JPS603241B2 - duplexer - Google Patents
duplexerInfo
- Publication number
- JPS603241B2 JPS603241B2 JP1213078A JP1213078A JPS603241B2 JP S603241 B2 JPS603241 B2 JP S603241B2 JP 1213078 A JP1213078 A JP 1213078A JP 1213078 A JP1213078 A JP 1213078A JP S603241 B2 JPS603241 B2 JP S603241B2
- Authority
- JP
- Japan
- Prior art keywords
- circular waveguide
- waveguide
- dedicated
- wave
- waves
- 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
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
Description
【発明の詳細な説明】
この発明は多周波数帯の伝搬波を高周波数帯の波と低周
波数帯の波に分波するマイクロ波分波器の改良に関する
ものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a microwave splitter that splits propagating waves in multiple frequency bands into waves in a high frequency band and waves in a low frequency band.
ここでは説明の便宜上、高い周波数の波をfHとし、低
い周波数帯の波をfLとし、fMとfLとの分波器につ
いて述べる。Here, for convenience of explanation, a high frequency wave is referred to as fH, a low frequency band wave is referred to as fL, and a duplexer for fM and fL will be described.
第1図に従来の分波器の破断側面図を示す。FIG. 1 shows a cutaway side view of a conventional duplexer.
図中1は共用円形導波管、2は共用円形導波管1にコル
ゲート溝を形成するための隔壁、3は隔壁2によって形
成されるコルゲート溝、4は専用円形導波管、5は結合
孔、6は共用円形導波管1に設けられた結合孔5を介し
て接続された方形導波瞥、7は方形導波管6内に設けら
れた低域通過ワッフルアイアンフィル夕、8は方形導波
管6、ワツフルアイアンフィル夕7、結合孔5、共用円
形導波管1、専用円形導波管4で礎成される同軸線路形
偏分波器、9は専用円形導波管4に直交して設けられる
方形導波管「 10は専用円形導波管4に共軸的に設け
られる方形導波管、11は短絡板、12は方形導波管9
.10、結合孔5で構成される円形導波管形偏分波器、
14は共用円形導波管1と専用円形導波管4とで構成さ
れる同軸線路、13は同軸線礎14に設けられたfHの
波を反射するポスト形低域通過フィル夕である。従釆第
1図に示す分波器の動作原理を説明する前に、この発明
の説明に必要な範囲においてコルゲート溝3の動作を説
明する。コルゲート溝3の間隔が共用円形導波管1を伝
搬する波の波長に比べて十分小さいと、コルゲート簿3
はコルゲート溝3の深さが入/4と^/2との間の周波
数では容量性サセプタンスを呈し、コルゲート溝3の深
さが^/4より浅い周波数では誘導性サセプタンスを呈
する。In the figure, 1 is a shared circular waveguide, 2 is a partition for forming a corrugated groove in the shared circular waveguide 1, 3 is a corrugated groove formed by the partition 2, 4 is a dedicated circular waveguide, and 5 is a coupling 6 is a rectangular waveguide connected via the coupling hole 5 provided in the common circular waveguide 1; 7 is a low-pass waffle iron filter provided in the rectangular waveguide 6; 8 is a A coaxial line type polarization splitter consisting of a rectangular waveguide 6, a Watsuful iron filter 7, a coupling hole 5, a common circular waveguide 1, and a dedicated circular waveguide 4, 9 is a dedicated circular waveguide. A rectangular waveguide provided orthogonally to the dedicated circular waveguide 4; 10 is a rectangular waveguide provided coaxially with the dedicated circular waveguide 4; 11 is a shorting plate; 12 is a rectangular waveguide 9;
.. 10, a circular waveguide polarization splitter composed of a coupling hole 5;
14 is a coaxial line composed of a common circular waveguide 1 and a dedicated circular waveguide 4, and 13 is a post-shaped low-pass filter provided on the coaxial line base 14 to reflect the fH wave. Before explaining the operating principle of the duplexer shown in FIG. 1, the operation of the corrugated groove 3 will be explained to the extent necessary for explaining the present invention. If the interval between the corrugated grooves 3 is sufficiently small compared to the wavelength of the wave propagating in the shared circular waveguide 1, the corrugated grooves 3
exhibits capacitive susceptance at frequencies where the depth of the corrugated grooves 3 is between I/4 and ^/2, and exhibits inductive susceptance at frequencies where the depth of the corrugated grooves 3 is shallower than ^/4.
