JPH053922B2 - - Google Patents
Info
- Publication number
- JPH053922B2 JPH053922B2 JP19998684A JP19998684A JPH053922B2 JP H053922 B2 JPH053922 B2 JP H053922B2 JP 19998684 A JP19998684 A JP 19998684A JP 19998684 A JP19998684 A JP 19998684A JP H053922 B2 JPH053922 B2 JP H053922B2
- Authority
- JP
- Japan
- Prior art keywords
- notch filter
- terminal
- coupling
- circuit
- mode
- 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 - Lifetime
Links
- 230000008878 coupling Effects 0.000 claims description 36
- 238000010168 coupling process Methods 0.000 claims description 36
- 238000005859 coupling reaction Methods 0.000 claims description 36
- 239000000523 sample Substances 0.000 claims description 15
- 230000037431 insertion Effects 0.000 claims description 8
- 238000003780 insertion Methods 0.000 claims description 8
- 230000001939 inductive effect Effects 0.000 claims description 7
- 230000005540 biological transmission Effects 0.000 description 17
- 238000010586 diagram Methods 0.000 description 16
- 238000002955 isolation Methods 0.000 description 13
- 230000005236 sound signal Effects 0.000 description 7
- 230000000694 effects Effects 0.000 description 6
- 238000004519 manufacturing process Methods 0.000 description 5
- 230000004323 axial length Effects 0.000 description 4
- 239000004020 conductor Substances 0.000 description 4
- 230000005684 electric field Effects 0.000 description 4
- 239000011159 matrix material Substances 0.000 description 3
- 230000035559 beat frequency Effects 0.000 description 1
- 230000008901 benefit Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 230000009977 dual effect Effects 0.000 description 1
- 238000003786 synthesis reaction Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/20—Frequency-selective devices, e.g. filters
- H01P1/207—Hollow waveguide filters
- H01P1/208—Cascaded cavities; Cascaded resonators inside a hollow waveguide structure
- H01P1/2082—Cascaded cavities; Cascaded resonators inside a hollow waveguide structure with multimode resonators
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、例えばテレビジヨン放送装置におい
て映像信号搬送波と音声信号搬送波とを合成する
ために用いられる定インピーダンスダイプレクサ
(以下、CINダイプレクサと略記する。)等の構成
部品として好適なノツチフイルタに関するもので
ある。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a constant impedance diplexer (hereinafter abbreviated as CIN diplexer) used for combining a video signal carrier wave and an audio signal carrier wave in, for example, a television broadcasting device. The present invention relates to a notch filter that is suitable as a component such as the above.
従来の技術
第15図は、テレビジヨン放送装置において映
像信号搬送波と音声信号搬送波とを合成するため
に、従来用いられているCINダイプレクサの一例
を示す図で、121及び122はハイブリツド回
路、161及び162はカラービート周波数、即
ち、fV−3.58(MHz)(fVは映像信号搬送波の周波
数)に共振する共振器、171及び172は音声信
号搬送波fA(MHz)に共振する共振器で、ハイブ
リツド回路121の入力端子1211に映像信号搬
送波fVと映像信号送信機において発生したfV−
3.58のカラービートが加えられると、アイソレー
シヨン端子1212に接続された無反射終端器14
にカラービートfV−3.58が吸収される。ハイブリ
ツド回路122の入力端子1221に音声信号搬送
波fAが加えられると、アイソレーシヨン端子12
22から映像信号搬送波fVと音声信号搬送波fAが送
出される。そして第15図に示したCINダイプレ
クサにおける共振器161,162,171及び1
72としては、例えば第16図に断面概略を示す
ような半同軸空胴共振器又は第17図に断面概略
を示すような矩形導波管空胴共振器が用いられて
いるため、4個の空胴共振器を必要とし、共振器
間の接続器の数も比較的多数となり、その結果、
全体の構成が複雑大形で、コスト高となる欠点が
ある。BACKGROUND ART FIG. 15 is a diagram showing an example of a CIN diplexer conventionally used to synthesize a video signal carrier wave and an audio signal carrier wave in a television broadcasting device, and 12 1 and 12 2 are hybrid circuits; 16 1 and 16 2 are resonators that resonate at the color beat frequency, that is, f V −3.58 (MHz) (f V is the frequency of the video signal carrier wave), and 17 1 and 17 2 are resonators that resonate at the audio signal carrier wave f A (MHz). The resonator resonates, and the video signal carrier f V and the video signal carrier f V − generated in the video signal transmitter are connected to the input terminal 12 11 of the hybrid circuit 12 1 .
When a color beat of 3.58 is added, the non-reflection terminator 14 connected to the isolation terminal 12 12
The color beat f V −3.58 is absorbed. When the audio signal carrier f A is applied to the input terminal 12 21 of the hybrid circuit 12 2 , the isolation terminal 12
22 , a video signal carrier wave fV and an audio signal carrier wave fA are sent out. And resonators 16 1 , 16 2 , 17 1 and 1 in the CIN diplexer shown in FIG.
For example, a semi-coaxial cavity resonator whose cross section is shown in FIG. 16 or a rectangular waveguide cavity resonator whose cross section is shown in FIG. cavity resonators are required, and the number of connectors between the resonators is also relatively large, resulting in
The disadvantage is that the overall structure is complicated and large, and the cost is high.
