JPS6340485B2 - - Google Patents
Info
- Publication number
- JPS6340485B2 JPS6340485B2 JP3495682A JP3495682A JPS6340485B2 JP S6340485 B2 JPS6340485 B2 JP S6340485B2 JP 3495682 A JP3495682 A JP 3495682A JP 3495682 A JP3495682 A JP 3495682A JP S6340485 B2 JPS6340485 B2 JP S6340485B2
- Authority
- JP
- Japan
- Prior art keywords
- waveguide
- tube
- section
- main
- wave
- 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
Links
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
- H01P1/213—Frequency-selective devices, e.g. filters combining or separating two or more different frequencies
- H01P1/2138—Frequency-selective devices, e.g. filters combining or separating two or more different frequencies using hollow waveguide filters
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
Description
【発明の詳細な説明】
この発明は、2つの周波数帯の同じ偏波の電磁
波を各周波数帯の電磁波に分波する分波器に関す
るものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a splitter that splits electromagnetic waves of the same polarization in two frequency bands into electromagnetic waves of each frequency band.
ここでは便宜上2つの周波数帯の周波数を、そ
れぞれH,L(H>L)とし添字H,Lで周波数
帯を区別する。 Here, for convenience, the frequencies of the two frequency bands are respectively referred to as H and L ( H > L ), and the frequency bands are distinguished by subscripts H and L.
まず第1図と第2図に示す従来の分波器につい
て説明する。 First, a conventional duplexer shown in FIGS. 1 and 2 will be explained.
第1図において、1はH,Lの波が伝搬する方
形導波管2およびLの波を完全に反射し、Hの波
が通過するテーパ導波管3により構成される主導
波管、4は主導波管1の方形導波管2の広い面に
設けられた分岐導波管、5はHの周波数帯専用方
形導波管、6は方形導波管2に設けられた結合
孔、7は分岐導波管4に設けられたLの波を通過
させHの波をしや断する低域通過フイルタでこの
図では直列共振素子の場合を示している。 In Fig. 1, 1 is a main waveguide consisting of a rectangular waveguide 2 through which the H and L waves propagate, and a tapered waveguide 3 which completely reflects the L wave and through which the H wave passes; is a branch waveguide provided on a wide surface of the rectangular waveguide 2 of the main waveguide 1, 5 is a rectangular waveguide dedicated to the H frequency band, 6 is a coupling hole provided in the rectangular waveguide 2, and 7 is a low-pass filter provided in the branch waveguide 4 that passes the L wave and cuts off the H wave, and this figure shows the case of a series resonant element.
第2図は、主導波管1の方形導波管2の狭い面
に、分岐導波管4を設けた場合を示す図である。 FIG. 2 is a diagram showing a case where a branch waveguide 4 is provided on a narrow surface of the rectangular waveguide 2 of the main waveguide 1.
いま、主導波管1の方形導波管2に周波数L,
Hの波が導入された場合、Hの波は低域通過フイ
ルタ7により、分岐導波管4に結合することなく
Hの周波数帯専用方形導波管5に伝搬する。一
方、Lの波はテーパ導波管3のしや断特性により
等価的な反射面を形成しているために完全に反射
され、結合孔6の位置をテーパ導波管3で形成さ
れる反射面から適当な距離に選定することにより
結合孔6を介して分岐導波管4に分波される。 Now, the frequency L ,
When the H wave is introduced, the H wave is passed through the low pass filter 7 without being coupled to the branch waveguide 4.
The signal propagates to the rectangular waveguide 5 dedicated to the H frequency band. On the other hand, the L wave forms an equivalent reflecting surface due to the shearing characteristics of the tapered waveguide 3, so it is completely reflected, and the position of the coupling hole 6 is reflected by the reflection formed by the tapered waveguide 3. By selecting an appropriate distance from the plane, the wave is branched into the branch waveguide 4 via the coupling hole 6.