ここで^は自由空間波長である。さてコルゲート溝3の
呈するマドミタンスYcは等価回路表示をすると伝法線
路に直列に分布する。Here ^ is the free space wavelength. Now, the madmitance Yc exhibited by the corrugated groove 3 is distributed in series with the transmission line when expressed as an equivalent circuit.
したがって、コルゲート簿3の深さをdとすると、^/
4‐ミd<^/2の場合にはYc/i20となり円形導
波瞥の位相速度よりコルゲート溝3を設けた導波管部の
位相速度が速くなる。Therefore, if the depth of corrugated book 3 is d, then ^/
When d<^/2, Yc/i20, and the phase velocity of the waveguide section provided with the corrugated groove 3 becomes faster than the phase velocity of the circular waveguide beam.
また、^/4>dの場合にはYc/j<0となり円形導
波管の位相速度よりコルゲート溝3を設けた導波管部の
位相速度が遅くなる。Further, when ^/4>d, Yc/j<0, and the phase velocity of the waveguide section provided with the corrugated groove 3 becomes slower than the phase velocity of the circular waveguide.
位相速度が遅くなると、いわゆる表面波の特性を伝搬波
が呈するようになる。As the phase velocity decreases, the propagating wave begins to exhibit the characteristics of a so-called surface wave.
すなわち、伝搬波のエネルギーはほとんどコルゲート溝
3の入口部に集中し、導波管の中心部では少なくなる。
当然のことながら位相速度が速い場合にはこの逆の現象
が生じる。いま、fHに対してYc/20、fLに対し
てYc/i〈0となるようにコルゲート溝3の深さを選
ぶと、共用円形導波管1に入射したfH、fLの波はコ
ルゲート溝3の働きにより、fLの波のエネルギーはコ
ルゲート溝3の入口部に集中し、fHの波のエネルギー
は管軸部に集中して伝搬するようになる。That is, most of the energy of the propagating wave is concentrated at the entrance of the corrugated groove 3, and is reduced at the center of the waveguide.
Naturally, the opposite phenomenon occurs when the phase velocity is high. Now, if we choose the depth of the corrugated groove 3 so that fH is Yc/20 and fL is Yc/i<0, the waves of fH and fL incident on the common circular waveguide 1 will pass through the corrugated groove. 3, the energy of the wave fL is concentrated at the entrance of the corrugated groove 3, and the energy of the wave fH is concentrated at the tube axis and propagated.
したがって、専用円形導波管4の先端を共用円形導波管
1のコルゲート溝3を施した部分に設置すると、fHの
波は専用円形導波管4に、fLの波は同軸線路14に分
波される。Therefore, if the tip of the dedicated circular waveguide 4 is installed in the corrugated groove 3 of the shared circular waveguide 1, the fH wave will be split into the dedicated circular waveguide 4, and the fL wave will be split into the coaxial line 14. be waved.
このとき、fLの波に対しては専用円形導波管4がしや
断特性を呈するように設計されるのでfLの波はfHの
出力端である円形導波管形隅分波器12の方形導波管9
,10に漏洩しない。At this time, since the dedicated circular waveguide 4 is designed to exhibit a shearing characteristic for the fL wave, the fL wave is transmitted to the circular waveguide corner splitter 12 which is the output end of fH. square waveguide 9
, 10.
しかし、fHの波のうち一部の電力は、fLの波が伝搬
する同軸線路14に漏洩し、fLの出力端である同軸形
偏分波器8の方形導波管6に漏洩するのでポスト形の低
域通過フィル夕13が設けられている。However, some of the power of the fH wave leaks into the coaxial line 14 through which the fL wave propagates, and leaks into the rectangular waveguide 6 of the coaxial polarization splitter 8, which is the output end of fL. A shaped low-pass filter 13 is provided.
