JPS61210701A - Waveguide device - Google Patents
Waveguide deviceInfo
- Publication number
- JPS61210701A JPS61210701A JP5125985A JP5125985A JPS61210701A JP S61210701 A JPS61210701 A JP S61210701A JP 5125985 A JP5125985 A JP 5125985A JP 5125985 A JP5125985 A JP 5125985A JP S61210701 A JPS61210701 A JP S61210701A
- Authority
- JP
- Japan
- Prior art keywords
- waveguide
- sub
- mode
- cross
- transmission line
- 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.)
- Pending
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/16—Auxiliary devices for mode selection, e.g. mode suppression or mode promotion; for mode conversion
Landscapes
- Waveguides (AREA)
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
この発明は、低損失かつ高品質なマイクロ波通信信号の
伝送を要求される導波管伝送路に発生する不要モードな
らびに交差偏波成分を消去する導波管装置に関する。Detailed Description of the Invention (Industrial Application Field) This invention eliminates unnecessary modes and cross-polarization components that occur in waveguide transmission lines that require low-loss, high-quality microwave communication signal transmission. The present invention relates to a waveguide device for erasing.
(従来の技術)
マイクロ波伝送系において離れた場所に設置されている
マイクロ波アンテナと送受信器との入出力端子間を接続
する場合など、比較的長い距離にわたって低損失かつ高
品質な導波管伝送路が要求されることがある。一般に同
一周波数において、導波管はその断面形状が大きいほど
低損失であることから、上記のように特に低損失特性を
要求される導波管伝送路では通常邑該周波数帯に用いら
れる基本モード導波管よシも断面形状の大きないわゆる
オーバーサイズ導波管が用いられる。そして前記導波管
伝送路の両端、即ちアンテナや送受信器の入出力端の近
くでオーバーサイズ導波管と基本モード導波管との変換
器が設けられて整合がとられる。(Prior art) Waveguides with low loss and high quality can be used over relatively long distances, such as when connecting the input/output terminals of a microwave antenna and a transmitter/receiver that are installed in a remote location in a microwave transmission system. A transmission line may be required. In general, at the same frequency, the larger the cross-sectional shape of a waveguide, the lower the loss. Therefore, in waveguide transmission lines that require particularly low loss characteristics as described above, the fundamental mode used for the frequency band is usually As for the waveguide, a so-called oversized waveguide with a large cross-sectional shape is used. Then, converters between an oversized waveguide and a fundamental mode waveguide are provided at both ends of the waveguide transmission path, that is, near the input/output ends of the antenna and the transceiver to achieve matching.
(発明が解決しようとする問題点)
ところがオーバーサイズ導波管は基本モードの他に高次
モードのマイクロ波信号をも通過させてしまうので、導
波管の裏作誤差等に起因する不連続部分や断面形状の非
対称性、あるいは前記変換器の不連続性などによ多発生
する高次モードや交差偏波成分が一旦この伝送路内に混
入すると、これらの高次モードや交差偏波成分は変換器
で整合されずに反射して伝送線路内に閉じこめられる。(Problem to be solved by the invention) However, since oversized waveguides allow microwave signals in higher order modes to pass in addition to the fundamental mode, discontinuous portions caused by errors in the fabrication of the waveguide, etc. Once higher-order modes and cross-polarization components that often occur due to cross-sectional shape asymmetry, discontinuity of the converter, etc. enter this transmission path, these higher-order modes and cross-polarization components It is not matched by the converter and is reflected and confined within the transmission line.
このようにして伝送路は高次モードや交差偏波成分に対
して一種の共振器として作用し、伝送路の通過特性に共
振現象として現われることがある。この共振は伝送信号
の遅延特性を着るしく劣化させることとなり、高品質な
伝送特性が得られないという欠点があった。この発明は
、以上の欠点を除去し、高品質なマイクロ波信号の伝送
が可能な低損失導波管伝送路を提供することを目的とし
ている。In this way, the transmission line acts as a type of resonator for higher-order modes and cross-polarized components, which may appear as a resonance phenomenon in the transmission characteristics of the transmission line. This resonance seriously deteriorates the delay characteristics of the transmitted signal, resulting in the disadvantage that high-quality transmission characteristics cannot be obtained. An object of the present invention is to eliminate the above-mentioned drawbacks and provide a low-loss waveguide transmission line that is capable of transmitting high-quality microwave signals.