本発明者は、CINダイプレクサの構成部品とし
て好適で、第15図に示したCINダイプレクサの
欠点を除き得るデユアルモード円形導波管空胴共
振器より成るノツチフイルタをさきに提案した
(特願昭53−019121)。第18図は、その構成を示
す断面図、第19図は、第18図のA−A断面図
で、両図において、18は円形導波管空胴共振
器、19は短絡壁に穿つた結合孔、20は結合線
路、21は主線路で、結合線路20と共にT分岐
回路を形成する。22及び23は同軸端子で、各
内部導体を主線路21の端部に接続してある。第
20図は、上記ノツチフイルタを用いて成るCIN
ダイプレクサを示す図で、241及び242は第1
8図及び第19図に示したノツチフイルタで、ノ
ツチフイルタ241の同軸端子22をハイブリツ
ド回路121の結合端子1213に、同軸端子23
をハイブリツド回路122の結合端子1223にそ
れぞれ接続し、ノツチフイルタ242の同軸端子
22及び23をハイブリツド回路121の結合端
子1214及びハイブリツド回路122の結合端子
1224にそれぞれ接続してある。 The present inventor previously proposed a notch filter consisting of a dual-mode circular waveguide cavity resonator that is suitable as a component of a CIN diplexer and can eliminate the drawbacks of the CIN diplexer shown in FIG. −019121). Fig. 18 is a cross-sectional view showing its configuration, and Fig. 19 is a cross-sectional view taken along line A-A in Fig. 18. In both figures, 18 is a circular waveguide cavity resonator, and 19 is a hole in the short-circuit wall. A coupling hole, 20 a coupling line, and 21 a main line, which together with the coupling line 20 form a T-branch circuit. Coaxial terminals 22 and 23 connect each internal conductor to the end of the main line 21. Figure 20 shows a CIN using the above notch filter.
In the diagram showing the diplexer, 24 1 and 24 2 are the first
8 and 19, the coaxial terminal 22 of the notch filter 24 1 is connected to the coupling terminal 12 13 of the hybrid circuit 12 1, and the coaxial terminal 23 of the notch filter 24 1 is connected to the coupling terminal 12 13 of the hybrid circuit 12 1.
are connected to the coupling terminals 12 23 of the hybrid circuit 12 2 , respectively, and the coaxial terminals 22 and 23 of the notch filter 24 2 are respectively connected to the coupling terminal 12 14 of the hybrid circuit 12 1 and the coupling terminal 12 24 of the hybrid circuit 12 2 . .
ハイブリツド回路121の入力端子1211にfV波
及びfV−3.58波を加えると、ノツチフイルタ241
及び242の各結合線路20及び結合孔19間の
磁気結合によつて、結合線路20と45°の角度差
を有しfV波に対応する電界E〓Vと、結合線路20と
45°の角度差を有すると共に電界E〓Vと直交しfV−
3.58波に対応する電界E〓V-3.58とが空胴共振器内に
共存して共振し、fV−3.58波はノツチフイルタ2
41及び242で反射されてアイソレーシヨン端子
1212に接続された無反射終端器14に吸収さ
れ、fV波はハイブリツド回路122のアイソレー
シヨン端子1222に現出する。又、ハイブリツド
回路122の入力端子1221に加えられたfA波はノ
ツチフイルタ241及び242で反射されてアイソ
レーシヨン端子1222に現出し、fV波と合成され
る。 When f V waves and f V -3.58 waves are applied to the input terminal 12 11 of the hybrid circuit 12 1 , the notch filter 24 1
Due to the magnetic coupling between each coupled line 20 and the coupling hole 19 of 24 and 2 , an electric field E 〓
It has an angular difference of 45° and is perpendicular to the electric field E〓 V , f V −
The electric field E = V-3.58 corresponding to the 3.58 wave coexists and resonates in the cavity resonator, and the f V -3.58 wave is generated by the notch filter 2.
4 1 and 24 2 and absorbed by the non-reflection terminator 14 connected to the isolation terminal 12 12 , the fV wave appears at the isolation terminal 12 22 of the hybrid circuit 12 2 . Further, the f A wave applied to the input terminal 12 21 of the hybrid circuit 12 2 is reflected by the notch filters 24 1 and 24 2 and appears at the isolation terminal 12 22 , where it is combined with the f V wave.
このCINダイプレクサにおいては、空胴共振器
の数が2個で足りるから、それだけ全体の構成を
簡潔小形ならしめ得ると共に、空胴共振器に共存
共振する互に周波数の異なる2波の各々における
負荷Qが互に等しいという利点を有するが、空胴
共振器における結合部分の構成が複雑で、結合孔
及び結合線路等のように調整を要する個所が比較
的多いため、ノツチフイルタの製作が比較的困難
で、コスト高となる欠点を免れることが出来な
い。 In this CIN diplexer, since only two cavity resonators are required, the overall structure can be made simpler and smaller, and the load on each of the two waves of different frequencies that co-resonate in the cavity resonator. Although it has the advantage that Q is equal to each other, the structure of the coupling part in the cavity resonator is complicated, and there are relatively many parts that require adjustment such as coupling holes and coupling lines, so it is relatively difficult to manufacture a notch filter. However, it cannot avoid the disadvantage of high cost.
本発明が解決しようとする問題点
本発明は、上記従来の欠点、即ち、ダイプレク
サ等を構成する場合、一般に比較的多数のノツチ
フイルタを必要とし、比較的少数で足りるように
構成したノツチフイルタにおいても、構成が複雑
で製作が困難なために、コスト高となる欠点を除
き、構成及び製作調整が簡潔容易で、コストを低
廉ならしめ、ダイプレクサ等の構成部品として好
適なノツチフイルタを実現することを目的とす
る。Problems to be Solved by the Present Invention The present invention solves the above-mentioned drawbacks of the conventional art, that is, when constructing a diplexer etc., generally a relatively large number of notch filters are required, and even in a notch filter constructed so that a relatively small number is sufficient. The purpose of this invention is to eliminate the drawbacks of high cost due to the complicated structure and difficulty in manufacturing, and to realize a notch filter that is simple and easy to adjust in structure and manufacturing, reduces costs, and is suitable as a component of a diplexer, etc. do.
