JPS62203410A - Series connection type infinite phase shifter - Google Patents
Series connection type infinite phase shifterInfo
- Publication number
- JPS62203410A JPS62203410A JP4583186A JP4583186A JPS62203410A JP S62203410 A JPS62203410 A JP S62203410A JP 4583186 A JP4583186 A JP 4583186A JP 4583186 A JP4583186 A JP 4583186A JP S62203410 A JPS62203410 A JP S62203410A
- Authority
- JP
- Japan
- Prior art keywords
- phase
- phase shifter
- output
- infinite
- hyb
- 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
- 230000010363 phase shift Effects 0.000 claims abstract description 6
- 230000015572 biosynthetic process Effects 0.000 claims 1
- 238000003786 synthesis reaction Methods 0.000 claims 1
- 238000010586 diagram Methods 0.000 description 9
- 230000000694 effects Effects 0.000 description 4
- 230000002542 deteriorative effect Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000005562 fading Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔概要〕
直列接続型無限移相器において、2つの無限移相器を直
列接続し、第1及び第2の振幅変調器に加える制御電圧
をvl・sin θ、V 2=cosθ及びV 2゜−
Vlとすることにより、0度から360度まで入力信号
の位相を移相しても周波数特性の改善された信号を取出
す様にしたものである。[Detailed Description of the Invention] [Summary] In a series-connected infinite phase shifter, two infinite phase shifters are connected in series, and the control voltages applied to the first and second amplitude modulators are set to vl·sin θ, V 2=cos θ and V 2゜-
By setting Vl, a signal with improved frequency characteristics can be extracted even if the phase of the input signal is shifted from 0 degrees to 360 degrees.
本発明は、例えばスペースダイハシチ方式に使用する無
限移相器の改良に関するものである。The present invention relates to an improvement of an infinite phase shifter used, for example, in a space die-cut system.
近年、ディジタル多重無線方式が広く用いられているが
、フェージングの発生する可能性のある伝搬路において
はスペースダイバシチ方式が採用される。この方式は、
主アンテナと副アンテナで受信された広いスペクトラム
分布を持つ信号を、例えばそれぞれ中間周波数帯の信号
に変換し、副アンテナよりの信号を無限移相器で移相さ
せた後に主アンテナの信号と同相合成して、常に合成波
のレベルが最大になる様に無限移相器の移相量を制御す
る。In recent years, digital multiplex radio systems have been widely used, but space diversity systems are employed in propagation paths where fading may occur. This method is
For example, the signals with a wide spectrum distribution received by the main antenna and the auxiliary antenna are converted into intermediate frequency band signals, and after the signal from the auxiliary antenna is phase-shifted by an infinite phase shifter, it is in phase with the signal of the main antenna. The amount of phase shift of the infinite phase shifter is controlled so that the level of the synthesized wave is always maximized.
この時、無限移相器は副アンテナよりの信号の位相を周
波数特性を劣化させずに0度から360度まで移相させ
ることが必要である。At this time, the infinite phase shifter is required to shift the phase of the signal from the auxiliary antenna from 0 degrees to 360 degrees without deteriorating the frequency characteristics.
第3図は従来例のブロック図、第4図は第3図の動作説
明図で、1は無限移相器を示す。FIG. 3 is a block diagram of a conventional example, and FIG. 4 is an explanatory diagram of the operation of FIG. 3, where 1 indicates an infinite phase shifter.
以下、第4図を参照して第3図の動作を説明する。The operation shown in FIG. 3 will be explained below with reference to FIG.
第3図において、振幅Aの入力信号は90度ハイブリッ
ド回路(以下90度11VBと省略する)11で90度
の位相差のある第1及び第2の信号に分配されて振幅変
調器12.13に加えられる。この振幅変調器は、例え
ばリング変調器で構成され、第1の制御電圧VH以下V
lと省略する)・sinθ、第2の制御電圧ν2(以下
ν2と省略する)= cosθが加えられているで、θ
の値を変化することにより、第1及び第2の信号の振幅
が変化する。In FIG. 3, an input signal of amplitude A is distributed by a 90 degree hybrid circuit (hereinafter abbreviated as 90 degrees 11VB) 11 into first and second signals having a phase difference of 90 degrees, and is divided into first and second signals having a phase difference of 90 degrees, and the input signal is divided into amplitude modulators 12 and 13. added to. This amplitude modulator is composed of, for example, a ring modulator, and is lower than or equal to the first control voltage VH.
