JPH061845B2 - Multiple wave demultiplexer / multiplexer - Google Patents
Multiple wave demultiplexer / multiplexerInfo
- Publication number
- JPH061845B2 JPH061845B2 JP20151886A JP20151886A JPH061845B2 JP H061845 B2 JPH061845 B2 JP H061845B2 JP 20151886 A JP20151886 A JP 20151886A JP 20151886 A JP20151886 A JP 20151886A JP H061845 B2 JPH061845 B2 JP H061845B2
- Authority
- JP
- Japan
- Prior art keywords
- stage
- line
- lmn
- characteristic impedance
- distribution loss
- 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 - Fee Related
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Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は、例えばアンテナ共用装置等として複数波を分
波又は合波する複数波分・合波装置に関するものであ
る。Description: TECHNICAL FIELD The present invention relates to a multi-wave demultiplexing / multiplexing device that demultiplexes or multiplexes a plurality of waves, for example, as an antenna sharing device.
(従来技術) 従来の共振器と結合線路を使った複数波分・合波装置
は、第3図に示すように、それぞれ異なる周波数f
111,f112,…flmnの信号波を出す送信機1
111,1112,…1lmnを対応する共振周波数の共
振器2111,2112,…2lmnに1対1に接続し、
これら共振器2111〜2lmnをグループ単位で長さl
1がそれぞれ(2n1+1)λ0/4(ただし、λ0=
中心周波数の波長、n1=0,1,2…)の電気長を有
する特性インピーダンスZの第1段の結合線路
3111,3112,…3lmnを介して接続して第1段
の複数のジャンクション部411,412,…41Nを形
成し、第1段の複数のジャンクション部411〜41Nを
グループ単位で長さl2がそれぞれn2λ0/2(ただ
し、n2=1.2…)の電気長を有する特性インピーダ
ンスZの第2段の結合線路521,522…52Mを介し
て接続して第2段の複数のジャンクション部621…6
2Mを形成し、第2段のジャンクション部621…62Mを
長さl3がそれぞれn3λ0/2(ただし、n3=1,
2,…)の電気長を有する特性インピーダンスZの第3
段の結合線路731,73Lを介して接続して最終段(第
3段)のジャンクション部83Lを形成し、この最終段の
ジャンクション部83Lを共用端子部としてアンテナ部9
に接続した構造であった。このような複数波分・合波装
置は、各ジャンクション部411〜41N,621〜
62M,83Lにて合波するチャンネルのアドミタンスを無
限大として他チャンネルへのもれ込みによる損失(以
下、分配損失という)を小さくして複数の波(L×M×
N)を合波している。(Prior Art) A conventional multi-wave division / multiplexing device using a resonator and a coupling line has different frequencies f as shown in FIG.
Transmitter 1 for generating signal waves 111 , f 112 , ... F lmn
111, 1 112, connect ... 1 lmn resonator 2 111, 2 112 of the corresponding resonant frequency, ... to 2 lmn one-to-one,
These resonators 2 111 to 2 lmn have a length l in units of groups.
1 each (2n 1 +1) λ 0/ 4 ( However, λ 0 =
Wavelength of the center frequency, n 1 = 0, 1, 2 ... in the first stage of the characteristic impedance Z having an electrical length of) the coupling line 3 111, 3 112, a plurality of first stage connected via a ... 3 lmn junction section 4 11, 4 12, ... 4 1N is formed, length l 2 are each a plurality of junction portions 4 11 to 4 1N first stage in groups n 2 λ 0/2 (although, n 2 = 1.2 ...) in the second stage of the characteristic impedance Z having an electrical length coupling line 5 21, 5 22 ... plurality of the second stage are connected via a 5 2M junctions 6 21 ... 6
Forming a 2M, the junction portion 6 21 ... 6 2M in the second stage a length l 3, respectively n 3 λ 0/2 (although, n 3 = 1,
The third of the characteristic impedance Z having an electric length of 2, ...)
The junction portion 8 3L of the final stage (third stage) formed by connecting via the coupling line 7 31, 7 3L stages antenna portion 9 junction portion 8 3L of the final stage as a common terminal portion
It was a structure connected to. Such multiple wave component-multiplexing apparatus, each junction portions 4 11 ~4 1N, 6 21 ~
The admittance of the channels multiplexed at 6 2M and 8 3L is set to infinity to reduce the loss (hereinafter referred to as distribution loss) due to leaking into other channels, and multiple waves (L × M ×
N) is multiplexed.
