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高功率小型化阶梯型双半圆波导模转天线设计

陈雅欣 李相强 张健穹 王庆峰 唐先锋

陈雅欣, 李相强, 张健穹, 等. 高功率小型化阶梯型双半圆波导模转天线设计[J]. 强激光与粒子束, 2025, 37: 053001. doi: 10.11884/HPLPB202537.240391
引用本文: 陈雅欣, 李相强, 张健穹, 等. 高功率小型化阶梯型双半圆波导模转天线设计[J]. 强激光与粒子束, 2025, 37: 053001. doi: 10.11884/HPLPB202537.240391
Chen Yaxin, Li Xiangqiang, Zhang Jianqiong, et al. Design of high power miniaturized stepped double semicircular waveguide mode-transducing antenna[J]. High Power Laser and Particle Beams, 2025, 37: 053001. doi: 10.11884/HPLPB202537.240391
Citation: Chen Yaxin, Li Xiangqiang, Zhang Jianqiong, et al. Design of high power miniaturized stepped double semicircular waveguide mode-transducing antenna[J]. High Power Laser and Particle Beams, 2025, 37: 053001. doi: 10.11884/HPLPB202537.240391

高功率小型化阶梯型双半圆波导模转天线设计

doi: 10.11884/HPLPB202537.240391
基金项目: 国家自然科学基金项目(62301459)
详细信息
    作者简介:

    陈雅欣,m15184399601@163.com

    通讯作者:

    李相强,xiangqiang_li@163.com

  • 中图分类号: TN82

Design of high power miniaturized stepped double semicircular waveguide mode-transducing antenna

  • 摘要: 在高功率微波辐射领域中,模式变换器加喇叭天线是实现旋转轴对称模定向辐射的常用技术,但模式变换器与喇叭天线的分离设计往往会使得天线轴向和口面尺寸较大。为了满足实际应用场景对天线小型化的需求,提出了一种模式控制与辐射一体化的阶梯型双半圆波导辐射天线。该天线由圆波导TM01模输入,通过插板将圆波导TM01模分成两路相位相反的半圆波导TE11模,之后再连接两个不对称的阶梯型半圆波导辐射器实现微波辐射。功分器采用了渐变圆波导进行匹配,同时采用大半径的内导体以提高功率容量。双半圆波导辐射器利用模式匹配法结合粒子群优化算法进行相位调节和模式控制。通过分区域的模式控制和辐射一体化设计,在辐射口面处达到更加均匀的同相电场分布,实现定向辐射,从而缩短了天线长度、降低了口面大小。优化设计了一个中心频率为2.85 GHz的天线模型,天线尺寸为1.18λ×1.18λ × 2.42λ。仿真结果表明:在2.75~2.96 GHz内天线回波损耗大于15 dB,在2.71~3 GHz内实际增益大于15.5 dBi,中心频点的实际增益为16.14 dBi,真空功率容量为906 MW。相比于传统的模式转换器加喇叭天线的技术路线,该天线具有高功率容量、小型化的特点。
  • 图  1  天线剖面图

    Figure  1.  Antenna profile

    图  2  单级波导突变模式耦合

    Figure  2.  Mode coupling of single step waveguide

    图  3  多级突变级联耦合示意图

    Figure  3.  Multistep discontinuous geometry

    图  4  阶梯半圆波导辐射器

    Figure  4.  Stepped semicircular waveguide radiator

    图  5  数值计算S参数

    Figure  5.  Numerical calculation of S parameters

    图  6  数值计算方向图

    Figure  6.  Numerical calculation of patterns

    图  7  功分器剖面图

    Figure  7.  Power divider profile

    图  8  功分器电场分布示意图

    Figure  8.  Electric field distribution of power divider

    图  9  功分器S参数

    Figure  9.  Power divider S parameters

    图  10  功分器传输相位情况

    Figure  10.  Power divider transmission phases

    图  11  某一时刻下天线的电场分布

    Figure  11.  Electric field distribution of the antenna at a given time

    图  12  天线S参数及增益随频率变化曲线

    Figure  12.  Antenna S parameters and gain curve vs. frequency

    图  13  天线最值电场分布情况

    Figure  13.  Distribution of the antenna's maximum electric field

    表  1  优化后参数

    Table  1.   Optimized parameters (mm)

    r1r2r3rm1rm2rm3L1L2L3L4L5
    47.7865.3035.719.1012.345.577.272.702.673.066.51
    下载: 导出CSV

    表  2  与分离设计技术路线的对比

    Table  2.   Comparison with separately designed technical routes

    Ref. mode converter type
    and antenna type
    mode converter
    length
    horn size combined size power capacity
    [11] coaxial conductor with inserted plate, horn 4.73λ 1.4λ×1.4λ×1.5λ 1.4λ×1.4λ×6.28λ not mentioned@4.05 GHz
    [12] 2 CirWG-to-4-orthometric-RecWGs, horn >4.75λ 1.4λ×1.4λ×1.5λ 1.4λ×1.4λ×(>6.25λ) 2 GW@9.5 GHz
    [13] rectangular plate, horn 2λ 1.4λ×1.4λ×1.5λ 1.4λ×1.4λ×3.55λ 558 MW@8.45 GHz
    [14] triangular plate, horn 2.46λ 1.4λ×1.4λ×1.5λ 1.4λ×1.4λ×4.01λ 1 GW@3.4 GHz
    this work rectangular plate with
    stepped-expanding aperture
    1.18λ×1.18λ×2.43λ 906 MW@2.85 GHz
    下载: 导出CSV
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出版历程
  • 收稿日期:  2024-11-12
  • 修回日期:  2025-02-23
  • 录用日期:  2025-02-23
  • 网络出版日期:  2025-03-15
  • 刊出日期:  2025-03-31

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