問題点を解決するための手段(実施例 1)
第1図は、本発明の一実施例を示す断面図、第
2図は、第1図のA−A断面図、第3図は、第1
図のB−B断面図で、各図において、1は円形導
波管空胴共振器の円筒状側壁で、その軸長、即
ち、共振長を管内波長λgのほぼ1/2に形成してあ
る。2は短絡壁、3は結合プローブで、円筒状側
壁1から管内に挿入された棒状導体より成り、そ
の管内挿入方向を円筒状側壁1の半径方向にほぼ
一致せしめてある。4は同軸端子、5はHモード
の共振周波数微調整素子で、円筒状側壁1から管
内に挿入した棒状導体より成り、その管内挿入長
を微細に変化せしめ得ると共に、その管内挿入方
向が、結合プローブ3と45°及び135°(又はほぼ45°
及びほぼ135°)の角度差を有するように形成して
ある。6はVモードの共振周波数微調整素子で、
その管内挿入方向が素子5と直角(又はほぼ直
角)をなすように形成する他は素子5と同様の構
成である。7はモード結合微調整素子で、その管
内挿入方向が素子5及び6とそれぞれ45°(又はほ
ぼ45°)の角度差をもつように形成する他は、素
子5及び6と同様の構成である。尚、円筒状側壁
1の軸長のほぼ1/2の個所に素子5ないし7を設
けた場合に、調整効果を最も大ならしめ得るが、
上記個所から軸方向に適宜離れた個所に設けるよ
うにしてもよい。又、図には素子5を中心軸に対
称の側壁個所に2本設けた場合を例示したが、何
れか一方を省いてもよく、素子6も同様に何れか
一方を省いても差支えない。更に、素子7も図示
のように4本を設ける代りに、4本の素子の中、
管内挿入方向が互に直交し、素子5及び6と45°
又は135°の角度差を有する2本の素子を以てモー
ド結合微調整素子を形成してもよい。Means for Solving the Problems (Embodiment 1) FIG. 1 is a sectional view showing one embodiment of the present invention, FIG. 2 is a sectional view taken along line A-A in FIG. 1, and FIG. 1
In each figure, 1 is a cylindrical side wall of a circular waveguide cavity, whose axial length, that is, the resonance length, is approximately 1/2 of the tube wavelength λg. be. 2 is a short circuit wall, and 3 is a coupling probe, which is made of a rod-shaped conductor inserted into the tube from the cylindrical side wall 1, and its insertion direction into the tube is made to substantially coincide with the radial direction of the cylindrical side wall 1. 4 is a coaxial terminal, and 5 is an H-mode resonant frequency fine adjustment element, which is made of a rod-shaped conductor inserted into the tube from the cylindrical side wall 1, and can minutely change the insertion length into the tube, and whose insertion direction into the tube can be adjusted depending on the connection. Probe 3 and 45° and 135° (or almost 45°
and approximately 135°). 6 is a V mode resonant frequency fine adjustment element;
It has the same configuration as element 5 except that its insertion direction into the tube is formed at right angles (or approximately at right angles) to element 5. Reference numeral 7 denotes a mode coupling fine adjustment element, which has the same configuration as elements 5 and 6, except that its insertion direction into the tube has an angular difference of 45° (or approximately 45°) from that of elements 5 and 6, respectively. . Note that the adjustment effect can be maximized when the elements 5 to 7 are provided at approximately 1/2 of the axial length of the cylindrical side wall 1;
It may be provided at a location appropriately separated from the above location in the axial direction. Further, although the figure shows an example in which two elements 5 are provided at side wall locations symmetrical about the central axis, one of them may be omitted, and one of the elements 6 may be similarly omitted. Furthermore, instead of providing four elements 7 as shown in the figure, among the four elements,
The directions of insertion into the pipe are perpendicular to each other and 45° with elements 5 and 6.
Alternatively, a mode coupling fine adjustment element may be formed using two elements having an angular difference of 135°.
作用及び効果
同軸端子4及び結合プローブ3を介して互に周
波数の異なる2波により円形導波管空胴共振器を
励振すると、第2図に示すように、電界E〓H及び
E〓Vが互に直交するHモードとVモードが同時に
共振すること第18図及び第19図に示したノツ
チフイルタと同様であるが、本発明ノツチフイル
タは第1図ないし第3図から明らかなように、結
合部分が単なる棒状導体より成り、第18図及び
第19図に示したノツチフイルタにおける結合部
分に比し遥かに構造が簡潔で製作が容易であるか
ら、コストを低廉ならしめ得ると共に次のような
特長を有する。Functions and Effects When a circular waveguide cavity is excited by two waves with different frequencies through the coaxial terminal 4 and the coupling probe 3, the electric field E〓 H and
The fact that the H mode and V mode, in which E = V are orthogonal to each other, resonates at the same time.This is similar to the notch filter shown in FIGS. 18 and 19, but as is clear from FIGS. In addition, the connecting portion is made of a simple rod-shaped conductor, and has a much simpler structure and is easier to manufacture than the connecting portion in the notch filter shown in FIGS. It has the following characteristics.
一般に円形導波管空胴共振器の直径をDとする
と、H11モードの遮断波長λcは、
λc=1.706D …(1)
管内波長λgは、自由空間波長をλとすると、
λ(mm)=300/f(GHz)
又、円形導波管空胴共振器の共振長は管内波
長のほぼ1/2で、負荷Q(QL)に応じて管内波長
の1/2以下に変化する。 In general, if the diameter of a circular waveguide cavity is D, the cutoff wavelength λ c of the H 11 mode is λ c = 1.706D...(1) The internal wavelength λ g is, if the free space wavelength is λ, λ (mm) = 300/f (GHz) In addition, the resonance length of a circular waveguide cavity is approximately 1/2 of the wavelength in the tube, and depending on the load Q (Q L ), it is less than 1/2 of the wavelength in the tube. Changes to
本発明ノツチフイルタにおける結合プローブ3
を、何れか一方の短絡壁2から中心軸方向にλg/4
=cだけ離れた個所に設けると共に、共振周波
数微調整素子5及び6の何れか一方、例えば6を
省き、更に、モード結合微調整素子7を省き、素
子5と結合プローブ3との角度差θHを0°又は180°
となした場合、即ち、従来の円形導波管空胴共振
器と同様構成となした場合の負荷QをQLOとする
と、プローブ3の直径がDP、その管内挿入長が
Pの場合、QLOはDP -4に比例して高くなると共
に、P -2に比例して高くなる。θHを前述のよう
に0°又は180°に保ち、cを変化せしめた場合の負
荷QをQL cとすると、
QL c=QLO/sin2 cπ/ …(3)
素子5及び7を省き、素子6と結合プローブ3
との角度差θVを0°又は180°となした場合も同様で
ある。 Binding probe 3 in the Notti filter of the present invention
is provided at a location separated by λg/4 = c from one of the shorting walls 2 in the central axis direction, one of the resonant frequency fine adjustment elements 5 and 6, for example 6, is omitted, and furthermore, a mode coupling fine adjustment element is provided. Adjustment element 7 is omitted, and the angular difference θ H between element 5 and coupling probe 3 is set to 0° or 180°.