この場合の送信周波数flmnについての等価回路は第4
図に示すようになりジャンクション部411における全
アドミタンスY11は次のようになる。なお、図におい
て、G0,GLは正規化アドミタンスである。The equivalent circuit for the transmission frequency f lmn in this case is the fourth
All admittance Y 11 at junctions 4 11 becomes as shown in FIG is as follows. In the figure, G 0 and G L are normalized admittances.
ここで、αは線路の減衰定数、Yは共振器のアドミタン
ス ジャンクション部621における全アドミタンスY2は 同じようにしてジャンクション部83Lにおける全アドミ
タンスY3は ただし、Y2Mは式(1),(4)を使って求める。 Here, α is the attenuation constant of the line, Y is the admittance of the resonator, and the total admittance Y 2 at the junction unit 6 21 is Similarly, the total admittance Y 3 at the junction 8 3L is However, Y 2M is obtained by using equations (1) and (4).
以上のように求めてゆくと、第5図のような等価回路と
なり、この分配損失は次式のSマトリクスから求めるこ
とができる。When obtained as described above, an equivalent circuit as shown in FIG. 5 is obtained, and this distribution loss can be obtained from the S matrix of the following equation.
ただし、βnは各線路の位相定数分配損失 L=20log|A+B+C+D|/2 …(11) 以上の式より分配損失を計算すると、合波数が多くなる
ほど結合線路3111〜73Lの分配損失の周波数特性
が劣化する。 However, β n is the phase constant distribution loss of each line L = 20 log | A + B + C + D | / 2 (11) When the distribution loss is calculated from the above equation, the coupling line 3 111 increases as the number of multiplexing increases. The frequency characteristic of the distribution loss of ˜73 L is deteriorated.
第6図は簡単なモデルとして共振器の代りに等価な短絡
器をつけた結合線路の分配損失の周波数特性を示す。FIG. 6 shows, as a simple model, the frequency characteristic of the distribution loss of the coupled line in which an equivalent short circuit is attached instead of the resonator.
(発明が解決しようとする問題点) 上記したように従来の複数波分・合波装置は、合波数が
多くなるほど各結合線路の分配損失の周波数特性が劣化
する問題点があった。(Problems to be Solved by the Invention) As described above, the conventional multiple wave demultiplexing / multiplexing device has a problem that the frequency characteristic of distribution loss of each coupling line deteriorates as the number of multiplexing increases.
本発明の目的は、分配損失を低減できる複数波分・合波
装置を提供するにある。An object of the present invention is to provide a multiple wave demultiplexing / multiplexing device that can reduce distribution loss.
(問題点を解決するための手段) 上記の目的を達成するための本発明の構成を、実施例に
対応する第1図を参照して説明すると、本発明は複数の
共振器2111,2112,…2lmnをグループ単位で
それぞれ(2n1+1)λ0/4(ただし、λ0=中心
周波数の波長、n1=0,1,2…)の電気長を有する
第1段の結合線路3111,3112,…3lmnを介し
て接続した第1の複数のジャンクション部411,4
12,……41Nを形成し、前記第1段の複数のジャンク
ション部411,412……41Nをそれぞれn2λ0/
2(ただし、n2=0,1,2…)の電気長を有する第
2段の結合線路521,522,…52Mを介して接続し
て第2段のジャンクション部621〜62Mを形成し、最
終段のジャンクション部83Lを共用端子部とした複数波
分・合波装置において、前記第2段以上の結合線路5
21〜732はその特性インピーダンスが前記第1段の
結合線路3111,3112,……3lmnの特性インピ
ーダンスより高く定められていることを特徴とする。(Means for Solving the Problems) The configuration of the present invention for achieving the above object will be described with reference to FIG. 1 corresponding to the embodiment. The present invention will be described with reference to a plurality of resonators 2 111 and 2 2. 112, ... 2 lmn respectively a group unit (2n 1 +1) λ 0/ 4 ( provided that, lambda 0 = wavelength of the center frequency, n 1 = 0,1,2 ...) coupling the first stage having an electrical length of First plurality of junction sections 4 11 , 4 connected via lines 3 111 , 3 112 , ... 3 lmn
12 ... 4 1N are formed, and each of the plurality of first-stage junction portions 4 11 , 4 12 ... 4 1N is n 2 λ 0 /
2 (however, n 2 = 0, 1, 2 ...) of the coupling line 5 21 of the second stage having an electrical length, 5 22, the second stage are connected via a ... 5 2M junctions 6 21-6 In the multiple wave demultiplexing / multiplexing device that forms 2M and uses the junction section 8 3L at the final stage as a common terminal section, the coupled line 5 at the second stage or higher
21-7 32 is characterized in that its characteristic impedance is set higher than the characteristic impedance of the first stage of the coupling line 3 111, 3 112, ...... 3 lmn.
(作用) このように第2段以上の結合線路521〜732の特性
インピーダンスを第1段の結合線路3111〜3lmnの
特性インピーダンスより高くすることにより分配損失の
周波数特性を平坦に近づけて該分配損失を低減すること
ができる。(Operation) As described above, the characteristic impedance of the coupling lines 5 21 to 7 32 of the second stage and above is made higher than the characteristic impedance of the coupling lines 3 111 to 3 lmn of the first stage, thereby making the frequency characteristic of the distribution loss close to flat. The distribution loss can be reduced.
(実施例) 以下本発明の実施例を第1図を参照して説明する。な
お、前述した第3図と対応する部分には同一符号を付し
て示している。(Embodiment) An embodiment of the present invention will be described below with reference to FIG. The parts corresponding to those in FIG. 3 described above are designated by the same reference numerals.
本実施例では、第2段以上の結合線路521,522,
…732の特性インピーダンスを、第1段の結合線路3
111,3112,…3lmnより高くした構造として
いる。In the present embodiment, the coupled lines 5 21 , 5 22 of the second stage and above,
The characteristic impedance of 7 32 is set to the coupled line 3 of the first stage.
The structure is higher than 111 , 3 112 , ... 3 lmn .
即ち、本実施例では、末端が32条の結合線路の例につ
いて示している。各送信機1111〜1lmnからの各波
は、50Ω線路を伝わつて各共振器2111〜2lmnに
入力されるようになっている。各共振器2111〜2
lmnは4個づつ電気長がl1=(2n1+1)λ0/4
の第1段の結合線路3111〜3lmnで結合されて第1
段のジャンクション部411,412…418が形成さ
れている。第1段の結合線路3111〜3lmnに特性イ
ンピーダンスはZ1Ωに定められている。第1段のジャ
ンクション部411〜418は4個づつ電気長がl2=
n2λ0/2の第2段の結合線路521,522…5
28で結合されて第2段のジャンクション部621,6
22が形成されている。第2段の結合線路521〜5
28の特性インピーダンスはZ2Ωに定められている。
第2段のジャクション部621,622は電気長がl3
=n3λ0/2の第3段の結合線路731,732で結
合されて第3段(最終段)のジャンクション部831が
形成されている。第3段の結合線路731,732の特
性インピーダンスはZ3Ωに定められている。最終段の
ジャンクション部831は50Ω線路でアンテナ端9に
接続されている。最終段のジャンクション部31は50
Ω線路でアンテナ線9に接続されている。That is, in the present embodiment, an example of a coupled line having 32 ends is shown. Each wave from each transmitter 1 111 to 1 lmn is adapted to be inputted One Tsutawa the 50Ω line to each of the resonators 2 111 to 2 lmn. Each resonator 2 111 to 2
lmn is four by one electrical length l 1 = (2n 1 +1) λ 0/4
Of the first stage coupled lines 3 111 to 3 lmn
Junction portions 4 11 , 4 12 ... 4 18 in steps are formed. The characteristic impedance of the first-stage coupled lines 3 111 to 3 lmn is set to Z 1 Ω. Junctions 4 11-4 18 four increments electrical length of the first stage is l 2 =
n 2 lambda 0/2 of the second stage of the coupling line 5 21, 5 22 ... 5
The second-stage junction parts 6 21 , 6 are connected by 28.
22 is formed. Coupling line of the second stage 5 21-5
The characteristic impedance of 28 is set to Z 2 Ω.
The electric lengths of the second-stage junctions 6 21 and 6 22 are l 3
= Junctions 8 31 n 3 lambda 0 / coupling line 7 31 of the third stage 2, 7 32 third stage is coupled with (final stage) are formed. The characteristic impedance of the third-stage coupled lines 7 31 and 7 32 is set to Z 3 Ω. Junctions 8 31 of the final stage is connected to the antenna terminal 9 at 50Ω line. The junction section 31 at the final stage is 50
It is connected to the antenna line 9 by an Ω line.
