JPH04111501A - Directional coupler - Google Patents

Directional coupler

Info

Publication number
JPH04111501A
JPH04111501A JP23224790A JP23224790A JPH04111501A JP H04111501 A JPH04111501 A JP H04111501A JP 23224790 A JP23224790 A JP 23224790A JP 23224790 A JP23224790 A JP 23224790A JP H04111501 A JPH04111501 A JP H04111501A
Authority
JP
Japan
Prior art keywords
signal
signals
phase difference
directional couplers
directional coupler
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
JP23224790A
Other languages
Japanese (ja)
Inventor
Masahiko Kohama
正彦 小浜
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 JP23224790A priority Critical patent/JPH04111501A/en
Publication of JPH04111501A publication Critical patent/JPH04111501A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain a high directionality by distributing a signal into two to give a phase difference and synthesizing signals again after taking out them by directional couplers and not only efficiently synthesizing effective signals but also excluding unnecessary signals by the phase difference. CONSTITUTION:The high frequency power inputted from a point 1 is outputted to power lines 14a and 14b as signals Pi1a and Pi1b by a 3dB coupler 12a, and they are inputted to directional couplers 13a and 13b having a coupling degree C. In directional couplers, the signal Pi1a is partially coupled with a signal Pi2a outputted to a power line 16a and a signal going to a resistive terminator in accordance with the degree C of coupling, and a signal Pi2b is taken out from the signal Pi1b in the same manner. That is, the signal is distributed to two main lines with the same amplitude by the distributor, and signals are taken out from these signals, to which the phase difference is given, by two directional couplers 13a and 13b, and taken-out signals are synthesized to obtain a coupling degree, and signals hindering the directionality are led to resistive terminators 11a to 11c by the phase difference. Thus, a high directionality is obtained.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、主として高周波帯で用いられる方向性結合
器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a directional coupler mainly used in a high frequency band.

〔従来の技術〕[Conventional technology]

第4図は従来の方向性結合器の構成図であり、第5図は
その分解参4図である。これら図において、1及び2は
入力端子、3は出力端子、5aは1次側結合線路、5b
は2次側結合線路である。
FIG. 4 is a block diagram of a conventional directional coupler, and FIG. 5 is an exploded view of the same. In these figures, 1 and 2 are input terminals, 3 is an output terminal, 5a is a primary side coupling line, and 5b
is the secondary side coupled line.

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

入力端子1より入射された高周波電力P 11は1次側
結合線路を伝搬して入力端子2に出力されるが、途中2
次側結合線路5bとの電磁結合により出力端子3に一部
がP lとして出力される。また一部はP 12として
無反射終端器4にも向かうが、二〇PI!は無反射終端
器に吸収され消失する。ここで入力端子2に無反射終端
器を接続したとき、で表されるCを一般に結合度という
The high frequency power P11 input from input terminal 1 propagates through the primary side coupling line and is output to input terminal 2.
A part of it is outputted to the output terminal 3 as Pl due to electromagnetic coupling with the next side coupling line 5b. A portion also goes to the non-reflection terminator 4 as P 12, but 20 PI! is absorbed by the non-reflection terminator and disappears. Here, when a non-reflection terminator is connected to the input terminal 2, C expressed by is generally called the degree of coupling.

また逆に入力端子2より入射された高周波電力Prlは
同様に出力端子3に一部がP、2として出力され、また
一部がPr3として無反射終端器4に向かい、吸収され
消失する。ここで入力端子lに無反射終端器を接続した
とき、 て表されるIを一般にアイソレーションという。
Conversely, a portion of the high frequency power Prl input from the input terminal 2 is similarly outputted to the output terminal 3 as P, 2, and a portion goes to the non-reflection terminator 4 as Pr3, where it is absorbed and disappears. Here, when a non-reflection terminator is connected to the input terminal l, I, which is expressed as , is generally called isolation.

また、 D= l I−Cl  (dB) て表されるDを方向性という。Also, D= I I-Cl (dB) D, which is expressed as , is called directionality.