In other words, when the configuration is the same as that of a conventional circular waveguide cavity resonator, and the load Q is Q LO , the diameter of the probe 3 is D P and its insertion length in the pipe is
For P , Q LO increases proportionally to D P -4 and increases proportionally to P -2 . If θ H is kept at 0° or 180° as described above and the load Q is Q L c when c is changed, then Q L c = Q LO /sin 2 c π/ …(3) Element 5 and 7 is omitted, element 6 and coupling probe 3
The same holds true when the angular difference θ V is 0° or 180°.
本発明ノツチフイルタにおいては、結合プロー
ブ3と短絡壁2との距離cをほぼλg/4に保ち、素
子5とプローブ3の角度差θH及び素子6とプロー
ブ3の角度差θVの和、θH+θVを90°に保持しなが
らθHとθVの大きさを変化せしめた場合、Hモード
における負荷QをQL〓H、Vモードにおける負荷Q
をQL〓Vとすると、各負荷Qは次式から求めること
が出来る。 In the notch filter of the present invention, the distance c between the coupling probe 3 and the shorting wall 2 is maintained at approximately λ g /4, and the sum of the angular difference θ H between the element 5 and the probe 3 and the angular difference θ V between the element 6 and the probe 3, If the magnitudes of θ H and θ V are changed while holding θ H + θ V at 90°, the load Q in H mode becomes Q L 〓 H , and the load Q in V mode
When Q L 〓 V , each load Q can be obtained from the following formula.
QL〓H=QLO/sin2θH …(4)
QL〓V=QLO/sin2θV …(5)
cを任意に変化せしめると共に、θHとθVの和
を90°に保ちながらθHとθVの大きさを変化せしめ
た場合のHモードにおける負荷QをQL c〓H、V
モードにおける負荷QをQL c〓Vとすると、各負
荷Qは次式で与えられる。 Q L 〓 H = Q LO /sin 2 θ H …(4) Q L 〓 V = Q LO /sin 2 θ V …(5) While c is arbitrarily changed, the sum of θ H and θ V is set to 90°. The load Q in H mode when changing the magnitudes of θ H and θ V while maintaining
If the load Q in the mode is Q L c 〓 V , each load Q is given by the following equation.
QL cθV=QLO/sin2 c/π・sin2θH…(6)
QL cθV=QLO/sin2 c/π・sin2θV…(7)
本発明ノツチフイルタは第4図に等価回路を示
すように、Hモード及びVモードに対してそれぞ
れ独立の共振回路として動作し、Hモードに対す
るアドミツタンスY〓H及びVモードに対するアド
ミツタンスY〓Vは、(8)式及び(9)式から求めること
が出来る。 Q L c θ V = Q LO /sin 2 c /π・sin 2 θ H …(6) Q L c θ V = Q LO /sin 2 c /π・sin 2 θ V …(7) The notch filter of the present invention is As shown in the equivalent circuit in Fig. 4, it operates as an independent resonant circuit for H mode and V mode, and the admittance Y for H mode = the admittance Y for H and V modes = V is calculated by equation (8) and It can be obtained from equation (9).
Y〓H=〔QL cθH(f/fOH−fOH/f)〕-1 …(8)
Y〓V=〔QL cθV(f/fOV−fOV/f)〕-1 …(9)
但し、
f:任意の周波数
fOH:Hモードにおける共振周波数
fOV:Vモードにおける共振周波数
第4図に示した等価回路の基本マトリツクス
[F〓HV]は、
[F〓HV]=1
Y〓H 0
11
Y〓V 0
1=1
Y〓H+Y〓V 0
1=A〓 B〓
C〓 D〓 …(10)
(8)式、(9)式及び(10)式から伝送特性LHVは、
LHV=10og|A〓+B〓+C〓+D〓|2/4=10og|
1+0+(Y〓H+Y〓V)+1|2/4
=10og|1+Y〓H+Y〓V/2|2=20og|1
+Y〓H+Y〓V/2|…(11)
本発明者が試作品について求めた実測値は(11)
式から得られる理論値と極めて良く一致し、その
伝送特性曲線は、第5図(横軸は周波数fMHz、
縦軸は減衰量ATTdB)に示す通りである。 Y〓 H = [Q L c θ H (f/f OH −f OH /f)] -1 …(8) Y〓 V = [Q L c θ V (f/f OV −f OV /f)] -1 ...(9) However, f: arbitrary frequency f OH : resonant frequency in H mode f OV : resonant frequency in V mode The basic matrix [F〓 HV ] of the equivalent circuit shown in Figure 4 is [F〓 HV ]=1 Y〓 H 0 11 Y〓 V 0 1=1 Y〓 H +Y〓 V 0 1=A〓 B〓 C〓 D〓 …(10) Equation (8), Equation (9) and (10) From the formula, the transmission characteristic L HV is: L HV = 10og | A〓 + B〓 + C〓 + D〓 | 2 / 4 = 10og |
1+0+( Y〓H + Y〓V )+1| 2 /4=10og|1+ Y〓H + Y〓V /2| 2 =20og|1
+Y〓 H +Y〓 V /2|…(11) The actual measured value obtained by the inventor for the prototype is (11)
It agrees extremely well with the theoretical value obtained from the formula, and its transmission characteristic curve is shown in Figure 5 (the horizontal axis is the frequency fMHz,
The vertical axis is as shown in the attenuation amount (ATTdB).