このように従来の第1図に示す分波器においては、共用
円形導波管1に入射したfL、 fHは、コルゲート溝
3の働きによりfLの波はコルゲート溝3の入口部に沿
うように伝搬し同軸線路14に、また、fHの波は管軸
部に集中して伝搬し専用円形導波管4に、それぞれ分波
される。In this way, in the conventional duplexer shown in FIG. 1, the waves fL and fH incident on the common circular waveguide 1 are caused by the action of the corrugated groove 3 so that the wave of fL follows the entrance of the corrugated groove 3. The wave of fH propagates to the coaxial line 14, and the wave of fH propagates concentrated in the tube shaft portion, and is split into the dedicated circular waveguide 4, respectively.
その後fLおよびfHの波は、それぞれ、同軸形偏分波
器8および円形導波管形偏分波器12によって、入射偏
波の状態に応じて各偏分波器の分岐方形導波管6,9,
1川こ分波される。しかし、従来の分波器においては、
ポスト形低域通過フィルター3が、同軸線路14に漏洩
したfHの波のうちの基本モード波に対してしか有効で
ないため、高次モード波に対するフィル夕としてワッフ
ルアイアンフィル夕7を同軸形偏分波器の方形導波管6
中に設ける必要があり、このため、同軸形偏分波器8の
構造が複雑となり、かつ良好な整合を得にくい欠点があ
った。Thereafter, the waves fL and fH are transferred to a branch rectangular waveguide 6 of each polarization splitter according to the state of the incident polarization by a coaxial polarization splitter 8 and a circular waveguide polarization splitter 12, respectively. ,9,
One river is waved. However, in conventional duplexers,
Since the post-type low-pass filter 3 is effective only for the fundamental mode wave of the fH waves leaked into the coaxial line 14, the waffle iron filter 7 is used as a filter for higher-order mode waves. Rectangular waveguide 6
Therefore, the structure of the coaxial polarization splitter 8 becomes complicated, and it is difficult to obtain good matching.
また、fHの波を良好な整合を得ながら専用円形導波管
4に分波するには、内径の大きな専用円形導波管4が必
要であるが内径を大きくするとfLの波に対する影響が
生じるため、専用円形導波管4の内径を十分大きくでき
ず、専用円形導波管4先端における反射が大きい欠点が
あった。In addition, in order to branch the fH wave into the dedicated circular waveguide 4 while obtaining good matching, a dedicated circular waveguide 4 with a large inner diameter is required, but increasing the inner diameter will have an effect on the fL wave. Therefore, the inner diameter of the dedicated circular waveguide 4 could not be made sufficiently large, and there was a drawback that reflection at the tip of the dedicated circular waveguide 4 was large.
この発明はこれらの欠点を除去するため、同軸線路14
部に設けられるコルゲート溝3をワッフルアイアン形の
フィル夕にするとともに専用円形導波管4の内壁にコル
ゲート溝を新たに設けたもので、以下図面について詳細
に説明する。第2図はこの発明の一実施例を示す。In order to eliminate these drawbacks, the present invention provides a coaxial line 14
The corrugated groove 3 provided in the section is changed to a waffle iron type filter, and a corrugated groove is newly provided on the inner wall of the dedicated circular waveguide 4.The drawings will be described in detail below. FIG. 2 shows an embodiment of the invention.
また第3図に、第2図におけるA−A′断面図を礎造を
明確にするために示す。第1図に示す従釆の分波器に比
べて、共用円形導波管1と同軸線路14とにまたがって
設けられるコルゲート溝3のうち同轍線路14部に設け
られるコルゲート溝3の隔壁2が第3図に示すような形
状に変形され同軸線路形ワッフルアイアンフィル夕を形
成していること、および専用円形導波管4の内壁にfH
の波に対してYcが誘導性サセプタンスを呈するコルゲ
ート溝3を新たに設けられている点に特徴がある。Further, FIG. 3 shows a sectional view taken along line A-A' in FIG. 2 to clarify the foundation structure. Compared to the secondary branching filter shown in FIG. is deformed into the shape shown in FIG. 3 to form a coaxial line type waffle iron filter, and the inner wall of the dedicated circular waveguide 4 is
A feature is that a corrugated groove 3 is newly provided in which Yc exhibits an inductive susceptance with respect to waves of .
