JPS636904A - Power distribution circuit - Google Patents
Power distribution circuitInfo
- Publication number
- JPS636904A JPS636904A JP15018886A JP15018886A JPS636904A JP S636904 A JPS636904 A JP S636904A JP 15018886 A JP15018886 A JP 15018886A JP 15018886 A JP15018886 A JP 15018886A JP S636904 A JPS636904 A JP S636904A
- Authority
- JP
- Japan
- Prior art keywords
- coaxial line
- impedance
- waveguide
- power distribution
- transformer
- 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 35
- 238000006243 chemical reaction Methods 0.000 abstract description 5
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 230000009466 transformation Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 1
Landscapes
- Waveguide Aerials (AREA)
Abstract
Description
【発明の詳細な説明】
技術分野
本発明は電力分配回路に関し、特に同軸導波管変換機能
を有する電力分配回路に関するものである。TECHNICAL FIELD The present invention relates to a power distribution circuit, and more particularly to a power distribution circuit having a coaxial waveguide conversion function.
従来技術
従来のこの種の電力分配回路の1例が第12図に示され
ており、図は1部破断面を含む斜視図である。方形導波
管1の内部にはこの内部を2分割すべくH面に平行に設
けられた分割用導体板5が取付けられている。この導体
板5の前端縁51はこの導波管1のE面に対して直交し
ており、この前端縁51の当該E面に近接する部分に同
軸線路との結合孔3が穿設されている。この結合孔3に
おいて同軸線路と導波管とが電気的に結合されることに
なる。BACKGROUND ART An example of a conventional power distribution circuit of this type is shown in FIG. 12, which is a perspective view including a partially broken surface. A dividing conductor plate 5 is attached to the inside of the rectangular waveguide 1 and is provided parallel to the H plane to divide the inside into two parts. The front edge 51 of the conductor plate 5 is perpendicular to the E plane of the waveguide 1, and a coupling hole 3 with a coaxial line is bored in a portion of the front edge 51 close to the E plane. There is. In this coupling hole 3, the coaxial line and the waveguide are electrically coupled.
そのために、同軸線路の中心導体2が導体板5の前端縁
51の結合孔3に望む部分と電気的に接続されている。For this purpose, the center conductor 2 of the coaxial line is electrically connected to a portion of the front edge 51 of the conductor plate 5 that is desired to be connected to the coupling hole 3.
また、同軸線路の外導体4が導波管のE面と電気的に接
続されるが、第12図においては図面上に現われない。Further, the outer conductor 4 of the coaxial line is electrically connected to the E plane of the waveguide, but it does not appear on the drawing in FIG.
かかる構成の装置を電力分配回路として用いる場合には
、例えば同軸線路からの供給電力が導体板5の作用によ
り、この導体板5の上下に形成された導波管路へ夫々同
相にて分割されて導波管1へ給電されるのである。When a device with such a configuration is used as a power distribution circuit, for example, the power supplied from a coaxial line is divided into waveguide paths formed above and below this conductor plate 5 in the same phase by the action of the conductor plate 5. Power is then supplied to the waveguide 1.
この種の電力分配回路における同’Nl /導波管変換
部において、同軸線路の特性インピーダンスZocは第
13図において示す如く、外導体直径をR2中心導体直
径をr1両導体間誘電体の比誘電率をε、とした場合、
Z =(138/7)flo(1(R/r)C
となる。−般にマイクロ波帯の同軸線路では、50Ωで
ある。In this type of power distribution circuit, the characteristic impedance Zoc of the coaxial line is as shown in Figure 13. If the ratio is ε, then Z = (138/7)flo(1(R/r)C. - Generally, in a coaxial line in the microwave band, it is 50Ω.
一方、方形導波管の特性インピーダンスZ。rは、第1
4図に示す如く導波管1の横寸法をa、1寸法をす、波
動インピーダンスをZllとすると、2o、=2.<π
b/2a)
と表わされる。分岐導波管では、横寸法aと縦寸法すと
の比が約4:1となっているので、Zo−よ約180Ω
となる。On the other hand, the characteristic impedance Z of the rectangular waveguide. r is the first
As shown in Figure 4, if the lateral dimension of the waveguide 1 is a, 1 dimension, and the wave impedance is Zll, then 2o, = 2. <π
b/2a). In the branch waveguide, the ratio of the horizontal dimension a to the vertical dimension is approximately 4:1, so Zo- is approximately 180Ω.
becomes.
ここで、同軸線路の端子と分岐導波管との接続を考えた
場合、その等何回路は第15図の如くなり、よって同軸
線路の端子からみた入力インピーダンスZ・は、Zor
が並列に接続されているので、n
Zorの1/2となって約90Ωとなる。If we consider the connection between the terminal of the coaxial line and the branch waveguide, the circuit will be as shown in Figure 15, and therefore the input impedance Z as seen from the terminal of the coaxial line will be Zor
are connected in parallel, so it becomes 1/2 of n Zor and becomes about 90Ω.
