JP3223742B2 - Microstrip antenna - Google Patents
Microstrip antennaInfo
- Publication number
- JP3223742B2 JP3223742B2 JP01933495A JP1933495A JP3223742B2 JP 3223742 B2 JP3223742 B2 JP 3223742B2 JP 01933495 A JP01933495 A JP 01933495A JP 1933495 A JP1933495 A JP 1933495A JP 3223742 B2 JP3223742 B2 JP 3223742B2
- Authority
- JP
- Japan
- Prior art keywords
- conductor plate
- microstrip antenna
- radiation conductor
- radiation
- shape
- 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 - Fee Related
Links
Landscapes
- Waveguide Aerials (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、無線LAN、入退室管
理システム等、マイクロ波やミリ波を利用するシステム
の送受信アンテナ素子として用いられるマイクロストリ
ップアンテナに関するものであり、特に一点給電で円偏
波を放射させるものに関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a microstrip antenna used as a transmission / reception antenna element of a system utilizing microwaves or millimeter waves, such as a wireless LAN, an entry / exit management system, and the like. It relates to something that emits waves.
【0002】[0002]
【従来の技術】マイクロストリップアンテナは、接地導
体板を持つ誘電体基板上に四角形、三角形、円形などの
各種幾何学形状をした放射導体板を設けたものが一般的
である。これは放射導体板の一点もしくは複数点から、
マイクロストリップ線路あるいは同軸ケーブルを介して
給電することにより、放射導体板に励振された電流が放
射源となって、空間中に電波を放射するものであり開放
共振型アンテナである。2. Description of the Related Art Generally, a microstrip antenna is provided with a radiation conductor plate having various geometric shapes such as a square, a triangle, and a circle on a dielectric substrate having a ground conductor plate. This is from one or more points of the radiation conductor plate,
By feeding power through a microstrip line or a coaxial cable, the current excited in the radiation conductor plate serves as a radiation source to radiate radio waves into space, and is an open resonance antenna.
【0003】従来、マイクロストリップアンテナで円偏
波を発生させるために、正方形や円形等の、中心のまわ
りに90度回転するともとの図形と完全に重なる点対称
な形状(以下、直交点対称形状という)をした放射導体
板上の直交する二点に、90度ハイブリッド等の外部回
路を通して、等振幅で90度の位相差をもつ信号を給電
し、誘電体基板と垂直な方向に円偏波を放射する二点給
電方式がある。しかしながらこの方式は、円偏波の軸比
特性が90度ハイブリッドに大きく依存され、また給電
回路の構造が複雑になるという欠点がある。Conventionally, in order to generate a circularly polarized wave with a microstrip antenna, a point-symmetrical shape (hereinafter referred to as an orthogonal point symmetry, such as a square or a circle) that completely overlaps the original figure when rotated by 90 degrees around the center. A signal having an equal amplitude and a phase difference of 90 degrees is supplied to two orthogonal points on the radiating conductor plate having the same shape through an external circuit such as a 90-degree hybrid and circularly polarized in a direction perpendicular to the dielectric substrate. There is a two-point feeding system that emits waves. However, this method has a drawback that the axial ratio characteristic of the circularly polarized wave largely depends on the 90-degree hybrid, and the structure of the feed circuit becomes complicated.
【0004】そこで上記二点給電方式の欠点を補うもの
として、直交点対称形状の放射導体板の持つ二つの直交
共振モードを利用する一点給電方式がある。この動作原
理は、二つの共振モードの電流の経路長に摂動を与える
ことで縮退を解き、二つの共振モードに対応する二つの
対角線と45度の角度をなす位置から給電することによ
り、互いに90度の位相差を持ち、等しい振幅を持つ直
交電流を発生させて、円偏波を励振するというものであ
る。In order to compensate for the drawbacks of the two-point feeding method, there is a one-point feeding method using two orthogonal resonance modes of a radiation conductor plate having a symmetrical orthogonal point shape. The principle of operation is that the degeneracy is solved by perturbing the path lengths of the currents of the two resonance modes, and power is supplied from a position at an angle of 45 degrees with the two diagonal lines corresponding to the two resonance modes, so that 90 A quadrature current having a phase difference of degrees and an equal amplitude is generated to excite circularly polarized waves.
