JPH02189035A - Antenna system - Google Patents

Antenna system

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Publication number
JPH02189035A
JPH02189035A JP887489A JP887489A JPH02189035A JP H02189035 A JPH02189035 A JP H02189035A JP 887489 A JP887489 A JP 887489A JP 887489 A JP887489 A JP 887489A JP H02189035 A JPH02189035 A JP H02189035A
Authority
JP
Japan
Prior art keywords
phase
wave
outputs
fading
polarizer
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
Application number
JP887489A
Other languages
Japanese (ja)
Inventor
Katsuhiko Aoki
青木 克比古
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 JP887489A priority Critical patent/JPH02189035A/en
Publication of JPH02189035A publication Critical patent/JPH02189035A/en
Pending legal-status Critical Current

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  • Radio Transmission System (AREA)

Abstract

PURPOSE:To prevent an interference wave and to improve the reliability by a stationary and simple circuit by applying phase shift processing to two outputs of an orthogonally polarized branching filter including a wave reflected in a sea surface and synthesizing the result of the processing. CONSTITUTION:A 90 deg. polarizer 2, an orthogonally polarized branching filter (OMT) 3 and a phase shifter 51 feeding a phase lead of 45 deg. or no phase shift to an output of the polarizer, a phase shifter 52 feeding a phase lag of 45 deg. or a phase shift of + or -90 deg. and a combiner(COMB) 6 combining outputs of both the phase shifters 51, 52 are provided to the system. Thus, it is notified that a 45 deg. component appears in combined X, Y component of a direct wave and an interference wave, and the two outputs of the polarizer are combined by feeding phase shifts of +45 deg., -45 deg. to the outputs respectively. Since fading due to the reflection in the sear surface is eliminated, fading is eliminated inexpensively with high reliability and a small and stationary circuit.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、アンテナ装置に関し、特に衛星通信など無
線通信分野における海面反射によるフェージングによる
干渉波の防止を図ったものに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an antenna device, and particularly to an antenna device that prevents interference waves due to fading due to sea surface reflection in the field of wireless communication such as satellite communication.

〔従来の技術〕[Conventional technology]

第5図は例えば「電波研季報: Vol、34.特6.
 March 1988 Jに示された従来のフェージ
ングによる干渉波除去装置を示すブロック図であり、図
において、1はアンテナ、2は円偏波発生器(pola
rizerH以降90@−POLと呼ぶ)、3は直交偏
波分波器(Ortho−sode transduce
r;以降OMTと呼ぶ)、4は減衰器41と移相器42
とからなる干渉波除去回路である。なお、上記文献では
2と3とをまとめて90”−3dB  ハイブリッド3
1と呼んでいる。
Figure 5 shows, for example, "Radio Research Quarterly Report: Vol. 34.Special 6.
It is a block diagram showing a conventional interference wave removal device using fading shown in March 1988 J. In the figure, 1 is an antenna, 2 is a circularly polarized wave generator (pola
90@-POL from riserH onwards), 3 is an ortho-sode transduce
r; hereinafter referred to as OMT), 4 is an attenuator 41 and a phase shifter 42
This is an interference wave removal circuit consisting of. In addition, in the above document, 2 and 3 are combined into 90"-3dB hybrid 3
It is called 1.

次に動作について説明する。Next, the operation will be explained.

インマルサット海事衛星通信では衛星仰角5度以上の海
域を通信のサービス領域としている。ところで、左旋円
偏波(正旋成分)が海面に入射した場合、反射波は左旋
(正旋)と右旋(逆旋)成分とに分離され、かつ仰角5
度以上であれば逆旋成分が正旋成分より大きくなること
が知られている。
Inmarsat Maritime Satellite Communication's communication service area is the sea area where the satellite elevation angle is 5 degrees or more. By the way, when a left-handed circularly polarized wave (normal rotation component) is incident on the sea surface, the reflected wave is separated into left-handed (normal rotation) and right-handed (anti-rotation) components, and the angle of elevation is 5.
It is known that the anti-rotational component becomes larger than the normal-rotating component if the rotational angle is greater than 1°.

一方、円偏波アンテナの端子T3には直接波である正旋
成分と海面反射による正旋成分Eっとの和が、またT4
には海面反射による逆旋成分ELが以下のように出力さ
れる。
On the other hand, at the terminal T3 of the circularly polarized antenna, the sum of the normal rotation component, which is a direct wave, and the normal rotation component E, which is a direct wave, is transmitted to the terminal T3.
The anti-rotation component EL due to sea surface reflection is output as follows.

