JPH0318101A - Constant current circuit for polarizer - Google Patents
Constant current circuit for polarizerInfo
- Publication number
- JPH0318101A JPH0318101A JP15306389A JP15306389A JPH0318101A JP H0318101 A JPH0318101 A JP H0318101A JP 15306389 A JP15306389 A JP 15306389A JP 15306389 A JP15306389 A JP 15306389A JP H0318101 A JPH0318101 A JP H0318101A
- Authority
- JP
- Japan
- Prior art keywords
- positive
- constant current
- waveguide coil
- negative
- coil
- 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
- 238000005388 cross polarization Methods 0.000 abstract description 5
- 230000005389 magnetism Effects 0.000 abstract 1
- 230000002441 reversible effect Effects 0.000 abstract 1
- 230000000694 effects Effects 0.000 description 5
- 230000010287 polarization Effects 0.000 description 4
- 239000000523 sample Substances 0.000 description 4
- 230000004907 flux Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 1
Landscapes
- Waveguide Switches, Polarizers, And Phase Shifters (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、交差偏波方式の無線通信にあって、垂直偏波
と水平偏波又は右旋.左旋の円偏波を識別するための受
信装置であるポーラライザの導波管コイルへ正・負逆向
きの定電流を供給する回路に関するものである.
〔従来の技術〕
無線通信方式では、通信容量を坩大させ且つ無線チャン
ネル間での干渉を避けるために、交差偏波方式を採用し
ている。すなわち、マイクロ波帯以上の周波数帯では、
直交する2偏波(円偏波における右旋偏波と左!!偏波
又は直線偏波における垂直偏波と水平偏波)を同時に利
用し、通信容量を1曽加させると共に無線チャンネル間
での干渉を避けることが多い.そのため、受信側では、
直交する2偏波を識別することが必要である.2偏波を
識別し得る能力を交差偏@識別度という。このような交
差偏波を識別する器具をポーラライザと称している.
ポーラライザは、第4図に示すように、パラボラアンテ
ナlの反射面の焦点位置に設置される一次放射器2内へ
組み込まれている.従来のポーラライザの一つに、第5
図に示すように、電波を受信するプローブ3の周囲に導
波管コイル4を設置し、該導波管コイル4に定電流を流
すことで、受信した電波にファラデ−回転を生起させ、
交差偏波織別を行うようにしたポーラライザ5がある。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to cross-polarized wireless communication, in which vertically polarized waves, horizontally polarized waves, or right-handed polarized waves are used. This relates to a circuit that supplies constant currents in opposite directions, positive and negative, to the waveguide coil of a polarizer, which is a receiving device for identifying left-handed circularly polarized waves. [Prior Art] In wireless communication systems, a cross-polarization system is adopted in order to expand communication capacity and avoid interference between wireless channels. In other words, in the frequency band above the microwave band,
By simultaneously using two orthogonal polarizations (right-handed polarization in circularly polarized waves and left-handed polarized waves or vertical and horizontal polarized waves in linearly polarized waves), the communication capacity is increased by 1, and the communication capacity is increased by 1. Interference with the system is often avoided. Therefore, on the receiving side,
It is necessary to distinguish between two orthogonal polarized waves. The ability to distinguish between two polarized waves is called cross-polarized@discrimination. A device that identifies such cross-polarized waves is called a polarizer. As shown in FIG. 4, the polarizer is incorporated into the primary radiator 2 installed at the focal point of the reflecting surface of the parabolic antenna l. One of the conventional polarizers is the fifth polarizer.
As shown in the figure, a waveguide coil 4 is installed around a probe 3 that receives radio waves, and a constant current is passed through the waveguide coil 4 to cause Faraday rotation in the received radio waves.
There is a polarizer 5 that performs cross-polarization discrimination.
而して、従来のこの種ポーラライザ5は、導波管コイル
4に定電流を流すか又は流さないかの二形態により、交
差偏波識別を行っている。つまり、例えば導波管コイル
4へ定電流を流した場合には、垂直偏波を受信し、導波
管コイル4へ電流を流さない場合には、水平偏波を受信
するようにして交差偏波識別を行っている。なお、4波
管コイル4へ流す電流を一定とする理由は、電流値の変
化により、交差偏波の位相角が変化し、正確な偏波識別
ができなくなるからである。Thus, the conventional polarizer 5 of this type performs cross-polarized wave discrimination by either passing a constant current through the waveguide coil 4 or not. In other words, for example, when a constant current is passed through the waveguide coil 4, vertically polarized waves are received, and when no current is passed through the waveguide coil 4, horizontally polarized waves are received and cross-polarized waves are received. Wave identification is performed. The reason why the current flowing through the four-wave tube coil 4 is kept constant is that a change in the current value changes the phase angle of the cross-polarized waves, making accurate polarization identification impossible.