(問題点を解決するための手段)
本発明は上記の目的を達成するため次のような構成とな
っている。(Means for Solving the Problems) In order to achieve the above object, the present invention has the following configuration.
即ち、基本モードの他に高次モードのマイクロ波信号が
伝搬しうるオーバーサイズの導波管と同じ断面を有する
主導波管の外周に、該主導波管との結合孔を介して前記
高次モードのマイクロ波信号のみを結合吸収させる副導
波管と交差偏波成分のみを結合吸収させる副導波管の両
者又はいずれか一方を有する導波管装置である。That is, the high-order mode is connected to the outer periphery of the main waveguide, which has the same cross section as an oversized waveguide through which microwave signals of higher-order modes in addition to the fundamental mode can propagate, through coupling holes with the main waveguide. This is a waveguide device having both or one of a sub-waveguide that couples and absorbs only a mode microwave signal and a sub-waveguide that couples and absorbs only a cross-polarized wave component.
(作 用)
1つの導波管の側面に他の導波管を設は両者間に適切な
形状寸法の結合孔を設けることによ)、特定モード或い
は特定偏波のt磁波を前記他の導波管へ導くことができ
る。本発明の導波管装置は高次モードのマイクロ波が伝
搬し得るオーバーサイズの主導波管の外周に結合孔を介
して前記高次モードのマイクロ波のみを結合吸収させる
副導管と交差偏波成分のみを結合吸収させる副導波管の
両者又はいずれか一方が設けられているので、本発明の
導波管装置に接続される導波系の導波管の製作誤差等に
起因する不連続部分や断面形状の非対称性或いは本発明
導波管装置に接続される基本モード導波管への変換器の
不連続性等により発生した高次モードの電磁波や交差偏
波成分が本発明導波管装置内へ混入してきてもその大部
分が結合孔を介して副導波へ導かれ副導波管内部に設け
られた吸収体や無反射終端器に吸収される。従って高次
モードや交差偏波成分が変換器での不整合により反3
゛
射されて主導波管内に閉じ込められるということがなく
なり、そのため伝送路の通過特性に共振現象とし現われ
ることがなくなる。この共振現象は伝送信号の遅延特性
を著しく劣化させこのため伝送特性の品質が著しく低下
するのであるが、本発明の導波管装置においてはこの共
振現象が起らぬため伝送特性の品質の低下を回避するこ
とができる。(Function) By installing another waveguide on the side surface of one waveguide, a coupling hole of an appropriate shape and size is provided between the two waveguides. It can be guided into a waveguide. The waveguide device of the present invention has an oversized main waveguide through which high-order mode microwaves can propagate, and a sub-conduit that couples and absorbs only the high-order mode microwaves through coupling holes, and a cross-polarized waveguide. Since both or one of the sub-waveguides that couple and absorb only the components are provided, there is no discontinuity due to manufacturing errors of the waveguide of the waveguide system connected to the waveguide device of the present invention. Higher-order mode electromagnetic waves and cross-polarized components generated by the asymmetry of parts or cross-sectional shapes or the discontinuity of the converter to the fundamental mode waveguide connected to the waveguide device of the present invention are transmitted to the waveguide of the present invention. Even if it enters the tube device, most of it is guided to the sub-waveguide through the coupling hole and absorbed by the absorber and non-reflection terminator provided inside the sub-waveguide. Therefore, higher-order modes and cross-polarization components are caused by mismatching in the converter.
This eliminates the possibility that the light is radiated and confined within the main waveguide, and therefore does not appear as a resonance phenomenon in the transmission characteristics of the transmission path. This resonance phenomenon significantly deteriorates the delay characteristics of the transmitted signal, resulting in a significant deterioration in the quality of the transmission characteristics, but in the waveguide device of the present invention, this resonance phenomenon does not occur, so the quality of the transmission characteristics deteriorates. can be avoided.
(実施例) 以下本発明の実施例を図面に基づいて説明する。(Example) Embodiments of the present invention will be described below based on the drawings.