ところで、従来のこの種の電力分配回路では、第12図
にて示した如く同軸線路と分岐用導体板5とが直接に接
続されている。よって、同軸部の特性インピーダンスZ
。0と分岐導波管の入力インピーダンスZioとがそれ
ぞれ50Ωと90Ωと互いに大きく異なることになる。By the way, in this type of conventional power distribution circuit, the coaxial line and the branching conductor plate 5 are directly connected as shown in FIG. Therefore, the characteristic impedance Z of the coaxial section
. 0 and the input impedance Zio of the branch waveguide are 50Ω and 90Ω, respectively, which are significantly different from each other.
その結果、同軸端子及び分岐導波管の入力VSWR(電
圧定在波比)が悪化し、調整ネジ等で調整してもインピ
ーダンス整合のとれる周波数帯域が狭くなり、電力分配
特性も狭帯域になるという欠点がある。As a result, the input VSWR (voltage standing wave ratio) of the coaxial terminal and branch waveguide deteriorates, the frequency band in which impedance matching can be achieved becomes narrower even if adjusted with adjustment screws, etc., and the power distribution characteristics also become narrowband. There is a drawback.
1里辺ユ遭
本発明は上記従来のものの欠点を解決すべくなされたも
のであって、その目的とするところは、電力分配特性を
広帯域にnっで良好とし得る電力分配回路を提供するこ
とにある。The present invention has been made to solve the above-mentioned drawbacks of the conventional circuits, and its purpose is to provide a power distribution circuit that can provide good power distribution characteristics over a wide band. It is in.
発明の構成
本発明によれば、方形導波管と、この方形導波管の内部
を分割すべくこの導波管のH面に平行に設けられた導体
板と、外導体が前記導波管の1面に接続され°中心導体
が前記導体板に接続された同軸線路とにより構成された
電力分配回路であって、前記同軸線路の中心導体と前記
導体板との接続部分にインピーダンストランスフォーマ
を設けたことを特徴とする電力分配回路が得られる。Structure of the Invention According to the present invention, there is provided a rectangular waveguide, a conductor plate provided parallel to the H-plane of the waveguide to divide the inside of the rectangular waveguide, and an outer conductor that is connected to the waveguide. a coaxial line connected to one side of the conductive plate and having a center conductor connected to the conductive plate, the power distribution circuit comprising an impedance transformer at a connection portion between the center conductor of the coaxial line and the conductive plate. A power distribution circuit characterized by the following characteristics is obtained.
実施例 以下、図面を用いて本発明の詳細な説明する。Example Hereinafter, the present invention will be explained in detail using the drawings.
第1図は本発明の一実施例の1部破断面を含む斜視図で
あり、第12図と同等部分は同一符号により示している
。図示する如く、本発明においては、H面に平行な分岐
のための導体板5の前端縁51と同軸線路の中心導体2
とを、従来例の第12図とは異なり(従来例ではこれ等
両者を直接に接続している)、インピーダンストランス
フォーマ6を介して接続している。FIG. 1 is a perspective view including a partially broken surface of an embodiment of the present invention, and parts equivalent to those in FIG. 12 are indicated by the same reference numerals. As shown in the figure, in the present invention, the front edge 51 of the conductor plate 5 for branching parallel to the H plane and the center conductor 2 of the coaxial line
are connected via an impedance transformer 6, unlike the conventional example shown in FIG. 12 (in the conventional example, these two are directly connected).
このインピーダンストランスフォーマ6は、導体板5の
前端縁51から同軸線路の中心導体2までの間の形状が
滑らかなテーパとなった両側縁を有している。すなわち
、トランスフォーマ6を構成する導体板の両側縁と矩形
導波管1両側面(1面に相当)との間の離間距ll1i
r 及びr2が夫々滑らかに曲線的に変化する様に構
成されている。This impedance transformer 6 has smooth tapered side edges between the front edge 51 of the conductor plate 5 and the center conductor 2 of the coaxial line. That is, the distance ll1i between both side edges of the conductor plate constituting the transformer 6 and both side surfaces (corresponding to one surface) of the rectangular waveguide 1
The structure is such that r and r2 each change smoothly in a curved manner.
こうすることにより、インピーダンス変換がこのインピ
ーダンストランスフォーマ部分6にて滑らかに行われ、
同軸線路と導波管との間のインビーダン整合が可能とな
るのである。よって、広い周波数帯域でインピーダンス
整合がとれて、全ての入出力端子における入出力インピ
ーダンス及び電力分配特性が広い周波数帯域で良好とな
る。By doing this, impedance conversion is performed smoothly in this impedance transformer portion 6,
In-vehicle matching between the coaxial line and the waveguide becomes possible. Therefore, impedance matching can be achieved over a wide frequency band, and the input/output impedance and power distribution characteristics at all input/output terminals are good over a wide frequency band.
