高功率TEA CO2激光器主机结构优化设计

邵明振; 邵春雷; 卢启鹏; 郭劲; 李殿军

doi:10.3788/fgxb20133403.0388

您当前的位置：

首页 >

文章列表页 >

高功率TEA CO₂激光器主机结构优化设计

半导体发光、激光和光电性质 | 更新时间：2020-08-12

- 高功率TEA CO₂激光器主机结构优化设计
- Design on Mainframe of High Power TEA CO₂ Laser and Optimization
- 发光学报 2013年34卷第3期页码：388-393
- 作者机构：
  
  1. 中国科学院大学北京,100049
  2. 中国科学院长春光学精密机械与物理研究所激光与物质相互作用国家重点实验室,吉林长春,130033
- 作者简介：
- 基金信息：
  
  中国科学院知识创新工程领域前沿(O72z32c070)资助项目()
- DOI：10.3788/fgxb20133403.0388
  中图分类号： TN248.2
- 纸质出版日期：2013-3-10，
  
  收稿日期：2012-12-21，
  
  修回日期：2013-1-22，
扫描看全文
邵明振, 邵春雷, 卢启鹏, 郭劲, 李殿军. 高功率TEA CO2激光器主机结构优化设计[J]. 发光学报, 2013,34(3): 388-393

SHAO Ming-zhen, SHAO Chun-lei, LU Qi-peng, GUO Jin, LI Dian-jun. Design on Mainframe of High Power TEA CO2 Laser and Optimization[J]. Chinese Journal of Luminescence, 2013,34(3): 388-393
邵明振, 邵春雷, 卢启鹏, 郭劲, 李殿军. 高功率TEA CO2激光器主机结构优化设计[J]. 发光学报, 2013,34(3): 388-393 DOI： 10.3788/fgxb20133403.0388.

SHAO Ming-zhen, SHAO Chun-lei, LU Qi-peng, GUO Jin, LI Dian-jun. Design on Mainframe of High Power TEA CO2 Laser and Optimization[J]. Chinese Journal of Luminescence, 2013,34(3): 388-393 DOI： 10.3788/fgxb20133403.0388.

摘要

为促进高功率TEA CO

激光器的工程化应用

对主机结构进行了小型化轻量化研究。设计了一种新型环形流道式主机结构

取代原来的圆筒式结构。采用计算机有限元分析方法对壳体结构的应力和变形进行模拟计算

通过对2种结构在刚度、稳定性和重量方面的对比分析

以有筋板的盒式壳体取代纯盒式壳体结构

壳体设计壁厚由7 mm下降到4 mm

最大变形减小了近1个数量级

由1.11 mm减小到0.126 mm。研制出的壳体实测变形与模拟计算结果最大误差仅为1.58%。经测量

新型的环形流道式主机比圆筒式主机体积减小约30%

重量减少约40%

放电区气流速度由84.8 m/s提高到97 m/s。在相同的工作参数下进行出光实验

新型主机与圆筒式主机相比

激光重复频率由400 Hz提高到了470 Hz

激光输出平均功率由6 800 W提高到7 900 W。

Abstract

To promote the engineering applications of high power TEA CO

lasers

the miniaturization and lightweight of the host structure was studied. A new type of host structure with annular flow channel replaced the original cylindrical structure. The way of finite element analysis was used to simulate the stress and deformation of the shell structure. Through the comparison between the two structures on the stiffness

stability and weight

the cassette shell with the ribs which reduced the thickness of shell from 7 mm to 4 mm replaced the shell without ribs. The maximum deformation was reduced nearly an order of magnitude which was from 1.11 mm to 0.126 mm. The developed shell's maximum error between measured deformation and the simulation results was only 1.58%.After measurement

comparing with the cylindrical host

the volume of the new annular flow channel host was reduced by 30% and the weight reduced by 40%. The airflow rate in the discharge zone increased from 84.8 m/s to 97 m/s. After the test of the optic under the same operating para-meters

it is showed that the repetition frequency of the new laser is improved from 400 Hz to 470 Hz and the average output power is improved from 6 800 W to 7 900 W.

关键词

TEA CO2激光器主机结构应力集中应变

Keywords

TEA CO2 laserhost structurestress concentrationstrain

references

Wang S W, Guo L H, Zhao S, et al. Experiments of high-power CO2 laser disturbance to far-field HgCdTe detectors [J]. Opt. Precision Eng.(光学精密工程), 2010, 18(4):799-803 (in Chinese).[2] Shao C L, Song X F, Zhang L M, et al. High power TEA CO2 laser with two wavelengths free shift output structure [J]. Opt. Precision Eng.(光学精密工程), 2011, 19(2):429-436 (in Chinese).[3] Wu W M, Leng J Y, Zhou P, et al. Research progress of high average power electric-energy laser [J]. Infrared and Laser Engineering (红外与激光工程), 2011, 40(2):204-209 (in Chinese).[4] Guo R H, Zhang H Y, Wang T F. Evaluation of far field optical quality of TEA CO2 laser with unstable resonator [J]. Opt. Precision Eng.(光学精密工程), 2011, 19(2):408-412 (in Chinese).[5] Razhev A M, Churkin D S. Pulsed inductive discharge gas lasers [J]. Opt. Precision Eng.(光学精密工程), 2011, 19(2):238-251 (in English).[6] Hasson V. Review of recent advancements in the development of compact high power CO2 laser radar system [J]. SPIE, 1999, 3707:499-512.[7] Cao J J, Liang S Y, Li D J. Experimental research on UV-preionized TEA CO2 laser [J]. Laser & Infrared(激光与红外), 2008, 38(2):128-131 (in Chinese).[8] Shao C L, Yang G L, Li D J, et al. 9.3 μm branch selection research of high power pulse CO2 laser [J]. Chin. J. Lasers(中国激光), 2011, 38(3):1-6 (in Chinese).[9] Brown R T. High repetition-rate effects in TEA laser [J]. IEEE J. Quantum Electron., 1973, QE-9(11):1120-1122.[10] Shao C L. Design of gas circulation system in high power TEA CO2 laser [J]. High Power Laser and Particle Beams(强激光与粒子束), 2009, 21(1):1-5 (in Chinese).[11] Hou H L, Zhu X. Explosion process to eliminate welding residual stress [J]. Ship & Ocean Eng.(船海工程), 2002:8-13 (in Chinese).[12] Xu J J, Chen L G, Ni C Z. Effect of mechanical stress relieving method on welding residual stress [J]. J. Mechanic. Eng.(机械工程学报), 2009,45(9):291-295 (in Chinese).[13] Li L. Stretch method to releve residual stress in a aluminium alloy plate [J]. Light Alloy Fabrication Technology (轻合金加工技术), 1999, 27(5):16-18 (in Chinese).[14] Liu H W. Mechanics of Materials [M]. Beijing: Higher Education Press, 2004 (in Chinese).

浏览量

下载量

CSCD

文章被引用时，请邮件提醒。

提交

工具集

关联资源

不同应变对Ge的光学性质影响的第一性原理研究

蓝宝石衬底上GaN/Al_xGa_1-xN超晶格插入层对Al_xGa_1-xN外延薄膜应变及缺陷密度的影响

纤锌矿GaN/Al_xGa_1-xN应变柱形量子点中杂质态结合能及其压力效应