T 3 : Eo  + Et  e j(φし900
〉T4:E、Ie’ハ 通常の円偏波アンテナでは端子T4に出力される反射に
よって生じる逆旋成分は終端抵抗により無駄な電力とし
て消費される。しかし、上式から理解されるように73
.T4の両出力をElとELの振幅を等しく、かつ逆位
相となるように加えるとEII8Jφ翼とEL8Jfφ
L−11g+’)の両成分は互いに相殺され、直接波成
分E0のみが取り出されることがわかる。第5図は、こ
のような原理に基づき構成されたフェージング除去機能
を示す、実際の構成はここで述べた原理を基に、合成器
、減衰器及び移相器による挿入損等を避けるため低雑音
増幅器(LNA)を2台用いており、OMTの2つの出
力の直後にそれぞれ挿入されている。
T 3: Eo + Et e j (φ and 900
> T4: E, Ie' C In a normal circularly polarized antenna, the anti-rotating component generated by reflection output to the terminal T4 is consumed as wasted power by the terminating resistor. However, as understood from the above formula, 73
.. When both outputs of T4 are added so that El and EL have equal amplitudes and opposite phases, EII8Jφ blade and EL8Jfφ
It can be seen that both components of L-11g+') cancel each other out, and only the direct wave component E0 is extracted. Figure 5 shows a fading removal function configured based on this principle.The actual configuration is based on the principle described here, with a low Two noise amplifiers (LNA) are used, each inserted immediately after the two outputs of the OMT.

この方式を採用すると振幅の制御はせず逆旋成分の移相
のみを制御して常に振幅が最大になるようにすることも
可能である。
If this method is adopted, it is also possible to control only the phase shift of the anti-rotational component without controlling the amplitude so that the amplitude is always maximized.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

従来の干渉波除去装置は以上のように構成されているの
で、小型アンテナ、特に開口径が10λ(λ:波長)以
下のようなアンテナで、かつ広帯域の高周波回路での干
渉波除去を行う場合、アンテナの背面に干渉波除去回路
を設置する必要があるので、干渉波除去回路付アンテナ
装置の実現が困難であった。また、干渉波の干渉量に応
じて、可変減衰量を与える減衰器(ATT)が必要とな
り、地球局のG/T性能の面からLNA (低雑音増幅
器)が必要となる。さらに移相器と減衰器を干渉量に応
じて制御する必要があった。
Conventional interference wave removal devices are configured as described above, so when performing interference wave removal with a small antenna, especially an antenna with an aperture diameter of 10λ (λ: wavelength) or less, and a wideband high frequency circuit. Since it is necessary to install an interference wave removal circuit on the back side of the antenna, it has been difficult to realize an antenna device with an interference wave removal circuit. Furthermore, an attenuator (ATT) that provides variable attenuation is required depending on the amount of interference of interference waves, and an LNA (low noise amplifier) is required from the perspective of G/T performance of the earth station. Furthermore, it was necessary to control the phase shifter and attenuator according to the amount of interference.

この発明は上記のような従来のものの問題点を解決する
ためになされたもので、回路を小型化できるとともに簡
単な回路とし、かつ一定の結合量をもたせて干渉波防止
(低?:Ii)を実現できるアンテナ装置を得ることを
目的とするものである。
This invention was made to solve the above-mentioned problems of the conventional circuit, and it is possible to miniaturize the circuit, make it simple, and provide a certain amount of coupling to prevent interference waves (low?: Ii). The purpose of this invention is to obtain an antenna device that can realize the following.

〔課題を解決するための手段〕[Means to solve the problem]

この発明に係るアンテナ装置は、90@位相蓋板(90
”−Polarizer)と偏分波器(OMT)及び偏
分波器の一方の出力に45#位相(45”進み)または
00位相を与える移相器、偏分波器の他方の出力に一4
5@位相(45°遅れ)または±90°位相を与える移
相器、さらに両移相器の出力を合成する合成器(COM
B)を設けたものである。
The antenna device according to the present invention has a 90@phase cover plate (90
"-Polarizer) and a polarization splitter (OMT), a phase shifter that gives a 45# phase (45" lead) or a 00 phase to one output of the polarization splitter, and a -Polarizer to the other output of the polarization splitter.
A phase shifter that provides 5@phase (45° delay) or ±90° phase, and a synthesizer (COM) that combines the outputs of both phase shifters.
B).

