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JPS6038884B2 - Electromagnetic wave synthesizer - Google Patents
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JPS6038884B2 - Electromagnetic wave synthesizer - Google Patents

Electromagnetic wave synthesizer

Info

Publication number
JPS6038884B2
JPS6038884B2 JP3831179A JP3831179A JPS6038884B2 JP S6038884 B2 JPS6038884 B2 JP S6038884B2 JP 3831179 A JP3831179 A JP 3831179A JP 3831179 A JP3831179 A JP 3831179A JP S6038884 B2 JPS6038884 B2 JP S6038884B2
Authority
JP
Japan
Prior art keywords
input end
electromagnetic wave
reflective
boat
frequency
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
Application number
JP3831179A
Other languages
Japanese (ja)
Other versions
JPS55132103A (en
Inventor
秀男 石井
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.)
Shimada Rika Kogyo KK
Original Assignee
Shimada Rika Kogyo KK
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 Shimada Rika Kogyo KK filed Critical Shimada Rika Kogyo KK
Priority to JP3831179A priority Critical patent/JPS6038884B2/en
Publication of JPS55132103A publication Critical patent/JPS55132103A/en
Publication of JPS6038884B2 publication Critical patent/JPS6038884B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/20Frequency-selective devices, e.g. filters
    • H01P1/213Frequency-selective devices, e.g. filters combining or separating two or more different frequencies

Landscapes

  • Control Of Motors That Do Not Use Commutators (AREA)

Description

【発明の詳細な説明】 本発明はマイクロ波通信回線等において共通の空中線に
周波数の異なる2つ以上の送信機を結合する場合等の用
途に用いる電磁波合成装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electromagnetic wave combining device used for coupling two or more transmitters of different frequencies to a common antenna in a microwave communication line or the like.

従来のこの種の装置は、第1図に示すように、サーキュ
レーターと帯域通過炉波器2とを組合せ、第1のボート
P,は周波数〆,の第1の送信機(図示せず)を接続す
る1つの信号入力端とし、第2のボートP2は周波数〆
2 の第2の送信機(図示せず)を接続する他の1つの
信号入力端とし、第3のボートP3は共通の空中線(図
示せず)を接続する信号出力端とした構造であった。
A conventional device of this kind, as shown in FIG. The second boat P2 is the other signal input terminal to which a second transmitter (not shown) of frequency 2 is connected, and the third boat P3 is the common antenna. (not shown) was used as a signal output terminal for connection.

しかしながらこのような電磁波合成装置では、周波数選
択回路(帯域通過炉波器2)を用いるため、その伝送特
性により、位相歪や振幅歪が発生する欠点があった。
However, since such an electromagnetic wave synthesizer uses a frequency selection circuit (bandpass wave generator 2), there is a drawback that phase distortion and amplitude distortion occur due to its transmission characteristics.

また、送信周波数を可変する場合には、帯域通過炉波器
の共振周波数をその都度調整しなければならない欠点が
あった。本発明の目的は、電力損失が少なく、且つ位相
歪や振幅歪をほとんど生じない電磁波合成装置を提供す
るにある。
Furthermore, when changing the transmission frequency, there is a drawback that the resonant frequency of the bandpass wave generator must be adjusted each time. SUMMARY OF THE INVENTION An object of the present invention is to provide an electromagnetic wave synthesis device that has low power loss and hardly produces phase distortion or amplitude distortion.

以下本発明の具体例を図面を参照して詳細に説明する。Hereinafter, specific examples of the present invention will be described in detail with reference to the drawings.