第1図に示す従来の分波器では、結合孔6は主
導波管1中の磁界の横方向成分で結合波を生じ
る。結合孔6による結合波は主導波管1の広い面
を軸方向に流れる電流を分岐することになる。従
つて結合孔6の位置をテーパ導波管3の等価反射
面から適当な距離に選定してもLの波に対して方
形導波管2と分岐導波管4との間で反射の少い伝
送が可能な周波数帯域が狭帯域になるという欠点
があつた。 In the conventional duplexer shown in FIG. 1, the coupling hole 6 produces a coupled wave with the transverse component of the magnetic field in the main waveguide 1. The coupled wave caused by the coupling hole 6 branches the current flowing in the axial direction across the wide surface of the main waveguide 1 . Therefore, even if the position of the coupling hole 6 is selected at an appropriate distance from the equivalent reflection surface of the tapered waveguide 3, there will be little reflection between the rectangular waveguide 2 and the branch waveguide 4 for the L wave. The drawback was that the frequency band in which high-speed transmission was possible was narrow.
また第2図に示す従来の分波器では結合孔6は
主導波管1中の磁界の管軸方向成分で結合波を生
じる。結合孔6による結合波は分岐点で電圧が一
定で、電流が分岐導波管4に流れることになる。
従つて結合孔6の位置をテーパ導波管3の等価反
射面から適当な距離に選定するとLの波に対して
方形導波管2と分岐導波管4の間で反射の少い伝
送が可能な周波数帯域は広くなるものである。 Further, in the conventional duplexer shown in FIG. 2, the coupling hole 6 generates a coupled wave using the component of the magnetic field in the main wave tube 1 in the direction of the tube axis. The voltage of the wave coupled by the coupling hole 6 is constant at the branch point, and current flows into the branch waveguide 4.
Therefore, if the position of the coupling hole 6 is selected at an appropriate distance from the equivalent reflection surface of the tapered waveguide 3, the L wave can be transmitted between the rectangular waveguide 2 and the branched waveguide 4 with less reflection. The possible frequency bands are becoming wider.
しかし複数個の分波器を当該分波器の主導波管
1の狭い面で互いに接するように並べて配列しな
ければならないアンテナの一次放射系としては空
間の制約から構成することができないという欠点
があつた。 However, it has the disadvantage that it cannot be constructed as a primary radiation system of an antenna, which requires multiple branching filters to be arranged side by side so that they touch each other on the narrow surface of the main wave tube 1 of the branching filter, due to space constraints. It was hot.
この発明は、これらの欠点を解決するためにな
されたもので主導波管1の方形導波管2およびテ
ーパ導波管3の管軸方向にまたがつて、狭い面の
管壁面に接近して広い面の管壁面に結合孔6を設
けることにより広帯域な分波特性を得ることがで
きるとともに、複数個の分波器を当該分波器の主
導波管1の狭い面で互いに接するように並べて配
列して構成出来る分波器を提供するものである。 The present invention has been made to solve these drawbacks, and is to straddle the rectangular waveguide 2 and the tapered waveguide 3 of the main waveguide 1 in the tube axis direction, and to approach the narrow tube wall surface. Broadband demultiplexing characteristics can be obtained by providing coupling holes 6 on a wide tube wall surface, and a plurality of demultiplexers can be connected to each other on the narrow surface of the main wave tube 1 of the duplexer. The present invention provides a duplexer that can be configured by arranging them side by side.
以下、第3図に示すこの発明の一実施例につい
て説明する。 An embodiment of the present invention shown in FIG. 3 will be described below.
第3図において、1は主導波管、2はH,Lの
波を伝搬する方形導波管、3はテーパ導波管、4
および6は主導波管1の方形導波管2とテーパ導
波管3の管軸方向にまたがつて、狭い面の管壁面
に接近して、広い面の管壁面に設けられた分岐導
波管および結合孔、5はHの周波数帯専用方形導
波管、7は低域通過フイルタである。 In Figure 3, 1 is a main waveguide, 2 is a rectangular waveguide that propagates H and L waves, 3 is a tapered waveguide, and 4 is a rectangular waveguide that propagates H and L waves.
and 6 are branch waveguides provided on the wide tube wall surface, close to the narrow tube wall surface, straddling the rectangular waveguide 2 and the tapered waveguide 3 of the main waveguide 1 in the tube axis direction. A tube and a coupling hole, 5 is a rectangular waveguide dedicated to the H frequency band, and 7 is a low-pass filter.
