CN106229635B - A kind of omnidirectional's dual circularly polarized antenna of ipsilateral feed - Google Patents
A kind of omnidirectional's dual circularly polarized antenna of ipsilateral feed Download PDFInfo
- Publication number
- CN106229635B CN106229635B CN201610634955.1A CN201610634955A CN106229635B CN 106229635 B CN106229635 B CN 106229635B CN 201610634955 A CN201610634955 A CN 201610634955A CN 106229635 B CN106229635 B CN 106229635B
- Authority
- CN
- China
- Prior art keywords
- impedance matching
- matching structure
- coaxial
- inner conductor
- radiation
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Active
Links
- 230000009977 dual effect Effects 0.000 title claims abstract description 17
- 230000003447 ipsilateral effect Effects 0.000 title 1
- 230000005855 radiation Effects 0.000 claims abstract description 30
- 230000005284 excitation Effects 0.000 claims abstract description 29
- 238000006243 chemical reaction Methods 0.000 claims abstract description 22
- 239000002184 metal Substances 0.000 claims abstract description 16
- 239000004020 conductor Substances 0.000 claims description 68
- 230000010287 polarization Effects 0.000 description 17
- 238000010586 diagram Methods 0.000 description 6
- 238000002955 isolation Methods 0.000 description 4
- 238000004088 simulation Methods 0.000 description 3
- 239000004809 Teflon Substances 0.000 description 2
- 229920006362 Teflon® Polymers 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 2
- 238000013332 literature search Methods 0.000 description 2
- 238000003491 array Methods 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q1/00—Details of, or arrangements associated with, antennas
- H01Q1/36—Structural form of radiating elements, e.g. cone, spiral, umbrella; Particular materials used therewith
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q5/00—Arrangements for simultaneous operation of antennas on two or more different wavebands, e.g. dual-band or multi-band arrangements
- H01Q5/20—Arrangements for simultaneous operation of antennas on two or more different wavebands, e.g. dual-band or multi-band arrangements characterised by the operating wavebands
- H01Q5/28—Arrangements for establishing polarisation or beam width over two or more different wavebands
Landscapes
- Waveguide Aerials (AREA)
- Variable-Direction Aerials And Aerial Arrays (AREA)
Abstract
本发明提供了一种同侧馈电的全向双圆极化天线,包括:辐射结构、类同轴阻抗匹配结构、射频激励转换T型连接结构,所述类同轴阻抗匹配结构分为上类同轴阻抗匹配结构和下类同轴阻抗匹配结构,所述辐射结构的上、下端分别连接上类同轴阻抗匹配结构的下端和下类同轴阻抗匹配结构的上端,上类同轴阻抗匹配结构的上端用金属圆片封闭,下类同轴阻抗匹配结构的下端连接射频激励转换T型连接结构,射频激励转换T型连接结构的接口能够直接采用SMA接头馈线进行射频激励。本发明全向性能以及轴比性能良好,具有一定工作带宽,‑10dB带宽600M(5.2GHz‑5.8GHz),带内增益大于5.2dB,最高达6.7dB。
The present invention provides an omnidirectional dual circularly polarized antenna fed from the same side, comprising: a radiation structure, a coaxial-like impedance matching structure, and a radio frequency excitation switching T-shaped connection structure, and the coaxial-like impedance matching structure is divided into the following A similar coaxial impedance matching structure and a lower coaxial impedance matching structure, the upper and lower ends of the radiation structure are respectively connected to the lower end of the upper coaxial impedance matching structure and the upper end of the lower coaxial impedance matching structure, the upper coaxial impedance The upper end of the matching structure is closed with a metal disc, and the lower end of the coaxial impedance matching structure is connected to the RF excitation conversion T-connection structure. The interface of the RF excitation conversion T-connection structure can directly use the SMA connector feeder for RF excitation. The present invention has good omnidirectional performance and axial ratio performance, and has a certain working bandwidth, a -10dB bandwidth of 600M (5.2GHz-5.8GHz), and an in-band gain greater than 5.2dB, up to 6.7dB.
Description
技术领域technical field
本发明涉及一种天线,具体地,涉及一种同侧馈电实现全向双圆极化的天线。The present invention relates to an antenna, in particular to an antenna capable of realizing omnidirectional dual circular polarization by feeding on the same side.
