关奇, 杜太焦, 陈志华, 闫伟, 彭国良. 亚声速球/柱尾流对激光传输影响的数值模拟[J]. 红外与激光工程, 2017, 46(9): 906005-0906005(7). DOI: 10.3788/IRLA201746.0906005
引用本文: 关奇, 杜太焦, 陈志华, 闫伟, 彭国良. 亚声速球/柱尾流对激光传输影响的数值模拟[J]. 红外与激光工程, 2017, 46(9): 906005-0906005(7). DOI: 10.3788/IRLA201746.0906005
Guan Qi, Du Taijiao, Chen Zhihua, Yan Wei, Peng Guoliang. Numerical simulation of laser propagation effects through subsonic hemispherical/cylindrical wake[J]. Infrared and Laser Engineering, 2017, 46(9): 906005-0906005(7). DOI: 10.3788/IRLA201746.0906005
Citation: Guan Qi, Du Taijiao, Chen Zhihua, Yan Wei, Peng Guoliang. Numerical simulation of laser propagation effects through subsonic hemispherical/cylindrical wake[J]. Infrared and Laser Engineering, 2017, 46(9): 906005-0906005(7). DOI: 10.3788/IRLA201746.0906005

亚声速球/柱尾流对激光传输影响的数值模拟

Numerical simulation of laser propagation effects through subsonic hemispherical/cylindrical wake

  • 摘要: 采用大涡模拟方法计算了来流速度为0.4 Ma情况下球/柱形结构附近的流场,根据密度数据计算了光程差及气动相屏,并研究了尾流对激光传输的影响。结果表明:光程差空间均方根的时间平均值随发射角增大而增大,发射角从120增加到148时,其数值从0.11 m增加到0.28 m;光程差空间均方根随时间变化剧烈,发射角为148时,其时间均方根可达0.04 m;球/柱尾流对激光传输有很大影响,发射角为148情况下,Strehl比的时间平均值为0.33,并且Strehl比的时间平均值随发射角的增大而减小,发射角从120增加到148过程中,Strehl比的时间平均值减小了59%;Strehl比随时间变化剧烈,其时间均方根大于0.05。

     

    Abstract: Compressible large eddy simulation was carried out to study the flow field around a hemispherical/cylindrical structure at Mach number of Ma=0.4. Optical path difference and aero-optical phase were calculated according to density data obtained by the large eddy simulation method, and then the aero-optical effect of the wake was studied. The results show that the time-averaged root-mean-square of optical path difference increases with the angle of projection, and it varies from 0.11 m to 0.28 m when the angle of projection increases from 120to 148. Besides, the root-mean-square of optical path difference changes dramatically over time, and its temporal root-mean-square value reaches 0.04 m when the angle of projection is 148. The wake of the hemispherical/cylindrical structure has great effect on laser propagation, and the time-averaged Strehl ratio is 0.33 for the angle of projection of 148. The time-averaged Strehl ratio decreases with the angle of projection, and it reduces 59% when angle of projection increases from 120to 148. The Strehl ratio also changes dramatically over time, and its temporal root-mean-square value is 0.05.

     

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