このように、導波管コイル4への電流のON,OFFに
より、交差偏波織別を行うポーラライザ5にあっては、
導波管コイル4への残溜磁束の影響により交差偏波の位
相角が変化し、受信不良を来すという欠点があった。す
なわち、例えば導波管コイル4へ定電流を流して垂直偏
波を受信した後に、導波管コイル4への電流を遮断し、
水平偏波を受信すると、導波管コイル4に残溜磁束が発
生する。In this way, in the polarizer 5 that performs cross-polarization discrimination by turning on and off the current to the waveguide coil 4,
There is a drawback that the phase angle of the cross-polarized waves changes due to the influence of the residual magnetic flux on the waveguide coil 4, resulting in poor reception. That is, for example, after passing a constant current to the waveguide coil 4 and receiving vertically polarized waves, the current to the waveguide coil 4 is cut off,
When horizontally polarized waves are received, residual magnetic flux is generated in the waveguide coil 4.
そのため、水平偏波の位相角が水平状態からズレるよう
になる。水平B ’131の位相角がズレると、プロー
ブ3における水平偏波の受信状態が不良となることは言
うまでもないことである。Therefore, the phase angle of the horizontally polarized wave deviates from the horizontal state. It goes without saying that if the phase angle of the horizontal B' 131 deviates, the receiving condition of the horizontally polarized wave at the probe 3 will be poor.
本発明は、従来の前記課題に鑑みてこれを改良除去した
ものであって、位相角のズレを起こすことなく交M偏波
識別を可能ならしめるための正・逆り)lj!!可能な
定Ml/R回路を提供せんとするものである.
而して、前記課題を解決するために本発明が採用した手
段は、ポーラライザの導波管コイルへ正・負の電源を{
Jj給するための定電冶回路であって、正電源と負i¥
!源との間に、NPN接続されたトランジスタとPNP
接続されたトランジスタとを直列接続し、導波管コイル
の一端側を前記二種類のトランジスタ同士の中間接続点
へ接続すると共に、導波管コイルの他端測をアースへ接
続し、NPN トランジスタ及びPNP トランジ
スタのベース側に夫々正・負逆向きのダイオードを接続
している。The present invention has been made to improve and eliminate the above-mentioned conventional problems, and to enable cross-M polarization discrimination without causing a phase angle shift. ! The purpose is to provide a possible constant Ml/R circuit. Therefore, the means adopted by the present invention to solve the above problem is to supply positive and negative power to the waveguide coil of the polarizer.
A constant electric circuit for supplying Jj, with a positive power supply and a negative i\
! An NPN-connected transistor and a PNP
The connected transistors are connected in series, one end of the waveguide coil is connected to the intermediate connection point between the two types of transistors, and the other end of the waveguide coil is connected to ground. Diodes with opposite positive and negative directions are connected to the base side of the PNP transistor.
本発明にあっては、NPN トランジスタとPNP ト
ランジスタとを、正電源と負電源との間へ接続し、両ト
ランジスタの中間接続点を、導波管コイルの一端側へ接
続し、導波管コイルの他端則をアースへ接続している.
そして、前記両トランジスタのヘース側に夫々正・負逆
向きのダイオードを接続している.
これにより、正の電源を仇給した場合は、PNPトラン
ジスタのベース測に正のベース電圧が印加され、tiP
NP}ランジスタがON動作する。そして、PNP ト
ランジスタの工夫フタ側から導波管コイルへ正の定電流
が供給され、例えば垂直偏波を受信することが可能であ
る.
また負の電源を供給した場合は、NPN トランジスタ
のベース側へ負のベース電圧が印加され、該NPN ト
ランジスタがON動作する。そのため、アース側から導
波管コイルを通してNPN }ランジスタの工さツタ側
及びコレクタ則へ負の定電魔が流れる。In the present invention, an NPN transistor and a PNP transistor are connected between a positive power source and a negative power source, and the intermediate connection point of both transistors is connected to one end side of a waveguide coil. The other end of the line is connected to ground.