背景技术Background technique
圆极化天线由于其可以接收、发射任意极化来波的特性而得到越来越广泛的应用。在很多应用场景中,接收、发射的信号来自四面八方,为了能较好得处理这些信号,必须实现全向的圆极化性能。但是由于全向所带来的增益下降较为明显。Circularly polarized antennas are more and more widely used because of their ability to receive and transmit incoming waves with arbitrary polarization. In many application scenarios, received and transmitted signals come from all directions. In order to better handle these signals, omnidirectional circular polarization performance must be achieved. However, the gain reduction due to omnidirectional is more obvious.
经文献检索,Dan Yu,Shu-Xi Gong等人2014年在IEEE Trans.Antennas Propag.期刊上发表的文章“Wideband Omnidirectional Circularly Polarized Patch AntennaBased on Vortex Slots and Shorting Vias”提出了一种全向圆极化天线,虽然10dB阻抗带宽达到51.7%,3dB轴比带宽也达到了57.8%,但带内增益不到2dBic。After literature search, the article "Wideband Omnidirectional Circularly Polarized Patch AntennaBased on Vortex Slots and Shorting Vias" published in IEEE Trans.Antennas Propag. in 2014 by Dan Yu, Shu-Xi Gong et al. proposed an omnidirectional circularly polarized For the antenna, although the 10dB impedance bandwidth reaches 51.7%, and the 3dB axial ratio bandwidth also reaches 57.8%, the in-band gain is less than 2dBic.
此外,即使能实现较高的全向增益和双圆极化特性,能否保证双圆极化之间不相互干扰也是一个问题。经文献搜索,Zhou Bin,Junping Geng等人2015年发表在International Journal of Antennas and Propagation期刊上的文章“Dual CircularlyPolarized Omnidirectional Antenna with Slot Array on Coaxial Cylinder”提出了一种全向双圆极化天线,虽然在频带内实现了5dBic左右的增益和良好的圆极化特性,但是由于其左右旋圆极化馈电端口分布在天线的两端,如果天线要实现水平全向圆极化,天线竖直放置时下端馈电口用线缆连接较为方便,但上端馈电端口所接线缆的下垂部分必定会对辐射方向图造成影响,从而破环天线的圆极化特性,导致天线需要实现不同圆极化时需要重新安装,给使用者带来不便。In addition, even if a high omnidirectional gain and dual circular polarization characteristics can be achieved, it is still a problem to ensure that the dual circular polarizations do not interfere with each other. After literature search, the article "Dual Circularly Polarized Omnidirectional Antenna with Slot Array on Coaxial Cylinder" published by Zhou Bin, Junping Geng and others in the International Journal of Antennas and Propagation in 2015 proposed an omnidirectional dual circularly polarized antenna, although In the frequency band, the gain of about 5dBic and good circular polarization characteristics are realized. However, since the left and right circular polarization feed ports are distributed at both ends of the antenna, if the antenna wants to achieve horizontal omnidirectional circular polarization, the antenna must be placed vertically. At present, it is more convenient to use a cable to connect the lower feeder port, but the drooping part of the cable connected to the upper feeder port will definitely affect the radiation pattern, thus destroying the circular polarization characteristics of the loop antenna, resulting in the antenna needing to implement different circular poles. It needs to be reinstalled when upgrading, which brings inconvenience to users.
发明内容Contents of the invention
针对现有技术中的缺陷,本发明的目的是提供一种具有一定工作带宽的的全向双圆极化天线。该天线-10dB带宽达到10.9%,并且在整个带宽内水平全向轴比小于3dB,带内水平全向增益大于5.2dB,最高增益达6.7dB。In view of the defects in the prior art, the object of the present invention is to provide an omnidirectional dual circularly polarized antenna with a certain working bandwidth. The -10dB bandwidth of the antenna reaches 10.9%, and the horizontal omnidirectional axial ratio within the entire bandwidth is less than 3dB, the horizontal omnidirectional gain in the band is greater than 5.2dB, and the highest gain reaches 6.7dB.