第2図は本発明の第1実施例を示したものである。本実
施例の電磁波合成装置は、第1のボートP,とサーキュ
レータ1との間に、非反射入力端(入射波をほぼ損失な
く通過させる入力端)と反射入力端(入射波を殆んど反
射させる入力端)をもつ反射形単向管よりなる非可逆回
路3を、その非反射入力端を第1のボートP,側に向け
、その反射入力端をサーキュレータ1に向けて接続して
構成したものである。このような電磁波合成装置は、第
1のボートP,は周波数〆.の送信機(図示せず)を接
続する1つの信号入力端とし、第2のボートP2は周波
数〆2 の第2の送信機(図示せず)を接続する他の1
つの信号入力端とし、第3のボートP3は共通の空中線
(図示せず)を接続する信号出力端として使用する。反
射形単向管よりなる非可逆回路3は、この非可逆回路3
とサーキュレ−夕1との間に設けられた第4のボートP
4からの入射波は殆んと完全に反射し、第1のボートP
,からの入射波はほぼ損失なく第4のボートP4に伝送
し得る伝送特性をもっている。本装置は、以上のような
構成になっているので、第2の送信機からの周波数ナ2
の出力は、第2のボートP2より第4のボートP4に伝
送されるが、反射形単向管よりなる非可逆回路3により
完全反射されて再び第4のボートP4を経て第3のボー
トP3を通り空中線に伝送されることになる。一方、第
1の送信機からの周波数〆,の出力は、反射形単向管よ
りなる非可逆回路3をほぼ損失なく通過し、第4のボー
トP4及び第3のボートP3を経て空中線に伝送される
ことになる。第3図は反射形単向管よりなる非可逆回路
3の具体例を示したものである。
FIG. 2 shows a first embodiment of the present invention. The electromagnetic wave synthesizer of this embodiment has a non-reflective input end (an input end that allows incident waves to pass through with almost no loss) and a reflective input end (an input end that allows incident waves to pass through almost without loss) between the first boat P and the circulator 1. A non-reciprocal circuit 3 made of a reflective unidirectional tube with an input end for reflection) is connected with its non-reflection input end facing the first boat P, and its reflection input end facing the circulator 1. This is what I did. In such an electromagnetic wave synthesizer, the first boat P has a frequency . The second port P2 has one signal input terminal to which a transmitter (not shown) is connected, and the second port P2 is the other signal input terminal to which a second transmitter (not shown) with a frequency of 2 is connected.
The third port P3 is used as a signal output terminal to which a common antenna (not shown) is connected. The irreversible circuit 3 made of a reflective unidirectional tube is
and the fourth boat P installed between the
The incident wave from P 4 is almost completely reflected and
, has transmission characteristics that allow it to be transmitted to the fourth boat P4 with almost no loss. Since this device has the above configuration, the frequency signal from the second transmitter is
The output is transmitted from the second boat P2 to the fourth boat P4, but it is completely reflected by the irreversible circuit 3 made of a reflective unidirectional tube, and then passes through the fourth boat P4 again to the third boat P3. The signal is then transmitted to the antenna. On the other hand, the frequency output from the first transmitter passes through the irreversible circuit 3 made of a reflective unidirectional tube with almost no loss, and is transmitted to the antenna via the fourth boat P4 and the third boat P3. will be done. FIG. 3 shows a specific example of the irreversible circuit 3 made of a reflective unidirectional tube.

