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CN108173007A - A double-layer waveguide slot near-field focusing array antenna based on four-corner feeding - Google Patents

A double-layer waveguide slot near-field focusing array antenna based on four-corner feeding Download PDF

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Publication number
CN108173007A
CN108173007A CN201711396030.9A CN201711396030A CN108173007A CN 108173007 A CN108173007 A CN 108173007A CN 201711396030 A CN201711396030 A CN 201711396030A CN 108173007 A CN108173007 A CN 108173007A
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waveguide
slot
feeding
radiation
feed
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张淼
蒋柏林
段保权
柳清伙
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Xiamen University
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Xiamen University
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q21/00Antenna arrays or systems
    • H01Q21/0006Particular feeding systems
    • H01Q21/0037Particular feeding systems linear waveguide fed arrays
    • H01Q21/0043Slotted waveguides
    • H01Q21/005Slotted waveguides arrays
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q1/00Details of, or arrangements associated with, antennas
    • H01Q1/50Structural association of antennas with earthing switches, lead-in devices or lightning protectors
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q13/00Waveguide horns or mouths; Slot antennas; Leaky-waveguide antennas; Equivalent structures causing radiation along the transmission path of a guided wave
    • H01Q13/10Resonant slot antennas

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  • Variable-Direction Aerials And Aerial Arrays (AREA)
  • Waveguide Aerials (AREA)

Abstract

A kind of double-deck Waveguide slot near field focus array antenna based on quadrangle feed, is related to a kind of Waveguide slot antenna.It is made of the feed waveguide of lower floor and the radiating guide on upper strata;Incidence wave passes through feed waveguide successively from feed port, couple gap, radiating guide, space is finally radiated outside by radiating slot, the feed port and feed waveguide pass through central aperture feed-in using standard feed waveguide from the back side, it is fed using quadrangle and replaces traditional apex drive, by having the feed waveguide of 4 arms that signal is extended to 4 antenna angles from center, it is fed in the same direction from both ends to intermediate constant amplitude, PMC boundaries can be formed in feed waveguide center, thus come replace metal boundary reduce size, reduce design cost, the length of feed waveguide is 44.8mm, width is 5mm, highly it is 2mm.

Description

一种基于四角馈电的双层波导缝隙近场聚焦阵列天线A double-layer waveguide slot near-field focusing array antenna based on four-corner feeding

技术领域technical field

本发明涉及一种波导缝隙天线,尤其是涉及可用于无线电通信、近场通信、医疗检测等领域的一种基于四角馈电的双层波导缝隙近场聚焦阵列天线。The invention relates to a waveguide slot antenna, in particular to a double-layer waveguide slot near-field focusing array antenna based on four-corner feeding, which can be used in the fields of radio communication, near-field communication, medical detection and the like.

背景技术Background technique

天线阵列(或阵列天线)是许多相同的单个天线按一定规律排列组成的天线系统,以发射或接收无线电波。各个天线单元通过馈线连接到单个接收器或发射器,馈线以特定相位关系将能量馈送到各个天线单元。由每个单独天线辐射的无线电波组合并叠加,加在一起(可通过人为控制)以增强在期望方向上辐射的功率,并且减少在其它方向上辐射的功率。其中波导阵列天线是指在波导宽边或窄边上开有缝隙,并切断波导内壁上电流的天线([1]宋铮,张建华,黄治.天线与电波传播.西安电子科技大学出版社.2003.7)。根据缝隙单元间距和馈电方式不同,目前波导缝隙天线阵列主要有两种:An antenna array (or array antenna) is an antenna system composed of many identical individual antennas arranged in a certain order to transmit or receive radio waves. Each antenna element is connected to a single receiver or transmitter by a feedline that feeds energy to each antenna element in a specific phase relationship. The radio waves radiated by each individual antenna combine and add up, adding together (possibly by human control) to boost the power radiated in the desired direction and reduce the power radiated in other directions. Among them, the waveguide array antenna refers to an antenna that has a slit on the wide or narrow side of the waveguide and cuts off the current on the inner wall of the waveguide ([1] Song Zheng, Zhang Jianhua, Huang Zhi. Antenna and Radio Wave Propagation. Xidian University Press. 2003.7). According to the gap between the slot units and the feeding method, there are two main types of waveguide slot antenna arrays:

一种谐振式缝隙阵,所有缝隙都得到同相激励,最大辐射方向与天线轴线垂直,波导终端通常加短路活塞。谐振式天线通常带宽较窄,效率高。A resonant slot array, all slots are excited in the same phase, the maximum radiation direction is perpendicular to the antenna axis, and the waveguide terminal is usually equipped with a short-circuit piston. Resonant antennas typically have narrow bandwidth and high efficiency.