为达到上述目的,本发明所采用的技术方案如下:In order to achieve the above object, the technical scheme adopted in the present invention is as follows:
一种同侧馈电的全向双圆极化天线,包括:辐射结构、类同轴阻抗匹配结构、射频激励转换T型连接结构,所述类同轴阻抗匹配结构分为上类同轴阻抗匹配结构和下类同轴阻抗匹配结构,所述辐射结构的上、下端分别连接上类同轴阻抗匹配结构的下端和下类同轴阻抗匹配结构的上端,上类同轴阻抗匹配结构的上端用金属圆片封闭,下类同轴阻抗匹配结构的下端连接射频激励转换T型连接结构,射频激励转换T型连接结构的接口能够直接采用SMA接头馈线进行射频激励。An omnidirectional dual circularly polarized antenna fed from the same side, comprising: a radiation structure, a coaxial-like impedance matching structure, and a radio frequency excitation conversion T-shaped connection structure, and the coaxial-like impedance matching structure is divided into the above-mentioned coaxial impedance matching structure A matching structure and a lower-type coaxial impedance matching structure, the upper and lower ends of the radiation structure are respectively connected to the lower end of the upper-type coaxial impedance matching structure and the upper end of the lower-type coaxial impedance matching structure, and the upper end of the upper-type coaxial impedance matching structure Closed with a metal disc, the lower end of the lower coaxial impedance matching structure is connected to the RF excitation conversion T-connection structure, and the interface of the RF excitation conversion T-connection structure can directly use the SMA connector feeder for RF excitation.
所述辐射结构包括辐射结构内导体、辐射结构外导体、内芯,均为金属圆柱,内芯顶端与金属圆片相连,辐射结构内导体与辐射结构顶端之间隔开一定距离以提供能量流入/流出的通道。The radiating structure includes an inner conductor of the radiating structure, an outer conductor of the radiating structure, and an inner core, all of which are metal cylinders, the top of the inner core is connected to the metal disc, and a certain distance is separated between the inner conductor of the radiating structure and the top of the radiating structure to provide energy inflow/ outflow channel.
所述辐射结构内导体与外导体之间、辐射结构内导体与内芯之间填充介质。A medium is filled between the inner conductor and the outer conductor of the radiating structure, and between the inner conductor and the inner core of the radiating structure.
所述辐射结构外壁开设有两两互成90度的矩形缝隙,The outer wall of the radiation structure is provided with two rectangular gaps forming 90 degrees to each other,
所述缝隙绕辐射结构外壁的一周开设多个,上下多组向外辐射电磁波。A plurality of said slits are opened around the outer wall of the radiation structure, and the upper and lower groups radiate electromagnetic waves outward.
所述类同轴阻抗匹配结构包括匹配结构内导体、介质、匹配结构外导体,所述匹配结构内导体为多小段外径和长短各不同的金属圆柱。The quasi-coaxial impedance matching structure includes a matching structure inner conductor, a medium, and a matching structure outer conductor, and the matching structure inner conductor is a plurality of metal cylinders with different outer diameters and lengths.
所述匹配结构内导体与外导体之间填充介质。A medium is filled between the inner conductor and the outer conductor of the matching structure.
所述射频激励转换连接T型结构有两个端口,其中下馈端口通有射频激励转换连接T型结构内导体与内芯;侧馈端口内芯与下馈端口的射频激励转换连接T型结构内导体连接,侧馈端口整体为渐变同轴线结构,两个端口都能与标准SMA头连接。The radio frequency excitation conversion connection T-shaped structure has two ports, wherein the feed-down port is connected to the inner conductor and the inner core of the radio frequency excitation conversion connection T-shaped structure; The inner conductor is connected, and the side feed port is a gradual coaxial line structure as a whole, and both ports can be connected to standard SMA heads.
所述天线从T型连接结构从下馈端口馈电,能量从内芯和内导体之间的介质中向上传播至内导体和外导体之间的介质部分(由于内导体不与顶部金属圆片连接,使内外层介质之间联通),再向下边传播边通过缝隙辐射,实现左旋圆极化。从T型连接结构侧馈端口馈电,能量从渐变同轴线传输进入内外导体间的介质中,一边向上传播,一边从缝隙辐射能量,实现右旋圆极化。The antenna is fed from the lower feed port from the T-shaped connection structure, and the energy propagates upward from the medium between the inner core and the inner conductor to the medium part between the inner conductor and the outer conductor (because the inner conductor is not connected to the top metal disc connection, so that the inner and outer media are connected), and then propagate downwards while radiating through the gap to realize left-handed circular polarization. Feed from the side-feed port of the T-shaped connection structure, the energy is transmitted from the tapered coaxial line into the medium between the inner and outer conductors, and propagates upward while radiating energy from the gap to realize right-handed circular polarization.
与现有技术相比,本发明具有如下的有益效果:Compared with the prior art, the present invention has the following beneficial effects:
1、本发明全向双圆极化天线效率较高,两端口间隔离度较好,因而具有较高的增益。1. The omnidirectional dual circularly polarized antenna of the present invention has higher efficiency and better isolation between two ports, thus having higher gain.
2、本发明全向性能好。2. The present invention has good omnidirectional performance.
