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基于载体对消方法的缝隙小角域散射特性研究

赵京城 杨涛 付鑫如 高旭 柴建忠

赵京城, 杨涛, 付鑫如, 等 . 基于载体对消方法的缝隙小角域散射特性研究[J]. 北京航空航天大学学报, 2018, 44(7): 1554-1561. doi: 10.13700/j.bh.1001-5965.2017.0498
引用本文: 赵京城, 杨涛, 付鑫如, 等 . 基于载体对消方法的缝隙小角域散射特性研究[J]. 北京航空航天大学学报, 2018, 44(7): 1554-1561. doi: 10.13700/j.bh.1001-5965.2017.0498
ZHAO Jingcheng, YANG Tao, FU Xinru, et al. Scattering characteristics of slit based on carrier cancellation method in small angular domain[J]. Journal of Beijing University of Aeronautics and Astronautics, 2018, 44(7): 1554-1561. doi: 10.13700/j.bh.1001-5965.2017.0498(in Chinese)
Citation: ZHAO Jingcheng, YANG Tao, FU Xinru, et al. Scattering characteristics of slit based on carrier cancellation method in small angular domain[J]. Journal of Beijing University of Aeronautics and Astronautics, 2018, 44(7): 1554-1561. doi: 10.13700/j.bh.1001-5965.2017.0498(in Chinese)

基于载体对消方法的缝隙小角域散射特性研究

doi: 10.13700/j.bh.1001-5965.2017.0498
详细信息
    作者简介:

    赵京城  男, 博士, 讲师, 硕士生导师。主要研究方向:微波毫米波成像、微波数字信号处理、辐射散射测量

    杨涛  男, 硕士研究生。主要研究方向:微波毫米波测量及成像、VxWorks系统嵌入式应用-雷达模拟器

    通讯作者:

    赵京城.E-mail:19644928@qq.com

  • 中图分类号: V218

Scattering characteristics of slit based on carrier cancellation method in small angular domain

More Information
  • 摘要:

    缝隙散射是隐身飞机散射的重要组成部分,已有的缝隙散射研究并未给出小角域(-30°~30°)入射时缝隙散射的结果。基于叠加原理的载体对消方法应用于缝隙散射源的电磁散射计算中,可以更精确地研究缝隙的电磁散射特性。通过单缝隙板的一维成像验证了载体对消方法的有效性和准确性,然后研究了在10 GHz频率下,缝隙散射在小角域内随宽度、长度的变化规律,以及极化特性。不同缝隙宽度的研究结果表明:在小角域内,当缝隙宽度小于1/4波长时,水平极化下缝隙散射比垂直极化下大,而当缝隙宽度大于1/4波长时,水平极化下缝隙散射比垂直极化下小;当缝隙宽度增大时,缝隙在垂直极化下的雷达散射截面(RCS)增长速度更快。不同缝隙长度的研究结果表明:在小角域内,缝隙电磁散射均值随着缝隙长度(200~1 000 mm)的增加而增加,散射均值的大致范围:-22.2~-8.4 dBsm(水平极化),-27.3~-13.3 dBsm(垂直极化);在小角域内,2种极化下,可拟合出RCS均值与缝隙长度的关系,得到某一缝隙长度的RCS,可计算出不同缝隙长度对应的RCS的大致范围。

     

  • 图 1  单缝隙板的计算模型

    Figure 1.  Calculation model of a plate with slit

    图 2  光板和单缝隙板的RCS随入射角变化

    Figure 2.  RCS of a plate and a plate with slit versus incidence angle

    图 3  光板、单缝隙板、对消后缝隙的一维像

    Figure 3.  One-dimensional images of a plate, a plate with slit, and slit after cancellation

    图 4  变宽度单缝隙计算模型

    Figure 4.  Calculation model of single slit with variable width

    图 5  变长度单缝隙计算模型

    Figure 5.  Calculation model of single slit with variable length

    图 6  矢量对消前后不同宽度单缝隙的RCS(HH极化)

    Figure 6.  RCS of single slit with different width before and after vector cancellation (HH polarization)

    图 7  矢量对消前后不同宽度单缝隙的RCS(VV极化)

    Figure 7.  RCS of single slit with different width before and after vector cancellation (VV polarization)

    图 8  矢量对消前后不同长度单缝隙的RCS(HH极化)

    Figure 8.  RCS of single slit with different length before and after vector cancellation (HH polarization)

    图 9  矢量对消前后不同长度单缝隙的RCS(VV极化)

    Figure 9.  RCS of single slit with different length before and after vector cancellation (VV polarization)

    图 10  小角域RCS均值随缝隙宽度的变化

    Figure 10.  Variation of RCS mean with slit width in small angular domain

    图 11  不同角域下RCS均值随缝隙长度的变化

    Figure 11.  Variation of RCS mean with slit length in different angular domains

    表  1  不同宽度单缝隙RCS均值

    Table  1.   RCS means of single slit with different width

    缝隙宽度/mm RCS均值/dBsm
    -30°~30°入射(HH极化) -30°~30°入射(VV极化) -15°~15°入射(HH极化) -15°~15°入射(VV极化)
    1 -35.324 -52.172 -35.108 -51.829
    3 -28.099 -35.902 -27.904 -35.252
    5 -22.185 -27.292 -22.042 -26.600
    8 -16.632 -18.450 -16.412 -17.666
    12 -12.669 -9.787 -12.211 -8.857
    16 -10.349 -5.926 -9.524 -4.842
    下载: 导出CSV

    表  2  不同长度单缝隙RCS均值

    Table  2.   RCS means of single slit with different length

    缝隙长度/mm RCS均值/dBsm
    -30°~30°入射(HH极化) -30°~30°入射(VV极化) -90°~90°入射(HH极化) -90°~90°入射(VV极化)
    200 -22.217 -27.297 -21.690 -37.478
    300 -19.108 -23.837 -18.464 -34.365
    400 -16.321 -21.282 -15.720 -31.694
    500 -14.465 -19.365 -13.840 -29.822
    600 -13.097 -17.835 -12.358 -28.306
    700 -11.522 -16.421 -10.772 -26.810
    800 -10.400 -15.282 -9.656 -25.722
    900 -9.438 -14.242 -8.687 -24.635
    1 000 -8.436 -13.336 -7.560 -23.632
    下载: 导出CSV
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  • 收稿日期:  2017-07-20
  • 录用日期:  2017-10-20
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