【0005】ここで図3に一点給電方式の従来例を示
す。図はマイクロストリップ線路で給電する正方形の放
射導体板をもつマイクロストリップアンテナを示してい
る。接地導体板1を有する誘電体基板2上には、ストリ
ップ導体3および放射導体板4を形成してあり、ストリ
ップ導体3は、放射導体板4の一辺の中心に接続してあ
る。放射導体板4には、それぞれの対角に凹部及び凸部
形状をした縮退分離素子5a,5b,6a,6bを設け
ている。FIG. 3 shows a conventional example of a single-point power supply system. The figure shows a microstrip antenna having a square radiating conductor plate fed by a microstrip line. A strip conductor 3 and a radiation conductor plate 4 are formed on a dielectric substrate 2 having a ground conductor plate 1, and the strip conductor 3 is connected to the center of one side of the radiation conductor plate 4. The radiation conductor plate 4 is provided with degenerate separation elements 5a, 5b, 6a, 6b having concave and convex shapes at respective diagonals.
【0006】放射導体板4に設けた縮退分離素子5a,
5b,6a,6bにより、二つの共振モードの縮退を解
き共振周波数を分離する。そして両共振周波数の丁度中
間の周波数で、ストリップ導体3から給電することによ
り、縮退分離素子5a,5bおよび6a,6b方向にそ
れぞれ互いに90度の位相差を持ち、かつ等振幅な直交
電流が発生する。これらの合成により誘電体基板2と垂
直な方向に円偏波が放射される。The degenerate separation elements 5a provided on the radiation conductor plate 4
By using 5b, 6a, and 6b, the two resonance modes are degenerated to separate resonance frequencies. By feeding power from the strip conductor 3 at a frequency exactly intermediate between the two resonance frequencies, a quadrature current having a phase difference of 90 degrees from each other in the direction of the degenerate separation elements 5a, 5b and 6a, 6b and having the same amplitude is generated. I do. By combining these, a circularly polarized wave is radiated in a direction perpendicular to the dielectric substrate 2.
【0007】[0007]
【発明が解決しようとする課題】しかしながら上述の凹
凸形状の縮退分離素子を設ける構成については以下のよ
うな問題点がある。すなわち、二つの共振モードに対す
る電流は、縮退分離素子5a,5b及び6a,6bの二
本の対角線に沿って流れる。このときの電流分布は、各
対角線の中心において最も大きく、端に近づくにつれて
減少する。However, the configuration in which the degenerate separation element having the above-mentioned uneven shape is provided has the following problems. That is, the currents for the two resonance modes flow along two diagonals of the degenerate separation elements 5a, 5b and 6a, 6b. The current distribution at this time is largest at the center of each diagonal, and decreases as approaching the end.
【0008】しかし放射の大部分を占める放射導体板4
の端部では、対角線5a,5b方向ではその凹部形状の
ために電流が二分して流れ、一方、対角線6a,6b方
向ではその凸部形状のために電流が集中して流れるた
め、各対角線で電流分布に大きな違いが生じる。この違
いは、円偏波の軸比特性と、二つの対角線方向での放射
パターンの均一性を悪化させる。However, the radiation conductor plate 4 occupying most of the radiation
At the end of the diagonal line 5a, 5b, the current flows in two due to the concave shape, and in the diagonal line 6a, 6b, the current flows intensively due to the convex shape. A large difference occurs in the current distribution. This difference degrades the axial ratio characteristics of the circular polarization and the uniformity of the radiation pattern in the two diagonal directions.
【0009】また、縮退分離の度合いは、縮退分離素子
の面積のみに関係し、高い放射効率を得ようとすれば、
縮退分離素子の面積を大きくする必要がある。しかし素
子形状を上述のような凹凸部で実現すると、二つの対角
線長の差が広がり、二つの対角線方向の放射パターンの
均一性をさらに悪化させてしまう。The degree of the degenerate separation is related only to the area of the degenerate separation element.