問題点を解決するための手段(実施例 2)
第6図は、本発明の他の実施例を示す図で、8
は第1図ないし第3図に示した本発明ノツチフイ
ルタ、9は誘導性の補償回路で、例えばλg/4以下
の軸長を有する短絡形同軸スタブより成り、同軸
線路より成る十字形分岐回路10を介して同軸端
子4に接続してある。Means for Solving Problems (Embodiment 2) FIG. 6 is a diagram showing another embodiment of the present invention.
1 is a notch filter of the present invention shown in FIGS. 1 to 3; 9 is an inductive compensation circuit consisting of a short-circuited coaxial stub having an axial length of λg/4 or less; and a cruciform branch circuit 10 consisting of a coaxial line. It is connected to the coaxial terminal 4 via.
作用及び効果
第7図は、その等価回路図で、Y〓Lは補償回路
9のアドミツタンスである。この等価回路の基本
マトリツクス[F〓HVL]は、
[F〓HVL]=1
Y〓H+Y〓V+Y〓L 0
1 …(12)
伝送特性は、
LHVL=20og|1+Y〓H+Y〓V+Y〓L/2| …(13)
となり、伝送特性曲線は第8図(横軸及び縦軸
は、第5図と同じ。)に示す通りで、同図から明
らかなように、誘導性の補償回路を付加すること
により、NTSCテレビジヨン方式のように映像信
号搬送波fVと音声信号搬送波fAの間にfV<fAなる
関係のある場合に好適なノツチフイルタを形成す
ることが出来る。即ち、ほぼfV−3.58MHzないし
ほぼfV+4.18MHz(カラー副搬送波fS=fV+3.58M
Hzを含む。)の伝送特性及びグループ遅延時間特
性の良好なノツチフイルタを形成せしめ得る。Actions and Effects FIG. 7 is its equivalent circuit diagram, where Y L is the admittance of the compensation circuit 9. The basic matrix [F〓 HVL ] of this equivalent circuit is [F〓 HVL ]=1 Y〓 H +Y〓 V +Y〓 L 0 1 …(12) The transmission characteristic is L HVL = 20og|1+Y〓 H +Y〓 V +Y〓 L /2 | ...(13), and the transmission characteristic curve is as shown in Figure 8 (the horizontal and vertical axes are the same as Figure 5), and as is clear from the figure, the inductive By adding a compensation circuit, it is possible to form a notch filter suitable for cases where there is a relationship of f V <f A between the video signal carrier f V and the audio signal carrier f A , such as in the NTSC television system. That is, approximately f V -3.58MHz to approximately f V +4.18MHz (color subcarrier f S = f V +3.58M
Including Hz. ) can form a notch filter with good transmission characteristics and group delay time characteristics.
問題点を解決するための手段(実施例 3)
第9図もまた本発明の他の実施例を示す図で、
11は容量性の補償回路で、例えば軸長がλg/4以
下の開放形同軸スタブより成る。他の符号は第6
図と同様である。Means for solving the problem (Embodiment 3) FIG. 9 is also a diagram showing another embodiment of the present invention,
Reference numeral 11 denotes a capacitive compensation circuit, which is composed of, for example, an open coaxial stub with an axial length of λg/4 or less. Other codes are 6th
It is similar to the figure.
作用及び効果
第10図は、その等価回路で、Y〓Cは容量性補
償回路のアドミツタンスである。この等価回路の
基本マトリツクス[F〓HVC]は、
[F〓HVC]=1
Y〓H+Y〓V+Y〓C 0
1 …(14)
となり、伝送特性は、
LHVC=20og|1+Y〓H+Y〓V+Y〓C/2| …(15)
となる。Actions and Effects Figure 10 shows its equivalent circuit, where Y〓 C is the admittance of the capacitive compensation circuit. The basic matrix [F〓 HVC ] of this equivalent circuit is [F〓 HVC ]=1 Y〓 H +Y〓 V +Y〓 C 0 1...(14), and the transmission characteristic is L HVC = 20og|1+Y〓 H +Y 〓 V + Y〓 C /2 | …(15)
第11図(横軸及び縦軸は第5図と同じ。)は、
第9図に示した本発明ノツチフイルタの伝送特性
を示す曲線図で、同図から明らかなように容量性
補償回路を付加することによりfV>fAなる周波数
関係を有するテレビジヨン方式等に好適なノツチ
フイルタを形成することが出来る。 Figure 11 (horizontal and vertical axes are the same as Figure 5):
FIG. 9 is a curve diagram showing the transmission characteristics of the notch filter of the present invention. As is clear from the diagram, by adding a capacitive compensation circuit, it is suitable for television systems etc. which have a frequency relationship of f V > f A. A notch filter can be formed.
