JPH03234103A - Microwave power distribution synthesizer - Google Patents
Microwave power distribution synthesizerInfo
- Publication number
- JPH03234103A JPH03234103A JP3016390A JP3016390A JPH03234103A JP H03234103 A JPH03234103 A JP H03234103A JP 3016390 A JP3016390 A JP 3016390A JP 3016390 A JP3016390 A JP 3016390A JP H03234103 A JPH03234103 A JP H03234103A
- Authority
- JP
- Japan
- Prior art keywords
- coaxial
- power distribution
- terminal
- radial waveguide
- microwave power
- 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
- 239000004020 conductor Substances 0.000 claims abstract description 9
- 238000006243 chemical reaction Methods 0.000 claims abstract description 6
- 230000005540 biological transmission Effects 0.000 claims abstract description 3
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 239000000523 sample Substances 0.000 description 2
- 239000002131 composite material Substances 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000002441 reversible effect Effects 0.000 description 1
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明はマイクロ波電力分配合成器に関し、特に低損失
で広帯域なマイクロ波電力分配合成器に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a microwave power distribution/combiner, and more particularly to a low-loss, broadband microwave power distribution/combiner.
従来、この種のマイクロ波電力分配合成器は、ウィルキ
ンソン型電力分配合成器やTM、、。モード円筒空洞共
振器を用いたマイクロ波電力分配合成器が用いられてい
る。ウィルキンソン型電力分配合成器は同軸回路を基本
とした回路であるために広帯域であるが、回路ロスが大
きく、特に低損失特性が要求される電力増幅器等に使用
することは不適当である。一方、後者の円筒空洞共振器
を用いたマイクロ波電力分配合成器は第3図の平面図お
よび第3図のB−B断面を示す第4図の断面図に示すよ
うに、分配器として使用する場合には、マイクロ波を入
力する分配入力端子30の電界結合プローブ30A、こ
のプローブ31Aで励振されるTMOIOモード共振器
39、さらに結合棒33により分配側の周波数調整ねじ
付きのTM、、。モード共振器40に励振され、磁界結
合ループ31A、35Aから分配出力端子31゜35へ
分配されたマイクロ波を取り出す構成となっている。な
お、ほかの分配出力端子32〜38からも同様に出力さ
れる。この空洞共振器を使用したマイクロ波分配合成器
は回路損失は少ないが、使用周波数帯の広帯域化に難点
があり、7Mモード共振器をさらに2段重ねとした電力
分配合成器も考慮されているが、周波数比帯域は10%
程度の帯域より得られなかった。Conventionally, this type of microwave power divider/combiner is a Wilkinson type power divider/combiner or TM. A microwave power distribution combiner using a mode cylindrical cavity resonator is used. Since the Wilkinson type power distribution/combiner is a circuit based on a coaxial circuit, it has a wide band, but it has a large circuit loss and is not suitable for use in a power amplifier or the like that particularly requires low loss characteristics. On the other hand, the latter microwave power distribution combiner using a cylindrical cavity resonator is used as a distributor, as shown in the plan view of Figure 3 and the sectional view of Figure 4 showing the BB cross section of Figure 3. In this case, an electric field coupling probe 30A of the distribution input terminal 30 that inputs microwaves, a TMOIO mode resonator 39 excited by this probe 31A, and a TM with a frequency adjustment screw on the distribution side by a coupling rod 33. The configuration is such that microwaves excited by the mode resonator 40 and distributed from the magnetic field coupling loops 31A and 35A to the distribution output terminals 31 and 35 are taken out. Note that the signals are similarly outputted from the other distribution output terminals 32 to 38. A microwave distributor/combiner using this cavity resonator has low circuit loss, but it has a difficulty in widening the frequency band used, and a power distributor/combiner with two additional stages of 7M mode resonators is also being considered. However, the frequency ratio band is 10%
It was not possible to obtain more than a certain degree of bandwidth.
上述した従来のマイクロ波電力分配合成器は、ウィルキ
ンソン型電力分配合成器は周波数の広帯域性はよいが、
回路にロスが多く、7Mモード共振の円筒空洞共振器を
用いた電力分配合成器は回路ロスはよいが周波数の広帯
域性に問題があり、回路ロスと周波数の広帯域の両者を
満足するマイクロ波分配合成器が得られない欠点があっ
た。As for the conventional microwave power divider/combiner mentioned above, the Wilkinson type power divider/combiner has a good frequency broadband property, but
There is a lot of loss in the circuit, and a power distribution combiner using a cylindrical cavity resonator with 7M mode resonance has good circuit loss but has a problem with wide frequency band characteristics.Microwave distribution that satisfies both circuit loss and wide frequency band characteristics There was a drawback that a synthesizer could not be obtained.
本発明のマイクロ波分配合成器はマイクロ波信号を一つ
の第1同軸端子から入力(又は出力)し複数の第2同軸
端子からマイクロ波信号を出力(又は入力)するマイク
ロ波電力分配合成器において、前記第1同軸端子と前記
第2同軸端子との間の伝送路を薄型の中空円筒部で形成
するラジアル導波路と、前記ラジアル導波路の中空円筒
部の円形の中心に前記第1同軸端子を取り付け、前記中
心から所定の半径の位置に前記第2同軸端子を取り付け
、前記第1および第2同軸端子の中心導体の先端に前記
ラジアル導波路へのインピーダンス整合をとる円すい状
の同軸ラジアル導波路変換部を設けている。The microwave power distribution combiner of the present invention is a microwave power distribution combiner that inputs (or outputs) a microwave signal from one first coaxial terminal and outputs (or inputs) microwave signals from a plurality of second coaxial terminals. , a radial waveguide forming a transmission path between the first coaxial terminal and the second coaxial terminal with a thin hollow cylindrical part, and the first coaxial terminal located at the center of the circle of the hollow cylindrical part of the radial waveguide. and the second coaxial terminal is attached at a predetermined radius from the center, and a conical coaxial radial conductor is attached to the tips of the center conductors of the first and second coaxial terminals for impedance matching to the radial waveguide. A wave path converter is provided.
次に本発明について図面を参照して説明する。 Next, the present invention will be explained with reference to the drawings.
第1図は本発明の一実施例の平面図、第2図は第1図の
A−A断面図を示す0図において、1は分配器入力端子
(又は、合成器出力端子)、11〜18は分配器出力端
子(又は合成器入力端子)、2はラジアル導波路、2A
はラジアル導波路外壁、3A、3Bはラジアル導波路の
断面導体壁、20〜28は円すい状同軸導波路変換部で
ある。FIG. 1 is a plan view of an embodiment of the present invention, and FIG. 2 is a cross-sectional view taken along line A-A in FIG. 18 is a distributor output terminal (or combiner input terminal), 2 is a radial waveguide, 2A
3A and 3B are the radial waveguide outer walls, 3A and 3B are the cross-sectional conductor walls of the radial waveguide, and 20 to 28 are conical coaxial waveguide converters.
まず、本実施例のマイクロ波電力分配合成器の構造を説
明する。ラジアル導波路2はラジアル導波路外壁2Aで
かこまれた中空の幅りの薄型円筒形である。中心部に分
配入力端子1が取り付けられている8円すい状同軸導波
路変換部20は同軸状の中心導体がラジアル導波路2内
に入ると円すい状にひろがって底面に接している0本実
施例で示される8個の分配出力端子11〜18はラジア
ル導波路2の内面の端面導体壁3A、3Bから1なる距
離に同軸の中心を置いて取り付けられている。この8個
の分配出力端子のそれぞれの円すい状同軸導波路変換部
21〜28は円すい状同軸導波路変換部20と同じ構造
である。First, the structure of the microwave power distribution/synthesizer of this embodiment will be explained. The radial waveguide 2 is a hollow, thin cylinder surrounded by a radial waveguide outer wall 2A. The 8-cone-shaped coaxial waveguide converter 20 has the distribution input terminal 1 attached to the center, and when the coaxial center conductor enters the radial waveguide 2, it expands into a conical shape and touches the bottom surface. The eight distributed output terminals 11 to 18 shown are attached with their coaxial centers placed at a distance of 1 from the end conductor walls 3A and 3B on the inner surface of the radial waveguide 2. The conical coaxial waveguide converters 21 to 28 of the eight distribution output terminals have the same structure as the conical coaxial waveguide converter 20.
次に本実施例の分配器の場合の動作について説明する0
分配入力端子1より入力された信号は、円すい状同軸導
波路変換部20で同軸のインピーダンスからラジアル導
波路インピーダンスに変換される0例えば同軸部のイン
ピーダンスが50Ωの場合には、図に示す角度θを約4
5°とし、hをマイクロ波の波長のぼは0.2波長程度
に選ぶと良い変換特性が得られる。このように分配入力
端子1より入力された信号は中心からラジアルな波紋状
にラジアル導波路2内に導かれてひろがって行く、その
一部の波紋は例えば円すい状同軸導波路変換部25で捕
そくされて分配出力端子15より出力される。このとき
一部の信号は円すい状変換部の側を通り抜け、&=1/
4波長先に波長端面導体壁3Aにより反射される。この
反射波と分配入力端子1からの直接波の反射渡分とが打
ち消し合うように、分配入力端子1と分配出力端子15
の距離を選定すると、入力端子から出力端子への不整合
のない分配器が構成出来る0合成器として使う場合も可
逆動作なので、同じように不整合を生じない。Next, the operation of the distributor of this embodiment will be explained.
The signal input from the distribution input terminal 1 is converted from coaxial impedance to radial waveguide impedance by the conical coaxial waveguide converting section 20. For example, when the impedance of the coaxial section is 50Ω, the angle θ shown in the figure is about 4
Good conversion characteristics can be obtained by setting the angle to 5° and selecting h to be about 0.2 wavelength of the microwave wavelength. In this way, the signal input from the distribution input terminal 1 is guided into the radial waveguide 2 in the form of radial ripples from the center and spreads out, and some of the ripples are captured by the conical coaxial waveguide converter 25, for example. The signal is then output from the distribution output terminal 15. At this time, a part of the signal passes through the conical conversion part, &=1/
It is reflected by the wavelength end face conductor wall 3A four wavelengths ahead. The distribution input terminal 1 and distribution output terminal 15
If the distance is selected, a distributor with no mismatch from the input terminal to the output terminal can be constructed.Even when used as a 0 combiner, no mismatch will occur since the operation is reversible.
以上説明したように本発明では、円すい状同軸導波路変
換部とラジアル導波路とを効果的に組合わせることによ
り、広帯域な周波数特性を有し、かつ低損失な電力分配
合成器を実現することが出来る効果がある。さらに、薄
型のラジアル導波路と円すい状の変換部とにより従来例
に比して小形化されたマイクロ波電力分配合成器を実現
出来る効果もある。As explained above, in the present invention, by effectively combining a conical coaxial waveguide converter and a radial waveguide, it is possible to realize a power distribution/synthesizer that has broadband frequency characteristics and low loss. There is an effect that can be done. Furthermore, the thin radial waveguide and the conical converting section have the effect of realizing a microwave power distribution/synthesizer that is more compact than the conventional example.
11〜18.31〜38・・・分配出力端子(又は合成
入力端子)、20〜28・・・円すい状同軸導波路変換
部、3A、3B・・・ラジアル導波路の端面導体壁、3
9・・・TMo!oモード共振器、40・・・TM、ア
0モード共振器。11-18. 31-38... Distribution output terminal (or composite input terminal), 20-28... Conical coaxial waveguide conversion section, 3A, 3B... End face conductor wall of radial waveguide, 3
9...TMo! o mode resonator, 40...TM, a0 mode resonator.
Claims (2)
は出力)し複数の第2同軸端子からマイクロ波信号を出
力(又は入力)するマイクロ波電力分配合成器において
、前記第1同軸端子と前記第2同軸端子との間の伝送路
を薄型の中空円筒部で形成するラジアル導波路と、前記
ラジアル導波路の中空円筒部の円形の中心に前記第1同
軸端子を取り付け、前記中心から所定の半径の位置に前
記第2同軸端子を取り付け、前記第1および第2同軸端
子の中心導体の先端に前記ラジアル導波路へのインピー
ダンス整合をとる円すい状の同軸ラジアル導波路変換部
を設けたことを特徴とするマイクロ波電力分配合成器。1. In a microwave power distribution combiner that inputs (or outputs) a microwave signal from one first coaxial terminal and outputs (or inputs) microwave signals from a plurality of second coaxial terminals, the first coaxial terminal and the first coaxial terminal A radial waveguide in which a transmission path between two coaxial terminals is formed by a thin hollow cylindrical part, and the first coaxial terminal is attached to the circular center of the hollow cylindrical part of the radial waveguide, and the first coaxial terminal is attached at a predetermined radius from the center. The second coaxial terminal is attached at a position, and a conical coaxial radial waveguide converting portion for impedance matching to the radial waveguide is provided at the tips of the center conductors of the first and second coaxial terminals. Microwave power distribution combiner.
ラジアル導波路変換部の位置が前記ラジアル導波路の側
壁から1/4波長の距離にあり、かつ、円すい部のテー
パ角度が同軸のインピーダンスに応じて所定の角度を有
することを特徴とする請求項1記載のマイクロ波電力分
配合成器。2. The conical coaxial radial waveguide conversion section attached to the second coaxial terminal is located at a distance of 1/4 wavelength from the side wall of the radial waveguide, and the taper angle of the conical section corresponds to the coaxial impedance. 2. The microwave power distribution combiner according to claim 1, wherein the microwave power distribution combiner has a predetermined angle.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3016390A JPH03234103A (en) | 1990-02-08 | 1990-02-08 | Microwave power distribution synthesizer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3016390A JPH03234103A (en) | 1990-02-08 | 1990-02-08 | Microwave power distribution synthesizer |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH03234103A true JPH03234103A (en) | 1991-10-18 |
Family
ID=12296088
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3016390A Pending JPH03234103A (en) | 1990-02-08 | 1990-02-08 | Microwave power distribution synthesizer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH03234103A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR20240046518A (en) | 2021-08-30 | 2024-04-09 | 도쿄 케이키 가부시키가이샤 | power distribution synthesizer |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5564403A (en) * | 1978-11-02 | 1980-05-15 | Raytheon Co | Microwave power coupler |
JPS63299502A (en) * | 1987-05-29 | 1988-12-07 | Nec Corp | Rotary transmission equipment |
JPH01147903A (en) * | 1987-12-04 | 1989-06-09 | Hitachi Ltd | High frequency power synthesizer |
-
1990
- 1990-02-08 JP JP3016390A patent/JPH03234103A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5564403A (en) * | 1978-11-02 | 1980-05-15 | Raytheon Co | Microwave power coupler |
JPS63299502A (en) * | 1987-05-29 | 1988-12-07 | Nec Corp | Rotary transmission equipment |
JPH01147903A (en) * | 1987-12-04 | 1989-06-09 | Hitachi Ltd | High frequency power synthesizer |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR20240046518A (en) | 2021-08-30 | 2024-04-09 | 도쿄 케이키 가부시키가이샤 | power distribution synthesizer |
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