It is necessary to increase the area of the degenerate separation element. However, when the element shape is realized by the above-described uneven portions, the difference between the two diagonal lengths increases, and the uniformity of the radiation patterns in the two diagonal directions further deteriorates.
【0010】加えてマイクロストリップアンテナは、パ
ターン印刷、エッチング等の回路基板作製技術を用いて
製作される。しかしアンテナの使用周波数がミリ波領域
に近くなると、放射導体板の大きさが小さくなるととも
に、縮退分離素子の面積も小さくなってくる。このため
複雑な凹凸形状の素子を正確に製作することが困難にな
るという問題点があった。[0010] In addition, the microstrip antenna is manufactured by using a circuit board manufacturing technique such as pattern printing and etching. However, as the operating frequency of the antenna approaches the millimeter wave region, the size of the radiation conductor plate decreases, and the area of the degenerate separation element also decreases. For this reason, there has been a problem that it is difficult to accurately manufacture an element having a complicated uneven shape.
【0011】本発明は上記の問題点を解決するものであ
り、優れた軸比特性と均一な放射パターンを有し、ミリ
波領域においても製作が容易なマイクロストリップアン
テナを提供することを目的とする。An object of the present invention is to provide a microstrip antenna which has excellent axial ratio characteristics and a uniform radiation pattern, and can be easily manufactured even in a millimeter wave region. I do.
【0012】[0012]
【課題を解決するための手段】上記課題を解決するため
に、本発明のマイクロストリップアンテナは、誘電体層
を介して接地導体板に対向して放射導体板を形成したマ
イクロストリップアンテナにおいて、前記放射導体板の
形状をひし形とし、四辺のうちの一辺上の中点から給電
することにより、円偏波を放射させることを特徴とする
ものである。In order to solve the above-mentioned problems, a microstrip antenna according to the present invention is a microstrip antenna having a radiation conductor plate formed opposite a ground conductor plate via a dielectric layer. The radiating conductor plate has a rhombic shape, and circularly polarized waves are radiated by feeding power from a midpoint on one of the four sides.
【0013】[0013]
【作用】上記構成によれば、放射導体板上の二つの対角
線の長さを異ならせることにより、円偏波を発生させる
に必要な縮退分離を行う。このため二つの対角線方向で
の電流分布の形状は相似となり、また縮退分離に必要な
素子面積は、導体板周辺部に均等に割り当てられるた
め、導体板の形状変化が少ない。その結果、二つの対角
線方向の電流分布の形状変化はさらに少なくなり、優れ
た円偏波軸比および均一な放射パターンが得られること
になる。According to the above construction, the degenerate separation required for generating circularly polarized waves is performed by making the lengths of two diagonal lines on the radiation conductor plate different. Therefore, the shapes of the current distributions in the two diagonal directions are similar, and the element area required for degenerate separation is uniformly allocated to the periphery of the conductor plate, so that the shape change of the conductor plate is small. As a result, the shape change of the current distribution in the two diagonal directions is further reduced, and an excellent circular polarization axis ratio and a uniform radiation pattern can be obtained.
【0014】また上記構成によれば、放射導体板の形状
は単純な四辺形であることから、使用周波数がアンテナ
寸法が微小になるミリ波領域においても、精度の高い製
作が可能となる。Further, according to the above configuration, since the shape of the radiation conductor plate is a simple quadrilateral, it is possible to manufacture the radiation conductor plate with high accuracy even in a millimeter wave region where the antenna frequency is small.
【0015】[0015]
【実施例】以下、本発明のマイクロストリップアンテナ
について、その実施例を図面を参照しながら具体的に説
明する。図1は本発明のマイクロストリップアンテナの
一実施例を示す平面図である。従来のマイクロストリッ
プアンテナと異なる点は、誘電体基板2上に形成する放
射導体板4の形状を、各角が直角の正方形ではないひし
形に形成した点であり、放射導体板4において、両対角
線の長さを異ならせていることを特徴としている。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, embodiments of the microstrip antenna of the present invention will be specifically described with reference to the drawings. FIG. 1 is a plan view showing one embodiment of the microstrip antenna of the present invention. The difference from the conventional microstrip antenna is that the shape of the radiating conductor plate 4 formed on the dielectric substrate 2 is not a square with right angles but a diamond shape. Is characterized by having different lengths.
