JPH0116046B2 - - Google Patents
Info
- Publication number
- JPH0116046B2 JPH0116046B2 JP56156000A JP15600081A JPH0116046B2 JP H0116046 B2 JPH0116046 B2 JP H0116046B2 JP 56156000 A JP56156000 A JP 56156000A JP 15600081 A JP15600081 A JP 15600081A JP H0116046 B2 JPH0116046 B2 JP H0116046B2
- Authority
- JP
- Japan
- Prior art keywords
- polarization
- waveguide
- electromagnetic waves
- wave
- main
- 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
Links
- 230000010287 polarization Effects 0.000 claims description 29
- 230000008878 coupling Effects 0.000 claims description 12
- 238000010168 coupling process Methods 0.000 claims description 12
- 238000005859 coupling reaction Methods 0.000 claims description 12
- 239000006096 absorbing agent Substances 0.000 claims description 4
- 230000001902 propagating effect Effects 0.000 claims description 2
- 230000000694 effects Effects 0.000 description 5
- 230000006866 deterioration Effects 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/20—Frequency-selective devices, e.g. filters
- H01P1/213—Frequency-selective devices, e.g. filters combining or separating two or more different frequencies
- H01P1/2138—Frequency-selective devices, e.g. filters combining or separating two or more different frequencies using hollow waveguide filters
Landscapes
- Waveguide Switches, Polarizers, And Phase Shifters (AREA)
- Waveguide Aerials (AREA)
- Control Of Motors That Do Not Use Commutators (AREA)
Description
【発明の詳細な説明】
この発明は、多周波数帯の電磁波を円偏波で導
入する一次放射器の改良に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a primary radiator that introduces electromagnetic waves in multiple frequency bands in circularly polarized waves.
なお、ここでは説明を簡単にするために、二つ
の周波数帯に限定し、この二つの周波数帯の低い
周波数帯の電磁波をL、高い周波数帯の電磁波を
Hとして説明する。 In order to simplify the explanation, we will limit the explanation to two frequency bands, and of these two frequency bands, we will refer to the electromagnetic waves in the lower frequency band as L , and the electromagnetic waves in the higher frequency band as L.
This will be explained as H.
従来のこの種一次放射器としては第1図に示す
ものがあつた。 A conventional primary radiator of this type is shown in FIG.
図において、1はLを導入する方形導波管、2
は直交した偏波のL8aとH8bを分波する偏分
波器、3は主導波管、4は方形導波管の低域遮断
特性を用いた高域通過導波管、5はH8bを導入
する方形導波管、6はL8a,H8bの直線偏波
と円偏波との偏波を変換する偏波変換器、7は電
磁ホーンである。 In the figure, 1 is a rectangular waveguide introducing L , 2
is a polarization demultiplexer that separates orthogonal polarized waves L 8a and H 8b, 3 is a main waveguide, 4 is a high-pass waveguide using the low-cut characteristics of a rectangular waveguide, and 5 is H 8b is a rectangular waveguide that introduces it, 6 is a polarization converter that converts the linearly polarized wave and circularly polarized wave of L 8a and H 8b, and 7 is an electromagnetic horn.
いま、Lを送信波8a,Hを受信波8bとして
偏分波器2に導入された場合、Lの電磁波は偏波
変換器6により円偏波に変換され電磁ホーン7か
らアンテナに給電される。ところで、この電磁ホ
ーン7は開口部の寸法をLの周波数帯の波長に比
べて十分大きくとれない場合が通常であるため
に、開口部において反射波を生じる。開口部にお
けるLの反射波は逆の円偏波となつて反射され、
偏波変換器6により直線偏波に変換されHと同じ
偏波として主導波管3を伝搬し高域通過導波管4
に至る。しかしながら、方形導波管5には受信波
としてHのみ導入する必要性から、Lの周波数帯
で遮断域となるようにH面横断面寸法9を選定し
た高域通過導波管4によりLは反射され偏波変換
器6に至る。したがつて、偏波変換器には位相の
異なる2個のLの電磁波が導入されるために、楕
円偏波率が劣化する原因となる。 Now, when L is introduced into the polarization demultiplexer 2 as a transmitting wave 8a and H as a receiving wave 8b, the electromagnetic wave of L is converted into a circularly polarized wave by the polarization converter 6 and is fed to the antenna from the electromagnetic horn 7. . By the way, since the size of the aperture of this electromagnetic horn 7 cannot usually be made sufficiently large compared to the wavelength of the frequency band L , reflected waves are generated at the aperture. The reflected wave of L at the aperture is reflected as an opposite circularly polarized wave,
It is converted into a linearly polarized wave by the polarization converter 6, and propagates through the main waveguide 3 as the same polarized wave as H , and is transmitted through the high-pass waveguide 4.