〔作用〕[Effect]

この発明においては、上述のように構成することにより
、OMT出力の直交2偏波成分を移相処理したものを合
成するようにしたので、小型、簡単かつ固定の回路によ
りフェージングを除去できる。
In the present invention, with the above-described configuration, two orthogonal polarized components of the OMT output are phase-shifted and synthesized, so that fading can be removed using a small, simple, and fixed circuit.

〔実施例〕〔Example〕

以下、この発明の一実施例を図について説明する。第1
図は本発明の一実施例によるアンテナ装置を示し、図に
おいて、第5図と同一符号は同一のものを示す、51は
45°移相器、52は一45°移相器であり、この図の
場合、OMT3のX−POL成分方向(水平方向)に合
成器6を設けている。また12はフェージングを顕著に
生ずる角度が一般には接地角で10″′〜20”にある
ことに着目し、その角度に対応するアンテナ仰角に応じ
てフェージング防止回路を0N10FFするスイッチで
ある。なお、この回路は衛星が右旋偏波を使用している
場合のフェージング防止回路であり、衛星が左旋円偏波
の場合は第1図の6と12がY−POL成分方向(垂直
方向)に入れ換わる以外は同じ回路でよい。
An embodiment of the present invention will be described below with reference to the drawings. 1st
The figure shows an antenna device according to an embodiment of the present invention. In the figure, the same reference numerals as in FIG. In the case of the figure, the synthesizer 6 is provided in the X-POL component direction (horizontal direction) of the OMT 3. Also, 12 is a switch that turns the fading prevention circuit ON to 10FF in accordance with the antenna elevation angle corresponding to the angle where fading occurs noticeably, generally in the ground angle of 10'' to 20''. This circuit is a fading prevention circuit when the satellite uses right-handed circular polarization, and when the satellite uses left-handed circular polarization, 6 and 12 in Figure 1 are in the Y-POL component direction (vertical direction). The same circuit is sufficient except that it is replaced with .

以下、数式を用いて本実施例を説明する。The present embodiment will be described below using mathematical formulas.

一般に衛星が楕円偏波を使用している場合、その到来波
をX、Y成分に分けると、 となる。
Generally, when a satellite uses elliptically polarized waves, dividing the arriving wave into X and Y components gives the following equation.

ここで、E、、ELはそれぞれ右旋成分、左旋成分で、
Tは楕円の長軸がX軸に対してなす角(チルト角と呼ば
れる)である。
Here, E, EL are the dextrorotatory component and the levorotary component, respectively,
T is the angle (referred to as tilt angle) that the long axis of the ellipse makes with the X axis.

第2図は海上船舶に搭載したアンテナが衛星からの直接
波と海面からの反射波を受ける模様を示す、第2図にお
いて、7は船舶20に搭載されたアンテナ11の受信パ
ターンであり、8は衛星の電波の状態、9は海面からの
反射波、gは受信パターンの反射波方向の相対電界強度
である。また第3図は海面での反射係数を示す。また1
0は入射波の海面への接地角θ(=90”−入射角)を
示す。
Figure 2 shows how an antenna mounted on a marine vessel receives direct waves from a satellite and reflected waves from the sea surface. In Figure 2, 7 is the reception pattern of the antenna 11 mounted on a vessel 20, and 8 is the state of the satellite radio wave, 9 is the reflected wave from the sea surface, and g is the relative electric field strength in the direction of the reflected wave of the reception pattern. Figure 3 also shows the reflection coefficient at the sea surface. Also 1
0 indicates the grounding angle θ (=90″−incident angle) of the incident wave on the sea surface.

第4回はθが10@以上の場合のEx 、Ey  (入
射電界)と海面30からの反射波E’、、E’との関係
を描いたものである。つまり、0とみなしてよい、さて
(1)式の直接波および(3)式の反射波がアンテナに
入力したとき、90”POLを通過し、OMTのX、Y
方向成分の出力はそれぞれ次のようになる。つまり直接
波のOMT出力Eつ。+Evoは となる。また反射波のOMT出力Er8゜、E′7゜は ここで、rは海面の反射係数(振幅)、δは海面の反射
係数(位相)である。
The fourth part depicts the relationship between Ex, Ey (incident electric field) and reflected waves E', E' from the sea surface 30 when θ is 10@ or more. In other words, when the direct wave in equation (1) and the reflected wave in equation (3) are input to the antenna, they pass through 90"POL, and the X, Y of OMT
The output of each direction component is as follows. In other words, there are two direct wave OMT outputs. +Evo becomes. Further, the OMT outputs Er8° and E'7° of the reflected waves are here, r is the reflection coefficient (amplitude) of the sea surface, and δ is the reflection coefficient (phase) of the sea surface.

よって、 なお、周波数を10GHz以上とすると、δ=となる。Therefore, Note that when the frequency is 10 GHz or more, δ=.

ここで、Bは直接波と反射波の光路差による位相遅れに
相当する。
Here, B corresponds to a phase delay due to the optical path difference between the direct wave and the reflected wave.

よって、直接波と反射波を合成した出力E″8゜。Therefore, the combined output of the direct wave and reflected wave is E″8°.

E”V。はそれぞれ となる。E”V. are each becomes.

よって衛星が右旋円偏波の場合、EL−0となり・ となる、ここで第(方式の上式の()内の第2゜第3項
および下式の()内の第1項、第2項が反射波によって
生じる干渉波である。このうちgrはgより小さくて、
(7)式は近似的には次のようになる。
Therefore, if the satellite is right-handed circularly polarized, it becomes EL-0, where, The second term is the interference wave caused by the reflected wave. Among these, gr is smaller than g,
Equation (7) is approximated as follows.

上記と同じ< grを無視すればα[相]式は近似的に
従って「8゜e J 4十I!”1゜e−J7を作れば
合成波の電界Eは れば合成波の電界Eは B = f ELej tJ’         ・・
・(2)で示される。
Same as above < If gr is ignored, the α [phase] formula approximately follows: "8°e J 40I!" If 1°e-J7 is created, the electric field E of the composite wave is B = f ELej tJ'...
- Indicated by (2).

このように、本実施例によれば、直接波と干渉波の合成
X、Y成分に45°成分が現れることに着目し、偏分波
器の2つの出力にそれぞれ+45゜−45°の位相を与
えて合成することにより、海面反射によるフェージング
を除去するようにしたので、小型かつ固定の回路により
高い信頼性で安価にフェージングを除去することができ
る。
In this way, according to this embodiment, focusing on the fact that a 45° component appears in the combined X and Y components of the direct wave and interference wave, the two outputs of the polarization demultiplexer have a phase of +45° - 45°. Since fading due to sea surface reflection is removed by giving and combining the signals, fading can be removed with high reliability and at low cost using a small and fixed circuit.

なお、上記実施例では+4!y@移相器および一45″
移相器を用いたものを示したが、これらは相対的な位相
を与えればよいので、+45°移相器を06とすれば一
45″移相器を一90@移相器(右旋偏波の場合)、+
90°移相器(左旋偏波の場合)としてもよい。
In addition, in the above example, +4! y@phase shifter and -45″
Although the phase shifter is shown here, it is sufficient to give a relative phase, so if the +45° phase shifter is set to 06, the 145" phase shifter becomes the 190@ phase shifter (right rotation). For polarized waves), +
It may also be a 90° phase shifter (in the case of left-handed polarization).

また上記実施例ではOMT出力の直交2偏波成分を位相
処理し、合成することにより、干渉波(フェージング波
)を防止することとしたが、前述の(8)式およびaυ
式で示されるように、単にgを小さくすることによって
も同じ効果が得られる。
In addition, in the above embodiment, interference waves (fading waves) are prevented by performing phase processing and combining two orthogonal polarization components of the OMT output, but the above-mentioned equation (8) and aυ
As shown in the formula, the same effect can be obtained by simply reducing g.

このgを小さくする方法として、いわゆる低サイドロー
ブアンテナを使用すればよいが、単なる低サイドローブ
アンテナでは開口能率が下がる。
A so-called low side lobe antenna may be used as a method of reducing this g, but a mere low side lobe antenna will reduce the aperture efficiency.

よってここでは第6図に示すように仰角面内に非対称の
サイドロープを持つアンテナとすることにより、上記実
施例と同様の効果が期待できる。
Therefore, by using an antenna having asymmetric side ropes in the elevation plane as shown in FIG. 6, the same effects as in the above embodiment can be expected.