一种非谐振式缝隙阵,波导的一端加激励信号,另一端加匹配负载。与谐振式天线相比,非谐振式天线频带较宽,但效率较低。若缝隙单元数足够多,则被负载吸收的能量有限,因此与谐振式天线效率差距不大。A non-resonant slotted array, the excitation signal is applied to one end of the waveguide, and the matching load is applied to the other end. Compared with resonant antennas, non-resonant antennas have a wider frequency band, but are less efficient. If the number of slot units is large enough, the energy absorbed by the load is limited, so there is not much difference in efficiency from the resonant antenna.

中国专利201410744296.8公开一种宽带单腔波导缝隙谐振天线,该设计提供了一种具有良好的宽频带、低交叉极化特性、特别是天线高度压缩、结构简单的矩形波导宽边纵向直辐射缝隙天线。Chinese patent 201410744296.8 discloses a wide-band single-cavity waveguide slot resonant antenna. The design provides a rectangular waveguide wide-side longitudinal direct radiation slot antenna with good broadband, low cross-polarization characteristics, especially high antenna compression and simple structure. .

中国专利201110146539.4公开一种幅相加权的窄边波导缝隙阵列天线,该设计提供了一种更适于星载天线应用的结构紧凑、加工简单、不规则波束赋形的高增益窄边波导缝隙阵列赋形天线。Chinese patent 201110146539.4 discloses an amplitude-phase weighted narrow-side waveguide slot array antenna. This design provides a high-gain narrow-side waveguide slot array with compact structure, simple processing, and irregular beamforming that is more suitable for spaceborne antenna applications. Shaped antenna.

然而,这些波导缝隙阵大多馈电端口在中心,当阵列规模大时,难以控制阵元激励实现常见的泰勒分布、高斯分布等。而且,这些天线工作于远场,少有近场聚焦的方式,一般使用金属作为隔离终端,多数情况下采用铜来作为隔离电磁波的材料,这样在一些情况下会增大成本。However, most of these waveguide slot arrays have feed ports at the center. When the array is large in scale, it is difficult to control the element excitation to achieve the common Taylor distribution, Gaussian distribution, etc. Moreover, these antennas work in the far field, and there are few near-field focusing methods. Generally, metal is used as the isolation terminal, and copper is used as the material for isolating electromagnetic waves in most cases, which will increase the cost in some cases.

发明内容Contents of the invention

本发明的目的在于克服上述现有波导缝隙阵列天线的不足与未考虑之处,提供在波导内部等效形成的PMC边界和PEC边界,减小天线尺寸,降低结构成本,工作于近场区域,可用于医疗检测、近场通信等领域,馈电方式提高抗干扰性且更易于控制阵元泰勒激励,实现天线低副瓣的一种基于四角馈电的双层波导缝隙近场聚焦阵列天线。The purpose of the present invention is to overcome the deficiencies and unconsidered points of the above-mentioned existing waveguide slot array antenna, provide the PMC boundary and PEC boundary formed equivalently inside the waveguide, reduce the size of the antenna, reduce the structural cost, and work in the near field area. It can be used in medical detection, near-field communication and other fields. The feeding method improves anti-interference and is easier to control the Taylor excitation of the array element. It is a double-layer waveguide slot near-field focusing array antenna based on four-corner feeding to achieve low sidelobe of the antenna.