この発明を実施した分波器においては、同軸線路14に
漏洩したfHの波に対して同軸線賂形のワッフルアイア
ンフィル夕7が働く。In the duplexer embodying the present invention, a waffle iron filter 7 in the form of a coaxial line acts on the fH wave leaked into the coaxial line 14.
このワッフルアイアンフィル夕7はfHの波のすべての
モード波に対してしや断特性を呈するため、第1図に示
す従来の発明のように同軸線路形偏分波器8の方形導波
管6にワッフルアイアンフィル夕を設ける必要がなくな
る。このため、fLの波を分波する同軸線路形偏分波器
8が簡単になるとともに、整合を得やすくなり良好なV
SWR特性が得られる。また、第2図のこの発明の実施
例では専用円形導波管4中にfHの波に対してYcが誘
導性サセプタンスを呈するコルゲート溝3が設けられて
いる。Since this waffle iron filter 7 exhibits a shearing characteristic for all mode waves of the fH wave, the rectangular waveguide of the coaxial line type polarization splitter 8 is used as shown in the conventional invention shown in FIG. There is no need to provide a waffle iron filler in 6. Therefore, the coaxial line type polarization splitter 8 that separates the wave of fL becomes simple, and matching is easily obtained and a good V
SWR characteristics can be obtained. Further, in the embodiment of the present invention shown in FIG. 2, a corrugated groove 3 in which Yc exhibits an inductive susceptance to waves of fH is provided in the dedicated circular waveguide 4.
このコルゲート溝3の動作原理は共用円形導波管1に設
けられているコルゲート溝3の場合と同じである。した
がって、コルゲート簿3の深さを適当に選ふくと、専用
円形導波管4を伝搬するfHの波のエネルギーの管墜部
分を伝搬する童を円形導波管の場合に比べて多くするこ
とができる。The operating principle of this corrugated groove 3 is the same as that of the corrugated groove 3 provided in the shared circular waveguide 1. Therefore, by appropriately selecting the depth of the corrugated waveguide 3, it is possible to increase the amount of energy of the fH wave propagating through the dedicated circular waveguide 4 through the trajectories compared to the case of a circular waveguide. I can do it.
これは、専用円形導波管4の内径を等価的に大きくした
効果をもたらする。そのため、従来の分波器に比べて、
コルゲート溝3が設けられた共用円形導波管1部を伝搬
する管軸部にエネルギーの集中したfHの波のエネルギ
ーは、より容易にコルゲート溝3の設けられた専用円形
導波管4に分波されるようになり、専用円形導波管4先
端でのfHの波に対するVSWR特性を良好にすること
ができる。This has the effect of equivalently increasing the inner diameter of the dedicated circular waveguide 4. Therefore, compared to conventional duplexers,
The energy of the fH wave propagating through the common circular waveguide 1 provided with the corrugated groove 3 and concentrated in the tube axis is more easily divided into the dedicated circular waveguide 4 provided with the corrugated groove 3. As a result, the VSWR characteristics for fH waves at the tip of the dedicated circular waveguide 4 can be improved.
なお、以上は、fLとfHとの2周波数帯について説明
したが、この発明はこれに限らず、fL、fHの中にさ
らに多周波数帯の波が含まれている場合にも適用できる
ことは明らかである。Although the above description has been made regarding two frequency bands, fL and fH, it is clear that the present invention is not limited to this, but can also be applied to cases where fL and fH include waves in multiple frequency bands. It is.