なお、このような特定面内(この場合仰角方向)で非対
称のサイドロープを作るには、アンテナの開口分布の位
相分布に3次15次コマ収差を与えればよい。
Note that in order to create such an asymmetrical side rope within a specific plane (in this case, in the elevation angle direction), it is sufficient to give a third-order and 15th-order coma aberration to the phase distribution of the aperture distribution of the antenna.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明に係るアンテナ装置によれば、
海面反射波を含む直交偏分波器の2つの出力を移相処理
して合成するようにしたので、固定かつ簡単な回路によ
り干渉波を防止でき、装置を小型で安価にでき、しかも
信顛性の高いものが得られる効果がある。
As described above, according to the antenna device according to the present invention,
Since the two outputs of the orthogonal polarization splitter, including the waves reflected from the sea surface, are phase-shifted and synthesized, interference waves can be prevented using a fixed and simple circuit, and the device can be made small and inexpensive, while also being highly reliable. It has the effect of obtaining something with high sexiness.

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

第1図は本発明の一実施例を示す図、第2図は海面反射
によるフェージングによる干渉波の経路を示す干渉概念
図、第3図は海水の反射特性(理論値)を示す図、第4
図は海面の反射の模式図、第5図は従来の実施例を示す
図、第6図は海面の方向の低サイドローブ化を図った非
対称形サイドロープ形状を示す図である。 図において、1はアンテナ、2は円偏波発生器、3は直
交偏分波器、51.52は移相器、6は合成器、12は
スイッチ、13はダミーロードである。
Fig. 1 is a diagram showing an embodiment of the present invention, Fig. 2 is an interference conceptual diagram showing the path of interference waves due to fading due to sea surface reflection, Fig. 3 is a diagram showing seawater reflection characteristics (theoretical values), 4
This figure is a schematic diagram of reflection on the sea surface, FIG. 5 is a diagram showing a conventional embodiment, and FIG. 6 is a diagram showing an asymmetric side rope shape that aims to reduce side lobes in the direction of the sea surface. In the figure, 1 is an antenna, 2 is a circularly polarized wave generator, 3 is an orthogonal polarization splitter, 51 and 52 are phase shifters, 6 is a combiner, 12 is a switch, and 13 is a dummy load.

Claims (1)

【特許請求の範囲】[Claims] (1)アンテナ装置において、 受信信号に基づき円偏波を発生する90°位相蓋板、該
90°位相蓋板の出力を相互に直交した2偏波に分離す
る偏分波器、該偏分波器の一方のポートに45°または
0°の進み位相を与える移相器、他方のポートに45°
または±90°の遅れ位相を与える移相器、該両移相器
の出力を合成する合成器からなるフェージング防止回路
を備えたことを特徴とするアンテナ装置。
(1) In the antenna device, a 90° phase cover plate that generates a circularly polarized wave based on a received signal, a polarization splitter that separates the output of the 90° phase cover plate into two mutually orthogonal polarized waves, and the polarization splitter A phase shifter that gives a 45° or 0° advance phase to one port of the wave shifter, and 45° to the other port.
Alternatively, an antenna device comprising a fading prevention circuit comprising a phase shifter that provides a delayed phase of ±90°, and a combiner that combines the outputs of both phase shifters.
JP887489A 1989-01-17 1989-01-17 Antenna system Pending JPH02189035A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP887489A JPH02189035A (en) 1989-01-17 1989-01-17 Antenna system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP887489A JPH02189035A (en) 1989-01-17 1989-01-17 Antenna system

Publications (1)

Publication Number Publication Date
JPH02189035A true JPH02189035A (en) 1990-07-25

Family

ID=11704831

Family Applications (1)

Application Number Title Priority Date Filing Date
JP887489A Pending JPH02189035A (en) 1989-01-17 1989-01-17 Antenna system

Country Status (1)

Country Link
JP (1) JPH02189035A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7791431B2 (en) * 2006-12-04 2010-09-07 Electronics And Telecommunications Research Institute 3-port orthogonal mode transducer and receiver and receiving method using the same

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7791431B2 (en) * 2006-12-04 2010-09-07 Electronics And Telecommunications Research Institute 3-port orthogonal mode transducer and receiver and receiving method using the same

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