【0016】図2はそれぞれ実施例の動作を説明するた
めの線図であり、図中の矢印7a,7bは、正方形とひ
し形の放射導体板4に流れる二つの共振モードの電流を
示している。FIGS. 2A and 2B are diagrams for explaining the operation of the embodiment. Arrows 7a and 7b in FIG. 2 indicate currents of two resonance modes flowing through the square and rhombic radiating conductor plates 4, respectively. .
【0017】図2(a)に示す正方形の放射導体板4で
は、対角線の長さがともに等しいため、二つの共振モー
ドは縮退して同一の共振周波数をもつ。ここで放射導体
板4の一辺の中心に、ストリップ導体3から共振周波数
で給電すると、放射導体板4の対角線方向に縮退する二
つの共振モードに対応する等振幅で同位相の共振電流7
a,7bが流れ、これらの合成から直線偏波が空間中に
放射される。In the square radiation conductor plate 4 shown in FIG. 2A, since the lengths of the diagonal lines are equal, the two resonance modes degenerate and have the same resonance frequency. Here, when power is supplied from the strip conductor 3 to the center of one side of the radiation conductor plate 4 at a resonance frequency, the resonance currents 7 having the same amplitude and the same phase corresponding to the two resonance modes degenerate in the diagonal direction of the radiation conductor plate 4.
a and 7b flow, and a linearly polarized wave is radiated into space from the combination thereof.
【0018】給電位置をそのままに、図2(b)に示す
ように、放射導体板4の対角線の長さにわずかな摂動を
与えて、流れる電流の経路長を変化させると、二つの共
振モードは縮退が解かれて、異なる共振周波数をもつよ
うになる。As shown in FIG. 2 (b), while maintaining the power supply position, a slight perturbation is given to the length of the diagonal line of the radiation conductor plate 4 to change the path length of the flowing current. Are degenerate and have different resonance frequencies.
【0019】図2(b)においては、一方の対角線に流
れる電流経路が他方の対角線に流れる電流経路より短い
ため、7a方向の共振モードの共振周波数は、7b方向
の共振モードの共振周波数より高くなる。In FIG. 2B, since the current path flowing in one diagonal is shorter than the current path flowing in the other diagonal, the resonance frequency of the resonance mode in the 7a direction is higher than the resonance frequency of the resonance mode in the 7b direction. Become.
【0020】そこで両対角線の長さを適切に設定し、さ
らに上記の両共振周波数の間の適切な周波数で給電する
ことにより、7a,7b方向に互いに90度の位相差を
持ち、且つ等振幅な直交電流を発生させることができ、
これらの合成から空間中に円偏波を放射することが可能
となる。Therefore, by appropriately setting the lengths of the two diagonal lines and supplying power at an appropriate frequency between the two resonance frequencies, a phase difference of 90 degrees is obtained in the directions of 7a and 7b, and the amplitude is equal. Can generate a large orthogonal current,
It becomes possible to radiate circularly polarized waves into space from the combination of these.
【0021】このように、放射導体板上の二つの対角線
の長さを異ならせて縮退分離を行えば、二つの対角線方
向での電流分布の形状が相似となり、また縮退分離に必
要な素子面積が導体板周辺部に均等に割り当てられ導体
板の形状変化が少ない。このため二つの対角線方向の電
流分布の形状変化が少なくなり、優れた円偏波軸比およ
び均一な放射パターンが得られることになる。As described above, if the degenerate separation is performed by changing the lengths of the two diagonal lines on the radiation conductor plate, the current distribution shapes in the two diagonal directions become similar, and the element area required for the degenerate separation is obtained. Are uniformly allocated to the periphery of the conductive plate, and the shape change of the conductive plate is small. For this reason, the shape change of the current distribution in the two diagonal directions is reduced, and an excellent circular polarization axis ratio and a uniform radiation pattern can be obtained.