本发明由下层的馈电波导和上层的辐射波导组成;入射波从馈电端口依次经过馈电波导、耦合缝隙、辐射波导,最终由辐射缝隙辐射到外部空间,所述馈电端口和馈电波导采用标准馈电波导从背面通过中央孔径馈入,采用四角馈电代替传统的中心馈电,通过具有4个臂的馈电波导将信号从中心延伸到4个天线角,由两端向中间等幅同向馈电,在馈电波导中央能形成PMC边界,由此来代替金属边界减小尺寸,降低设计成本,馈电波导的长度为44.8mm,宽度为5mm,高度为2mm;The present invention consists of a feeder waveguide on the lower layer and a radiation waveguide on the upper layer; the incident wave passes through the feeder waveguide, the coupling slot, and the radiation waveguide sequentially from the feeder port, and finally radiates to the external space through the radiation slot. The waveguide adopts the standard feed waveguide to be fed from the back through the central aperture, and the four-corner feed is used instead of the traditional center feed, and the signal is extended from the center to the 4 antenna angles through the feed waveguide with 4 arms, from both ends to the middle Equal-amplitude and same-direction feeding can form a PMC boundary in the center of the feeding waveguide, thereby replacing the metal boundary to reduce size and reduce design costs. The length of the feeding waveguide is 44.8mm, the width is 5mm, and the height is 2mm;

所述耦合缝隙为同相馈电方式,耦合缝隙开于馈电波导上表面,它具有规则排布和抑制二阶波束的优点,耦合缝隙数目为2×8;耦合缝隙的一维泰勒分布由耦合缝隙的偏转角控制,耦合缝隙的长度为3.75mm,宽度为1mm,厚度为0.4mm;相邻耦合缝隙之间的间距Lc为0.5λgf,终端耦合缝隙距离波导终端端面的距离为0.5λgf,λgf为馈电波导波长。The coupling slots are fed in the same phase. The coupling slots are opened on the upper surface of the feeding waveguide. It has the advantages of regular arrangement and suppression of the second-order beam. The number of coupling slots is 2×8; the one-dimensional Taylor distribution of the coupling slots is determined by the coupling The deflection angle of the slot is controlled, the length of the coupling slot is 3.75mm, the width is 1mm, and the thickness is 0.4mm; the distance L c between adjacent coupling slots is 0.5λ gf , and the distance between the terminal coupling slot and the end face of the waveguide is 0.5λ gf , λ gf is the wavelength of the feeding waveguide.

所述辐射波导置于下层的馈电波导上部,采用馈电波导上表面所开耦合缝隙同相馈电,长度为42.8mm,宽度为5.2mm,高度为2mm;在辐射波导中央水平方向能等效成PEC终端,这种等效终端可以代替金属边界,降低成本。The radiation waveguide is placed on the upper part of the feed waveguide of the lower layer, and the coupling gap opened on the upper surface of the feed waveguide is used to feed in the same phase. The length is 42.8mm, the width is 5.2mm, and the height is 2mm; Into a PEC terminal, this equivalent terminal can replace the metal border and reduce costs.

所述辐射缝隙采用波导缝隙阵列,辐射缝隙开于辐射波导上表面,由聚焦位置计算其相位,幅度为泰勒分布,辐射缝隙数目为8×8,每个辐射缝隙的长度为3.87mm,宽度为1.5mm,厚度为0.4mm;相邻辐射缝横向之间的间距Lr为λg,纵向之间的间距取决于所需聚焦位置,终端四角辐射缝隙中心距离波导上下终端面的距离为0.5λgr,λgr为辐射波导波长。The radiation slot adopts a waveguide slot array, the radiation slot is opened on the upper surface of the radiation waveguide, its phase is calculated from the focus position, the amplitude is Taylor distribution, the number of radiation slots is 8×8, the length of each radiation slot is 3.87mm, and the width is 1.5mm, the thickness is 0.4mm; the distance L r between adjacent radial slits in the transverse direction is λ g , the distance between the longitudinal direction depends on the required focus position, and the distance between the center of the four-corner radiation slit at the terminal and the upper and lower terminal surfaces of the waveguide is 0.5λ gr , λ gr is the wavelength of the radiation waveguide.