Then, diodes with opposite positive and negative directions are connected to the base sides of both transistors. As a result, when a positive power supply is supplied, a positive base voltage is applied to the base voltage of the PNP transistor, and tiP
NP} transistor turns on. Then, a constant positive current is supplied to the waveguide coil from the contrived lid side of the PNP transistor, making it possible to receive, for example, vertically polarized waves. Further, when a negative power source is supplied, a negative base voltage is applied to the base side of the NPN transistor, and the NPN transistor is turned on. Therefore, a negative constant electric current flows from the ground side through the waveguide coil to the NPN transistor side and collector side.
従って、導波管コイル6こ負の定電疏が流れることにな
り、例えば水平偏波を受信ずることが可能である。Therefore, a negative constant current flows through the waveguide coil 6, making it possible to receive, for example, horizontally polarized waves.
このように本発明にあっては、傳波管コイルへ正・負逆
向きの定電疏を疏している。導波管コイルへ流す定電疏
の向きを正・負逆向きに切り換えると、受信する電波の
位相角が両者間においてファラーデ一回転の効果により
90度異なることになる.そのため、正の定電疏を流し
た場合と、負の定電流を流した場合とにあって、垂直偏
波と水平偏波とを夫々受信することが可能であり、交差
偏波識別を行うことが可能である。As described above, in the present invention, the constant current wires having opposite positive and negative directions are connected to the wave tube coil. When the direction of the constant current flowing through the waveguide coil is switched between positive and negative, the phase angle of the received radio waves will differ by 90 degrees due to the effect of one Farade rotation. Therefore, it is possible to receive vertically polarized waves and horizontally polarized waves respectively when a positive constant current is applied and when a negative constant current is applied, making it possible to perform cross-polarized wave identification. Is possible.
〔実施例〕
以下に、本発明の構成を図面に示す実施例に基づいて説
明すると次の通りである。[Example] Below, the configuration of the present invention will be described based on an example shown in the drawings.
第1図は、本発明の第1の実施例に係る定電流回路図で
ある。同図に示す如く、この実施例にあっては、PNP
トランジスタl1とNPN トランジスタ12とのエ
ミッタ同士を接続している。そして、トランジスタl1
のコレクタ側を+IOVの正電源へ接続し、トランジス
タ12のコレクタ側を−10Vの負電源へ接続している
.また工さツタ同士の中間接続点を、導波管コイル13
の一端側へ接続している.導波管コイルl3の他端側は
、アースヘ′Wi続されている.またPNP トランジ
スタllのベース側は、正方向のダイオードl4を介し
てオペアンプl5の出力側に接続されている。これに対
してNPN トランジスタl2のヘース側は、負方向の
ダイオードl6を介してオペアンプl5の出力側に接続
されている。尚、第1図において、17は可変電圧源.
18は抵抗器である.
このように構戒されたポーラライザの定電流回路にあっ
て、今、正電源を印加したと仮定する。FIG. 1 is a constant current circuit diagram according to a first embodiment of the present invention. As shown in the figure, in this embodiment, PNP
The emitters of the transistor l1 and the NPN transistor 12 are connected to each other. And transistor l1
The collector side of the transistor 12 is connected to the positive power supply of +IOV, and the collector side of the transistor 12 is connected to the negative power supply of -10V. In addition, the intermediate connection point between the vines is connected to the waveguide coil 13.
It is connected to one end of the . The other end of the waveguide coil l3 is connected to ground. Further, the base side of the PNP transistor 11 is connected to the output side of the operational amplifier 15 via a positive diode 14. On the other hand, the base side of the NPN transistor l2 is connected to the output side of the operational amplifier l5 via a negative diode l6. In FIG. 1, 17 is a variable voltage source.
18 is a resistor. Assume that a positive power supply is now applied to the constant current circuit of the polarizer configured as described above.
この場合には、オペアンプl5からPNP }ランジス
タ11のベース側へ正のベース電圧が印加され、トラン
ジスタl1がON動作する。そのため、トランジスタl
1のコレクタ側から工ξソタ側へ電流が疏れる。この電
流は、導波管コイル13を通してアース側へ流れるよう
になる.即ち、導波管コイル13に正の定電流が印加さ
れ、導波管内のプローブは、導波管コイル13の電磁力
の作用によるファラデー回転効果により、例えば垂直偏
波を受信することが可能である.
次に、負電源を印加した場合を仮定する.この場合には
、オペアンプ15からNPN }ランジスタl2のヘー
ス側へ負のベース電圧が印加される.そのため、今度は
NPN }ランジスタ12がON動作し、アース側から
導波管コイルl3を経てトランジスタ12の工ξソタ及
びコレクタを経て負電源側へ負の定電疏が流れる閉回路
が形成される.すなわち、導波管コイルl3に負の定電
流が印加されることになり、導波管内のプローブは、例
えば水平偏波を受信することが可能である.
