JP4224864B2 - Antenna device - Google Patents
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- JP4224864B2 JP4224864B2 JP2007101098A JP2007101098A JP4224864B2 JP 4224864 B2 JP4224864 B2 JP 4224864B2 JP 2007101098 A JP2007101098 A JP 2007101098A JP 2007101098 A JP2007101098 A JP 2007101098A JP 4224864 B2 JP4224864 B2 JP 4224864B2
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- radiator
- antenna
- pipe
- coaxial cable
- metal pipe
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Description
本発明はアンテナ装置であって、さらに詳しくは基本的な長さを要するアンテナ長の短縮を図った或いは無線運用の出来る周波数帯域の広いダイポール形アンテナに関するものである。 The present invention relates to an antenna device, and more particularly to a dipole antenna having a wide frequency band in which the antenna length requiring a basic length can be shortened or wirelessly operated.
ダイポール形アンテナはヘルツが初めて電波を発生させるために用いたアンテナで、以来形状は変わらず現在も無線通信に於ける基本形のアンテナとして使用されている。構造は長さ1/2λの放射器(ラジエーター)を中央で分割し、その位置から給電させる。いたってシンプルなアンテナである。このダイポール形アンテナは一般的に短波帯から超短波帯の送信及び受信用のアンテナとして使用されている。 The dipole antenna is the first antenna used by Hertz to generate radio waves, and since then its shape has not changed and is still used as the basic antenna in wireless communications. In the structure, a radiator having a length of 1 / 2λ is divided at the center, and power is supplied from that position. It is a simple antenna. This dipole antenna is generally used as an antenna for transmission and reception from a short wave band to an ultra short wave band.
無線通信でのアマチュア無線の運用は比較的波長の長い波長域においても運用されている。実用的な周波数の下限はアマチュア無線では1.9MHzであり、これは波長およそ160mであり、従来の1/2λダイポール・アンテナは約80m、1/4λ垂直形アンテナでも約40mとなり、アンテナの架設は物理的に困難であった。これを解決するため従来は短縮コイルや頂冠キャパシティを使用していたが、短縮させるが故に運用出来る周波数帯域も狭くなってしまった。 The operation of amateur radio in wireless communication is also operated in a wavelength region having a relatively long wavelength. The lower limit of the practical frequency is 1.9 MHz for amateur radio, which is about 160 m in wavelength, about 80 m for a conventional 1 / 2λ dipole antenna, and about 40 m for a 1 / 4λ vertical antenna. Was physically difficult. In order to solve this problem, a shortened coil and a crown capacity have been used in the past, but the frequency band that can be operated has been narrowed because of shortening.
同軸ケーブルを使用して素材の絶縁物の持つ速度係数(短縮率)を利用したアンテナを発明することが出来れば短縮コイルや頂冠キャパシティを省略した短縮されたアンテナが実現出来るという考え方は過去多くの無線に関わった人たちが実験・可能性について挑戦したが成し得ることが出来なかった。最近もその可能性について詳細に理論立てて実験されたにも拘らず完成には至っていない。(非特許文献1を参照) The idea that a shortened antenna that omits the shortening coil and crown cap capacity can be realized if an antenna that uses the speed coefficient (shortening rate) of a material insulator using a coaxial cable can be invented. Many people involved in radio challenged the experiment and possibility, but could not be achieved. Although it has recently been theoretically tested in detail about the possibility, it has not been completed. (See Non-Patent Document 1)
従来のアンテナ技術に同様な給電方法が見出されてはいたが、周波数帯域幅を確保するためのスタブとして使用されており、アンテナ自体は短縮されては作動していなかった。この様な規格化されて市販されている素材だけを給電し、短縮されたアンテナを実現するには至らなかった。(非特許文献1、非特許文献2、特許文献1を参照) Although a similar power feeding method has been found in the conventional antenna technology, it has been used as a stub for securing a frequency bandwidth, and the antenna itself has not been shortened to operate. It was impossible to realize a shortened antenna by feeding only such standardized and commercially available materials. (See Non-Patent
(特許紹介参考文献1)
アンテナ装置は小形化すると給電インピーダンスが下がり効率が低下し、また運用出来る周波数帯域が狭くなる性質があって短縮された小形のアンテナは使い難いアンテナ装置であった。 When the antenna device is downsized, the feeding impedance is lowered, the efficiency is lowered, and the frequency band that can be operated is narrowed. Therefore, the shortened small antenna is difficult to use.