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

従来の方向性結合器は以上のように構成されており、入
力端子2からの入射電力p r+による結合出力Pr2
が存在せず、発生したP r2が完全に無反射終端器で
吸収された結果アイソレーション、結合度ともに無限大
となることが望ましい。しかし、現実にはP r2が存
在しまた発生したP r2も完全には無反射終端器に吸
収されずに一部反射されて出力端子3に向かうため、こ
の種の方向性結合器の方向性は一般に22dB〜40d
B程度の値しか得られないという問題点があった。
The conventional directional coupler is configured as described above, and the combined output Pr2 due to the incident power p r+ from the input terminal 2
It is desirable that no P r2 exists and that the generated P r2 is completely absorbed by the non-reflection terminator, resulting in infinite isolation and coupling. However, in reality, P r2 exists and the generated P r2 is not completely absorbed by the non-reflective terminator but is partially reflected and goes to the output terminal 3, so the directionality of this type of directional coupler is is generally 22dB to 40d
There was a problem that only a value of about B could be obtained.

この発明は方向性か30〜50dBと大きい方向性結合
器を得ることを目的とする。
The object of this invention is to obtain a directional coupler with a high directionality of 30 to 50 dB.

〔課題を解決するための手段〕 この発明に係る方向性結合器は分配器により2本の主線
路に等しい振幅で分配し、位相差を持たせた信号から2
個の方向性結合器により信号を取り出し、取り出した信
号を合成することにより結合度を得るとともに、位相差
により方向性を阻害する信号を無反射終端器に導くよう
に構成したものである。
[Means for Solving the Problems] The directional coupler according to the present invention distributes signals with equal amplitude to two main lines using a divider, and separates two signals from a signal having a phase difference.
The signal is taken out by two directional couplers, and the degree of coupling is obtained by combining the taken out signals, and the signal that obstructs the directionality is guided to the non-reflection terminator due to the phase difference.

〔作用〕[Effect]

この発明においては、入力信号を等振幅で、位相差を有
する2系列の信号に分配し、2個の方向性結合器により
その各々より信号を取り出し、取り出した信号を合成し
て結合度を得るとともに、位相差により方向性を阻害す
る信号を無反射終端器に導くように構成したから、方向
性が悪化せず、大きな方向性を得ることができる。
In this invention, an input signal is divided into two series of signals with equal amplitude and a phase difference, a signal is extracted from each signal using two directional couplers, and the extracted signals are combined to obtain the degree of coupling. In addition, since the structure is configured such that a signal that obstructs directivity is guided to the non-reflection terminator due to a phase difference, the directivity is not deteriorated and a large directivity can be obtained.

〔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。 An embodiment of the present invention will be described below with reference to the drawings.

第1図は本発明による方向性結合器の構成を示す図であ
る。図において12a、12b、12cは3dB結合器
であり、13a、13bは任意の結合度をCを持つ方向
性結合器、lla、llb。
FIG. 1 is a diagram showing the configuration of a directional coupler according to the present invention. In the figure, 12a, 12b, and 12c are 3 dB couplers, and 13a, 13b are directional couplers with arbitrary coupling degree C, lla, and llb.

11cは無反射終端器である。11c is a non-reflection terminator.

また、14a、14b、15a、15b、16a、16
bはそれぞれ同一長さの電送線路である。
Also, 14a, 14b, 15a, 15b, 16a, 16
b are electrical transmission lines having the same length.

点1〜10は位置を示す。Points 1-10 indicate positions.

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

点lから入力された高周波電力は3dB結合器12aに
より、電送線路14a、14bにそれぞれP lla 
I P IToとして出力される。P llbはP l
1mに比べて振幅は同じで位相が90°遅れた信号とな
っている。
The high frequency power input from point l is connected to transmission lines 14a and 14b by a 3dB coupler 12a, respectively.
It is output as I P ITo. P llb is P l
Compared to the 1m signal, the amplitude is the same, but the phase is delayed by 90°.