第1図は本発明の導波管装置の一部断面の構造斜視図で
ある。同図において主導波管2は伝送路と同一の断面形
状を有し、伝送路の途中に挿入される。この主導波管の
、基本モード(TE 、、モード)の電界方向1に平行
な側面には複数個の結合孔5を介して副導波管3が設け
られている。FIG. 1 is a partially sectional structural perspective view of the waveguide device of the present invention. In the figure, the main waveguide 2 has the same cross-sectional shape as the transmission line, and is inserted in the middle of the transmission line. A sub-waveguide 3 is provided on a side surface of the main waveguide parallel to the electric field direction 1 of the fundamental mode (TE mode) via a plurality of coupling holes 5 .
この副導波管3の断面形状は、副導波管3のTE 、o
Dモードの管内波長と主導波管2のTM 、:モ° 4
゛
一部の管内波長が等しくなるような寸法を有している。The cross-sectional shape of this sub-waveguide 3 is TE of the sub-waveguide 3, o
D-mode pipe wavelength and main waveguide 2 TM :Mo° 4
``It has dimensions such that some wavelengths within the tube are the same.
このため、結合孔の数を最適となるように選べば、主導
波管2の中に閉じこめられているTM 、、。モードの
ほとんどすべてを副導波管3へ訪導することができる。Therefore, if the number of coupling holes is optimally selected, the TM,..., is confined within the main waveguide 2. Almost all modes can be guided to the sub waveguide 3.
さらにとの副導波管3の両端には無反射終端M。Furthermore, non-reflection terminations M are provided at both ends of the sub-waveguide 3.
器4が挿入されており、ここで不要TBo+ モード
を吸収することができる。また基本モード(TE□、。A device 4 is inserted, which can absorb unnecessary TBo+ modes. Also basic mode (TE□,.
モード)の副導波管3への漏洩については、結合孔を充
分に小さくすることによってほとんど無視することがで
きる。Leakage of mode) to the sub-waveguide 3 can be almost ignored by making the coupling hole sufficiently small.
さらに、結合孔の間隔を、TE、1゜モードの管内波長
の174に選ぶことで、結合孔は主導波管のVSWR特
性に影響を与えることはない。Furthermore, by selecting the spacing between the coupling holes to be 174, which corresponds to the tube wavelength of the TE, 1° mode, the coupling holes do not affect the VSWR characteristics of the main waveguide.
一方、同図において基本モード電界方向1に直角な主導
波管2の側面には管軸方向に沿って幅の狭くかつ円形導
波管の断面形状を変化させない程度の長さを有するスリ
ット7が数カ所設けられている。このスリットは交差偏
波成分に対する結合孔として作用する。すなわち、伝送
路内に発生した交差偏波成分はこのスリットを介して副
導波管6へ誘導される。さらに1誘導された交差偏波成
分は副導波管6のスリットとの対面に設けられている電
波吸収体8に吸収される。1.た、前述のようにスリッ
トは基本モードの電界方向に直角に設けられでいること
から、この場合もスリットが伝送信号である正偏波のT
E 、I。モードに与える影響はない。On the other hand, in the figure, on the side surface of the main waveguide 2 perpendicular to the fundamental mode electric field direction 1, there is a slit 7 along the tube axis direction, which has a narrow width and a length that does not change the cross-sectional shape of the circular waveguide. There are several locations. This slit acts as a coupling hole for cross-polarized components. That is, cross-polarized components generated within the transmission path are guided to the sub-waveguide 6 via this slit. Further, the single induced cross-polarized component is absorbed by the radio wave absorber 8 provided on the side facing the slit of the sub waveguide 6. 1. In addition, as mentioned above, the slit is provided perpendicular to the direction of the electric field of the fundamental mode, so in this case as well, the slit is located at the T of the positive polarized wave that is the transmission signal.
E, I. No effect on mode.
以上は円形導波管のTM。1゜モードを消去する場合に
ついて説明したが、他の断面形状の導波管や他の高次モ
ードを消去する場合についても、上記と同様の考えによ
りそれらに適切な方法で消去することが可能であること
はいうまでもない。The above is a circular waveguide TM. Although we have explained the case of canceling the 1° mode, it is also possible to cancel waveguides with other cross-sectional shapes and other higher-order modes using the same method as above using the appropriate method. Needless to say, it is.
