• Laser & Optoelectronics Progress
  • Vol. 60, Issue 21, 2116001 (2023)
Jixi Xu1,2, Xin Wang1, Jingping Tang1, Wei Chen1,*..., Shubin Chen1 and Lili Hu1|Show fewer author(s)
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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    DOI: 10.3788/LOP222656 Cite this Article Set citation alerts
    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 Copy Citation Text show less
    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
    Fig. 1. 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)
    Fig. 2. 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)
    Fig. 3. 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
    Fig. 4. (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)
    Fig. 5. 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
    Fig. 6. 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)
    Fig. 7. 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)
    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
    Table 1. Thermal recovery characteristic time of N41-type Nd-glass main amplifier slab under four kinds of unsymmetrical edge cooling conditions
    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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