第12図は、誘導性又は容量性補償回路を付加
した本発明ノツチフイルタの伝送特性と周波数f
における電圧反射係数Γ〓(f)との関係を説明す
る図で、ノツチフイルタ8の入力電力(周波数
f)をPIN(f)、出力電力をPOUT(f)、周波数f
における共振回路及び補償回路のアドミツタンス
をY〓H(f)、Y〓V(f)、Y〓L(f)及びY〓C(f)
とする
と、補償回路が誘導性の場合には
PIN(f)/POUT(f)=1/1−|Γ22(f)
|=|1+Y〓H(f)+Y〓V(f)+Y〓L(f)/2|
2
したがつて、
1/|1+YH(f)+YV(f)+YL(f)/2|
2=1−|Γ〓2(f)|
|Γ〓2(f)|=1−1/|1+YH(f)+YV
(f)+YL(f)/2|2
|Γ〓(f)|=〔1−1/|1+YH(f)+Yv
(f)+YL(f)/2|2〕1/2…(16)
周波数fにおける反射減衰量Lr(f)は、
Lr(f)=1/|Γ2(f)|=1/〔1−1/|
1+YH(f)+YV(f)+YL(f)/2|2〕…(17)
補償回路が容量性の場合は、
|Γ〓(f)|=〔1−1/|1+YH(f)+YV(
f)+YC(f)/2|2〕1/2…(18)
Lγ(f)=1/〔1−1/|1+YH(f)+YV(
f)+YC(f)/2|2〕…(19)
本発明ノツチフイルタをハイブリツド回路又は
サーキユレータ等と組合せることによつてダイプ
レクサを構成し得るが、第13図は、本発明ノツ
チフイルタをハイブリツド回路と組合せて構成し
たCINダイプレクサを示す図で、81及び82は第
1図ないし第3図について説明した本発明ノツチ
フイルタ、121及び122はハイブリツド回路、
1211及び1221は入力端子、1212及び1222
はアイソレーシヨン端子、1213,1214,12
23及び1224は結合端子、131及び132はT分
岐回路で、例えば同軸線路より成り、各分岐端子
をハイブリツド回路121及び122の結合端子1
213,1223及び1214,1224並にノツチフイ
ルタ81及び82の同軸端子41及び42(第1図及
び第3図の4)に接続してある。14は無反射終
端器である。 Figure 12 shows the transmission characteristics and frequency f of the notch filter of the present invention to which an inductive or capacitive compensation circuit is added.
This is a diagram explaining the relationship between the voltage reflection coefficient Γ〓(f) and the input power (frequency f) of the notch filter 8 as P IN (f), the output power as P OUT (f), and the frequency f as
The admittance of the resonant circuit and the compensation circuit at Y〓 H (f), Y〓 V (f), Y〓 L (f) and Y〓 C (f)
Then, if the compensation circuit is inductive, P IN (f)/P OUT (f) = 1/1 - |Γ 2 2 (f)
|=|1+Y〓 H (f)+Y〓 V (f)+Y〓 L (f)/2|
2 Therefore, 1/|1+Y H (f)+Y V (f)+Y L (f)/2|
2 =1-|Γ〓 2 (f)||Γ〓 2 (f)|=1-1/|1+Y H (f)+Y V
(f)+Y L (f)/2| 2 |Γ〓(f)|=[1-1/|1+Y H (f)+Y v
(f)+Y L (f)/2 | 2 ] 1/2 …(16) The return loss L r (f) at frequency f is L r (f)=1/|Γ 2 (f) |=1 /[1-1/|
1+Y H (f)+Y V (f)+Y L (f)/2 | 2 ]...(17) If the compensation circuit is capacitive, |Γ〓(f)|=[1-1/|1+Y H ( f)+Y V (
f)+Y C (f)/2 | 2 ] 1/2 …(18) Lγ(f)=1/[1-1/|1+Y H (f)+Y V (
f)+Y C (f)/2 | 2 ]...(19) A diplexer can be constructed by combining the notch filter of the present invention with a hybrid circuit or a circulator, and FIG. 13 shows the notch filter of the present invention in a hybrid circuit. 8 1 and 8 2 are the notch filters of the present invention explained with reference to FIGS. 1 to 3, and 12 1 and 12 2 are hybrid circuits.
12 11 and 12 21 are input terminals, 12 12 and 12 22
are isolation terminals, 12 13 , 12 14 , 12
23 and 12 24 are coupling terminals, 13 1 and 13 2 are T branch circuits, for example, made of coaxial lines, and each branch terminal is connected to the coupling terminal 1 of the hybrid circuits 12 1 and 12 2 .
2 13 , 12 23 and 12 14 , 12 24 as well as coaxial terminals 4 1 and 4 2 (4 in FIGS. 1 and 3) of notch filters 8 1 and 8 2 . 14 is a non-reflection terminator.
ハイブリツド回路121の結合係数をC、結合
線路の電気角をθ、特性インピーダンスをZO、結
合端子1213及び1214に接続される負荷インピ
ーダンスをZLとし、ZL=ZO=1とした場合、入力
端子1211に入力電圧E〓INを加えると、結合端子
1213,1214及びアイソレーシヨン端子1212
の各出力電圧E〓13,E〓14及びE〓12は、
E〓12≒0 …(22)
結合端子1213及び1214に電圧反射係数Γ〓な
る負荷を接結した場合における端子1213,12
14及び1212の各出力電圧E〓′13,E〓′14及びE〓′1
2は
入力端子1211への反射電圧E〓11〓及び入力端子
1211における電圧反射係数SINは、
SIN=|EIN|+|E11〓|/|EIN|−|E11〓|…(27
)
で表わされる。 The coupling coefficient of the hybrid circuit 12 1 is C, the electrical angle of the coupled line is θ, the characteristic impedance is Z O , the load impedance connected to the coupling terminals 12 13 and 12 14 is Z L , and Z L = Z O = 1. In this case, when the input voltage E〓 IN is applied to the input terminal 12 11 , the coupling terminals 12 13 , 12 14 and the isolation terminal 12 12
The respective output voltages E〓 13 , E〓 14 and E〓 12 are E〓 12 ≒0 …(22) Terminals 12 13 and 12 when a load with voltage reflection coefficient Γ is connected to coupling terminals 12 13 and 12 14
14 and 12 12 each output voltage E〓′ 13 , E〓′ 14 and E〓′ 1
2 is The reflected voltage E〓 11 〓 to the input terminal 12 11 and the voltage reflection coefficient S IN at the input terminal 12 11 are: S IN = | E IN | + | E 11 〓 | / | E IN | − | E 11 〓 |…(27
).