また上記は高次モードの消去装置と交差偏波成分の消去
装置を同時に具備している場合の実施例を示しているが
、これらのうちどちらか一方を必要に応じて設ける場合
においても有効な効果を発揮することができる。さらに
上記の例でTM 、、モードのみを消去する場合は、円
形導波管のまわりに同一の形状を有する四個の副導波管
3を90°おきにならべれば本装置自身で発生する交差
偏波成分は無視できるほど小さな値とすることができる
。Furthermore, although the above example shows an example in which a high-order mode canceling device and a cross-polarization component canceling device are provided at the same time, it is also effective when one of these is provided as necessary. It can be effective. Furthermore, in the above example, if you want to erase only the TM mode, you can generate it by this device itself by arranging four sub-waveguides 3 having the same shape at 90° intervals around the circular waveguide. The cross-polarization component can be set to a negligibly small value.
(発明の効果)
本発明の導波管装置は以上述べたような構成と作用によ
り、主導波管内に混入して来た高次モードのマイクロ波
信号や交差偏波成分等の不要成分を副導波管の方へ導き
吸収してしまうのでこれら不要成分に起因する伝送特性
の品質劣化を回避することができるという利点があシ、
その結果、長距離伝送のように、特に低損失特性を要求
されるために高次モードのマイクロ波をも伝送してしま
うオーバーサイズ導波管を用いている伝送路の途中に本
導波管装置を挿入することにより伝送路の伝送特性の劣
化を防止することができるという利点がある。(Effects of the Invention) With the configuration and operation described above, the waveguide device of the present invention subtracts unnecessary components such as higher-order mode microwave signals and cross-polarized components that have entered the main waveguide. Since it is guided toward the waveguide and absorbed, it has the advantage that it is possible to avoid quality deterioration of transmission characteristics caused by these unnecessary components.
As a result, this waveguide is used in the middle of a transmission line that uses an oversized waveguide that also transmits high-order mode microwaves because low loss characteristics are particularly required for long-distance transmission. There is an advantage that deterioration of the transmission characteristics of the transmission path can be prevented by inserting the device.
第1図は本発明の導波管装置の実施例の構成を示す斜視
図である。
・ 7 ・
3・・・副導波管、 4・・・無反射終端器、 5・
・・結合孔、 6・・・副導波管、 7・・・スリ
ット、8・・・電波吸収体FIG. 1 is a perspective view showing the configuration of an embodiment of the waveguide device of the present invention.・ 7 ・ 3...Sub-waveguide, 4...Reflection-free terminator, 5.
...Coupling hole, 6...Sub waveguide, 7...Slit, 8...Radio wave absorber
Claims (1)
うるオーバーサイズの導波管と同じ断面を有する主導波
管の外周に、該主導波管との結合孔を介して高次モード
のマイクロ波信号のみを結合吸収させる副導波管と交差
偏波成分のみを結合吸収させる副導波管の両者又はいず
れか一方を有することを特徴とする導波管装置。In addition to the fundamental mode, microwave signals in higher-order modes are connected to the outer periphery of the main waveguide, which has the same cross section as the oversized waveguide, through which microwave signals in higher-order modes can propagate, through coupling holes with the main waveguide. 1. A waveguide device comprising: a sub-waveguide that couples and absorbs only wave signals; and/or a sub-waveguide that couples and absorbs only cross-polarized components.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5125985A JPS61210701A (en) | 1985-03-14 | 1985-03-14 | Waveguide device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5125985A JPS61210701A (en) | 1985-03-14 | 1985-03-14 | Waveguide device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61210701A true JPS61210701A (en) | 1986-09-18 |
Family
ID=12881945
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5125985A Pending JPS61210701A (en) | 1985-03-14 | 1985-03-14 | Waveguide device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61210701A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5410318A (en) * | 1994-03-25 | 1995-04-25 | Trw Inc. | Simplified wide-band autotrack traveling wave coupler |
-
1985
- 1985-03-14 JP JP5125985A patent/JPS61210701A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5410318A (en) * | 1994-03-25 | 1995-04-25 | Trw Inc. | Simplified wide-band autotrack traveling wave coupler |
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