(abbreviated as l)・sin θ, second control voltage ν2 (hereinafter abbreviated as ν2) = cos θ is added, and θ
By changing the value of , the amplitudes of the first and second signals change.
即ち、第4図fatに示す様にθ=θ1の時の振幅変調
器12.13の出力信号の振幅は■、■′となるので、
これを同相!IYB 14で合成すると01だけ移相し
た信号が、θ=θ2の場合はθまたけ移相した信号がそ
れぞれ出力する。そして、例えばθ=0度の場合はsi
nθはQ、cosθは1になるので振幅変調器12の出
力はOとなって振幅変調器13から90度移相した信号
■だけか、θ=90度の場合は振幅変調器12より同相
の信号だけが同相!1YB 14を通って出力する。That is, as shown in FIG. 4 fat, when θ=θ1, the amplitudes of the output signals of the amplitude modulators 12 and 13 are ■, ■',
This is the same phase! When combined by IYB 14, a signal whose phase is shifted by 01 is output, and when θ=θ2, a signal whose phase is shifted by θ is output. For example, if θ=0 degrees, si
Since nθ is Q and cosθ is 1, the output of the amplitude modulator 12 is O, and either only the signal ■ whose phase is shifted by 90 degrees is output from the amplitude modulator 13, or when θ = 90 degrees, the output of the amplitude modulator 12 is output from the amplitude modulator 12. Only the signals are in phase! Output through 1YB14.
以上説明した従来例の無限移相器の場合、90度+1Y
B 11の周波数特性は第4図(b)に示す様に端子1
から端子2の周波数特性が、例えば下に凸に、端子1か
ら端子2の周波数特性は反対に上に凸になっているので
、端子2と3とを通った2つの信号が同相II Y B
14で合成されると補償されて周波数特性は平坦にな
るが、信号が1つの時は補償されず上に凸又は下に凸の
周波数特性を持つ信号が出力される。そこで、θが0度
、90度、180度、270度の時は同相+1VBに加
えられる信号は1つしかないので、90度+1Y[lで
発生した周波数特性を持つ信号がそのまま出力される。In the case of the conventional infinite phase shifter explained above, 90 degrees + 1Y
The frequency characteristics of B11 are as shown in Figure 4(b).
For example, the frequency characteristic of terminal 2 is convex downward, and the frequency characteristic of terminal 1 to terminal 2 is convex upward, so the two signals passing through terminals 2 and 3 are in phase II Y B
When the signals are combined in step 14, they are compensated and the frequency characteristics become flat, but when there is only one signal, the signals are not compensated and a signal with an upwardly convex or downwardly convex frequency characteristic is output. Therefore, when θ is 0 degrees, 90 degrees, 180 degrees, and 270 degrees, only one signal is added to the in-phase +1VB, so the signal with the frequency characteristics generated at 90 degrees + 1Y[l is output as is.
そこで、θを0度から360度まで変化した時に周波数
特性の劣化した信号が出力されると云う問題点がある。Therefore, there is a problem in that when θ is changed from 0 degrees to 360 degrees, a signal with deteriorated frequency characteristics is output.
この為、合成された信号のレベルが変動し誤り率が劣化
する可能性がある。Therefore, the level of the combined signal may vary and the error rate may deteriorate.
上記の問題点は第1図に示す如く、該無限移相器を直列
接続し、第1の無限移相器1の該第1及び第2の振幅変
調器12.13に制御電圧sin θ及びcos θを
、第2の無限移相器2の該第1及び第2の振幅変調器2
2.23に制?fll電圧5in(θ+モ及びcos
Cθ+シを加える様にした本発明の直列接続型無限移相
器により解決される。The above problem is solved by connecting the infinite phase shifters in series as shown in FIG. cos θ of the first and second amplitude modulators 2 of the second infinite phase shifter 2
Restricted on 2.23? fll voltage 5in (θ + mo and cos
This problem is solved by the series-connected infinite phase shifter of the present invention which adds Cθ+C.