本发明的工作原理是:馈电端口和馈电波导采用Q波段标准馈电波导从背面通过中央孔径馈入,通过具有4个臂的馈电电路将信号从中心延伸到四个天线角。在馈电波导中,耦合缝隙采用等幅同相的激励方式,馈电波导中,两端耦合缝隙中心距离左右终端为半波导波长,即0.5λgf。在本发明中采用四角馈电,由于从两端到中心的对称性,在中心形成等效PMC边界,可以代替金属边界,从而缩短一半波导波长,降低了结构复杂度,减少了加工成本。此外,等效PMC边界具有天线带宽更大的优点。在辐射波导和辐射缝隙中,因为采用四角馈电的方式,上下两个对称的子阵列同样具有相同的幅度和相位,在上下两个子阵列的中央水平方向等效形成PEC边界,可以代替金属边界。通过辐射缝隙距离每根辐射波导中心轴线的偏差可以控制激励幅度,通过辐射缝隙纵向的偏差可以控制激励相位,从而实现在近场内的聚焦。这些辐射缝隙隔断辐射波导上层导体表面电流,在辐射缝隙口径面获得激励,向外辐射电磁能量,成为在近场内聚焦的阵列天线。对于辐射缝隙,幅度采用泰勒分布,以降低近场横向副瓣电平。本发明由于使用独特的四角馈电方式,由于激励从四周到中心,相比较传统的中心馈电而言,对耦合缝隙和辐射缝隙的控制更为简单精确,也更易于实现幅度的泰勒分布。The working principle of the present invention is: the feeding port and the feeding waveguide adopt the Q-band standard feeding waveguide to feed in from the back through the central aperture, and the signal is extended from the center to the four antenna angles through the feeding circuit with 4 arms. In the feeding waveguide, the coupling slot adopts the excitation mode of equal amplitude and same phase. In the feeding waveguide, the distance between the centers of the coupling slots at both ends is half the wavelength of the waveguide, that is, 0.5λ gf . In the present invention, four-corner feeding is adopted, and due to the symmetry from both ends to the center, an equivalent PMC boundary is formed in the center, which can replace the metal boundary, thereby shortening half the waveguide wavelength, reducing structural complexity, and reducing processing costs. In addition, the equivalent PMC boundary has the advantage of larger antenna bandwidth. In the radiation waveguide and radiation slot, because of the four-corner feeding method, the upper and lower symmetrical sub-arrays also have the same amplitude and phase, and the central horizontal direction of the upper and lower two sub-arrays is equivalent to form a PEC boundary, which can replace the metal boundary. . The excitation amplitude can be controlled by the deviation of the radiation slit from the central axis of each radiation waveguide, and the excitation phase can be controlled by the longitudinal deviation of the radiation slit, so as to realize focusing in the near field. These radiation slots block the surface current of the upper layer conductor of the radiation waveguide, get excited on the aperture surface of the radiation slot, radiate electromagnetic energy outward, and become an array antenna focusing in the near field. For radiating slots, the amplitudes are Taylor distributed to reduce near-field lateral sidelobe levels. Because the present invention uses a unique four-corner feeding method, since the excitation is from the periphery to the center, compared with the traditional central feeding, the control of the coupling gap and the radiation gap is simpler and more accurate, and it is easier to realize the Taylor distribution of the amplitude.

附图说明Description of drawings

图1是本发明基于四角馈电的双层波导缝隙近场聚焦阵列天线结构示意图。FIG. 1 is a schematic diagram of the structure of a double-layer waveguide slot near-field focusing array antenna based on four-corner feeding in the present invention.

图2是本发明基于四角馈电的双层波导缝隙近场聚焦阵列天线馈电波导和馈电波导上表面耦合缝隙。Fig. 2 is the feeding waveguide and the coupling slot on the upper surface of the feeding waveguide of the double-layer waveguide slot near-field focusing array antenna based on quadrangular feeding in the present invention.

图3是本发明基于四角馈电的双层波导缝隙近场聚焦阵列天线辐射波导和辐射波导上表面辐射缝隙。Fig. 3 is the radiation waveguide of the double-layer waveguide slot near-field focusing array antenna and the radiation slot on the upper surface of the radiation waveguide based on four-corner feeding in the present invention.

图4是金属边界用于一般的馈电波导。Figure 4 shows the metal boundary used for a general feed waveguide.

图5是等效PMC边界应用于本发明中的馈电金属波导。Fig. 5 is the equivalent PMC boundary applied to the feeding metal waveguide in the present invention.

图6是金属边界用于一般的天线辐射波导。Figure 6 is a metal boundary used in a general antenna radiation waveguide.

图7是等效PEC边界应用于本发明中的辐射金属波导。Fig. 7 is a radiating metal waveguide in which the equivalent PEC boundary is applied in the present invention.

图8是本发明基于四角馈电的双层波导缝隙近场聚焦阵列天线耦合缝隙耦合因子参数图。Fig. 8 is a parameter diagram of the coupling factor of the double-layer waveguide slot near-field focusing array antenna coupling slot based on four-corner feeding in the present invention.

