier slab and heat transfer coefficient applied to surfaces of edge-cladding. Heat transfer coefficient applied to Nd-glass optical pass surface is 2.5 W/(m2·K)
    Conducted heat energy when N41-type Nd-glass main amplifier slab transmits through Nd-glass optical pass surface, short edge-cladding interface, and long edge-cladding interface. Heat transfer coefficient of Nd-glass is 2.5 W/(m2·K). Heat transfer coefficient of edge-cladding is (a) 2.5 W/(m2·K); (b) 5 W/(m2·K); (c) 15 W/(m2·K); (d) 30 W/(m2·K). Heat flux from edge-cladding to Nd-glass is negative and on the contrary, it is positive
    N41-type Nd-glass main amplifier slab dissipates heat energy outward through (a) short edge-cladding interface, (b) long edge-cladding interface, (c) Nd-glass optical pass surface, and (d) all interfaces of Nd-glass. Heat transfer coefficient applied to Nd-glass surface is 2.5 W/(m2·K), and heat transfer coefficient applied to edge-cladding surface is from 2.5 to 30 W/(m2·K)
    • Table 1. Thermal recovery characteristic time of N41-type Nd-glass main amplifier slab under four kinds of unsymmetrical edge cooling conditions

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      Table 1. Thermal recovery characteristic time of N41-type Nd-glass main amplifier slab under four kinds of unsymmetrical edge cooling conditions

      No.Edge cooling conditionThermal recovery time
      hedge-up /(W·m-2·K-1hedge-down /(W·m-2·K-1hedge-left and hedge-right /(W·m-2·K-1tslab-equilibration /mintself-equilibration /min
      1#23Linear transition from 2 to 3458342
      S1#2.52.52.5456280
      2#46Linear transition from 4 to 6406452
      3#1218Linear transition from 12 to 18338480
      4#2030Linear transition from 20 to 30318478
      S4#303030312476
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    Jixi Xu, Xin Wang, Jingping Tang, Wei Chen, Shubin Chen, Lili Hu. Effect of Asymmetry in Cooling on Residual Temperature Field of an N41-Type Neodymium Glass Main Amplifier Slab[J]. Laser & Optoelectronics Progress, 2023, 60(21): 2116001

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    Paper Information

    Category: Materials

    Received: Sep. 29, 2022

    Accepted: Oct. 24, 2022

    Published Online: Oct. 26, 2023

    The Author Email: Wei Chen (weichen@siom.ac.cn)

    DOI:10.3788/LOP222656

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