本発明は、90度+!Ynの端子1から端子3までの周
波数特性と端子1から端子2までの周波数特性は逆特性
になっていることを利用して、直列接続された第1及び
第2の無限移相器1,2のうち、第1の無限移相器の中
の90度+1YB 11の端子lから端子2に出力した
信号は第2の無限移相器の中の90度1(YB 21の
端子1から端子3に、90度HYB 11の端子lから
端子3に出力した信号は90度11YB 21の端子l
から端子2にそれぞれ出力させる様にした。The present invention is 90 degrees +! Utilizing the fact that the frequency characteristics from terminal 1 to terminal 3 and the frequency characteristic from terminal 1 to terminal 2 of Yn are opposite characteristics, the first and second infinite phase shifters 1, which are connected in series, 2, the signal output from terminal l of YB 11 to terminal 2 in the first infinite phase shifter is 90 degrees 1 in the second infinite phase shifter (from terminal 1 of YB 21 to terminal 3, the signal output from terminal l of 90 degree HYB 11 to terminal 3 is output to terminal l of 90 degree 11YB 21.
I made it output from terminal 2 respectively.
そこで、θが0度、90度、180度、270度の時は
90度+1YB 11と21の下に凸と上に凸の周波数
特性とが補償され、θを0度から360度まで変化した
時に周波数特性が改善された信号が出力する。Therefore, when θ is 0 degrees, 90 degrees, 180 degrees, and 270 degrees, the downward convex and upward convex frequency characteristics of 11 and 21 are compensated for by 90 degrees + 1 YB, and θ is changed from 0 degrees to 360 degrees. Sometimes a signal with improved frequency characteristics is output.
第1図は本発明の実施例のブロック図、第2図は第1図
の動作説明図を示す。尚、企図を通じて同一記号は同一
対象物を示す。FIG. 1 is a block diagram of an embodiment of the present invention, and FIG. 2 is an explanatory diagram of the operation of FIG. 1. It should be noted that the same symbols refer to the same objects throughout the design.
以下、θが0度の場合を例にして第2図を参照して第1
図の動作を説明する。Hereinafter, using the case where θ is 0 degrees as an example, and referring to FIG.
The operation of the diagram will be explained.
先ず、第1の無限移相器1に入力した信号は90度+1
YB 11で分配されて振幅変調器12.13に加えら
れるが、vlが0の為に振幅変調器12の出力は0とな
り、振幅変調器13の出力のみが同相11YB 14を
通って第2の無限移相器2に加えられる。First, the signal input to the first infinite phase shifter 1 is 90 degrees +1
It is distributed by YB 11 and applied to amplitude modulators 12 and 13, but since vl is 0, the output of amplitude modulator 12 is 0, and only the output of amplitude modulator 13 passes through in-phase 11YB 14 to the second Added to infinite phase shifter 2.
この人力信号は90度11’/B 21で分配されるが
、振幅変調器23の出力は0となるので振幅変調器22
の出力のみが同相+1VB 24より出力される。This human input signal is distributed at 90 degrees 11'/B 21, but since the output of the amplitude modulator 23 is 0, the amplitude modulator 22
Only the output is output from the in-phase +1VB 24.
この時、第2図のθ=0度に示す様に下に凸の周波数特
性を持った信号が同相11YB 14から出力されるが
、これは90度HYB 21の端子2より出力されるこ
とにより周波数特性が改善されて同相+1VB 24よ
り出力される。At this time, as shown at θ=0 degrees in Figure 2, a signal with a downwardly convex frequency characteristic is output from the in-phase 11YB 14, but this is because it is output from the terminal 2 of the 90 degree HYB 21. The frequency characteristics are improved and the signal is output from the in-phase +1VB 24.
の接続は2個の場合について説明したが、偶数個(でも
同様な効果を得ることは明らかである。The explanation has been made for the case where two connections are made, but it is clear that the same effect can be obtained even with an even number of connections.