【0022】さらに二つの対角線の長さが異なるだけ
で、放射導体板の形状は単純な四辺形であることから、
使用周波数がアンテナ寸法が微小になるミリ波領域にお
いても精度の高い製作が可能となる。Further, since the shape of the radiation conductor plate is a simple quadrilateral only by the difference between the lengths of the two diagonal lines,
High-precision fabrication is possible even in the millimeter-wave region where the antenna frequency is small when the frequency used is small.
【0023】[0023]
【発明の効果】以上のように放射導体板の形状をひし形
とし、四辺のうちの一辺上の中点から給電する本発明に
よれば、優れた円偏波軸比および均一な放射パターンを
持ち、使用周波数がアンテナ寸法が微小になるミリ波領
域においても、精度の高い製作が可能なマイクロストリ
ップアンテナを実現することができる。As described above, according to the present invention, in which the shape of the radiation conductor plate is rhombic and power is supplied from the middle point on one of the four sides, the radiation conductor plate has an excellent circular polarization axis ratio and a uniform radiation pattern. Also, it is possible to realize a microstrip antenna that can be manufactured with high accuracy even in a millimeter-wave region where the antenna size is minute when the operating frequency is minute.
【図1】本発明のマイクロストリップアンテナの一実施
例を示す平面図FIG. 1 is a plan view showing one embodiment of a microstrip antenna of the present invention.
【図2】同アンテナの動作説明をする線図FIG. 2 is a diagram illustrating the operation of the antenna.
【図3】従来のマイクロストリップアンテナを示す平面
図及び断面図FIG. 3 is a plan view and a sectional view showing a conventional microstrip antenna.
1 接地導体板 2 誘電体層 3 ストリップ導体 4 放射導体板 5a,5b,6a,6b 縮退分離素子 7a,7b 両共振モードの電流 DESCRIPTION OF SYMBOLS 1 Ground conductor plate 2 Dielectric layer 3 Strip conductor 4 Radiation conductor plate 5a, 5b, 6a, 6b Degenerate separation element 7a, 7b Current in both resonance modes
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平3−276904(JP,A) 特開 平5−29825(JP,A) 特開 平4−316202(JP,A) 特開 平3−49404(JP,A) 特開 平4−122105(JP,A) 特開 平6−232627(JP,A) 特開 昭59−161102(JP,A) 特開 昭60−197002(JP,A) 特開 平4−199903(JP,A) 特開 平6−326508(JP,A) (58)調査した分野(Int.Cl.7,DB名) H01Q 13/08 JICSTファイル(JOIS)──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-3-276904 (JP, A) JP-A-5-29825 (JP, A) JP-A-4-316202 (JP, A) JP-A-3-316 49404 (JP, A) JP-A-4-122105 (JP, A) JP-A-6-232627 (JP, A) JP-A-59-161102 (JP, A) JP-A-60-197002 (JP, A) JP-A-4-199903 (JP, A) JP-A-6-326508 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) H01Q 13/08 JICST file (JOIS)
Claims (1)
射導体板を形成したマイクロストリップアンテナにおい
て、前記放射導体板の形状をひし形とし、四辺のうちの
一辺上の中点から給電することにより、円偏波を放射さ
せることを特徴とするマイクロストリップアンテナ。1. A microstrip antenna in which a radiation conductor plate is formed facing a ground conductor plate via a dielectric layer, wherein the radiation conductor plate has a rhombic shape, and power is supplied from a midpoint on one of four sides. A microstrip antenna that emits circularly polarized waves.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP01933495A JP3223742B2 (en) | 1995-02-07 | 1995-02-07 | Microstrip antenna |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP01933495A JP3223742B2 (en) | 1995-02-07 | 1995-02-07 | Microstrip antenna |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH08213830A JPH08213830A (en) | 1996-08-20 |
| JP3223742B2 true JP3223742B2 (en) | 2001-10-29 |
Family
ID=11996514
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP01933495A Expired - Fee Related JP3223742B2 (en) | 1995-02-07 | 1995-02-07 | Microstrip antenna |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3223742B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100648903B1 (en) * | 1998-04-29 | 2007-03-02 | 교세라 가부시키가이샤 | Plane antenna, and portable radio using thereof |
-
1995
- 1995-02-07 JP JP01933495A patent/JP3223742B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH08213830A (en) | 1996-08-20 |
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