本発明はアンテナの長さを短縮し、運用周波数帯域幅を十分確保出来る広帯域なダイポール形アンテナ装置を作り出すことを目的とするものである。 An object of the present invention is to produce a wide-band dipole antenna device capable of shortening the length of an antenna and sufficiently securing an operating frequency bandwidth.
このアンテナの給電インピーダンスを把握することが出来たことにより、最適な給電方法を考案し課題を解決出来るに至った。 By being able to grasp the power supply impedance of this antenna, an optimal power supply method was devised and the problems could be solved.
同軸ケーブルにて構成するダイポール形アンテナについて図1に示す。このまま給電することは出来るが強度的に限られた条件の下にしか架設することが出来ないので、これを図2のように金属管(パイプ)内に配し、アンテナとしての強度を高め構成する。FIG. 1 shows a dipole antenna composed of coaxial cables. Although power can be supplied as it is, it can only be installed under conditions limited in strength, so it is arranged in a metal pipe (pipe) as shown in Fig. 2 to increase the strength as an antenna To do.
本発明に従った短縮されたダイポール形のアンテナ装置は放射器(ラジエーター)の素材の絶縁物固有の速度係数(短縮率)を活かして波長が短縮されるので、短縮コイルや頂冠キャパシティが不要で構造がシンプルであり、コストパフォーマンスに優れ応用性が高い。また周波数帯域幅も十分確保できる状態で作動する。実験で架設した50MHz用アンテナでは内装する同軸ケーブルにより2〜3MHzの周波数帯域幅を確保出来る。The shortened dipole antenna device according to the present invention shortens the wavelength by utilizing the speed coefficient (shortening rate) inherent to the insulator of the radiator (radiator) material, so that the shortened coil and the crown capacity are reduced. Unnecessary, simple structure, excellent cost performance and high applicability. It operates in a state where a sufficient frequency bandwidth can be secured. In the 50 MHz antenna installed in the experiment, a frequency bandwidth of 2 to 3 MHz can be secured by an internal coaxial cable.
本発明に従った原理は従来の基本的なダイポール形アンテナ及び、より複雑なアンテナ構成の反射器もしくは導波器を伴う通常の多素子の形式のダイポール形アンテナのすべてに適用可能である。 The principle according to the present invention is applicable to all conventional basic dipole antennas and conventional multi-element type dipole antennas with reflectors or directors of more complex antenna configurations.
基本的に一定のインピーダンスを持つ同軸ケーブルを使用し、それぞれを1/4λの電気的な長さの一対の放射器(ラジエーター)として使用し、その先端を短絡し、中央部を交差させて接続し、中央部の接続点を給電部とし、それぞれを金属管(パイプ)内に配し、先端部と中央部は金属管(パイプ)に接合してインピーダンス変換バランを介して給電することにより素材の絶縁物固有の速度係数(短縮率)を利用した波長の短縮された広帯域ダイポール形のアンテナ装置として作動させることが出来る。Basically, a coaxial cable with a constant impedance is used, and each is used as a pair of radiators (radiators) with an electrical length of 1 / 4λ, the tips are short-circuited, and the center is crossed and connected. The central connection point is used as a power feeding part, each is placed in a metal pipe (pipe), and the tip part and the central part are joined to the metal pipe (pipe) and fed through an impedance conversion balun. It is possible to operate as a wideband dipole antenna device with a shortened wavelength utilizing the speed coefficient (shortening rate) inherent to the insulator.