いま、方形導波管2の横断面の中央を貫いてZ
軸をとり、方形導波管2の長辺を2a、および短
辺を2bとし、長辺および短辺に平行に各々xお
よびyの座標軸をとる。 Now, passing through the center of the cross section of the rectangular waveguide 2,
The long side of the rectangular waveguide 2 is taken as 2a, and the short side is taken as 2b, and x and y coordinate axes are taken parallel to the long side and the short side, respectively.
TE10モードの管軸方向の磁界成分は
ただし、λg:方形導波管の管内波長
で表わされる。すなわち、管軸方向の磁界はx=
0(すなわち、長辺の中心部)で最小となり、x
=a(すなわち、短辺の管壁面)で最大となるこ
とから、結合孔6を管軸方向に長く、しかも狭い
面の管壁面に接近させて設けることにより、分岐
導波管4に主導波管1の管軸方向の磁界成分で結
合することができる。 The magnetic field component in the tube axis direction in TE 10 mode is However, λg is expressed by the guide wavelength of the rectangular waveguide. In other words, the magnetic field in the tube axis direction is x=
It is minimum at 0 (i.e., the center of the long side), and x
= a (i.e., the short side tube wall surface). Therefore, by providing the coupling hole 6 long in the tube axis direction and close to the narrow tube wall surface, the main wave is transmitted to the branch waveguide 4. Coupling can be achieved by a magnetic field component in the tube axis direction of the tube 1.
ここで、主導波管1の方形導波管2にL,Hの
波が導入された場合、Hの波に対しての動作原理
は従来のものと同様である。Lの波に対しては、
結合孔6の位置が方形導波管2とテーパ導波管3
にまたがつて設けられているので、テーパ導波管
3で形成される等価反射面から適当な距離に短く
して選定できるので結合孔6を介して分岐導波管
4に広帯域にわたり反射の少ない伝送を行うこと
ができる。 Here, when L and H waves are introduced into the rectangular waveguide 2 of the main waveguide 1, the operating principle for the H wave is the same as the conventional one. For the L wave,
The position of the coupling hole 6 is between the rectangular waveguide 2 and the tapered waveguide 3.
Since it is provided astride the tapered waveguide 3, it can be shortened to an appropriate distance from the equivalent reflection surface formed by the tapered waveguide 3, so it can be connected to the branch waveguide 4 via the coupling hole 6 over a wide band with little reflection. transmission can be carried out.
以上のようにこの発明によるとLの波に対して
方形導波管2と分岐導波管4の間で広帯域にわた
り反射の少ない伝送を行うことができ、また複数
個の分波器を当該分波器の主導波管1の狭い面で
互いに接するように並べて配列して構成できると
いう効果を有する。 As described above, according to the present invention, the L wave can be transmitted over a wide band with little reflection between the rectangular waveguide 2 and the branch waveguide 4, and a plurality of splitters can be connected to the branch waveguide 4. It has the advantage that it can be arranged side by side so as to touch each other on the narrow surface of the main wave tube 1 of the wave device.
第1図と第2図は従来の分波器を示す図、第3
図は本発明による一実施例を示す図である。
図中、1は主導波管、2は方形導波管、3はテ
ーパ導波管、4は分岐導波管、5は高周波数帯専
用導波管、6は結合孔、7は低域通過フイルタで
ある。なお、図中、同一あるいは相当部分には同
一符号を付して示してある。
Figures 1 and 2 are diagrams showing conventional duplexers;
The figure shows an embodiment according to the present invention. In the figure, 1 is a main waveguide, 2 is a rectangular waveguide, 3 is a tapered waveguide, 4 is a branched waveguide, 5 is a waveguide dedicated to high frequency bands, 6 is a coupling hole, and 7 is a low-pass waveguide. It's a filter. In the drawings, the same or corresponding parts are designated by the same reference numerals.