この非可逆回路3は、矩形TE,。導波管4の中に厚み
dの板状のフェライト5を一方の狭面に接近して挿入し
、直流磁界Hoを導波管4の広面に垂直に下から上に向
けて加える。いま、この導波管4に紙面に向って進む進
行波を加えたとすると、フェライト5の部分には正の円
偏波が生じ、この部分の透磁率は正の透磁率仏+として
動作する。これに対し、紙面より手前に進む逆行液を加
えた場合においては、フェライト5の部分には負の円偏
波が生じ、透磁率はム−として動作する。一方、この正
又は負の透磁率山十,ム−の値は、直流磁界の強さ日に
より第4図に示すように変化するので、図示のように直
流磁界の強さ凡を仏+が負となっているところを選ぶと
、電波はフェライト5の中に入り込まず、その電界分布
は第3図の実線(進行波)イのようになり、等価的に導
波管4の横幅がa′まで短かくなったことになる。従っ
て、これによって決定される遮断周波数〆cFより低い
周波数の波を使用すれば、これらの波は全部反射される
ことになる。これに比べ、逆方向の波に対する透磁率仏
‐は正の値であり、またフェライト5の比誘電率zは大
きな値であるので、電界はその部分に集中し、第3図の
破線(逆行波)口のようになり、その遮断周波数〆cc
はフェライト5が挿入されないときより低くなる。
This irreversible circuit 3 has a rectangular shape TE. A plate-shaped ferrite 5 with a thickness d is inserted into the waveguide 4 close to one narrow surface, and a DC magnetic field Ho is applied perpendicularly to the wide surface of the waveguide 4 from bottom to top. Now, if a traveling wave traveling toward the plane of the paper is applied to this waveguide 4, a positive circularly polarized wave is generated in the ferrite 5 portion, and the magnetic permeability of this portion operates as a positive magnetic permeability Buddha +. On the other hand, when a retrograde liquid is added that moves forward from the plane of the paper, negative circularly polarized waves are generated in the ferrite 5 portion, and the magnetic permeability operates as a mu. On the other hand, the value of this positive or negative magnetic permeability mountain changes as shown in Figure 4 depending on the strength of the DC magnetic field. If you choose a negative point, the radio wave will not enter the ferrite 5, and the electric field distribution will become like the solid line (traveling wave) A in Figure 3, and equivalently the width of the waveguide 4 will be a. This means that it has been shortened to . Therefore, if waves of a frequency lower than the cutoff frequency 〆cF determined by this are used, all of these waves will be reflected. In comparison, the magnetic permeability for waves in the opposite direction is a positive value, and the relative permittivity z of ferrite 5 is a large value, so the electric field is concentrated in that part, and the broken line in Figure 3 (reverse wave) becomes like a mouth, and its cutoff frequency 〆cc
is lower than when ferrite 5 is not inserted.

以上の原理により、使用周波数として導波管4の使用帯
域内で前述した遮断周波数〆cFより低い周波数を選べ
ば、一方のボートよりの入射波は完全に反射し、他方よ
りの入射波は殆んど損失なく伝送する特性をもつ非可逆
回路3である反射形単向管が実現できる。
According to the above principle, if a frequency lower than the aforementioned cutoff frequency 〆cF is selected within the operating band of the waveguide 4 as the operating frequency, the incident wave from one boat will be completely reflected, and the incident wave from the other boat will be almost completely reflected. This makes it possible to realize a reflective unidirectional tube, which is a non-reciprocal circuit 3 that has the characteristic of transmitting data without loss.

第5図は本発明の第2実施例を示したものである。FIG. 5 shows a second embodiment of the invention.

本実施例の電磁波合成装置は、4つのボートをもつサー
キュレーターを使用し、周波数が〆,,ナ2,ナ3と異
なる3種の入力信号の合成を行う例を示したものである
。第6図は本発明の第3実施例を示したものである。
The electromagnetic wave synthesizer of this embodiment uses a circulator with four ports to synthesize three types of input signals having different frequencies, ie, , na2, and na3. FIG. 6 shows a third embodiment of the present invention.

本実施例の電磁波合成装置は、第2図に示す構造のもの
を2段縦続援続して、周波数が〆,,ナ2,「3と異な
る3種の入力信号の合成を行う他の例を示したものであ
る。以上説明したように本発明に係る電磁波合成装置は
、サーキュレータと、一方よりの入射波は殆んど反射し
他方よりの入射波は殆んど損失なく通過させる伝送特性
をもつ非可逆回路との組合せにより形成したので、周波
数の異なる送信出力の合成に帯域炉波器等の周波数選択
回路を用いなくてもよく、このため振幅及び位相特性の
優れた電磁波合成装置を実現でき、超多重マイクロ波回
線等に用いれば非常に有益である。また、衛星通信地上
局のように送信周波数の変更がときどき行われる場合に
も周波数の調整が不要であり、且つ電力損失も極めて少
ない利点がある。
The electromagnetic wave synthesizer of this embodiment is another example in which the structures shown in FIG. As explained above, the electromagnetic wave synthesizer according to the present invention includes a circulator and a transmission characteristic that allows most of the incident waves from one side to be reflected and the incident waves from the other side to pass through with almost no loss. Since it is formed by combining a non-reciprocal circuit with It is very useful when used in ultra-multiplex microwave lines, etc.Also, when the transmission frequency is changed from time to time, such as in a satellite communication ground station, there is no need for frequency adjustment, and there is no power loss. There are very few advantages.