leading to. However, since it is necessary to introduce only H as a received wave into the rectangular waveguide 5, L is It is reflected and reaches the polarization converter 6. Therefore, two L electromagnetic waves having different phases are introduced into the polarization converter, which causes deterioration of the elliptical polarization coefficient.
この従来の一次放射器は、以上のように構成さ
れているので、所望の楕円偏波率を得るために
は、電磁ホーンの反射を少なくしなければなら
ず、特に電磁ホーンの開口寸法を小さくすること
が必要な場合には、整合素子を用いても広帯域に
わたつて反射を少なくすることができないため所
望の楕円偏波率を得ることができないという欠点
があつた。 This conventional primary radiator is configured as described above, so in order to obtain the desired elliptical polarization, the reflection of the electromagnetic horn must be reduced, and in particular, the aperture size of the electromagnetic horn must be made small. When it is necessary to do this, even if a matching element is used, it is not possible to reduce reflection over a wide band, so there is a drawback that a desired elliptic polarization cannot be obtained.
この発明は、この欠点を解決するためになされ
たもので、電磁ホーンの開口寸法が小さくて、か
つ電磁ホーンに整合素子を用いることなく、所望
の楕円偏波率を得ることができる一次放射器を提
供するものである。 This invention was made to solve this drawback, and is a primary radiator that has a small aperture size and can obtain a desired elliptical polarization without using a matching element in the electromagnetic horn. It provides:
以下、第2図に示すこの発明の一実施例につい
て説明する。 An embodiment of the present invention shown in FIG. 2 will be described below.
第2図において、1はLを導入する方形導波
管、2は偏分波器、3は主導波管、4は高域通過
導波管、5はHを導入する方形導波管、6は偏波
変換器、7は電磁ホーン、11は主導波管3のE
面に設けえられた結合孔、12は共振素子、13
は分岐導波管、14は分岐導波管に設けられた電
波吸収体である。 In Figure 2, 1 is a rectangular waveguide that introduces L , 2 is a polarization splitter, 3 is a main waveguide, 4 is a high-pass waveguide, 5 is a rectangular waveguide that introduces H , and 6 is a polarization converter, 7 is an electromagnetic horn, and 11 is E of the main waveguide 3.
A coupling hole provided in the surface, 12 is a resonant element, 13
14 is a branch waveguide, and 14 is a radio wave absorber provided in the branch waveguide.
いま、主導波管3にHと電磁ホーン7の反射さ
れたLの波が伝搬している場合、結合孔11に取
りつけられた共振素子12はLの波に対しては、
ほとんど影響しないが、Hの波に対しては直列共
振状態になるような寸法になつている。一方高域
通過導波管4はH面横断面寸法9がLの周波数で
遮断域となるように選定されており、さらに高域
通過導波管4は結合孔11からの位置がLの波に
対してほぼ近似的に
λL/4(1+2N)
ただし、
λL:Lの周波数帯の中心周波数での管内波長
N:0または任意の正の整数
なる寸法10だけ離して配置している。 Now, when the H wave and the L wave reflected from the electromagnetic horn 7 are propagating in the main wave tube 3, the resonant element 12 attached to the coupling hole 11 responds to the L wave as follows.