第14図は、第7図に示した本発明ノツチフイ
ルタをハイブリツド回路と組合せて構成したダイ
プレクサを示す図で、8′1及び8′2は第7図に示
した本発明ノツチフイルタ、151及び152は十
字形分岐回路で、他の符号は第13図と同じであ
る。 14 is a diagram showing a diplexer constructed by combining the notch filter of the present invention shown in FIG. 7 with a hybrid circuit, where 8' 1 and 8' 2 are the notch filters of the present invention shown in FIG. 7, 15 1 and 15 2 is a cross-shaped branch circuit, and the other symbols are the same as in FIG.
ハイブリツド回路121における入力端子12
11の周波数fなる入力電圧及び電力をE〓11N(f)
及びP11Nf)、ハイブリツド回路122における入
力端子1221の入力電圧及び入力電力をE〓21N(f)
及びP21N(f)、ハイブリツド回路122における
アイソレーシヨン端子1222の出力電圧及び出力
電力をE〓1OUT(f)、E〓2OUT(f)及びP1OUT(f)
、
P2OUT(f)とすると、ハイブリツド回路121の
入力端子1211とハイブリツド回路122のアイ
ソレーシヨン端子1222との間の電圧伝送特性及
び電力伝送特性は、
P11N(f)/P1OUT(f)=20ogE11N(f)/E1OUT
(f) (dB)
…(29)
ハイブリツド回路122の入力端子1221とハ
イブリツド回路121のアイソレーシヨン端子1
212との間の電圧伝送特性及び電力伝送特性は、
P2IN(f)/P2OUT(f)=20ogE2IN(f)/E2OUT
(f) (dB)
…(31)
(28)式及び(30)式において、
θ:周波数fにおけるハイブリツド回路の結合線
路の電気角
ハイブリツド回路121及び122における入力
端子1211,1221、アイソレーシヨン端子12
12,1222の各反射電圧をE〓〓(f)、各端子の入力
電圧をE〓K(f)とすると、各端子における反射電
圧比は次式で求めることが出来る。 Input terminal 12 in hybrid circuit 12 1
The input voltage and power with frequency f of 11 is E〓 11N (f)
and P 11N f), the input voltage and input power of the input terminal 12 21 in the hybrid circuit 12 2 are E〓 21N (f)
and P 21N (f), the output voltage and output power of the isolation terminal 12 22 in the hybrid circuit 12 2 are E〓 1OUT (f), E〓 2OUT (f) and P 1OUT (f).
,
When P 2OUT (f), the voltage transmission characteristics and power transmission characteristics between the input terminal 12 11 of the hybrid circuit 12 1 and the isolation terminal 12 22 of the hybrid circuit 12 2 are as follows. P 11N (f)/P 1OUT (f)=20ogE 11N (f)/E 1OUT
(f) (dB) ...(29) Input terminal 12 21 of hybrid circuit 12 2 and isolation terminal 1 of hybrid circuit 12 1
The voltage transmission characteristics and power transmission characteristics between 2 and 12 are: P 2IN (f) / P 2OUT (f) = 20ogE 2IN (f) / E 2OUT
(f) (dB) ...(31) In equations (28) and (30), θ: electrical angle of the coupled line of the hybrid circuit at frequency f Input terminals 12 11 , 12 21 in the hybrid circuits 12 1 and 12 2 , Isolation terminal 12
12 and 12 22 as E〓〓(f), and the input voltage of each terminal as E〓K (f), the reflected voltage ratio at each terminal can be determined by the following formula.
上記各端子の電圧反射係数Sは、
SK=1+|E〓(f)/|EK(f)/1−|E〓(f)
|/|EK(f)|…(33)
(32)式及び(33)式において、Kは各端子1211,
1221,1212及び1222の添字に対応する11,
21,12及び22である。 The voltage reflection coefficient S of each terminal above is S K = 1 + |E〓(f)/|E K (f)/1−|E〓(f)
|/|E K (f)|...(33) In equations (32) and (33), K is each terminal 12 11 ,
11 corresponding to the subscripts of 12 21 , 12 12 and 12 22 ,
21, 12 and 22.
第9図に示したノツチフイルタ、即ち、容量性
補償回路11を付加したノツチフイルタをハイブ
リツド回路と組合せた場合には、第14図、(28)
式、(30)式及び(32)式の各Y〓L(f)をY〓C(f)に置
換えることにより、前記と同様にしてハイブリツ
ド回路の入力端子とアイソレーシヨン端子間の電
圧及び電力伝送特性、各端子における反射電圧比
及び電圧反射係数等を求めることが出来る。 When the notch filter shown in FIG. 9, that is, the notch filter to which the capacitive compensation circuit 11 is added, is combined with a hybrid circuit, as shown in FIG. 14, (28)
By replacing Y〓 L (f) in Equations, (30) and (32) with Y〓 C (f), the voltage between the input terminal and isolation terminal of the hybrid circuit can be calculated in the same way as above. It is possible to determine the power transmission characteristics, the reflected voltage ratio and voltage reflection coefficient at each terminal, etc.
本発明者は、ダイプレクサの試作品について伝
送特性を求めたが、誘導性補償回路を付加したノ
ツチフイルタを組込んだ場合は第8図の特性曲線
と、容量性補償回路を付加したノツチフイルタを
組込んだ場合は第11図の特性曲線と、それぞれ
極めて良く一致する結果を得ることが出来た。 The present inventor determined the transmission characteristics of a diplexer prototype, and found that when a notch filter with an inductive compensation circuit was incorporated, the characteristic curve shown in Fig. 8 was obtained, and when a notch filter with a capacitive compensation circuit was incorporated. In this case, we were able to obtain results that matched extremely well with the characteristic curves shown in Figure 11.
