李建勋, 童中翔, 刘万俊, 王超哲, 张志波, 禚真福. 航空发动机红外辐射实验与仿真[J]. 红外与激光工程, 2013, 42(3): 549-555.
引用本文: 李建勋, 童中翔, 刘万俊, 王超哲, 张志波, 禚真福. 航空发动机红外辐射实验与仿真[J]. 红外与激光工程, 2013, 42(3): 549-555.
Li Jianxun, Tong Zhongxiang, Liu Wanjun, Wang Chaozhe, Zhang Zhibo, Zhuo Zhenfu. Infrared radiation characteristic experiment and simulation of aeroengine[J]. Infrared and Laser Engineering, 2013, 42(3): 549-555.
Citation: Li Jianxun, Tong Zhongxiang, Liu Wanjun, Wang Chaozhe, Zhang Zhibo, Zhuo Zhenfu. Infrared radiation characteristic experiment and simulation of aeroengine[J]. Infrared and Laser Engineering, 2013, 42(3): 549-555.

航空发动机红外辐射实验与仿真

Infrared radiation characteristic experiment and simulation of aeroengine

  • 摘要: 为研究航空发动机红外辐射分布规律和尾焰红外辐射特征,对地面试车条件下的某型发动机进行了红外辐射特性测试实验。实验结果表明:发动机红外特性在不同的Ma 数下变化较小,但因低压压气机出口的温度随飞行Ma 数增大而升高,发动机外壁面的红外辐射随之增加;发动机混合室璧面红外辐射最为强烈,其红外辐射强度随飞行Ma 数的增大呈非线性增大;尾焰的红外辐射呈现梨形包络,发动机在后方的辐射明显强于前方。在地面试车条件下,文中开发的尾焰红外辐射仿真程序的计算结果与实测结果基本吻合,相对误差不超过15%,并且其空间分布基本一致。

     

    Abstract: In order to study infrared radiation distribution along aeroengine and infrared characteristic of plume, the infrared radiation characteristic of an aeroengine was experimentally studied under the condition of ground engine testing. The experimental results show that the change of infrared characteristic along engine is small under different Mach number. The temperature of low compressor outlet increases with the Mach number. And the infrared radiation of engine's ektexine increases. The most intense infrared radiation is measured in the ektexine of blending box. Ektexine's radiation of blending box changes with non-linear feature and the increasing of the Mach number. The infrared radiation of plume is pyriform. The infrared radiation after engine is bigger than that before engine. Under the condition of ground engine testing, calculation program of infrared radiation for plume is presented. The computed results of directional radiance have tallied in general with the experimental results. Relative error between computed results and experimental results is not more than 15%. The spatial distribution of computed results is similar to experimental results.

     

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