従来、式(3),(6),(9),(10)では、線路の
特性インピーダンスを正規化してZL/Z0=1(ただ
し、Z0は特性インピーダンス50Ω)としていたが、
各線路の特性インピーダンスを入力できるように各式を
変換すると、 式(3)は YL1=50/Z1・coth{αl1+jπ(2n1+1)/2・(flmn-f0)f0}
…(12) 式(6)は YL2=50/Z2・coth{αl2+jπn2(flmlmn-f0)/f0}…(13) 式(9)は YL3=50/Z3・coth{αl3+jπn3(flmlmn-f0)/f0}…(14) となる。式(10)の中の線路l1の線路定数Sマトリッ
クスは である。線路l2,l3についても同様である。Conventionally, in equations (3), (6), (9), and (10), the characteristic impedance of the line was normalized to Z L / Z 0 = 1 (where Z 0 is the characteristic impedance 50Ω).
When each equation is converted so that the characteristic impedance of each line can be input, equation (3) yields Y L1 = 50 / Z 1 · coth {αl 1 + jπ (2n 1 +1) / 2 · (f lmn -f 0 ) f 0 }
(12) Formula (6) is Y L2 = 50 / Z 2 · coth {αl 2 + jπn 2 (flm lmn -f 0 ) / f 0 } (13) Formula (9) is Y L3 = 50 / Z 3 · coth {αl 3 + jπn 3 (flm lmn -f 0 ) / f 0 } (14) The line constant S matrix of the line l 1 in the equation (10) is Is. The same applies to the lines l 2 and l 3 .
式(6),式(9)におけるアドミタンスYL2,Y
L3は、この式よりできるだけ小さくなればよいため式
(13),式(14)において各線路の特性ンピーダンスZ
2,Z3は無限大の方が従来の50Ω線路よりアドミタ
ンスYL2,YL3が小さくなることがわかる。Admittances Y L2 and Y in equations (6) and (9)
Since L3 should be as small as possible than this equation, the characteristic impedance Z of each line in equations (13) and (14)
It can be seen that admittances Y L2 and Y L3 are smaller when 2 and Z 3 are infinite than in the conventional 50Ω line.
これらを計算すると、各線路の特性インピーダンス
Z2,Z3を無限大に、線路の特性インピーダンスZ1
を40〜50Ωにすれば、分配損失の周波数特性を平坦
に近づけて分配損失を低減できるが、実用上無限大の特
性インピーダンスは無理なので、Z2=Z3=87Ω,
Z1=50Ωとして共振器の代りに等価な短絡器を取り
付けた。このときの分配損失の周波数特性を第2図に実
線で示す。破線で示した従来タイプのものと比較する
と、分配損失は広帯域で低損失の特性になっていること
がわかる。When these are calculated, the characteristic impedances Z 2 and Z 3 of each line are set to infinity, and the characteristic impedance Z 1 of the line is set.
Is 40 to 50Ω, the frequency characteristic of the distribution loss can be brought close to a flat value to reduce the distribution loss. However, since infinite characteristic impedance is practically impossible, Z 2 = Z 3 = 87Ω,
An equivalent short circuiter was attached instead of the resonator with Z 1 = 50Ω. The frequency characteristic of the distribution loss at this time is shown by the solid line in FIG. Compared with the conventional type shown by the broken line, it can be seen that the distribution loss has a wide band and low loss characteristics.
なお、上記の実施例では結合線路の構成が3段の場合に
ついて示したが、本発明はこれに限定されるものではな
く、2段以上であれば何段でもよい。Although the above embodiment has shown the case where the coupling line has three stages, the present invention is not limited to this, and any number of stages may be used as long as it has two or more stages.
(発明の効果) 以上説明したように本発明に係る複数波分・合波装置
は、第2段以上の結合線路の特性インピーダンスを第1
段の結合線路の特性インピーダンスより高くしたので、
分配損失の周波数特性を平坦に近づけることにより該分
配損失を低減することができる。(Effects of the Invention) As described above, the multiple wave demultiplexing / multiplexing device according to the present invention has the characteristic impedance of the coupled line of the second stage or higher as the first characteristic impedance.
Since it is higher than the characteristic impedance of the coupled line of the stage,
The distribution loss can be reduced by making the frequency characteristic of the distribution loss close to flat.
第1図は本発明に係る複数波分・合波装置の一実施例の
概略構成を示すブロック図、第2図は本発明と従来の装
置の分配損失の周波数特性の対比図、第3図は従来の装
置のブロック図、第4図及び第5図は従来の装置の等価
回路図、第6図は従来の装置の分配損失の周波数特性図
である。 1111〜1lmn…送信機、2111〜2lmn…共振器、
3111〜3lmn…第1段の結合線路、521〜528
…第2段の結合線路、731,732…第3段の結合線
路、411〜418…第1段のジャンクション部、6
21,622…第2段のジャンクション部、831…最
終段のジャンクション部。FIG. 1 is a block diagram showing a schematic configuration of an embodiment of a multiple wave demultiplexing / multiplexing device according to the present invention, FIG. 2 is a comparison diagram of frequency characteristics of distribution loss between the present invention and a conventional device, and FIG. Is a block diagram of a conventional device, FIGS. 4 and 5 are equivalent circuit diagrams of the conventional device, and FIG. 6 is a frequency characteristic diagram of distribution loss of the conventional device. 1 111 to 1 lmn ... Transmitter, 2 111 to 2 lmn ... Resonator,
3 111 to 3 lmn ... First-stage coupled line, 5 21 to 5 28
... second stage coupling line, 7 31, 7 32 ... third stage coupling line, 4 11-4 18 ... junction portion of the first stage, 6
21 , 6 22 ... Second-stage junction section, 8 31 ... Final-stage junction section.
Claims (1)
(2n1+1)λ0/4(ただし、λ0=中心周波数の
波長、n1=0,1,2…)の電気長を有する第1段の
結合線路を介して接続して第1段の複数のジャンクショ
ン部を形成し、前記第1段の複数のジャンクション部を
それぞれn2λ0/2(ただし、n2=0,1,2…)
の電気長を有する第2段の結合線路を介して接続して第
2段のジャンクション部を形成し、最終段のジャンクシ
ョン部を共用端子部とした複数波分・合波装置におい
て、前記第2段以上の結合線路はその特性インピーダン
スが前記第1段の結合線路の特性インピーダンスより高
く定められていることを特徴とする複数波分・合波装
置。1. A plurality of resonators in groups (2n 1 +1) λ 0/ 4 ( provided that the wavelength of lambda 0 = center frequency, n 1 = 0, 1, 2 ...) first has an electrical length of through the one-stage coupling line to form a plurality of junctions of the first stage are connected, a plurality of junctions each n 2 λ 0/2 of the first stage (where, n 2 = 0, 1, 2 ...)
In the multi-wave demultiplexing / multiplexing device, the second-stage junction section is formed by connecting via the second-stage coupling line having the electric length of The multiple-wave demultiplexing / multiplexing device is characterized in that the characteristic impedance of the coupled line of more than one stage is set higher than the characteristic impedance of the coupled line of the first stage.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20151886A JPH061845B2 (en) | 1986-08-29 | 1986-08-29 | Multiple wave demultiplexer / multiplexer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20151886A JPH061845B2 (en) | 1986-08-29 | 1986-08-29 | Multiple wave demultiplexer / multiplexer |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6359102A JPS6359102A (en) | 1988-03-15 |
JPH061845B2 true JPH061845B2 (en) | 1994-01-05 |
Family
ID=16442373
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP20151886A Expired - Fee Related JPH061845B2 (en) | 1986-08-29 | 1986-08-29 | Multiple wave demultiplexer / multiplexer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH061845B2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6157272A (en) * | 1997-06-28 | 2000-12-05 | Kuo; Mei-Shong | Power network for collecting distributed powers |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2009120370A (en) * | 2007-11-16 | 2009-06-04 | Toshiba Elevator Co Ltd | Elevator |
JP5501268B2 (en) * | 2011-02-28 | 2014-05-21 | 株式会社日立製作所 | Elevator equipment |
-
1986
- 1986-08-29 JP JP20151886A patent/JPH061845B2/en not_active Expired - Fee Related
Also Published As
Publication number | Publication date |
---|---|
JPS6359102A (en) | 1988-03-15 |
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