图9是本发明基于四角馈电的双层波导缝隙近场聚焦阵列天线在纵轴传输方向归一化场图。在图9中,聚焦位置为50mm,3dB聚焦深度为38mm。FIG. 9 is a normalized field diagram of the double-layer waveguide slot near-field focusing array antenna based on four-corner feeding in the vertical axis transmission direction of the present invention. In Figure 9, the focus position is 50mm, and the 3dB focus depth is 38mm.

具体实施方式Detailed ways

下面结合附图对本发明的具体实施方式进行说明。Specific embodiments of the present invention will be described below in conjunction with the accompanying drawings.

本实施例的宽带单腔波导缝隙谐振天线工作于Q波段,工作中心频率f0为40.25GHz,下边频fL为39.5GHz,上边频fH为41.0GHz。中心频率下馈电波导波长λgf为11.2mm,中心频率辐射波导波长λgr为10.7mm。The broadband single-cavity waveguide slot resonant antenna of this embodiment works in the Q-band, the working center frequency f0 is 40.25 GHz, the lower side frequency f L is 39.5 GHz, and the upper side frequency f H is 41.0 GHz. The wavelength λgf of the feeding waveguide at the center frequency is 11.2mm, and the wavelength λgr of the radiation waveguide at the center frequency is 10.7mm.

如图1所示,本发明实施例设有馈电端口1、馈电波导2、耦合缝隙3、辐射波导4和辐射缝隙5。天线工作在Q波段,采用标准馈电波导从背面通过馈电端口馈入,通过具有四个臂的馈电波导,馈电波导上的耦合缝隙获得激励。耦合缝隙的长度为3.75mm,宽度为1mm,厚度为0.4mm。相邻耦合缝中心之间的间距Lc为0.5λgf,终端耦合缝距离波导终端端面的距离为0.5λgf,λgf为馈电波导波长。耦合缝隙将激励耦合进入辐射波导,辐射波导位于耦合波导上端,在辐射波导上表面开辐射缝隙,辐射缝隙隔断辐射波导上表面电流,在辐射缝隙口获得激励,并向外辐射能量,形成波导缝隙天线阵列。辐射缝隙采用阵元波导缝隙阵列,幅度为泰勒分布,每个辐射缝隙的长度为3.87mm,宽度为1.5mm,厚度为0.4mm。相邻辐射缝隙横向中心之间的间距Lr为λgr,纵向中心的间距取决于聚焦位置,如图9即为实施例的聚焦位置为50mm在纵轴传输方向归一化场强仿真图,其中聚焦位置50mm决定辐射缝隙纵向中心的间距。终端四角辐射缝隙距离波导终端端面的距离为0.5λgr,λgr为辐射波导波长。馈电波导波长和辐射波导波长上面均已给出。As shown in FIG. 1 , the embodiment of the present invention has a feed port 1 , a feed waveguide 2 , a coupling slot 3 , a radiation waveguide 4 and a radiation slot 5 . The antenna works in the Q-band, and the standard feed waveguide is used to feed in from the back through the feed port. Through the feed waveguide with four arms, the coupling slot on the feed waveguide is excited. The length of the coupling slot is 3.75 mm, the width is 1 mm, and the thickness is 0.4 mm. The distance L c between the centers of adjacent coupling slots is 0.5λ gf , the distance between the terminal coupling slots and the end face of the waveguide is 0.5λ gf , and λ gf is the wavelength of the feed waveguide. The coupling slit couples the excitation into the radiation waveguide. The radiation waveguide is located at the upper end of the coupling waveguide. A radiation slit is opened on the upper surface of the radiation waveguide. The radiation slit cuts off the current on the upper surface of the radiation waveguide. The excitation is obtained at the mouth of the radiation slit and radiates energy outward to form a waveguide slit. antenna array. The radiation slot adopts array element waveguide slot array, the amplitude is Taylor distribution, the length of each radiation slot is 3.87mm, the width is 1.5mm, and the thickness is 0.4mm. The distance L r between the lateral centers of adjacent radiation slots is λ gr , and the distance between the longitudinal centers depends on the focus position, as shown in Figure 9, which is the normalized field strength simulation diagram in the transmission direction of the longitudinal axis when the focus position of the embodiment is 50 mm. The focus position of 50 mm determines the distance between the longitudinal centers of the radiation slits. The distance between the radiation slots at the four corners of the terminal and the end face of the waveguide terminal is 0.5λ gr , where λ gr is the wavelength of the radiation waveguide. Both the feed waveguide wavelength and the radiating waveguide wavelength are given above.