次にP lla + P I11+はそれぞれ結合度C
を持つ方向性結合器13a、13bに入る。従来技術と
同様、方向性結合器内ではP l1mは結合度Cに対応
して一部が電送線路16aに出力される信号P、2゜と
無反射終端器に向かう信号とに結合される。またP l
lbからも同様にP llbという信号が取り出される
。方向性結合器内で一部取り出された残りの信号P 1
411 I  P tabはそれぞれ前述の90’の位
相差を保ったまま3dB結合器(12c)に入力される
が、同振幅で90°の位相差を持っているため、合成さ
れ、点6てP+6として出力されることになる。同様に
3dB結合器により取り出された信号P 12m + 
P 12bは同振幅で、90°の位相差を持っているた
め、合成され、点lOにP 11として出力される。こ
のP、2/P、が結合度Cて再度定義できる。
Next, P lla + P I11+ each have the degree of coupling C
directional couplers 13a and 13b having the following characteristics. As in the prior art, within the directional coupler, P l1m is partially coupled to the signal P,2° output to the transmission line 16a and to the signal directed to the non-reflection terminator, corresponding to the degree of coupling C. Also P l
Similarly, a signal called Pllb is extracted from lb. The remaining signal P1 partially taken out in the directional coupler
411 I P tab are each input to the 3 dB combiner (12c) while maintaining the aforementioned 90' phase difference, but since they have the same amplitude but a 90° phase difference, they are combined, and from point 6 to P+6 It will be output as Similarly, the signal P 12m + extracted by the 3 dB coupler
Since P 12b has the same amplitude and a phase difference of 90°, they are combined and output as P 11 to point lO. This P, 2/P, can be redefined with the degree of coupling C.

次に点6からの入力P、について考える。入力された高
周波電力P、は3dB結合器12cにより電送線路15
a、15bにそれぞれP rla +  P 、1bと
して出力されるか、p r+、はP rlbと比べて振
幅は同じで位相は90°遅れた信号となっている。
Next, consider the input P from point 6. The input high frequency power P is connected to the transmission line 15 by the 3 dB coupler 12c.
a and 15b as P rla + P and 1b, respectively, or p r+ is a signal that has the same amplitude but a phase delayed by 90° compared to P rlb.

方向性結合器内では入力P、のときと同様、P+2a+
P、2.が3dB結合器12bに向かう。また方向性結
合器内の無反射終端器で反射された信号も3dB結合器
12bに向かうが、この信号は位相の進み遅れが前述の
P 12a I  P ribの場合に比べて反転して
いるため、合成さた信号はP r2として無反射終端器
11bに吸収され点10には出力されない。方向性結合
器で結合した残りの信号は3dB結合器12aで合成さ
れ、Pt6として点1に出力される。アイソレーション
は点6における入力と、点lOにおける出力比であり、
点6における入力P、は点10には表れないためアイソ
レーションは無限大となる。その結果方向性も無限大と
なる。
In the directional coupler, P+2a+ as in the case of input P,
P, 2. goes to the 3dB coupler 12b. In addition, the signal reflected by the non-reflection terminator in the directional coupler also goes to the 3 dB coupler 12b, but since the phase lead/lag of this signal is reversed compared to the case of P 12a I P rib described above. , the combined signal is absorbed by the non-reflection terminator 11b as Pr2 and is not output to point 10. The remaining signals combined by the directional coupler are combined by the 3 dB coupler 12a and output to point 1 as Pt6. Isolation is the ratio of the input at point 6 to the output at point lO,
Since the input P at point 6 does not appear at point 10, the isolation becomes infinite. As a result, the directionality becomes infinite.

なお、上記実施例では3dB結合器12a、12cを使
用したか、第2図に示すように代わりに2分配20a、
20bと90°移相器21a、21bを用いてもP I
Is r  P llbの振幅9位相関係、およびP 
rim +  P rlbの振幅2位相関係は上記実施
例と同一であるため、同様の効果を奏することができる
In the above embodiment, the 3 dB couplers 12a and 12c were used, or as shown in FIG.
20b and 90° phase shifters 21a and 21b, P I
Is r P llb amplitude 9 phase relationship, and P
Since the amplitude two-phase relationship of rim + P rlb is the same as in the above embodiment, similar effects can be achieved.

また第3図は3dB結合器の代わりに90°移相器21
cとウィルキンソン型2分配22aを用いたものである
か、本実施例においてはP12arP1□、は同振幅、
同位相であるため、ウィルキンソン型2分配22aで損
失することなく合成されるが、不要な信号P r2a 
+  P r2b振幅は同一であるが位相がずれている
ため十分には合成されず、一部損失を伴って点10に出
力されることとなる。
Also, in Figure 3, a 90° phase shifter 21 is used instead of a 3dB coupler.
In this example, P12arP1□ are the same amplitude,
Since they are in the same phase, they are combined without loss in the Wilkinson type two-way distribution 22a, but the unnecessary signal P r2a
+P r2b The amplitudes are the same, but the phases are shifted, so they are not combined sufficiently and are output to point 10 with some loss.

二のためアイソレーションは無限大にはならないが従来
技術に比較すると改善されることとなる。
2, the isolation will not become infinite, but will be improved compared to the prior art.

〔発明の効果〕〔Effect of the invention〕

以上のようにこの発明によれば、方向性結合器は、信号
を2分配して位相差を持たせその信号を方向性結合器に
より取り出した後、再度合成するよう構成したので、そ
の位相差により有効な信号は効率よく合成し、不要な信
号は排除することかでき、その結果、大きな方向性を得
ることかできるという効果がある。
As described above, according to the present invention, the directional coupler is configured to divide the signal into two parts, give a phase difference, take out the signals by the directional coupler, and then combine them again. This has the effect that effective signals can be efficiently combined and unnecessary signals can be eliminated, and as a result, great directionality can be obtained.

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

第1図はこの発明の一実施例による方向性結合器を示す
図、第2図、第3図はこの発明の他の実施例を示す図、
第4図は従来の方向性結合器の構成図、第5図は従来の
方向性結合器の分解図である。 図において、12a、12b、12cは3dB結合器、
13a、13bは任意の結合度Cを持つ方向性結合器、
lla、llb、llcは無反射終端器、14aと14
b、15aと15b、16aと16bはそれぞれの同一
長さの電送線路である。 なお図中同一符号は同−又は相当部分を示す。 第1図
FIG. 1 is a diagram showing a directional coupler according to one embodiment of the invention, FIGS. 2 and 3 are diagrams showing other embodiments of the invention,
FIG. 4 is a block diagram of a conventional directional coupler, and FIG. 5 is an exploded view of the conventional directional coupler. In the figure, 12a, 12b, 12c are 3dB couplers,
13a and 13b are directional couplers having an arbitrary coupling degree C;
lla, llb, llc are non-reflection terminators, 14a and 14
b, 15a and 15b, and 16a and 16b are transmission lines having the same length. Note that the same reference numerals in the figures indicate the same or equivalent parts. Figure 1

Claims (1)

【特許請求の範囲】[Claims] (1)入力信号を等振幅で位相差を持った信号として2
系列の線路に分配する分配器と、 該分配された信号の各々よりその信号の一部を取り出す
2個の方向性結合器と、 該方向性結合器により取り出した二信号を合成する第1
の合成器と、 上記方向性結合器により取り出されずに残った二信号を
合成する第2の合成器とを備えたことを特徴とする方向
性結合器。
(1) Assign the input signal as a signal with equal amplitude and a phase difference.
a splitter that distributes to a series of lines; two directional couplers that extract a part of the signal from each of the distributed signals; and a first directional coupler that combines the two signals extracted by the directional couplers.
A directional coupler comprising: a combiner; and a second combiner that combines two signals remaining without being taken out by the directional coupler.
JP23224790A 1990-08-30 1990-08-30 Directional coupler Pending JPH04111501A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23224790A JPH04111501A (en) 1990-08-30 1990-08-30 Directional coupler

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23224790A JPH04111501A (en) 1990-08-30 1990-08-30 Directional coupler

Publications (1)

Publication Number Publication Date
JPH04111501A true JPH04111501A (en) 1992-04-13

Family

ID=16936281

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23224790A Pending JPH04111501A (en) 1990-08-30 1990-08-30 Directional coupler

Country Status (1)

Country Link
JP (1) JPH04111501A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5966057A (en) * 1997-11-18 1999-10-12 Trw Inc. Reflection reducing directional coupler
JP2003502932A (en) * 1999-06-22 2003-01-21 テレフオンアクチーボラゲット エル エム エリクソン(パブル) Structure in electronic systems
JP2006253150A (en) * 2005-03-10 2006-09-21 Huettinger Elektronik Gmbh & Co Kg Vacuum plasma generator

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5966057A (en) * 1997-11-18 1999-10-12 Trw Inc. Reflection reducing directional coupler
JP2003502932A (en) * 1999-06-22 2003-01-21 テレフオンアクチーボラゲット エル エム エリクソン(パブル) Structure in electronic systems
US8133347B2 (en) 2005-03-05 2012-03-13 Huettinger Elektronik Gmbh + Co. Kg Vacuum plasma generator
JP2006253150A (en) * 2005-03-10 2006-09-21 Huettinger Elektronik Gmbh & Co Kg Vacuum plasma generator

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