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矿井UWB定位系统中圆极化天线的优化设计和应用

鞠晨

鞠晨. 矿井UWB定位系统中圆极化天线的优化设计和应用[J]. 工矿自动化,2023,49(1):171-176.  doi: 10.13272/j.issn.1671-251x.18071
引用本文: 鞠晨. 矿井UWB定位系统中圆极化天线的优化设计和应用[J]. 工矿自动化,2023,49(1):171-176.  doi: 10.13272/j.issn.1671-251x.18071
JU Chen. Optimization design and application of circularly polarized antenna in mine UWB positioning system[J]. Journal of Mine Automation,2023,49(1):171-176.  doi: 10.13272/j.issn.1671-251x.18071
Citation: JU Chen. Optimization design and application of circularly polarized antenna in mine UWB positioning system[J]. Journal of Mine Automation,2023,49(1):171-176.  doi: 10.13272/j.issn.1671-251x.18071

矿井UWB定位系统中圆极化天线的优化设计和应用

doi: 10.13272/j.issn.1671-251x.18071
基金项目: 国家重点研发计划项目(2017YFC0804303);国家能源集团科技创新项目(GJNY2030XDXM-19-06.1)。
详细信息
    作者简介:

    鞠晨(1988—),男,辽宁北票人,工程师,从事矿井精确定位方面的工作,E-mail:10036293@chnenergy.com.cn

  • 中图分类号: TD655.3

Optimization design and application of circularly polarized antenna in mine UWB positioning system

  • 摘要: 天线是矿井UWB定位系统的重要组成部分,为了抑制矿井UWB定位系统接收到多径反射信号,提高矿井UWB定位系统的定位精度,对传统圆极化天线结构进行优化,设计了一种新型右旋圆极化微带天线。先将矩形开槽改为十字开槽,改变电流轨迹,使两正交线性极化电场的相差更接近90°,从而降低轴比,使天线的圆极化纯度更高;再将十字开槽平滑扩展为菱形开槽,达到提高交叉极化电平、抑制正交旋向的效果,使天线实现更高的右旋圆极化纯度。采用HFSS软件对该新型右旋圆极化微带天线进行仿真,仿真结果表明,主辐射方向交叉极化电平>10.4 dBi,可以达到很好的右旋圆极化效果。新型右旋圆极化微带天线样品的工作频带和回波实测结果同仿真结果基本吻合,说明该新型天线结构易于加工且正常容差内的工艺偏差对天线性能的影响程度相对较小。将制作的新型右旋圆极化微带天线样品用于基于到达相位差的UWB定位系统,并在隧道环境下进行现场测试,测试结果表明,信号到达相位差稳定性有明显改善,对多径效应有明显的抑制效果,可以有效提高UWB定位系统的定位精度。该新型右旋圆极化微带天线具有体积小、质量轻、易于制作等优点。

     

  • 图  1  常用的圆极化微带天线构造方式

    Figure  1.  Construction mode of commonly used circularly polarized microstrip antenna

    图  2  传统右旋圆极化天线结构

    Figure  2.  Structure of conventional right-handed circularly polarized antenna

    图  3  传统右旋圆极化天线E面、H面轴比曲线

    Figure  3.  Axial ratio curves of E-plane and H-plane of conventional right-handed circularly polarized antenna

    图  4  传统右旋圆极化天线E面、H面交叉极化增益方向

    Figure  4.  Cross-polarization gain direction of E-plane and H-plane of conventional right-handed circularly polarized antenna

    图  5  天线演化过程

    Figure  5.  Antenna evolution process

    图  6  新型右旋圆极化微带天线结构

    Figure  6.  Structure of novel right-handed circularly polarized microstrip antenna

    图  7  新型右旋圆极化微带天线和传统右旋圆极化天线E面、H面轴比曲线

    Figure  7.  Axial ratio curves of E-plane and H-plane of novel right-handed circularly polarized microstrip antenna and conventional right-handed circularly polarized antenna

    图  8  新型右旋圆极化微带天线E面、H面交叉极化增益方向

    Figure  8.  Cross-polarization gain direction of E-plane and H-plane of novel right-handed circularly polarized microstrip antenna

    图  9  新型右旋圆极化微带天线辐射电场的极化旋转效果

    Figure  9.  Polarization rotation effect of radiated electric field of novel right-handed circularly polarized microstrip antenna

    图  10  新型右旋圆极化微带天线实物

    Figure  10.  Material object of novel right-handed circularly polarized microstrip antenna

    图  11  仿真和实测回波曲线对比

    Figure  11.  Comparison between simulated and measured echo curves

    图  12  隧道实地测试环境

    Figure  12.  Tunnel field test environment

    图  13  使用传统线极化天线和新型右旋圆极化微带天线时到达相位差对比曲线

    Figure  13.  Comparison curves of phase difference of arrival when using conventional linearly polarized antenna and novel right-handed circularly polarized microstrip antenna

    表  1  新型右旋圆极化微带天线参数

    Table  1.   Parameters of novel right-handed circularly polarized microstrip antenna

    W/
    mm
    L/
    mm
    R/
    mm
    a/
    mm
    La/
    mm
    Lb/
    mm
    $ {\varepsilon _{\rm{r}}} $ h1/
    mm
    h2/
    mm
    t1/
    μm
    t2/
    μm
    t3/
    μm
    $ \omega $/
    mm
    32.7 40.6 9.3 3.4 11.2 6.44 4.2 1.58 0.4 26 16 26 0.7
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出版历程
  • 收稿日期:  2022-12-21
  • 修回日期:  2023-01-11
  • 网络出版日期:  2023-01-17

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