3、本发明具有较宽的-10dB带宽10.9%。3. The present invention has a wider -10dB bandwidth of 10.9%.
4、本发明的T型连接结构的下馈端口与侧馈端口可以直接连SMA头,方便连接使用。4. The down-feed port and side-feed port of the T-shaped connection structure of the present invention can be directly connected to the SMA head, which is convenient for connection and use.
5、本发明T型连接结构两个馈电点距离较近而隔离较好,可以根据需要方便得实现左右旋圆极化。避免了馈电点在天线两头而有可能造成的同时工作时对圆极化性能的影响。5. The distance between the two feed points of the T-shaped connection structure of the present invention is relatively close and the isolation is good, and the left and right circular polarization can be conveniently realized according to the needs. It avoids the impact on the circular polarization performance caused by the feed point at both ends of the antenna which may cause simultaneous operation.
附图说明Description of drawings
通过阅读参照以下附图对非限制性实施例所作的详细描述,本发明的其它特征、目的和优点将会变得更明显:Other characteristics, objects and advantages of the present invention will become more apparent by reading the detailed description of non-limiting embodiments made with reference to the following drawings:
图1为本发明全向双圆极化天线的结构示意图;Fig. 1 is the structural representation of omnidirectional dual circularly polarized antenna of the present invention;
图2是图1的分解图;Figure 2 is an exploded view of Figure 1;
图3为图1沿A-A的剖视图;Fig. 3 is a sectional view along A-A of Fig. 1;
图4是图1沿B-B的剖视图;Fig. 4 is a sectional view along B-B of Fig. 1;
图5为本发明实施例的全向双圆极化天线的回波损耗图;5 is a return loss diagram of an omnidirectional dual circularly polarized antenna according to an embodiment of the present invention;
图6为本发明实施例的5.2GHz、5.5GHz、5.8GHz之间三个频点的水平全向轴比图;FIG. 6 is a horizontal omnidirectional axial ratio diagram of three frequency points between 5.2GHz, 5.5GHz, and 5.8GHz according to an embodiment of the present invention;
图7为本发明实施例的5.2GHz、5.5GHz、5.8GHz之间三个频点的水平全向增益图。FIG. 7 is a horizontal omnidirectional gain diagram of three frequency points between 5.2GHz, 5.5GHz and 5.8GHz according to an embodiment of the present invention.
图中:1为天线的辐射结构,2为天线类同轴阻抗匹配结构,3为射频激励转换T型连接结构,4为其中一组辐射单元的上下缝隙,5为辐射缝隙阵列,6为天线辐射结构外导体,7为天线辐射结构填充介质(包括外导体与内导体之间的介质和内导体与内芯之间的介质),8为天线辐射结构内导体,9为射频激励转换T型连接结构外导体,10为射频激励转换T型连接结构填充介质,11为射频激励转换T型连接结构内导体,12为射频激励转换T型连接结构下馈端口,13为射频激励转换T型连接结构侧馈端口,14为上匹配结构内导体,15为下匹配结构内导体。In the figure: 1 is the radiation structure of the antenna, 2 is the coaxial impedance matching structure of the antenna, 3 is the RF excitation conversion T-shaped connection structure, 4 is the upper and lower slots of one group of radiation units, 5 is the radiation slot array, and 6 is the antenna The outer conductor of the radiation structure, 7 is the filling medium of the antenna radiation structure (including the medium between the outer conductor and the inner conductor and the medium between the inner conductor and the inner core), 8 is the inner conductor of the antenna radiation structure, and 9 is the radio frequency excitation conversion T-type The outer conductor of the connection structure, 10 is the filling medium of the radio frequency excitation conversion T-shaped connection structure, 11 is the inner conductor of the radio frequency excitation conversion T-shaped connection structure, 12 is the downfeed port of the radio frequency excitation conversion T-shaped connection structure, and 13 is the radio frequency excitation conversion T-shaped connection Structure side feed port, 14 is the inner conductor of the upper matching structure, and 15 is the inner conductor of the lower matching structure.
具体实施方式Detailed ways
下面结合具体实施例对本发明进行详细说明。以下实施例将有助于本领域的技术人员进一步理解本发明,但不以任何形式限制本发明。应当指出的是,对本领域的普通技术人员来说,在不脱离本发明构思的前提下,还可以做出若干变化和改进。这些都属于本发明的保护范围。The present invention will be described in detail below in conjunction with specific embodiments. The following examples will help those skilled in the art to further understand the present invention, but do not limit the present invention in any form. It should be noted that those skilled in the art can make several changes and improvements without departing from the concept of the present invention. These all belong to the protection scope of the present invention.