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

第1図は従来の電磁波合成装置の結線図、第2図は本発
明に係る電磁波合成装置の第1実施例を示す結線図、第
3図及び第4図は本発明で用いる非可逆回路の横断面図
及び磁界変化に対する透磁率の特性図、第5図及び第6
図は本発明に係る電磁波合成装置の第2,第3実施例の
結線図である。 1・・・・・・サーキュレータ、3・・・・・・非可逆
回路。 第1図第2図 第3図 第4図 第5図 第6図
Figure 1 is a wiring diagram of a conventional electromagnetic wave synthesizer, Figure 2 is a wiring diagram showing a first embodiment of the electromagnetic wave synthesizer according to the present invention, and Figures 3 and 4 are of a nonreciprocal circuit used in the present invention. Cross-sectional view and characteristic diagram of magnetic permeability against changes in magnetic field, Figures 5 and 6
The figure is a wiring diagram of second and third embodiments of the electromagnetic wave synthesis device according to the present invention. 1...Circulator, 3...Irreversible circuit. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6

Claims (1)

【特許請求の範囲】 1 複数のポートをもつサーキユレータの1つのポート
を1つの信号入力端とし、回転方向の次のポートに一方
(反射入力端)よりの入射波は殆んど反射し他方(非反
射入力端)よりの入射波はほぼ損失なく通過させる伝送
特性を有する非可逆回路の前記反射入力端を接続し、前
記非可逆回路の非反射入力端を他の信号入力端としたこ
とを特徴とする電磁波合成装置。 2 前記非可逆回路として反射形単向管を用いた特許請
求の範囲第1項に記載の電磁波合成装置。
[Claims] 1. One port of a circulator having a plurality of ports is used as one signal input end, and most of the incident waves from one (reflection input end) are reflected to the next port in the rotational direction, and the waves are reflected from the other (reflection input end). The reflective input end of a non-reciprocal circuit having transmission characteristics that allows the incident wave from the non-reflective input end to pass through with almost no loss is connected, and the non-reflective input end of the non-reciprocal circuit is used as another signal input end. Characteristic electromagnetic wave synthesis device. 2. The electromagnetic wave synthesis device according to claim 1, wherein a reflective unidirectional tube is used as the irreversible circuit.
JP3831179A 1979-04-02 1979-04-02 Electromagnetic wave synthesizer Expired JPS6038884B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3831179A JPS6038884B2 (en) 1979-04-02 1979-04-02 Electromagnetic wave synthesizer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3831179A JPS6038884B2 (en) 1979-04-02 1979-04-02 Electromagnetic wave synthesizer

Publications (2)

Publication Number Publication Date
JPS55132103A JPS55132103A (en) 1980-10-14
JPS6038884B2 true JPS6038884B2 (en) 1985-09-03

Family

ID=12521743

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3831179A Expired JPS6038884B2 (en) 1979-04-02 1979-04-02 Electromagnetic wave synthesizer

Country Status (1)

Country Link
JP (1) JPS6038884B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3316713B2 (en) * 1994-04-26 2002-08-19 株式会社村田製作所 Antenna duplexer
US20080169878A1 (en) * 2007-01-12 2008-07-17 Giuseppe Resnati Low loss combiner for narrowband and wideband rf signals
US9246524B2 (en) 2013-09-05 2016-01-26 Zte (Usa) Inc. Outdoor coupler unit utilizing circulator network

Also Published As

Publication number Publication date
JPS55132103A (en) 1980-10-14

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