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运转过程单斜晶系激光晶体的温度分布

沈鸿元, 张戈, 黄呈辉, 位民, 陈振强

沈鸿元, 张戈, 黄呈辉, 位民, 陈振强. 运转过程单斜晶系激光晶体的温度分布[J]. 激光技术, 2002, 26(4): 244-245,249.
引用本文: 沈鸿元, 张戈, 黄呈辉, 位民, 陈振强. 运转过程单斜晶系激光晶体的温度分布[J]. 激光技术, 2002, 26(4): 244-245,249.
Shen Hongyuan, Zhang Ge, Huang Chenghui, Wei Min, Chen Zhenqiang. Temperature distribution of monocline laser crystal in operation process[J]. LASER TECHNOLOGY, 2002, 26(4): 244-245,249.
Citation: Shen Hongyuan, Zhang Ge, Huang Chenghui, Wei Min, Chen Zhenqiang. Temperature distribution of monocline laser crystal in operation process[J]. LASER TECHNOLOGY, 2002, 26(4): 244-245,249.

运转过程单斜晶系激光晶体的温度分布

基金项目: 

国家自然科学基金资助项目

详细信息
    作者简介:

    沈鸿元,男,1937年8月出生.研究员,博士生导师.主要从事激光材料物理、新型激光器和激光医疗机的研究和应用工作.

  • 中图分类号: O711+.4

Temperature distribution of monocline laser crystal in operation process

  • 摘要: 计算了第Ⅰ类、第Ⅲ类边界条件下灯泵浦单斜晶系激光晶体垂直棒轴截面上的温度分布,结果表明,在第Ⅰ类边界条件下,温度分布为径向抛物线函数,等温线是圆;对于第Ⅲ类边界条件,温度分布是椭圆或双曲线函数,等温线是椭圆或双曲线。主热导率差别越大,冷却剂冷却效率越弱,偏离圆越严重,提高冷却剂的冷却效率将减小这种偏离。
    Abstract: For first and third class boundary condition the temperature distribution of monocline laser crystal in a cross section perpendicular to rod axis during the lamp pumping process is calculated in this paper.It is shown that the temperature distribution exhibits radial parabola function and the isothermal line is circularity for first class boundary condition,whereas it is elliptic or hyperbolic function and the isothermal line is ellipse or hyperbola for third class boundary condition.The larger the difference between the principal thermal conductivity is and the lower the cooling efficiency of cooling agent is,the larger the difference with circularity is.Increasing cooling efficiency of cooling agent the difference with circularity will be decreasing.
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    Foster J D,Osterink L M.J A P,1970,41(19):3656.

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    Patek K.Glass Laser.London:Iliffe Book,1970.

    [3]

    Yoshimura M,Furuya H,Kobayashi T et al.Opt Lett,1999,24:193.

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出版历程
  • 收稿日期:  2001-12-02
  • 发布日期:  2002-07-24

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