第1図の実施例では、同軸線路の中心導体と導波管分岐
用導体板との間のインピーダンス変換を曲線テーパ状の
インピーダンストランスフォーマ6により実現している
が、第2図〜第4図に示す実施例の如く、直線テーパ状
のインピーダンストランスフォーマ6を用いても同様に
広帯域特性が実現可能となる。In the embodiment shown in FIG. 1, the impedance transformation between the center conductor of the coaxial line and the waveguide branching conductor plate is realized by a curved tapered impedance transformer 6. Similarly, broadband characteristics can be achieved by using a linearly tapered impedance transformer 6 as in the embodiment shown.
更に、第5図及び第6図に示した実施例の様に、ステッ
プ状のインピーダンストランスフォーマ6を用いてステ
ップ的なインピーダンス変換を行うようにしても同様に
広帯域が実現される。Furthermore, as in the embodiments shown in FIGS. 5 and 6, a wide band can be similarly achieved by performing stepwise impedance transformation using a stepwise impedance transformer 6.
第7図〜第11図は第1図の実施例に示した曲線状の滑
らかなテーパによるインピーダンストランスフオー76
の他の変形例を夫々示すものである。また、インピーダ
ンスの変換を一般のインピーダンス変換と同様にTch
ebysheH(チエビシエフ)III数等によって実
現しても良いものである。7 to 11 show an impedance transformer 76 with a curved smooth taper shown in the embodiment of FIG. 1.
2 shows other modified examples of . In addition, impedance conversion can be performed using Tch as well as general impedance conversion.
It may also be realized by an ebysheH III number or the like.
1艶立皇j
叙上の如く、本発明によれば、極めて簡単な構成にて同
軸線路と導波管との間のインピーダンス整合が広い周波
数帯域に亘って可能となるので、電力分配特性を広帯域
とすることができるという効果がある。As mentioned above, according to the present invention, impedance matching between the coaxial line and the waveguide can be achieved over a wide frequency band with an extremely simple configuration, so that the power distribution characteristics can be improved. This has the effect of providing a wide band.
第1図〜第11図は本発明の各実施例を夫々示す図、第
12図は従来技術を説明する一部破断面を含む斜視図、
第13図は同軸線路断面図、第14図は導波管断面図、
第15図は同軸線路の中心導体端子からみた等価回路図
である。
主要部分の符号の説明
1・・・・・・方形導波管
2・・・・・・同軸線路中心導体
4・・・・・・同軸線路外導体
5・・・・・・導体板FIGS. 1 to 11 are views showing each embodiment of the present invention, and FIG. 12 is a perspective view including a partially broken surface explaining the prior art.
Figure 13 is a cross-sectional view of the coaxial line, Figure 14 is a cross-sectional view of the waveguide,
FIG. 15 is an equivalent circuit diagram seen from the center conductor terminal of the coaxial line. Explanation of symbols of main parts 1... Rectangular waveguide 2... Coaxial line center conductor 4... Coaxial line outer conductor 5... Conductor plate
Claims (1)
導波管のH面に平行に設けられた導体板と、外導体が前
記導波管のE面に接続され中心導体が前記導体板に接続
された同軸線路とにより構成された電力分配回路であつ
て、前記同軸線路の中心導体と前記導体板との接続部分
にインピーダンストランスフォーマを設けたことを特徴
とする電力分配回路。A rectangular waveguide, a conductor plate provided parallel to the H-plane of the waveguide to divide the inside of the rectangular waveguide, and an outer conductor connected to the E-plane of the waveguide and a center conductor. A power distribution circuit comprising a coaxial line connected to the conductor plate, the power distribution circuit comprising an impedance transformer at a connection portion between the center conductor of the coaxial line and the conductor plate.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15018886A JPS636904A (en) | 1986-06-26 | 1986-06-26 | Power distribution circuit |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15018886A JPS636904A (en) | 1986-06-26 | 1986-06-26 | Power distribution circuit |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS636904A true JPS636904A (en) | 1988-01-12 |
Family
ID=15491437
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP15018886A Pending JPS636904A (en) | 1986-06-26 | 1986-06-26 | Power distribution circuit |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS636904A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6897739B2 (en) * | 2003-03-13 | 2005-05-24 | Northrop Grumman Corporation | Waveguide power divider and combiner utilizing a resistive slot |
JP2009210393A (en) * | 2008-03-04 | 2009-09-17 | Nec Corp | Load pull measuring fixture |
-
1986
- 1986-06-26 JP JP15018886A patent/JPS636904A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6897739B2 (en) * | 2003-03-13 | 2005-05-24 | Northrop Grumman Corporation | Waveguide power divider and combiner utilizing a resistive slot |
JP2009210393A (en) * | 2008-03-04 | 2009-09-17 | Nec Corp | Load pull measuring fixture |
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