Although it has almost no effect, the dimensions are such that it will be in a series resonance state for H waves. On the other hand, the high-pass waveguide 4 is selected so that the H-plane cross-sectional dimension 9 becomes a cutoff region at the frequency L , and the position from the coupling hole 11 of the high-pass waveguide 4 is selected so that the cutoff region is at the frequency L. approximately λ L /4(1+2N) where λ L : tube wavelength at the center frequency of the frequency band L N: 0 or any positive integer, which is a dimension of 10.
したがつて、主導波管3に導入されたLの波は
高域通過導波管4で反射され結合孔11を介し
て、分岐導波管13に入る。 Therefore, the L wave introduced into the main waveguide 3 is reflected by the high-pass waveguide 4 and enters the branch waveguide 13 via the coupling hole 11.
また、分岐導波管13には電波吸収体14を設
けているので、分岐導波管に入つたLの波は吸収
される。一方、主導波管3に導入されたHの波に
対しては結合孔11の共振素子12の位置で電気
的に短絡された状態になり、Hの波は結合孔11
の影響をほとんど受けずに高域通過導波管4に至
り方形導波管5に導入される。 Further, since the branch waveguide 13 is provided with a radio wave absorber 14, the L wave entering the branch waveguide is absorbed. On the other hand, the H wave introduced into the main waveguide 3 is electrically short-circuited at the position of the resonant element 12 of the coupling hole 11, and the H wave enters the coupling hole 11.
It reaches the high-pass waveguide 4 with almost no influence from the waveguide and is introduced into the rectangular waveguide 5.
この発明による一次放射器はこのような動作を
するので、電磁ホーン7で反射波を生じても楕円
偏波率を劣化することなく所望の楕円偏波率を得
る一次放射器が実現でどきるとともに、電磁ホー
ン7の開口寸法を小さくすることができ、かつ整
合素子を用いる必要もないという効果を有してい
る。 Since the primary radiator according to the present invention operates in this way, it is possible to realize a primary radiator that obtains the desired elliptical polarization without deteriorating the elliptical polarization even if a reflected wave is generated by the electromagnetic horn 7. Additionally, the opening size of the electromagnetic horn 7 can be reduced, and there is no need to use a matching element.
第3図はこの発明の他の実施例を示すもので、
第2図に示した結合孔11を主導波管3のE面に
設けるかわりに、主導波管3のH面に設けたもの
であり、同様な効果を有している。 FIG. 3 shows another embodiment of this invention,
Instead of providing the coupling hole 11 shown in FIG. 2 on the E surface of the main wave tube 3, it is provided on the H surface of the main wave tube 3, and has the same effect.
なお、以上は主導波管3と高域通過導波管4が
方形導波管の場合について説明しているが、円形
導波管の場合でも高域通過導波管の内径寸法がL
の周波数に対して遮断域となるように選定されて
いれば同様な効果が得られる。 The above explanation is based on the case where the main waveguide 3 and the high-pass waveguide 4 are rectangular waveguides, but even in the case of circular waveguides, the inner diameter of the high-pass waveguide is L.
A similar effect can be obtained if the cutoff range is selected for the frequency of .
また、共振素子12のかわりに通過帯域がL、
阻止帯域がHとなるように選定されたワツフル形
波器を用いても同じような効果が得られる。 Also, instead of the resonant element 12, the passband is L ,
A similar effect can be obtained by using a Watsuful waveform generator selected so that the stopband is H.
さらに、以上は電磁ホーン7が1個の場合につ
いて説明しているが、複数の電磁ホーンを用いた
構成の場合にも同様の効果が得られる。 Furthermore, although the case in which the number of electromagnetic horns 7 is one is described above, similar effects can be obtained in the case of a configuration using a plurality of electromagnetic horns.