本发明将图4所示金属边界用于一般的馈电波导改进为图5中等效PMC边界应用于本发明中的馈电金属波导。由于四角馈电波导等幅同相馈电的特殊性,磁流线6在图5馈电波导中的分布表现出磁力线与等效PMC(理想磁导体)8垂直,因此可用PMC边界取代金属边界7,降低加工成本,提高辐射效率。In the present invention, the metal boundary shown in FIG. 4 is used for the general feeder waveguide, and the equivalent PMC boundary in FIG. 5 is applied to the feeder metal waveguide in the present invention. Due to the particularity of the four-corner feed waveguide equal-amplitude and in-phase feed, the distribution of the magnetic flow lines 6 in the feed waveguide in Figure 5 shows that the magnetic force lines are perpendicular to the equivalent PMC (ideal magnetic conductor) 8, so the metal boundary 7 can be replaced by the PMC boundary , reduce processing costs and improve radiation efficiency.

本发明将图6所示金属边界用于一般的天线辐射波导改进为图7中等效PEC边界应用于本发明中的辐射金属波导。由于辐射波导结构对称性,在辐射波导中央形成的等效PEC(理想电导体)边界10可以代替金属边界9,降低加工难度,节约成本。In the present invention, the metal boundary shown in FIG. 6 is used for the general antenna radiation waveguide, and the equivalent PEC boundary shown in FIG. 7 is applied to the radiation metal waveguide of the present invention. Due to the symmetry of the radiation waveguide structure, the equivalent PEC (Perfect Electric Conductor) boundary 10 formed in the center of the radiation waveguide can replace the metal boundary 9, which reduces processing difficulty and saves cost.

利用本发明的一种具体实施方式为:设计馈电网络时包括馈电端口,T形馈电波导。在馈电网络中,需要将T形馈电波导45°弯曲,如图2延伸到整个平面,并在馈电波导上表面开图2所示耦合缝隙,形成耦合阵列。设计辐射波导如图3,辐射缝隙需按照所给参数以及聚焦位置设计。馈电波导和辐射波导设计完毕后将两者粘合,整个结构需使用5层蚀刻金属板,所有的蚀刻金属板用针脚固定和对准以粘合在一起。此外,在结构的中心和外围可另加螺钉,以便用来固定在无线终端上。生产时考虑到结构紧凑,若空间有限,位于天线中心的辐射缝隙可以替换成螺钉通孔,但这样会影响到天线整体特性。对此,在生产时可加宽通孔周围的局部缝隙间距,以便分配通孔,这样既不需要用通孔来替代中心缝隙,辐射也能保持相对稳定。A specific implementation manner of utilizing the present invention is as follows: when designing the feed network, the feed port and the T-shaped feed waveguide are included. In the feeding network, it is necessary to bend the T-shaped feeding waveguide by 45°, extending to the entire plane as shown in Figure 2, and open the coupling slot shown in Figure 2 on the upper surface of the feeding waveguide to form a coupling array. The design of the radiation waveguide is shown in Figure 3, and the radiation slot needs to be designed according to the given parameters and focus position. After the feeding waveguide and radiation waveguide are designed, the two are bonded. The whole structure needs to use 5 layers of etched metal plates, and all the etched metal plates are fixed and aligned with pins to be bonded together. In addition, additional screws can be added at the center and periphery of the structure for fixing to the wireless terminal. Considering the compact structure during production, if the space is limited, the radiation slot at the center of the antenna can be replaced with a screw through hole, but this will affect the overall characteristics of the antenna. In this regard, the local gap spacing around the through hole can be widened during production to distribute the through hole, so that there is no need to replace the central gap with a through hole, and the radiation can remain relatively stable.