このアンテナは給電インピーダンスが通常よりやや高く、このままでは給電出来ないので、インピーダンスの変換を行わねばならない。一時側は送信機の出力形態によるが現在では50Ω不平衡出力がほとんどである。故に不平衡50Ω:平衡nnΩに変換しなくてはならない。この値は放射器(ラジエーター)に使用する同軸ケーブルの種類によって値が異なる。これにより素材の絶縁物固有の速度係数(短縮率)を活かした短縮されたダイポール形のアンテナ装置が実現出来る。 This antenna has a slightly higher feed impedance than usual and cannot be fed as it is, so the impedance must be converted. The temporary side depends on the output form of the transmitter, but currently 50Ω unbalanced output is almost all. Therefore, it must be converted to unbalanced 50Ω: balanced nnΩ. This value varies depending on the type of coaxial cable used for the radiator. As a result, a shortened dipole antenna device utilizing the speed coefficient (shortening rate) inherent to the insulating material can be realized.
実験で求めた給電インピーダンス値は金属管(パイプ)内に50Ω系同軸ケーブルを配した場合は250Ω。金属管(パイプ)内に75Ω系同軸ケーブルを配した場合は270Ω。インピーダンス及び不平衡・平衡の変換は一般的なトロイダルコア及びフェライトビーズを使用したバランで実現出来る。 The feed impedance value obtained in the experiment is 250Ω when a 50Ω coaxial cable is placed in the metal pipe. 270Ω when a 75Ω coaxial cable is placed in a metal pipe. Impedance and unbalance / balance conversion can be realized with a balun using a general toroidal core and ferrite beads.
VHF帯では給電インピーダンスが低くなる傾向があり、これより低い周波数帯にては若干高いインピーダンスで給電出来る。 In the VHF band, the feeding impedance tends to be low, and in a lower frequency band, the feeding can be performed with a slightly higher impedance.
図7の同軸ケーブルを金属管(パイプ)内に配したダイポール形アンテナは構造的にも強固となり多素子化の実現が容易となる。 The dipole antenna in which the coaxial cable shown in FIG. 7 is arranged in a metal tube (pipe) is structurally strong and easy to realize multiple elements.
1 電気的長さが1/4λの同軸ケーブル
2 電気的長さが1/4λの同軸ケーブルに相当した長さの金属管(パイプ)
3 給電ポイント、インピーダンス及び不平衡・平衡の変換をバランにて行い送信機へ1 Coaxial cable with an electrical length of 1 /
3 Feed point, impedance and unbalance / balance conversion by balun to transmitter
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Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2007101098A JP4224864B2 (en) | 2007-03-10 | 2007-03-10 | Antenna device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2007101098A JP4224864B2 (en) | 2007-03-10 | 2007-03-10 | Antenna device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JP2008228257A JP2008228257A (en) | 2008-09-25 |
| JP4224864B2 true JP4224864B2 (en) | 2009-02-18 |
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| Application Number | Title | Priority Date | Filing Date |
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| JP2007101098A Expired - Fee Related JP4224864B2 (en) | 2007-03-10 | 2007-03-10 | Antenna device |
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Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103872434A (en) * | 2012-12-18 | 2014-06-18 | 北京信威通信技术股份有限公司 | Antenna for field installation and production method thereof |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5018946B2 (en) | 2009-10-13 | 2012-09-05 | ソニー株式会社 | antenna |
| JP5648653B2 (en) * | 2009-10-13 | 2015-01-07 | ソニー株式会社 | antenna |
| JP5848287B2 (en) * | 2012-07-25 | 2016-01-27 | 高橋 康文 | Antenna device |
| EP3608925A1 (en) | 2018-08-08 | 2020-02-12 | Rohde & Schwarz GmbH & Co. KG | Magnetic core, method for manufacturing a magnetic core and balun with a magnetic core |
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2007
- 2007-03-10 JP JP2007101098A patent/JP4224864B2/en not_active Expired - Fee Related
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103872434A (en) * | 2012-12-18 | 2014-06-18 | 北京信威通信技术股份有限公司 | Antenna for field installation and production method thereof |
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| Publication number | Publication date |
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| JP2008228257A (en) | 2008-09-25 |
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