このように本実施例にあっては、導波管コイル13に正
・負全く逆方向の定電流を流すことで、垂直偏波と水平
偏波とを交差偏波識別するようにしている.導波管コイ
ル13に全く逆方向の定電流を流した場合、導波管コイ
ル13に残溜磁束が発生するという問題は皆無である.
それ故、交差偏波織別に際し、特定周波数帯域において
受信不良となる等のことがない.
第2図は、本発明の第2の実施例に係る定電流回路を示
す図面である。この実施例にあっては、第1図に示す実
施例の導波管コイル13の両端測へ接続ずる端子19.
20を短絡接続したり、誤ってアース接続した場合の
iy1?ii流保護機能として、トランジスタ21.
22及び抵抗23乃至27を設けたものである.基本的
な動作については、前記実施例の場合と同しであり、こ
こでの説明は省略する.また第3図は、PNP トラン
ジスタl1とNPN トランジタス12とのベース測へ
供給するベース電圧の{R給回路を、オペアンプ28.
29を用いて形成した場合の本発明の第3の実施例を
示すものである.この実施例の回路は、可変電圧源17
が正の電圧のみでコントロールできることからコンピュ
ーター接続に通した回路である.その他の構戒並びに作
用効果は、前述した第1及び第2実施例の場合と同じで
あり、ここでの説明は省略する.〔発明の効果〕
以上説明したように本発明にあっては、PNI’ トラ
ンジスタとNPN トランジスタとを直列に配置して正
・負の電源間へ接続し、両トランジスタのエミソタ間へ
導波管コイルの一端側を接続し、また導波管コイルの他
端側をアースへ接続している。In this case, a positive base voltage is applied from the operational amplifier l5 to the base side of the PNP transistor 11, and the transistor l1 is turned on. Therefore, transistor l
Current flows from the collector side of 1 to the ξ side. This current flows through the waveguide coil 13 to the ground side. That is, a positive constant current is applied to the waveguide coil 13, and the probe inside the waveguide can receive, for example, vertically polarized waves due to the Faraday rotation effect caused by the electromagnetic force of the waveguide coil 13. be. Next, assume that a negative power supply is applied. In this case, a negative base voltage is applied from the operational amplifier 15 to the base side of the NPN transistor l2. Therefore, this time, the NPN transistor 12 turns ON, and a closed circuit is formed in which a negative constant current flows from the ground side through the waveguide coil l3, through the output and collector of the transistor 12, and to the negative power supply side. .. That is, a negative constant current is applied to the waveguide coil l3, and the probe inside the waveguide can receive, for example, horizontally polarized waves. As described above, in this embodiment, by passing constant currents in completely opposite directions, positive and negative, through the waveguide coil 13, cross-polarized waves are discriminated between vertically polarized waves and horizontally polarized waves. When a constant current in the completely opposite direction is passed through the waveguide coil 13, there is no problem that residual magnetic flux is generated in the waveguide coil 13.
Therefore, when cross-polarized waves are distinguished, there is no possibility of poor reception in specific frequency bands. FIG. 2 is a drawing showing a constant current circuit according to a second embodiment of the present invention. In this embodiment, the terminal 19. which is connected to both ends of the waveguide coil 13 of the embodiment shown in FIG.
iy1 if 20 is short-circuited or accidentally connected to ground? As a second protection function, transistor 21.
22 and resistors 23 to 27 are provided. The basic operation is the same as in the previous embodiment, so the explanation here will be omitted. FIG. 3 also shows that the base voltage supply circuit for supplying the base voltages of the PNP transistor l1 and the NPN transistor 12 to the operational amplifier 28.
This figure shows a third embodiment of the present invention in which the structure is formed using No. 29. The circuit of this embodiment has a variable voltage source 17
This circuit is connected to a computer because it can be controlled using only positive voltage. The other structure, functions, and effects are the same as those of the first and second embodiments described above, and their explanations will be omitted here. [Effects of the Invention] As explained above, in the present invention, a PNI' transistor and an NPN transistor are arranged in series and connected between positive and negative power supplies, and a waveguide coil is connected between the emitters of both transistors. One end of the waveguide coil is connected to the waveguide coil, and the other end of the waveguide coil is connected to ground.