Claims (1)
る2つの周波数帯の同じ偏波の電磁波から、低周
波数帯の電磁波を上記主導波管に設けられた結合
孔を介して接続された分岐導波管部に分波する分
波器において、上記主導波管の横断面形状を方形
とし、上記主導波管の直線部とテーパ部の管軸方
向にまたがつて、狭い方の管壁面に接近して、広
い方の管壁面に上記結合孔、および上記分岐導波
管部を設け、かつ上記分岐導波管部はその開口面
の長辺方向が上記主導波管の直線部とテーパ部の
管軸方向と一致してなることを特徴とする分波
器。1. From electromagnetic waves of the same polarization in two frequency bands propagating through a main wave tube having a straight section and a tapered section, electromagnetic waves in a low frequency band are transferred to a branch guide connected through a coupling hole provided in the main wave tube. In a duplexer that separates waves into a wave tube section, the cross-sectional shape of the main wave tube is rectangular, and the main wave tube is straddled in the tube axis direction of the straight section and the tapered section, and approaches the narrower tube wall surface. The coupling hole and the branch waveguide section are provided on the wider tube wall surface, and the long side direction of the opening surface of the branch waveguide section is located between the straight section and the tapered section of the main waveguide. A duplexer characterized by being aligned with the tube axis direction.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3495682A JPS58151701A (en) | 1982-03-05 | 1982-03-05 | Branching filter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3495682A JPS58151701A (en) | 1982-03-05 | 1982-03-05 | Branching filter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58151701A JPS58151701A (en) | 1983-09-09 |
| JPS6340485B2 true JPS6340485B2 (en) | 1988-08-11 |
Family
ID=12428601
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3495682A Granted JPS58151701A (en) | 1982-03-05 | 1982-03-05 | Branching filter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58151701A (en) |
-
1982
- 1982-03-05 JP JP3495682A patent/JPS58151701A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58151701A (en) | 1983-09-09 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP2769615B2 (en) | Optical fiber mode selector | |
| US4026632A (en) | Frequency selective interwaveguide coupler | |
| RU2188512C2 (en) | Optical wavelength filter and optical demultiplexer | |
| US4498062A (en) | Waveguide structure for separating microwaves with mutually orthogonal planes of polarization | |
| JPH10509536A (en) | Optical integrated circuit including polarization converter | |
| JPS6014205A (en) | Balanced type optical guide connector | |
| US6236781B1 (en) | Duplicated-port waveguide grating router having substantially flat passbands | |
| US10288811B1 (en) | Optical switching between waveguides by adjacent resonant structure coupling | |
| KR101023254B1 (en) | Plasmon permeation filter | |
| JPS6340485B2 (en) | ||
| JPH02259610A (en) | Waveguide type light wavelength multiplexer | |
| JPS6046561B2 (en) | Dual polarization antenna feeder | |
| US5235297A (en) | Directional coupling manifold multiplexer apparatus and method | |
| SU919001A1 (en) | Wave-guide directional coupler | |
| JP3159631B2 (en) | Waveguide splitter | |
| JP2783362B2 (en) | Waveguide type optical star coupler | |
| JPH04346301A (en) | Optical multiplexer/demultiplexer | |
| JPS625531B2 (en) | ||
| JP2021157130A (en) | Optical waveguide element | |
| JPH03167903A (en) | T-shaped waveguide | |
| US20250208451A1 (en) | Acousto-optic based broadband directional optical device | |
| JP2946434B2 (en) | Multi-branch or multi-branch structure of optical fiber and optical waveguide | |
| JP3151785B2 (en) | Optical coupling branch circuit | |
| JPS6351701A (en) | Orthogonal polarization branching filter | |
| JPH04326308A (en) | Photomultiplexing separator |