请同时参阅图1~图4,本发明所提供的同侧馈电的全向双圆极化天线,包括:1、天线辐射结构,2、类同轴阻抗匹配结构,3、射频激励转换T型连接结构。上类同轴阻抗匹配结构上端用金属圆片封闭,下端接天线辐射结构。天线辐射结构下端再接下类同轴匹配结构。下类同轴匹配结构下端接射频激励转换T型连接结构。射频激励转换T型连接结构下端、侧端可直接采用SMA接头馈线进行射频激励。Please refer to Figs. 1 to 4 at the same time, the omnidirectional dual circularly polarized antenna provided by the present invention includes: 1, antenna radiation structure, 2, similar coaxial impedance matching structure, 3, radio frequency excitation conversion T type connection structure. The upper end of the above-mentioned coaxial impedance matching structure is closed with a metal disc, and the lower end is connected to the antenna radiation structure. The lower end of the antenna radiation structure is connected with a similar coaxial matching structure. The following type of coaxial matching structure is terminated with a radio frequency excitation conversion T-shaped connection structure. The lower end and side end of the RF excitation conversion T-shaped connection structure can directly use the SMA connector feeder for RF excitation.
进一步地,天线辐射结构1为类(似)双同轴线结构,辐射结构面外导体6为金属,厚度1.5mm,直径25mm,长度150.9mm,在辐射结构面外导体6上开互相垂直(夹角90度)的矩形缝隙4,一周4个,上下4组构成辐射缝隙阵。8为天线辐射结构内导体,直径1.5mm,与外导体等长度相等,内外导体之间填充介质7,该介质为Teflon,介电常数为2.1。内芯半径为0.46mm,长度与外导体相等。Further, the antenna radiation structure 1 is a similar (similar) dual-coax structure, and the outer conductor 6 of the radiation structure is metal, with a thickness of 1.5 mm, a diameter of 25 mm, and a length of 150.9 mm. There are 4 rectangular slits with an included angle of 90 degrees), 4 in a week, and 4 groups up and down to form a radiation slit array. 8 is the inner conductor of the antenna radiation structure, with a diameter of 1.5 mm and the same length as the outer conductor, and a medium 7 is filled between the inner and outer conductors. The medium is Teflon with a dielectric constant of 2.1. The radius of the inner core is 0.46mm and the length is equal to that of the outer conductor.
进一步地,在辐射结构1上下面都直接连接类(似)同轴阻抗匹配结构2,匹配结构外导体与辐射结构外导体6、内芯、内导体等连接。上、下类同轴阻抗匹配结构的上匹配结构内导体14和下匹配结构内导体15均为三段直径不同的金属圆柱,内径等于内导体外径,上类同轴阻抗匹配结构的3个作为匹配结构内导体的金属环直径分别为3.7mm、6.0mm、6.5mm,长度分别为7.9mm、6.0mm、6.5mm;下类同轴阻抗匹配结构的3个金属圆环直径分别为3.2mm、7.4mm、6.9mm,长度分别为8.1mm、5.5mm、8.1mm,它们直接相连,以传输线理论实现阻抗变换。匹配结构内导体与外导体之间填充介质10为Teflon。Further, the coaxial-like (similar) impedance matching structure 2 is directly connected to the upper and lower sides of the radiating structure 1, and the outer conductor of the matching structure is connected to the outer conductor 6, the inner core, and the inner conductor of the radiating structure. The inner conductor 14 of the upper matching structure and the inner conductor 15 of the lower matching structure of the upper and lower coaxial impedance matching structures are three sections of metal cylinders with different diameters, and the inner diameter is equal to the outer diameter of the inner conductor. The diameters of the metal rings used as the internal conductors of the matching structure are 3.7mm, 6.0mm, and 6.5mm, and the lengths are 7.9mm, 6.0mm, and 6.5mm respectively; the diameters of the three metal rings of the lower coaxial impedance matching structure are 3.2mm. , 7.4mm, 6.9mm, and the lengths are 8.1mm, 5.5mm, and 8.1mm respectively. They are directly connected, and the impedance transformation is realized by the transmission line theory. The filling medium 10 between the inner conductor and the outer conductor of the matching structure is Teflon.
进一步地,在下类同轴阻抗匹配结构下面连接射频激励转换T型连接结构3,下类同轴阻抗匹配结构外导体与T型头下端圆柱形接头通过渐变的结构连接,厚度与类同轴阻抗匹配结构外导体相同。T型头下端圆柱形接头内含的外导体9与内芯内径厚度均与辐射结构、类同轴阻抗匹配结构中的相同。T型头侧边的接头是渐变同轴线结构,内芯与T型头下端接头内的外导体9连接,直径与外导体相同,再渐变到标准的SMA接口。T型头下端接头和侧端接头均可以直接与SMA接头连接。Further, the RF excitation conversion T-shaped connection structure 3 is connected under the coaxial impedance matching structure of the following type, the outer conductor of the coaxial impedance matching structure of the following type is connected with the cylindrical joint at the lower end of the T-shaped head through a gradual structure, and the thickness is similar to the coaxial impedance The outer conductor of the matching structure is the same. The outer conductor 9 contained in the cylindrical joint at the lower end of the T-shaped head and the thickness of the inner diameter of the inner core are the same as those in the radial structure and the quasi-coaxial impedance matching structure. The joint on the side of the T-shaped head is a gradual coaxial cable structure, and the inner core is connected to the outer conductor 9 in the lower end of the T-shaped head. The diameter is the same as that of the outer conductor, and then gradually changes to a standard SMA interface. Both the lower end connector and the side end connector of the T-shaped head can be directly connected with the SMA connector.
本发明全向双圆极化的工作原理如下:The working principle of the omnidirectional dual circular polarization of the present invention is as follows:
如图1~图4所示,本发明所提供的同侧馈电的全向双圆极化天线,从射频激励转换T型连接结构的下馈端口和侧馈端口分别激励可以分别实现左旋和右旋的圆极化性能。天线从T型连接结构的下馈端口馈电,能量从内芯和内导体之间的介质中向上传播至内导体和外导体之间的介质部分(由于内导体不与顶部金属圆片连接,使内外层介质之间联通),再向下边传播边通过缝隙辐射,实现左旋圆极化。从T型连接结构侧馈端口馈电,能量从渐变同轴线传输进入内外导体间的介质中,一边向上传播,一边从缝隙辐射能量,实现右旋圆极化。As shown in Figures 1 to 4, the omnidirectional dual circularly polarized antenna provided by the present invention can realize left-handed and Right-handed circular polarization properties. The antenna is fed from the feed-down port of the T-shaped connection structure, and the energy propagates upward from the medium between the inner core and the inner conductor to the medium part between the inner conductor and the outer conductor (because the inner conductor is not connected to the top metal disc, Make communication between the inner and outer media), and then propagate downwards while radiating through the gap to realize left-handed circular polarization. Feed from the side-feed port of the T-shaped connection structure, the energy is transmitted from the tapered coaxial line into the medium between the inner and outer conductors, and propagates upward while radiating energy from the gap to realize right-handed circular polarization.
具体如图4所示,射频激励信号通过图4中下馈端口12对天线馈电,信号先通过内芯和射频激励转换T型连接结构内导体11及它们之间的介质10组成的类同轴线结构向上传播,到达天线顶部后向外扩散,开始沿内导体、外导体和它们之间的介质组成的类同轴线结构向下传播。由于内外类同轴结构阻抗有所失配,先经过上类同轴阻抗匹配结构,使得S11在5.2GHz-5.8GHz范围内小于-10dB,实现阻抗匹配。信号从辐射结构1上的缝隙阵列向外辐射,从而有较高增益。能量从第一个缝隙开始向外辐射,到第四个缝隙处已经很少,这样只有很少能量进入T型结构侧馈端口,从而使两个端口的隔离度较好。若需要实现更高的增益,可以适当增加辐射缝隙的数目。Specifically as shown in Figure 4, the RF excitation signal is fed to the antenna through the feed-down port 12 in Figure 4, and the signal first passes through the inner core and the RF excitation conversion T-shaped connection structure inner conductor 11 and the medium 10 between them. The axial structure propagates upwards, spreads outward after reaching the top of the antenna, and starts to propagate downward along the coaxial structure composed of inner conductor, outer conductor and the medium between them. Due to the impedance mismatch between the internal and external coaxial structures, the impedance matching structure of the above coaxial structure is first used to make the S11 less than -10dB in the range of 5.2GHz-5.8GHz to achieve impedance matching. The signal is radiated outward from the slot array on the radiation structure 1, so that there is a higher gain. The energy starts to radiate outward from the first slot, and there is very little energy at the fourth slot, so that only a little energy enters the T-shaped structure side feed port, so that the isolation between the two ports is better. If a higher gain needs to be achieved, the number of radiation slots can be appropriately increased.
类似的,射频激励信号通过图4中侧馈端口13对天线馈电,信号通过渐变同轴线传入辐射体,进入内导体和外导体及它们之间的介质组成的类外同轴线结构向上传播,边传播边从缝隙向外辐射能量。由于渐变同轴线(T型结构)与类外同轴结构阻抗有所失配,先经过下类同轴匹配结构,使得S22在5.2GHz-5.8GHz范围内小于-10dB,类同轴匹配结构的设计以传输线理论为基础,实现阻抗匹配。信号从辐射结构1上的四组缝隙阵列5向外辐射,从而有较高增益。能量从第四个缝隙开始向外辐射,到第一个缝隙处已经很少,这样只有很少能量进入内类同轴结构,直至下馈端口12,从而使两个端口的隔离度较好。Similarly, the radio frequency excitation signal is fed to the antenna through the side feed port 13 in Fig. 4, and the signal is transmitted to the radiator through the tapered coaxial line, and enters the outer coaxial line structure composed of the inner conductor, the outer conductor and the medium between them Propagate upward, radiating energy outward from the gap as it propagates. Due to the mismatch between the impedance of the tapered coaxial line (T-shaped structure) and the coaxial structure outside the class, first go through the following coaxial matching structure, so that the S22 is less than -10dB in the range of 5.2GHz-5.8GHz, which is similar to the coaxial matching structure The design is based on transmission line theory to achieve impedance matching. Signals are radiated outward from the four groups of slot arrays 5 on the radiation structure 1, so that there is a relatively high gain. Energy starts to radiate outward from the fourth slot, and there is very little energy at the first slot, so that only a little energy enters the inner coaxial structure until the feed-down port 12, so that the isolation between the two ports is better.
如图5所示是本实施例的仿真得到的回波损耗图。从图中可以看出,在5.2GHz-5.8GHz频段内回波损耗小于-10dB。As shown in FIG. 5 , the return loss diagram obtained by the simulation of this embodiment is shown. It can be seen from the figure that the return loss is less than -10dB in the 5.2GHz-5.8GHz frequency band.
如图6所示是本实例的仿真得到的在5.2GHz、5.5GHz、5.8GHz三个频点水平全向(Theta=90°)的轴比图。从图中可以看出,在5.2GHz-5.8GHz频段内,轴比最大均值基本都在3dB以下。As shown in FIG. 6 , the axial ratio diagrams obtained by the simulation of this example at three frequency points of 5.2GHz, 5.5GHz, and 5.8GHz are horizontally omnidirectional (Theta=90°). It can be seen from the figure that in the 5.2GHz-5.8GHz frequency band, the maximum average value of the axial ratio is basically below 3dB.
如图7所示是本实例的仿真得到的在5.2GHz、5.5GHz、5.8GHz三个频点水平全向(Theta=90°)的增益图。从图中可以看出,在5.2GHz-5.8GHz频段内,增益最小值均大于5.2dB,最大至5.7dB且天线的全向性能良好。As shown in FIG. 7 , the gain diagram obtained by the simulation of this example at three frequency points of 5.2GHz, 5.5GHz, and 5.8GHz is horizontally omnidirectional (Theta=90°). It can be seen from the figure that in the 5.2GHz-5.8GHz frequency band, the minimum value of the gain is greater than 5.2dB, and the maximum value reaches 5.7dB, and the omnidirectional performance of the antenna is good.
以上对本发明的具体实施例进行了描述。需要理解的是,本发明并不局限于上述特定实施方式,本领域技术人员可以在权利要求的范围内做出各种变化或修改,这并不影响本发明的实质内容。在不冲突的情况下,本申请的实施例和实施例中的特征可以任意相互组合。Specific embodiments of the present invention have been described above. It should be understood that the present invention is not limited to the specific embodiments described above, and those skilled in the art may make various changes or modifications within the scope of the claims, which do not affect the essence of the present invention. In the case of no conflict, the embodiments of the present application and the features in the embodiments can be combined with each other arbitrarily.
Claims (2)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201610634955.1A CN106229635B (en) | 2016-08-04 | 2016-08-04 | A kind of omnidirectional's dual circularly polarized antenna of ipsilateral feed |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201610634955.1A CN106229635B (en) | 2016-08-04 | 2016-08-04 | A kind of omnidirectional's dual circularly polarized antenna of ipsilateral feed |
Publications (2)
Publication Number | Publication Date |
---|---|
CN106229635A CN106229635A (en) | 2016-12-14 |
CN106229635B true CN106229635B (en) | 2019-10-08 |
Family
ID=57547203
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201610634955.1A Active CN106229635B (en) | 2016-08-04 | 2016-08-04 | A kind of omnidirectional's dual circularly polarized antenna of ipsilateral feed |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN106229635B (en) |
Families Citing this family (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108256368B (en) * | 2016-12-28 | 2021-10-26 | 航天信息股份有限公司 | Method and device for generating dual-port network |
CN108258426A (en) * | 2018-01-10 | 2018-07-06 | 西安电子工程研究所 | A kind of Circular polarized omni-directional Spiral slot antenna |
CN108777366A (en) * | 2018-04-18 | 2018-11-09 | 西安电子科技大学 | A kind of slotted coaxial antenna for realizing 45 ° of inclined polarizations of horizontal omnidirectional radiation |
CN110854519B (en) * | 2019-11-23 | 2022-08-12 | 武汉市联华飞创科技有限公司 | Conformal antenna device |
CN112086371B (en) * | 2020-08-19 | 2023-03-14 | 中国电子科技集团公司第二十九研究所 | Broadband radio frequency board level interconnection integration method, structure and device |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN201741801U (en) * | 2009-11-17 | 2011-02-09 | 上海航天测控通信研究所 | Small-sized high-gain circular polarized antenna |
CN103022705A (en) * | 2012-12-27 | 2013-04-03 | 北京理工大学 | Dielectric loaded wideband miniature dual circularly polarized antenna |
CN104505578A (en) * | 2014-12-31 | 2015-04-08 | 上海交通大学 | Omnidirectional dual circularly polarized antenna |
-
2016
- 2016-08-04 CN CN201610634955.1A patent/CN106229635B/en active Active
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN201741801U (en) * | 2009-11-17 | 2011-02-09 | 上海航天测控通信研究所 | Small-sized high-gain circular polarized antenna |
CN103022705A (en) * | 2012-12-27 | 2013-04-03 | 北京理工大学 | Dielectric loaded wideband miniature dual circularly polarized antenna |
CN104505578A (en) * | 2014-12-31 | 2015-04-08 | 上海交通大学 | Omnidirectional dual circularly polarized antenna |
Also Published As
Publication number | Publication date |
---|---|
CN106229635A (en) | 2016-12-14 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN106229635B (en) | A kind of omnidirectional's dual circularly polarized antenna of ipsilateral feed | |
US9799962B2 (en) | Dual-polarized dipole antenna | |
CN103236586B (en) | Small circularly-polarized horn antenna | |
Zou et al. | SIW-fed Yagi antenna and its application on monopulse antenna | |
CN109193110B (en) | High-gain Vivaldi circularly polarized antenna | |
CN104901004B (en) | A kind of high-gain end-fire millimeter wave antenna | |
US20210234279A1 (en) | Circularly polarized antenna | |
CN105048080B (en) | A kind of omni-directional circular polarization plane antenna based on electro magnetic dipole | |
CN104505578A (en) | Omnidirectional dual circularly polarized antenna | |
WO2020087390A1 (en) | Helical antenna and communication device | |
CN106299723A (en) | Common reflector | |
CN107046177B (en) | Feed source of back-feed type dual-polarized parabolic antenna | |
CN106299690A (en) | A kind of differential feed Broadband circularly polarized antenna | |
CN107134648A (en) | A kind of wideband dual polarized electromagnetic dipole antenna of L-band | |
TWI694635B (en) | Tri-band feed assembly systems and methods | |
CN207320331U (en) | Dual-band and dual-polarization Shared aperture waveguide trumpet planar array antenna | |
CN108172978A (en) | Dual polarization radiating unit and antenna device | |
CN104134854A (en) | Broadband circularly-polarized omnidirectional antenna based on rectangular rings | |
CN207217773U (en) | Antenna, transmitting device, receiving device and wireless communication system | |
US11594796B2 (en) | Cross slot polarizer | |
CN206789696U (en) | The Broadband circularly polarized antenna of coplanar wave guide feedback | |
CN115939740A (en) | Omnidirectional circularly polarized antenna, cascade antenna and antenna array | |
CN106252878B (en) | Space diversity covering transmitting-receiving system based on circularly polarized antenna | |
CN206850028U (en) | Broadband High Gain Vertically Polarized Omnidirectional Antenna | |
CN206225547U (en) | A kind of differential feed Broadband circularly polarized antenna |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |