• Infrared and Laser Engineering
  • Vol. 51, Issue 2, 20210455 (2022)
Zhongyang Xiong1, Chenguang Zhu1、2、*, Fanshun Duanmu1, and Jingwei Li1
Author Affiliations
  • 1School of Chemical Engineering, Nanjing University of Science and Technology, Nanjing 210094, China
  • 2Science and Technology on Electro-Optical Information Security Control Laboratory, Tianjin 300308, China
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    DOI: 10.3788/IRLA20210455 Cite this Article
    Zhongyang Xiong, Chenguang Zhu, Fanshun Duanmu, Jingwei Li. Research on infrared/passive millimeter wave compound decoy[J]. Infrared and Laser Engineering, 2022, 51(2): 20210455 Copy Citation Text show less

    Abstract

    An infrared/passive millimeter wave compound decoy was prepared. On the basis of MTV pyrotechnic composition, red phosphorus was used to replace part of magnesium powder, short carbon fiber was used as a functional additive, and a thin-film pyrotechnic material was prepared. The infrared radiation and millimeter wave radiation properties of this material were tested and analyzed. The research results show that the addition of a small amount of red phosphorus was beneficial to increase the radiation area; When the proportion of red phosphorus added is more than 10%, the average flame temperature, infrared radiation intensity and millimeter wave brightness temperature continue to decrease with the increase of red phosphorus content, after adding a suitable amount of carbon fiber, the burning rate, flame temperature and the infrared radiation are both enhanced; The millimeter wave brightness temperature continues to increase with the increase of carbon fiber content, when the amount of red phosphorus added is 10% and the carbon fiber content increases from 0 to 1.75%, the millimeter wave brightness temperature increased from 330 K to 458 K, brightness temperature greater than 400 K, longer duration.
    $ {B}_{f}=\frac{2hc}{{\lambda }^{3}}\frac{1}{{\rm{e}}^{\frac{hc}{KT \lambda }}-1} $(1)

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    $ {B}_{f}=\frac{2{f}^{2}KT}{{c}^{2}}=\frac{2 KT}{{\lambda }^{2}} $(2)

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    $ {B}_{b}={B}_{f}\Delta f=\frac{2 KT}{{\lambda }^{2}}\Delta f $(3)

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    $ {{B}}_{(\mathrm{\theta },\mathrm{\varphi })}=\frac{2{K}}{{\mathrm{\lambda }}^{2}}{{T}}_{{B}(\mathrm{\theta },\mathrm{\varphi })}\Delta{f} $(4)

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    $ \varepsilon =\frac{B(\theta ,\varphi )}{{B}_{b}}=\frac{{T}_{B(\theta ,\varphi )}}{T} $(5)

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    Zhongyang Xiong, Chenguang Zhu, Fanshun Duanmu, Jingwei Li. Research on infrared/passive millimeter wave compound decoy[J]. Infrared and Laser Engineering, 2022, 51(2): 20210455
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