本発明の効果のまとめ
以上の説明から明らかなように、本発明ノツチ
フイルタは構成、製作調整が簡潔容易で、電気的
特性が良好なると共にデユアルモード形であるか
ら、これをハイブリツド回路又はサーキユレータ
等と組合せてダイプレクサを形成するときは、全
体の構成が簡潔小形で、コストが低廉となり、特
に誘導性又は容量性補償回路を付加したノツチフ
イルタを用いた場合には、NTSCテレビジヨン方
式における映像及び音声信号搬送波の合成等に好
適なCINダイプレクサを構成し得るもので、その
効果甚だ大である。Summary of the effects of the present invention As is clear from the above description, the notch filter of the present invention is simple and easy to configure and manufacture and adjust, has good electrical characteristics, and is a dual mode type, so it can be used in a hybrid circuit or circulator, etc. When combined to form a diplexer, the overall structure is simple and compact, and the cost is low.Especially when a notch filter with an inductive or capacitive compensation circuit is used, it is suitable for video and audio signals in the NTSC television system. It can constitute a CIN diplexer suitable for carrier wave synthesis, etc., and its effects are enormous.
第1図ないし第3図は、本発明の一実施例を示
す図、第4図は、その等価回路図、第5図は、そ
の伝送特性曲線図、第6図及び第9図は、本発明
の他の実施例を示す図、第7図及び第10図は、
その等価回路図、第8図及び第11は、その伝送
特性曲線図、第12図は、その伝送特性と電圧反
射係数の関係を説明する図、第13図及び第14
図は、本発明ノツチフイルタを用いたダイプレク
サを示す図、第15図及び第20図は、従来のダ
イプレクサを示す図、第16図ないし第19図
は、従来のノツチフイルタを示す図で、1……円
筒状側壁、2……短絡壁、3……結合プローブ、
4,41及び42……同軸端子、5及び6……共振
周波数微調整素子、7……モード結合微調整素
子、8,81,82,8′1,及び8′2……本発明ノ
ツチフイルタ、9及び11……補償回路、10,
131,132,151及び152……分岐回路、1
21及び122……ハイブリツド回路、1211及び
1221……入力端子、1212及び1222……アイ
ソレーシヨン端子、1213,1214,1223及び
1224……結合端子、14……無反射終端器、1
61,162,171及び172……従来のノツチフ
イルタ、18……円形導波管空胴共振器、19…
…結合孔、20……結合線路、21……主線路、
22及び23……同軸端子である。
1 to 3 are diagrams showing one embodiment of the present invention, FIG. 4 is an equivalent circuit diagram thereof, FIG. 5 is a transmission characteristic curve diagram thereof, and FIGS. 6 and 9 are diagrams of the present invention. Figures 7 and 10 showing other embodiments of the invention are as follows:
Its equivalent circuit diagram, FIGS. 8 and 11 are transmission characteristic curve diagrams, FIG. 12 is a diagram explaining the relationship between its transmission characteristic and voltage reflection coefficient, and FIGS.
The figure shows a diplexer using the notch filter of the present invention, FIGS. 15 and 20 show a conventional diplexer, and FIGS. 16 to 19 show conventional notch filters. Cylindrical side wall, 2... short circuit wall, 3... coupling probe,
4, 4 1 and 4 2 ... coaxial terminal, 5 and 6 ... resonant frequency fine adjustment element, 7 ... mode coupling fine adjustment element, 8, 8 1 , 8 2 , 8' 1 , and 8' 2 ... Notch filter of the present invention, 9 and 11...compensation circuit, 10,
13 1 , 13 2 , 15 1 and 15 2 ...branch circuit, 1
2 1 and 12 2 ... hybrid circuit, 12 11 and 12 21 ... input terminal, 12 12 and 12 22 ... isolation terminal, 12 13 , 12 14 , 12 23 and 12 24 ... coupling terminal, 14 ... ...Reflectionless terminator, 1
6 1 , 16 2 , 17 1 and 17 2 ... conventional notch filter, 18 ... circular waveguide cavity resonator, 19 ...
...coupling hole, 20...coupling line, 21...main line,
22 and 23 are coaxial terminals.
Claims (1)
異なるHモード並にVモードの各共振周波数を各
別に調整する素子を設け、この素子の管内挿入方
向が互に直角で、前記結合プローブとの間にそれ
ぞれ45°又は135°の角度差を有するように形成し
た円形導波管空胴共振器より成ることを特徴とす
るノツチフイルタ。 2 結合プローブの端子に分岐回路を介して誘導
性の補償回路を付加した特許請求の範囲第1項記
載のノツチフイルタ。 3 結合プローブの端子に分岐回路を介して容量
性の補償回路を付加した特許請求の範囲第1項記
載のノツチフイルタ。[Claims] 1. A coupling probe and an element for individually adjusting the resonance frequencies of H mode and V mode, which have different frequencies, are provided on the cylindrical side wall, and the insertion directions of the elements into the tube are at right angles to each other, A notch filter comprising a circular waveguide cavity resonator formed to have an angular difference of 45° or 135° with respect to the coupling probe. 2. The notch filter according to claim 1, wherein an inductive compensation circuit is added to the terminal of the coupling probe via a branch circuit. 3. The notch filter according to claim 1, wherein a capacitive compensation circuit is added to the terminal of the coupling probe via a branch circuit.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19998684A JPS6178202A (en) | 1984-09-25 | 1984-09-25 | Notch filter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19998684A JPS6178202A (en) | 1984-09-25 | 1984-09-25 | Notch filter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6178202A JPS6178202A (en) | 1986-04-21 |
| JPH053922B2 true JPH053922B2 (en) | 1993-01-18 |
Family
ID=16416884
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19998684A Granted JPS6178202A (en) | 1984-09-25 | 1984-09-25 | Notch filter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6178202A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2697372B1 (en) * | 1992-10-22 | 1994-12-09 | Alcatel Telspace | Agile microwave bandpass filter with dual-mode cavities. |
-
1984
- 1984-09-25 JP JP19998684A patent/JPS6178202A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6178202A (en) | 1986-04-21 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |