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JPH0310242B2 - - Google Patents
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JPH0310242B2 - - Google Patents

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Publication number
JPH0310242B2
JPH0310242B2 JP15573985A JP15573985A JPH0310242B2 JP H0310242 B2 JPH0310242 B2 JP H0310242B2 JP 15573985 A JP15573985 A JP 15573985A JP 15573985 A JP15573985 A JP 15573985A JP H0310242 B2 JPH0310242 B2 JP H0310242B2
Authority
JP
Japan
Prior art keywords
feeding point
rectangular
microstrip antenna
conductor element
radiation conductor
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.)
Expired
Application number
JP15573985A
Other languages
Japanese (ja)
Other versions
JPS6216601A (en
Inventor
Yukihiro Yoshikawa
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP15573985A priority Critical patent/JPS6216601A/en
Publication of JPS6216601A publication Critical patent/JPS6216601A/en
Publication of JPH0310242B2 publication Critical patent/JPH0310242B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は誘電体基板を用いて構成する矩形マ
イクロストリツプアンテナに関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a rectangular microstrip antenna constructed using a dielectric substrate.

〔従来の技術〕[Conventional technology]

第4図は従来の矩形マイクロストリツプアンテ
ナの一例を示す図であり、図中、1は誘電体基
板、2は矩形放射導体素子、3は接地導体板、4
はストリツプ給電線路、5は矩形放射導体素子2
へのストリツプ給電線路4の給電点である。第4
図の従来の矩形マイクロストリツプアンテナの動
作原理を次に説明する。
FIG. 4 is a diagram showing an example of a conventional rectangular microstrip antenna, in which 1 is a dielectric substrate, 2 is a rectangular radiation conductor element, 3 is a ground conductor plate, and 4 is a diagram showing an example of a conventional rectangular microstrip antenna.
is a strip feed line, 5 is a rectangular radiation conductor element 2
This is the feeding point of the strip feed line 4 to. Fourth
The operating principle of the conventional rectangular microstrip antenna shown in the figure will now be explained.

第5図a及びbは第4図の従来の矩形マイクロ
ストリツプアンテナの一例の動作原理を説明する
ための矩形放射導体素子2の図である。第5図a
は給電点5がy軸上にある場合、第5図bは給電
点5が中心軸よりずれた場合である。基本モード
のみを考慮すると、第5図aの給電点5がy軸上
にある場合には、x軸に一様な表面電流6が矩形
放射導体素子2上をy方向に流れ、誘電体基板1
内の電界(以下、これを内部電界という。)EZ
x方向に一様でy方向に正弦波状の分布7を持
つ。したがつて、放射電界はy方向にのみ成分を
持つ直線偏波となる。
5A and 5B are diagrams of a rectangular radiation conductor element 2 for explaining the operating principle of an example of the conventional rectangular microstrip antenna of FIG. 4. FIG. Figure 5a
Fig. 5b shows a case where the feeding point 5 is on the y-axis, and Fig. 5b shows a case where the feeding point 5 is deviated from the central axis. Considering only the fundamental mode, if the feed point 5 in FIG. 1
The electric field within (hereinafter referred to as the internal electric field) E Z is uniform in the x direction and has a sinusoidal distribution 7 in the y direction. Therefore, the radiated electric field becomes a linearly polarized wave having a component only in the y direction.

一方、第5図bの給電点5が中心軸よりずれた
場合には、x軸に一様な表面電流6が矩形放射導
体素子2上をy方向に流れるだけでなく、y軸に
一様な表面電流8も矩形放射導体素子2上をx方
向に流れ、内部電界EZはy方向及びx方向にそ
れぞれ、正弦波状の分布7及び9を持つ。したが
つて、放射電界はy方向だけでなくx方向にも成
分を持つ楕円偏波となる。
On the other hand, when the feed point 5 in FIG. A surface current 8 also flows on the rectangular radiating conductor element 2 in the x direction, and the internal electric field E Z has sinusoidal distributions 7 and 9 in the y and x directions, respectively. Therefore, the radiated electric field becomes an elliptically polarized wave having components not only in the y direction but also in the x direction.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

第4図の従来の矩形マイクロストリツプアンテ
ナの一例を直線偏波アンテナとして用いる場合、
上記説明の通り、給電点5の位置を中心軸上に持
つてきた方が偏波特性が優れているが、インピー
ダンス整合あるいはアンテナ全体の構成より、給
電点5を中心軸よりずらした位置に持つてこなけ
ればいけないことがある。その場合には交差偏波
成分が生じ、アンテナとしての性能が劣化すると
いう問題点があつた。
When using an example of the conventional rectangular microstrip antenna shown in Fig. 4 as a linearly polarized antenna,
As explained above, the polarization characteristics are better if the feeding point 5 is located on the central axis, but due to impedance matching or the overall antenna configuration, the feeding point 5 may be placed off the central axis. There's something I need to bring. In that case, there was a problem in that cross-polarized components were generated and the performance as an antenna deteriorated.

この発明は、このような問題点を解決するため
になされたもので、給電点が中心軸よりずれた場
合でも交差偏波成分のない矩形マイクロストリツ
プアンテナを得ることを目的とする。
The present invention was made to solve these problems, and an object of the present invention is to obtain a rectangular microstrip antenna without cross-polarized components even when the feeding point is shifted from the central axis.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る矩形マイクロストリツプアンテ
ナは、主偏波方向と平行な矩形放射導体素子の中
心軸に対して、第一の給電点と対称な位置に第二
の給電点を設け、互いに等振幅等位相にて給電し
たものである。
In the rectangular microstrip antenna according to the present invention, the second feeding point is provided at a position symmetrical to the first feeding point with respect to the central axis of the rectangular radiation conductor element parallel to the main polarization direction, and the second feeding point is provided at a position symmetrical to the first feeding point, and the second feeding point is equidistant to the first feeding point. Power is supplied with equal amplitude and phase.

〔作用〕[Effect]

この発明においては、第二の給電点を設けるこ
とにより、交差偏波方向へ流れる電流を抑圧す
る。
In this invention, the current flowing in the cross polarization direction is suppressed by providing the second feeding point.

〔実施例〕〔Example〕

第1図はこの発明の一実施例を示す図であり、
図中、1〜5は第4図の従来の矩形マイクロスト
リツプアンテナの一例と全く同一のものであり、
10及び11はそれぞれ、新たに設けたストリツ
プ給電線路、及び矩形放射導体素子2へのストリ
ツプ給電線路10の給電点である。この発明によ
る矩形マイクロストリツプアンテナの一実施例の
動作原理を次に説明する。
FIG. 1 is a diagram showing an embodiment of the present invention,
In the figure, 1 to 5 are exactly the same as the example of the conventional rectangular microstrip antenna shown in FIG.
10 and 11 are a newly provided strip feed line and a feed point of the strip feed line 10 to the rectangular radiation conductor element 2, respectively. The operating principle of one embodiment of the rectangular microstrip antenna according to the present invention will now be described.

第2図a及びbは、それぞれ、給電点5及び1
1が単独にある場合の矩形放射導体素子2の表面
電流分布を示す図である。第2図aは第5図bの
従来の矩形マイクロストリプアンテナの一例の動
作原理を説明するための図と同一であり、第2図
bは第2図aをy軸に沿つて180度反転させたも
のに等しい。すなわち、主偏波方向であるy方向
については、表面電流6及び12は同じ向きに流
れ、交差偏波方向であるx方向については、表面
電流8及び13は逆向きに流れる。ゆえに、給電
点5及び11における矩形放射導体素子2への給
電振幅位相を互いに等振幅等位相にすれば、第3
図に示すように、矩形放射導体素子2上の表面電
流分布はy方向の表面電流14のみとなり、内部
電界EZは表面電流14に対する正弦波分布15
となる。したがつて、放射電界はy方向にのみ成
分を持つ直線偏波となり、良好な偏波特性を示
す。
Figure 2 a and b show feed points 5 and 1, respectively.
1 is a diagram showing a surface current distribution of a rectangular radiating conductor element 2 when there is only one radiating conductor element 1. Figure 2a is the same as Figure 5b for explaining the operating principle of an example of a conventional rectangular microstrip antenna, and Figure 2b is a 180 degree inversion of Figure 2a along the y-axis. It is equal to what was made. That is, in the y direction, which is the main polarization direction, the surface currents 6 and 12 flow in the same direction, and in the x direction, which is the cross polarization direction, the surface currents 8 and 13 flow in opposite directions. Therefore, if the feeding amplitude phases to the rectangular radiation conductor element 2 at feeding points 5 and 11 are made equal in amplitude and phase, the third
As shown in the figure, the surface current distribution on the rectangular radiation conductor element 2 is only the surface current 14 in the y direction, and the internal electric field E Z is a sine wave distribution 15 for the surface current 14.
becomes. Therefore, the radiated electric field becomes a linearly polarized wave having a component only in the y direction, and exhibits good polarization characteristics.