以上のように、この発明に係る分波器においては、同軸
線路14部に設ける同軸線路形のワッフルアイアンフィ
ル夕7により、同額線路形偏分波器8の構造を簡単にで
きるとともにVSWR特性が改善できる利点、および専
用円形導波管4内に設けるコルゲート溝3により専用円
形導波管4先端部のVSWR特性を良効にできる利点が
ある。As described above, in the duplexer according to the present invention, the coaxial line type waffle iron filter 7 provided in the coaxial line 14 portion simplifies the structure of the equal line type polarized duplexer 8 and improves the VSWR characteristic. There is an advantage that it can be improved, and that the corrugated groove 3 provided in the dedicated circular waveguide 4 can improve the VSWR characteristic of the tip of the dedicated circular waveguide 4.
第1図は従来の分波器の破断側面図、第2図はこの発明
の一実施例を示す被断側面図、第3図は第2図中のA−
A′断面図である。
図中、1‘ま共用円形導波管、2はコルゲート溝の隔壁
、3はコルゲート溝、4は専用円形導波管、7はワッフ
ルアイアンフィル夕、8は同軸線路形偏分波器、12は
円形導波管形偏分波器、13はポスト形低域通過フィル
夕、14は同軸線路である。
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。多1図
多Z図
巻ミ図FIG. 1 is a cutaway side view of a conventional duplexer, FIG. 2 is a cutaway side view showing an embodiment of the present invention, and FIG. 3 is a cutaway side view of a conventional duplexer.
It is an A' sectional view. In the figure, 1' is a common circular waveguide, 2 is a partition wall of a corrugated groove, 3 is a corrugated groove, 4 is a dedicated circular waveguide, 7 is a waffle iron filter, 8 is a coaxial line type polarization splitter, 12 1 is a circular waveguide type polarization splitter, 13 is a post-type low-pass filter, and 14 is a coaxial line. In the drawings, the same or corresponding parts are denoted by the same reference numerals. Many 1 drawings Many Z drawings Mi drawings
Claims (1)
数帯の波を伝搬する高周波数帯専用円形導波管を同心的
に設置し、この専用円形導波管の先端近傍が位置する共
用円形導波管部に複数のコルゲート溝を設けることによ
り、高周波数帯の波を専用円形導波管に、一方低周波数
帯の波を共用円形導波管と専用導波管とで構成される同
軸線路に分波する分波器において、同軸線路部に位置す
るコルゲート溝の隔壁をワツフルアイアンフイルタとし
、かつ上記専用導波管の内壁にコルゲート溝を設けるこ
とを特徴とした分波器。1 A circular waveguide dedicated to high frequency bands that propagates waves in a high frequency band is installed concentrically within a shared waveguide that propagates waves in multiple frequency bands, and the vicinity of the tip of this dedicated circular waveguide is located By providing multiple corrugated grooves in the shared circular waveguide section, waves in the high frequency band are placed in a dedicated circular waveguide, while waves in the low frequency band are configured in the shared circular waveguide and the dedicated waveguide. A branching filter for branching into a coaxial line, characterized in that the partition wall of the corrugated groove located in the coaxial line part is a Watsuful iron filter, and the inner wall of the dedicated waveguide is provided with a corrugated groove. vessel.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1213078A JPS603241B2 (en) | 1978-02-06 | 1978-02-06 | duplexer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1213078A JPS603241B2 (en) | 1978-02-06 | 1978-02-06 | duplexer |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS54105447A JPS54105447A (en) | 1979-08-18 |
JPS603241B2 true JPS603241B2 (en) | 1985-01-26 |
Family
ID=11796942
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1213078A Expired JPS603241B2 (en) | 1978-02-06 | 1978-02-06 | duplexer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS603241B2 (en) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH08139502A (en) * | 1994-11-14 | 1996-05-31 | Nec Corp | Circular polarized wave generator |
US6031434A (en) * | 1998-09-18 | 2000-02-29 | Hughes Electronics Corporation | Coaxially configured OMT-multiplexer assembly |
CN113131111B (en) * | 2021-04-17 | 2021-11-12 | 中国人民解放军国防科技大学 | W-band-pass filter |
-
1978
- 1978-02-06 JP JP1213078A patent/JPS603241B2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS54105447A (en) | 1979-08-18 |
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