如用基于有限元法的电磁仿真模拟器ANSYS HFSS用于天线的仿真,耦合波导和辐射波导需要分别仿真,注意如下:(1)调节单个谐振式辐射缝隙与单根波导中心轴线的偏移使得其耦合因子与图8相同。(2)单个辐射缝隙设计完成后,通过聚焦点计算相位分布,确定辐射缝隙中心纵向间距,然后将辐射缝隙排布成阵列。(3)耦合缝的设计中耦合因子的大小由耦合缝与波导中轴线的偏转角度来控制。If the electromagnetic simulation simulator ANSYS HFSS based on the finite element method is used for the simulation of the antenna, the coupling waveguide and the radiation waveguide need to be simulated separately, and the attention is as follows: (1) Adjust the offset of the single resonant radiation slot and the central axis of the single waveguide so that Its coupling factor is the same as in Figure 8. (2) After the design of a single radiation slot is completed, the phase distribution is calculated through the focal point to determine the longitudinal distance between the centers of the radiation slots, and then the radiation slots are arranged into an array. (3) The size of the coupling factor in the design of the coupling slot is controlled by the deflection angle between the coupling slot and the central axis of the waveguide.

本发明公开一种基于四角馈电的双层波导缝隙近场聚焦阵列天线的设计及基于对称馈电实现等效的PMC(理想磁导体)与PEC(理想电导体)终端边界条件,涉及一种波导缝隙天线的设计及馈电结构。本发明的波导缝隙阵列天线采用四角馈电,区别于传统的中心馈电或简单的一端馈电,易于实现泰勒分布并保持良好的带宽特性。等幅同相的对称馈电结构在馈电网络中央实现等效PMC终端,在缩短终端位置的基础上改善了传统PEC终端造成的对天线辐射特性的不良影响;另外,等幅同相馈电在辐射波导的中央实现等效PEC终端,进一步降低天线加工难度和成本。该天线聚焦在近场,在工作频率范围内回波损耗小、旁瓣抑制高、隔离度高、加工难度与成本低,具有广泛的应用价值。The invention discloses the design of a double-layer waveguide slot near-field focusing array antenna based on four-corner feeding and the realization of equivalent PMC (ideal magnetic conductor) and PEC (ideal electric conductor) terminal boundary conditions based on symmetrical feeding, and relates to a Design and feeding structure of waveguide slot antenna. The waveguide slot array antenna of the present invention adopts four-corner feeding, which is different from traditional central feeding or simple one-end feeding, and is easy to realize Taylor distribution and maintain good bandwidth characteristics. The symmetrical feed structure with equal amplitude and same phase realizes the equivalent PMC terminal in the center of the feed network, and improves the adverse effect on the radiation characteristics of the antenna caused by the traditional PEC terminal on the basis of shortening the terminal position; The center of the waveguide implements an equivalent PEC terminal, which further reduces the difficulty and cost of antenna processing. The antenna focuses on the near field, has small return loss, high sidelobe suppression, high isolation, low processing difficulty and low cost in the working frequency range, and has wide application value.

Claims (9)