そして、導波管コイルへ正・負の定電疏を流すようにし
ている.このように、導波管コイルへ流す定電流の向き
を正・負逆向きに切り換えると、受信する電波の位相角
がファラーデ一回転の効果により90度異なり、正の定
電流を流した場合と、負の定電疏を流した場合とにあっ
て、垂直偏波と水平偏波とを夫々受信することが可能で
ある.すなわち、交差偏波識別を行うことが可能である
.しかも、常時、正・負いずれかの電流が導波管コイル
へ流れているので、従来のように残溜磁東が発生して偏
波の位相角がズレ、受信不良となる等のことはない.Then, positive and negative constant currents are applied to the waveguide coil. In this way, when the direction of the constant current flowing through the waveguide coil is switched between positive and negative, the phase angle of the received radio wave will differ by 90 degrees due to the effect of one Farade rotation, and will differ from when a positive constant current is passed. , it is possible to receive vertically polarized waves and horizontally polarized waves, respectively, when a negative constant current is applied. In other words, it is possible to perform cross-polarization identification. Moreover, since either positive or negative current is always flowing to the waveguide coil, there is no possibility of residual magnetic east occurring, shifting the phase angle of polarized waves, and causing poor reception, as in the conventional case. do not have.
第1図乃至第3図はそれぞれ本発明の第1乃至第3の実
施例に係るポーラライザの定電流回路を示す図面であり
、第4図は一般的なパラボラアンテナを示す側面図、第
5図は従来のポーラライザの部分縦断面図である。
5・・・ポーラライザ
1l・・・PNP トランジスタ
12・・・NPN }ランジスタ
l3・・・導波管コイル
14. 16・・・ダイオード1 to 3 are drawings showing constant current circuits of polarizers according to first to third embodiments of the present invention, respectively, FIG. 4 is a side view showing a general parabolic antenna, and FIG. 5 is a partial longitudinal sectional view of a conventional polarizer. 5...Polarizer 1l...PNP Transistor 12...NPN }Transistor l3...Waveguide coil 14. 16...diode
Claims (1)
するための定電流回路であって、正電源と負電源との間
に、NPN接続されたトランジスタとPNP接続された
トランジスタとを直列接続し、導波管コイルの一端側を
前記二種類のトランジスタ同士の中間接続点へ接続する
と共に、導波管コイルの他端側をアースへ接続し、NP
Nトランジスタ及びPNPトランジスタのベース側に夫
々正・負逆向きのダイオードを接続したことを特徴とす
るポーラライザの定電流回路。1. This is a constant current circuit for supplying positive and negative power to the waveguide coil of a polarizer, in which an NPN-connected transistor and a PNP-connected transistor are connected in series between the positive power source and the negative power source. , one end of the waveguide coil is connected to the intermediate connection point between the two types of transistors, and the other end of the waveguide coil is connected to ground, and the NP
A constant current circuit of a polarizer characterized in that diodes with opposite positive and negative directions are connected to the base sides of an N transistor and a PNP transistor, respectively.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15306389A JPH0318101A (en) | 1989-06-15 | 1989-06-15 | Constant current circuit for polarizer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15306389A JPH0318101A (en) | 1989-06-15 | 1989-06-15 | Constant current circuit for polarizer |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0318101A true JPH0318101A (en) | 1991-01-25 |
Family
ID=15554174
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15306389A Pending JPH0318101A (en) | 1989-06-15 | 1989-06-15 | Constant current circuit for polarizer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0318101A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH05110302A (en) * | 1991-10-17 | 1993-04-30 | Fujitsu General Ltd | Primary radiator for both circular and linear polarization |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS54133049A (en) * | 1978-04-07 | 1979-10-16 | Mitsubishi Electric Corp | Parabola antenna |
| JPS6223484A (en) * | 1985-06-27 | 1987-01-31 | Nippon Gijutsu Kaihatsu Center:Kk | Method for lining inner wall surface of pipe |
-
1989
- 1989-06-15 JP JP15306389A patent/JPH0318101A/en active Pending
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS54133049A (en) * | 1978-04-07 | 1979-10-16 | Mitsubishi Electric Corp | Parabola antenna |
| JPS6223484A (en) * | 1985-06-27 | 1987-01-31 | Nippon Gijutsu Kaihatsu Center:Kk | Method for lining inner wall surface of pipe |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH05110302A (en) * | 1991-10-17 | 1993-04-30 | Fujitsu General Ltd | Primary radiator for both circular and linear polarization |
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