ところで上記説明では、この発明を単一直線偏
波アンテナに利用する場合について述べたが、直
交2偏波共用アンテナなどにも利用できる。
Incidentally, in the above description, the present invention is applied to a single linearly polarized antenna, but it can also be applied to an antenna that can share two orthogonal polarized waves.

〔発明の効果〕〔Effect of the invention〕

この発明は以上説明したとおり、主偏波方向と
平行な矩形放射導体素子の中心軸に対して、第一
の給電点と対称な位置に第二の給電点を設け、互
いに等振幅等位相にて給電することにより、給電
点が中心軸よりずれた場合でも良好な偏波特性が
得られるという効果がある。
As explained above, the present invention provides a second feeding point at a position symmetrical to the first feeding point with respect to the center axis of the rectangular radiation conductor element parallel to the main polarization direction, and has equal amplitude and phase with each other. By supplying power through the antenna, it is possible to obtain good polarization characteristics even when the power supply point is shifted from the central axis.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図はこの発明の一実施例を示す図、第2図
a及びbはこの発明の一実施例の動作原理を説明
するための図、第3図はこの発明の一実施例の表
面電流分布、及び内部電界分布を示す図、第4図
は従来の矩形マイクロストリツプアンテナの一例
を示す図、第5図a及びbは従来の矩形マイクロ
ストリツプアンテナの一例の動作原理を説明する
ための図である。 図において、1は誘電体基板、2は矩形放射導
体素子、3は接地導体板、5は第一の給電点、1
1は主偏波方向と平行な矩形放射導体素子2の中
心軸に対して、第一の給電点5と対称な位置に設
けた第二の給電点である。なお、各図中同一符号
は同一または相当部分を示す。
Fig. 1 is a diagram showing an embodiment of the present invention, Fig. 2 a and b are diagrams for explaining the operating principle of an embodiment of the invention, and Fig. 3 is a diagram showing the surface current of an embodiment of the invention. Figure 4 is a diagram showing an example of a conventional rectangular microstrip antenna, and Figures 5a and b explain the operating principle of an example of a conventional rectangular microstrip antenna. This is a diagram for In the figure, 1 is a dielectric substrate, 2 is a rectangular radiation conductor element, 3 is a ground conductor plate, 5 is a first feeding point, 1
Reference numeral 1 denotes a second feeding point provided at a position symmetrical to the first feeding point 5 with respect to the central axis of the rectangular radiation conductor element 2 parallel to the main polarization direction. Note that the same reference numerals in each figure indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 1 誘電体基板と、この誘電体基板の下面に置か
れた接地導体板と、上記誘電体基板を介して上記
接続導体板と対向する矩形放射導体素子とを有す
る矩形マイクロストリツプアンテナにおいて、主
偏波方向と平行な矩形放射導体素子の中心軸に対
して、第一の給電点と対称な位置に第二の給電点
を設け、互いに等振幅等位相にて給電したことを
特徴とする矩形マイクロストリツプアンテナ。
1. A rectangular microstrip antenna having a dielectric substrate, a ground conductor plate placed on the lower surface of the dielectric substrate, and a rectangular radiation conductor element facing the connection conductor plate via the dielectric substrate, A second feeding point is provided at a position symmetrical to the first feeding point with respect to the central axis of the rectangular radiation conductor element parallel to the main polarization direction, and the electricity is fed with equal amplitude and phase to each other. Rectangular microstrip antenna.
JP15573985A 1985-07-15 1985-07-15 Rectangular microstrip antenna Granted JPS6216601A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15573985A JPS6216601A (en) 1985-07-15 1985-07-15 Rectangular microstrip antenna

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15573985A JPS6216601A (en) 1985-07-15 1985-07-15 Rectangular microstrip antenna

Publications (2)

Publication Number Publication Date
JPS6216601A JPS6216601A (en) 1987-01-24
JPH0310242B2 true JPH0310242B2 (en) 1991-02-13

Family

ID=15612381

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15573985A Granted JPS6216601A (en) 1985-07-15 1985-07-15 Rectangular microstrip antenna

Country Status (1)

Country Link
JP (1) JPS6216601A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2562639B2 (en) * 1988-01-20 1996-12-11 三洋電機株式会社 Temperature control method for low temperature product storage case
CN114883798A (en) * 2022-05-10 2022-08-09 上海海积信息科技股份有限公司 Circularly polarized antenna

Also Published As

Publication number Publication date
JPS6216601A (en) 1987-01-24

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