又、第1の無限移相器にてθ、第2の無限移相器にて(
θ++)移相される為、合計(2θ++)の移相量とな
るので、全体でθ′の移相量となる場合はθ=キー÷と
すればよい。Also, the first infinite phase shifter has θ, and the second infinite phase shifter has (
Since the phase is shifted by θ++), the total phase shift amount is (2θ++), so if the total phase shift amount is θ', θ=key÷ may be used.
以上詳細に説明した様に、2つの無限移相器を直列接続
することによりθを0度から360度まで変化しても周
波数特性の改善された信号が得られると云う効果がある
。As explained in detail above, by connecting two infinite phase shifters in series, there is an effect that a signal with improved frequency characteristics can be obtained even when θ is changed from 0 degrees to 360 degrees.
第1図は本発明の実施例のブロック図、第2図は第1図
の動作説明図、
第3図は従来例のブロック図、
第4図は第3図の動作説明図を示す。
図において、
1.2は無限移相器、
11、21は90度ハイブリッド回路、12、13.2
2.23は振幅変富商器、14゜24は同相ハイブリッ
ド回路を示す。
ネ1 叫
(α)(b)
卒4 糾1 is a block diagram of an embodiment of the present invention, FIG. 2 is an explanatory diagram of the operation of FIG. 1, FIG. 3 is a block diagram of a conventional example, and FIG. 4 is an explanatory diagram of the operation of FIG. 3. In the figure, 1.2 is an infinite phase shifter, 11 and 21 are 90 degree hybrid circuits, 12 and 13.2
2.23 is an amplitude converter, and 14°24 is an in-phase hybrid circuit. Ne1 Shout (α) (b) Graduation 4
Claims (1)
分配する90度ハイブリッド回路と、移相量θに対して
sinθ及びcosθに対応する制御電圧V1及びV2
により該90度ハイブリッド回路の出力を振幅変調する
第1及び第2の振幅変調器と、該第1及び第2の振幅変
調器の出力を同相合成する同相ハイブリッド回路とから
構成された無限移相器において、 該無限移相器を2つ直列接続し、第1の無限移相器(1
)の該第1及び第2の振幅変調器(12,13)に制御
電圧V1及びV2を、第2の無限移相器(2)の該第1
及び第2の振幅変調器(22,23)に制御電圧V2及
び−V1を加える様にしたことを特徴とする直列接続型
無限移相器。[Claims] A 90 degree hybrid circuit that distributes an input signal into first and second signals with a 90 degree phase difference, and control voltages V1 and V2 corresponding to sin θ and cos θ with respect to the phase shift amount θ.
an infinite phase shift circuit comprising first and second amplitude modulators that amplitude modulate the output of the 90-degree hybrid circuit, and an in-phase hybrid circuit that performs in-phase synthesis of the outputs of the first and second amplitude modulators. In the device, the two infinite phase shifters are connected in series, and the first infinite phase shifter (1
) to the first and second amplitude modulators (12, 13), and control voltages V1 and V2 to the first and second amplitude modulators (12, 13) of the second infinite phase shifter (2).
and a series-connected infinite phase shifter, characterized in that control voltages V2 and -V1 are applied to the second amplitude modulator (22, 23).
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4583186A JPS62203410A (en) | 1986-03-03 | 1986-03-03 | Series connection type infinite phase shifter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4583186A JPS62203410A (en) | 1986-03-03 | 1986-03-03 | Series connection type infinite phase shifter |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62203410A true JPS62203410A (en) | 1987-09-08 |
Family
ID=12730173
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4583186A Pending JPS62203410A (en) | 1986-03-03 | 1986-03-03 | Series connection type infinite phase shifter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62203410A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2019522406A (en) * | 2016-10-18 | 2019-08-08 | 三菱電機株式会社 | Broadband power amplifier and method for designing a broadband power amplifier network |
-
1986
- 1986-03-03 JP JP4583186A patent/JPS62203410A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2019522406A (en) * | 2016-10-18 | 2019-08-08 | 三菱電機株式会社 | Broadband power amplifier and method for designing a broadband power amplifier network |
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