JPS63164502A - Microwave bipolar double-throw switch - Google Patents
Microwave bipolar double-throw switchInfo
- Publication number
- JPS63164502A JPS63164502A JP30810586A JP30810586A JPS63164502A JP S63164502 A JPS63164502 A JP S63164502A JP 30810586 A JP30810586 A JP 30810586A JP 30810586 A JP30810586 A JP 30810586A JP S63164502 A JPS63164502 A JP S63164502A
- Authority
- JP
- Japan
- Prior art keywords
- line
- characteristic impedance
- terminal
- switching elements
- lines
- 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
- 230000010354 integration Effects 0.000 abstract 1
- 230000002195 synergetic effect Effects 0.000 abstract 1
- 239000011159 matrix material Substances 0.000 description 5
- 238000010586 diagram Methods 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 2
- 238000004891 communication Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
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- 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、マイクロ波双極双投スイッチに関するもので
あって、特にマイクロ波平面回路に適する双極双投スイ
ッチに係る。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a microwave double-pole double-throw switch, and more particularly to a double-pole double-throw switch suitable for microwave planar circuits.
従来の双極双投スイッチの例を第2図に示す。 An example of a conventional double-pole double-throw switch is shown in FIG.
第2図において、51〜54は信号端子、55〜58は
スイッチング素子、59は立体交差部を表わしている。In FIG. 2, 51 to 54 represent signal terminals, 55 to 58 switching elements, and 59 a three-dimensional intersection.
スイッチング素子55,56がONでスイッチング素子
57.58がOFFの場合は端子51と端子52、端子
53と端子54がそれぞれ接続される (この状態を平
行モードと呼ぶことにする)。When switching elements 55 and 56 are ON and switching elements 57 and 58 are OFF, terminals 51 and 52 and terminals 53 and 54 are connected, respectively (this state will be referred to as parallel mode).
また、スイッチング素子55.56がOFFでスイッチ
ング素子57.58がONの場合は端子51と端子54
、端子52と端子53がそれぞれ接続される (この状
態を交差モードと呼ぶことにする)。In addition, when the switching elements 55 and 56 are OFF and the switching elements 57 and 58 are ON, the terminal 51 and the terminal 54
, terminals 52 and 53 are connected (this state will be referred to as cross mode).
上述したような従来の双極双投スイッチでは、■交差部
が立体的であるため、回路製作プロセスが複雑であり、
かつ、機械的強度や耐振性が劣る。In the conventional double-pole double-throw switch as mentioned above, the circuit manufacturing process is complicated because the intersection is three-dimensional.
In addition, mechanical strength and vibration resistance are poor.
■立体交差部における浮遊容量に起因する0N10FF
分離度の劣化がある。■0N10FF caused by stray capacitance at grade crossings
There is a deterioration in the degree of separation.
■スイッチング素子を多数(4個)必要とする。■A large number of switching elements (four) are required.
などの欠点があった。There were drawbacks such as.
本発明は、これら従来の問題点に鑑み、平面的構造で、
かつ、少数のスイッチング素子で構成できる双極双投ス
イッチを提供することを目的としている。In view of these conventional problems, the present invention has a planar structure,
Another object of the present invention is to provide a double-pole, double-throw switch that can be configured with a small number of switching elements.
本発明によれば、上述の目的は前記特許請求の範囲に記
載した手段により達成される。According to the invention, the above objects are achieved by the means specified in the claims.
すなわち、本発明のマイクロ波双極双投スイッチは、分
布定数線路とスイッチング素子2個を用いて信号端子間
を結ぶことを4I徴とするもので、従来必要であった立
体交差部が不要であり、一平面構造で双極双投スイッチ
を構成できる点において従来と異なるものである。In other words, the microwave double-pole double-throw switch of the present invention has the 4I feature of connecting signal terminals using a distributed constant line and two switching elements, and eliminates the need for the conventionally required grade-level intersection. , which is different from conventional devices in that it can form a double-pole, double-throw switch with a single-plane structure.
tI&1図は本発明の一実施例を示す図であって、マイ
クロ波平面回路双極双投スイッチの構成を示しており、
1〜4は信号端子、5〜7は1/4波長線路、8と9は
半波長線路を表わしている。Figure tI&1 is a diagram showing an embodiment of the present invention, and shows the configuration of a microwave planar circuit double-pole double-throw switch,
1 to 4 represent signal terminals, 5 to 7 represent quarter wavelength lines, and 8 and 9 represent half wavelength lines.
線路6は、線路8と線路9の中点どうしを結んでいる。A track 6 connects the midpoints of a track 8 and a track 9.
これら中点はそれぞれスイッチング素子10.11を介
して接地されている。線路5と線路7は特性インピーダ
ンスが等しく、これをZaとする。線路8と線路9は特
性インピーダンスが等しく、これをzbとする。線路6
の特性インピーダンスをZcとする。These midpoints are each grounded via a switching element 10.11. The line 5 and the line 7 have the same characteristic impedance, which is designated as Za. The line 8 and the line 9 have the same characteristic impedance, which is designated as zb. railroad track 6
Let Zc be the characteristic impedance of
これら線路の特性インピーダンスは相乗平均の関係すな
わち、 (1)式に示す関係を有しでいる。The characteristic impedances of these lines have a geometric mean relationship, that is, a relationship shown in equation (1).
zb=FT「77 ・・・・・・・・・・・・ (1
)以下、この実施例のマイクロ波双極双投スイッチの動
作についで説明する。zb=FT “77 ・・・・・・・・・・・・ (1
) The operation of the microwave double-pole double-throw switch of this embodiment will be explained below.
まず、スイッチング素子10.11をON (導通また
は短絡)とすると、線路8.9はそれぞれ2本の1/4
波艮短絡スタブとなる。First, when the switching elements 10.11 are turned ON (conducting or short-circuited), the lines 8.9 each become 1/4 of the two lines.
The wave becomes a short-circuit stub.
したがって、線路5ならびに線路7から見た線路8.9
のインピーダンスは無限大となり、結局、端子1からの
マイクロ波信号電流は全て線路5を通じて端子2へ流・
れる。Therefore, the track 8.9 seen from the track 5 and the track 7
The impedance of becomes infinite, and eventually all the microwave signal current from terminal 1 flows to terminal 2 through line 5.
It will be done.
同様に、端子3からのマイクロ波信号電流は全て線路7
を通じて端子4へ流れる。このようにしで、本回路は第
2図の回路における平行モードと等価な状態となる。Similarly, all microwave signal current from terminal 3 is transferred to line 7.
It flows to terminal 4 through. In this way, the present circuit becomes in a state equivalent to the parallel mode in the circuit of FIG.
つぎに、スイッチング素子1.0,11をOFF (切
断または開放)としたと外本回路が12図の回路におけ
る交差モードと等価な状態となることを以下に説明する
。Next, it will be explained below that when the switching elements 1.0 and 11 are turned off (cut off or opened), the main circuit enters a state equivalent to the crossing mode in the circuit of FIG. 12.
一般に、特性インピーダンスZの1/4波&線路を二端
子対網とみなした場合の7ドミタンス行列は、 (2)
式に示すとおりである。In general, the 7 domitance matrix when considering a 1/4 wave of characteristic impedance Z and the line as a two-terminal pair network is (2)
As shown in the formula.
(2)式における jは虚数単位である。j in equation (2) is an imaginary unit.
端子1〜4における信号電圧をそれぞれ■い■2、■8
、■、とし、半被艮線路8および9の中点の信号電圧を
それぞれVs、Vsとする。Set the signal voltage at terminals 1 to 4 to ■■2 and ■8, respectively.
, ■, and the signal voltages at the midpoints of the half-covered lines 8 and 9 are Vs and Vs, respectively.
これら6節点においてキルヒホッフの第1法則を適用し
、7本の枝に式(2)を適用すると、6元連立方程式、
Za Zb
Za Zb
Za Zb
を得る。When Kirchhoff's first law is applied to these six nodes and equation (2) is applied to the seven branches, a six-element simultaneous equation, Za Zb Za Zb Za Zb is obtained.
ここでI、〜I、はそれぞれ端子1〜4から流れ込む信
号電流である。式(7)と (8)を式(3)〜 (6
)に代入して■、とvaを消去すると、本回路の西端子
アドミタンス行列Yを得る。Here, I and ~I are signal currents flowing from terminals 1 to 4, respectively. Equations (7) and (8) are converted into equations (3) to (6
) and eliminate ■, and va to obtain the west terminal admittance matrix Y of this circuit.
この式に関係式(1)を代入すると、
なる対角行列となる。すなわち、隣り合う端子間には結
合が生じない。Substituting relational expression (1) into this equation results in a diagonal matrix. That is, no coupling occurs between adjacent terminals.
この西端子アドミタンス行列を、信号源・負荷インピー
ダンスを2゜とじた四端子散乱行列Sに変換すると、
となる。When this west terminal admittance matrix is converted into a four-terminal scattering matrix S in which the signal source and load impedances are multiplied by 2 degrees, the following is obtained.
ここで特にZ。=Zaの場合は、
となる。すなわち、本回路はZaに等しい信号源・負荷
インピーダンスに対して整合し、入力信号電力は全て対
角の端子に出力される。このようにして、本回路は交差
モードとなる。Especially Z here. In the case of =Za, it becomes. That is, this circuit is matched to a signal source/load impedance equal to Za, and all input signal power is output to diagonal terminals. In this way, the circuit is in cross mode.
以上説明したように本発明によるマイクロ披双極双投ス
イッチは、一平面の構造であるので回路製作、集積回路
への組み込みが容易であり、かつ、慨械的強度、耐振性
が優れているから、高信頼化を図ることができる。した
がって、例えば人工衛星に搭載するマイクロ波通信機器
の切替などに適している。As explained above, the micro double-pole double-throw switch according to the present invention has a one-plane structure, which makes it easy to manufacture circuits and incorporate it into integrated circuits, and has excellent mechanical strength and vibration resistance. , high reliability can be achieved. Therefore, it is suitable for switching microwave communication equipment mounted on an artificial satellite, for example.
第1図は本発明の一実施例を示す図、12図は従来の双
極双投スイッチの例を示す図である。
1〜4.51〜54 ・・・・・・信号端子、 5゜6
.7 ・・・・・・ 1/4披長線路、 8.9 ・
・・・・・半波gcM路、 10 .11 .55−
58・・・・・・スイッチング素子、 59 ・・・
・・・立体交差部
代理人 弁理士 本 間 崇悴 2 図FIG. 1 is a diagram showing an embodiment of the present invention, and FIG. 12 is a diagram showing an example of a conventional double-pole double-throw switch. 1~4.51~54...Signal terminal, 5゜6
.. 7 ・・・・・・ 1/4 length line, 8.9 ・
...Half-wave gcM path, 10. 11. 55-
58...Switching element, 59...
...Grade Intersection Agent Patent Attorney Takayoshi Honma 2 Figure
Claims (1)
1)と端子(2)、端子(3)と端子(4)をそれぞれ
等しい特性インピーダンスの1/4波長線路またはその
奇数倍長の線路(5)あるいは(7)で結び、隣り合う
端子(1)と端子(3)、端子(2)と端子(4)をそ
れぞれ等しい特性インピーダンスの半波長またはその整
数倍長の線路(8)あるいは(9)で結び、これら2本
の線路(8)および(9)のそれぞれの中点どうしを1
/4波長またはその奇数倍長の線路(6)で結び、該線
路(6)の特性インピーダンスと前記線路(5)あるい
は(7)の特性インピーダンスの相乗平均値を線路(8
)あるいは(9)の特性インピーダンスに等しくすると
ともに、該線路(8)および(9)の中点をスイッチン
グ素子を介して接地することを特徴とするマイクロ波双
極双投スイッチ。It has four terminals, and among these four terminals, adjacent terminals (
1) and terminal (2), and terminal (3) and terminal (4), respectively, are connected by a 1/4 wavelength line with equal characteristic impedance or a line (5) or (7) of an odd multiple of the length, and ) and the terminal (3), and the terminal (2) and the terminal (4), respectively, are connected by a line (8) or (9) of half a wavelength or an integral multiple thereof with equal characteristic impedance, and these two lines (8) and The midpoints of each of (9) are 1
/4 wavelength or an odd multiple thereof, and the geometric mean value of the characteristic impedance of the line (6) and the characteristic impedance of the line (5) or (7) is determined as the line (8).
) or (9), and the midpoint of the lines (8) and (9) is grounded via a switching element.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP30810586A JPS63164502A (en) | 1986-12-26 | 1986-12-26 | Microwave bipolar double-throw switch |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP30810586A JPS63164502A (en) | 1986-12-26 | 1986-12-26 | Microwave bipolar double-throw switch |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63164502A true JPS63164502A (en) | 1988-07-07 |
Family
ID=17976928
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP30810586A Pending JPS63164502A (en) | 1986-12-26 | 1986-12-26 | Microwave bipolar double-throw switch |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63164502A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2004236085A (en) * | 2003-01-31 | 2004-08-19 | Japan Radio Co Ltd | Cruciform t branch circuit |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2984797A (en) * | 1958-11-24 | 1961-05-16 | Raytheon Co | Coaxial switches and power dividers |
-
1986
- 1986-12-26 JP JP30810586A patent/JPS63164502A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2984797A (en) * | 1958-11-24 | 1961-05-16 | Raytheon Co | Coaxial switches and power dividers |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2004236085A (en) * | 2003-01-31 | 2004-08-19 | Japan Radio Co Ltd | Cruciform t branch circuit |
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