1.一种基于四角馈电的双层波导缝隙近场聚焦阵列天线,其特征在于由下层的馈电波导和上层的辐射波导组成;入射波从馈电端口依次经过馈电波导、耦合缝隙、辐射波导,最终由辐射缝隙辐射到外部空间。1. A double-layer waveguide slot near-field focusing array antenna based on quadrangular feeding is characterized in that it is made up of a feeding waveguide of the lower floor and a radiation waveguide of the upper floor; the incident wave passes through the feeding waveguide, coupling slot, The radiation waveguide finally radiates to the outer space through the radiation slot. 2.如权利要求1所述一种基于四角馈电的双层波导缝隙近场聚焦阵列天线,其特征在于所述馈电端口和馈电波导采用标准馈电波导从背面通过中央孔径馈入,采用四角馈电代替中心馈电,通过具有4个臂的馈电波导将信号从中心延伸到4个天线角,由两端向中间等幅同向馈电,在馈电波导中央能形成PMC边界。2. A double-layer waveguide slot near-field focusing array antenna based on four-corner feeding as claimed in claim 1, wherein the feeding port and the feeding waveguide adopt a standard feeding waveguide to feed in from the back through the central aperture, The four-corner feed is used instead of the center feed, and the signal is extended from the center to the four antenna angles through the feed waveguide with 4 arms, and the two ends are fed to the middle with equal amplitude and the same direction, and a PMC boundary can be formed in the center of the feed waveguide . 3.如权利要求1所述一种基于四角馈电的双层波导缝隙近场聚焦阵列天线,其特征在于馈电波导的长度为44.8mm,宽度为5mm,高度为2mm。3. A double-layer waveguide slot near-field focusing array antenna based on four-corner feeding as claimed in claim 1, wherein the length of the feeding waveguide is 44.8mm, the width is 5mm, and the height is 2mm. 4.如权利要求1所述一种基于四角馈电的双层波导缝隙近场聚焦阵列天线,其特征在于所述耦合缝隙为同相馈电方式,耦合缝隙开于馈电波导上表面,耦合缝隙数目为2×8。4. A kind of double-layer waveguide slot near-field focusing array antenna based on quadrangular feeding as claimed in claim 1, characterized in that the coupling slot is an in-phase feeding mode, the coupling slot is opened on the upper surface of the feeding waveguide, and the coupling slot The number is 2×8. 5.如权利要求1所述一种基于四角馈电的双层波导缝隙近场聚焦阵列天线,其特征在于所述耦合缝隙的一维泰勒分布由耦合缝隙的偏转角控制,耦合缝隙的长度为3.75mm,宽度为1mm,厚度为0.4mm。5. a kind of double-layer waveguide slot near-field focusing array antenna based on quadrangular feeding as claimed in claim 1, it is characterized in that the one-dimensional Taylor distribution of the coupling slot is controlled by the deflection angle of the coupling slot, and the length of the coupling slot is 3.75mm, width 1mm, thickness 0.4mm. 6.如权利要求1所述一种基于四角馈电的双层波导缝隙近场聚焦阵列天线,其特征在于所述相邻耦合缝隙之间的间距Lc为0.5λgf,终端耦合缝隙距离波导终端端面的距离为0.5λgf,λgf为馈电波导波长。6. A kind of double-layer waveguide slot near-field focusing array antenna based on four-corner feeding as claimed in claim 1, characterized in that the distance L c between the adjacent coupling slots is 0.5λgf , and the distance between the terminal coupling slots and the waveguide The distance between the terminal end faces is 0.5λ gf , where λ gf is the wavelength of the feeding waveguide. 7.如权利要求1所述一种基于四角馈电的双层波导缝隙近场聚焦阵列天线,其特征在于所述辐射波导置于下层的馈电波导上部,采用馈电波导上表面所开耦合缝隙同相馈电,长度为42.8mm,宽度为5.2mm,高度为2mm;在辐射波导中央水平方向能等效成PEC终端。7. A double-layer waveguide slot near-field focusing array antenna based on four-corner feeding as claimed in claim 1, wherein the radiation waveguide is placed on the upper part of the feed waveguide of the lower layer, and is coupled by the upper surface of the feed waveguide. The slot is fed in the same phase, the length is 42.8mm, the width is 5.2mm, and the height is 2mm; it can be equivalent to a PEC terminal in the horizontal direction in the center of the radiation waveguide. 8.如权利要求1所述一种基于四角馈电的双层波导缝隙近场聚焦阵列天线,其特征在于所述辐射缝隙采用波导缝隙阵列,辐射缝隙开于辐射波导上表面,由聚焦位置计算其相位,幅度为泰勒分布,辐射缝隙数目为8×8,每个辐射缝隙的长度为3.87mm,宽度为1.5mm,厚度为0.4mm。8. A double-layer waveguide slot near-field focusing array antenna based on four-corner feeding as claimed in claim 1, wherein the radiation slot adopts a waveguide slot array, and the radiation slot is opened on the upper surface of the radiation waveguide, calculated by the focus position Its phase and amplitude are Taylor distributed, the number of radiation slots is 8×8, the length of each radiation slot is 3.87mm, the width is 1.5mm, and the thickness is 0.4mm. 9.如权利要求1所述一种基于四角馈电的双层波导缝隙近场聚焦阵列天线,其特征在于所述相邻辐射缝横向之间的间距Lr为λg,纵向之间的间距取决于所需聚焦位置,终端四角辐射缝隙中心距离波导上下终端面的距离为0.5λgr,λgr为辐射波导波长。9. A kind of double-layer waveguide slot near-field focusing array antenna based on quadrangular feed as claimed in claim 1, is characterized in that the spacing L r between the horizontal direction of the adjacent radiation slots is λ g , and the vertical spacing Depending on the required focusing position, the distance between the center of the radiation slot at the four corners of the terminal and the upper and lower terminal surfaces of the waveguide is 0.5λ gr , where λ gr is the wavelength of the radiation waveguide.
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CN108902650A (en) * 2018-08-22 2018-11-30 江苏麦克威微波技术有限公司 A kind of microwave thawing equipment
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