第1図は従来の一次放射器を示す図、第2図、
第3図はこの発明による各実施例を示す図であ
る。図中、1,5は方形導波管、2は偏分波器、
3は主導波管、4は高域通過導波管、6は偏波変
換器、7は電磁ホーン、11は結合孔、12は共
振素子、13は分岐導波管、14は電波吸収体で
ある。なお、図中、同一あるいは相当部分には同
一符号を付して示してある。
Figure 1 shows a conventional primary radiator; Figure 2;
FIG. 3 is a diagram showing each embodiment according to the present invention. In the figure, 1 and 5 are rectangular waveguides, 2 is a polarization splitter,
3 is a main waveguide, 4 is a high-pass waveguide, 6 is a polarization converter, 7 is an electromagnetic horn, 11 is a coupling hole, 12 is a resonance element, 13 is a branch waveguide, and 14 is a radio wave absorber. be. In the drawings, the same or corresponding parts are denoted by the same reference numerals.
Claims (1)
波数帯の電磁波Hを導入し、直交した偏波の電磁
波LとHを分波する偏分波器と、上記偏分波器に
設けられた結合孔に接続され、上記電磁波Lを導
入する方形導波管と、上記偏分波器の一端に接続
され、直線偏波と円偏波との偏波を変換する偏波
変換器と、上記偏波変換器に接続された電磁ホー
ンと、上記偏分波器の他端に接続された主導波管
とから構成される一次放射器において、上記主導
波管を伝搬する多周波数帯の同じ偏波の電磁波か
ら低い周波数帯の電磁波を分波し、かつ吸収する
ように、上記主導波管に結合孔を設け、上記主導
波管の結合孔から低い周波数帯の電磁波に対して
遮断域となる高域通過導波管を上記主導波管の管
内波長の4分の1、またはその奇数倍に近い長さ
だけ離して設けるとともに、上記主導波管の結合
孔を介して接続された分岐導波管部に波器と電
波吸収体を設けたことを特徴とする一次放射器。1. A polarization demultiplexer that introduces electromagnetic waves L in a low frequency band and electromagnetic waves H in a high frequency band in a multifrequency band, and separates the electromagnetic waves L and H with orthogonal polarization, and a polarization demultiplexer installed in the polarization demultiplexer. a rectangular waveguide connected to the coupling hole and introducing the electromagnetic wave L ; a polarization converter connected to one end of the polarization splitter and converting the polarization between linear polarization and circular polarization; In a primary radiator composed of an electromagnetic horn connected to a polarization converter and a main waveguide connected to the other end of the polarization splitter, the same polarization of multiple frequency bands propagating through the main waveguide is used. A coupling hole is provided in the main wave tube so as to separate and absorb electromagnetic waves in a low frequency band from the electromagnetic waves of the waves, and the coupling hole in the main wave tube serves as a cutoff area for electromagnetic waves in a low frequency band. A high-pass waveguide is provided at a distance close to a quarter of the internal wavelength of the main waveguide or an odd multiple thereof, and a branch waveguide is connected to the main waveguide through a coupling hole. A primary radiator characterized by having a wave transmitter and a radio wave absorber installed in the pipe section.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15600081A JPS5857803A (en) | 1981-09-30 | 1981-09-30 | Primary radiator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15600081A JPS5857803A (en) | 1981-09-30 | 1981-09-30 | Primary radiator |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5857803A JPS5857803A (en) | 1983-04-06 |
JPH0116046B2 true JPH0116046B2 (en) | 1989-03-22 |
Family
ID=15618139
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP15600081A Granted JPS5857803A (en) | 1981-09-30 | 1981-09-30 | Primary radiator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5857803A (en) |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5753103A (en) * | 1980-07-31 | 1982-03-30 | Thomson Csf | Antenna transducer |
-
1981
- 1981-09-30 JP JP15600081A patent/JPS5857803A/en active Granted
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5753103A (en) * | 1980-07-31 | 1982-03-30 | Thomson Csf | Antenna transducer |
Also Published As
Publication number | Publication date |
---|---|
JPS5857803A (en) | 1983-04-06 |
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