JPH0434564Y2 - - Google Patents
Info
- Publication number
- JPH0434564Y2 JPH0434564Y2 JP15521287U JP15521287U JPH0434564Y2 JP H0434564 Y2 JPH0434564 Y2 JP H0434564Y2 JP 15521287 U JP15521287 U JP 15521287U JP 15521287 U JP15521287 U JP 15521287U JP H0434564 Y2 JPH0434564 Y2 JP H0434564Y2
- Authority
- JP
- Japan
- Prior art keywords
- waveguide
- cylindrical
- flexible
- waveguides
- 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
Links
- 230000005684 electric field Effects 0.000 description 4
- 238000010586 diagram Methods 0.000 description 3
- 238000003780 insertion Methods 0.000 description 3
- 230000037431 insertion Effects 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 1
Landscapes
- Waveguides (AREA)
Description
【考案の詳細な説明】
〔産業上の利用分野〕
本考案はマイクロ波用導波管に関し、詳しくは
トラツプされるTE11oモードの共振周波数を使用
帯域から外すようにした円筒可撓導波管に関す
る。[Detailed description of the invention] [Field of industrial application] The present invention relates to a microwave waveguide, and more specifically, a cylindrical flexible waveguide that excludes the resonant frequency of the trapped TE 11o mode from the operating band. Regarding.
導波管を形状から大別すると、矩形導波管と円
筒導波管があり、各々には可撓導波管と非可撓導
波管がある。第4図a,b及び第5図は従来の導
波管の例を示す図である。
Waveguides can be broadly classified into rectangular waveguides and cylindrical waveguides, and each type includes flexible waveguides and non-flexible waveguides. FIGS. 4a and 4b and FIG. 5 are diagrams showing examples of conventional waveguides.
第4図a,bでは、両端部に矩形導波管2,
2′を有する可撓円筒導波管1に円筒−矩形導波
管変換器3が形成されている。また、第5図で
は、円筒可撓導波管1′がn・λg/2の長さに
形成され、(n:整数、λg:管内波長)、該円筒
可撓部分がn・λg/2の変成器となり整合をと
るようになつている。 In Figures 4a and 4b, rectangular waveguides 2,
A cylindrical-to-rectangular waveguide converter 3 is formed in a flexible cylindrical waveguide 1 having a diameter 2'. In addition, in FIG. 5, the cylindrical flexible waveguide 1' is formed to have a length of n·λg/2 (n: integer, λg: wavelength in the tube), and the cylindrical flexible portion is n·λg/2. It is designed to be a transformer for matching.
これら円筒可撓導波管1,1′はTE11モード、
矩形導波管2,2′はTE10モードにてマイクロ波
を伝送する。 These cylindrical flexible waveguides 1, 1' have TE 11 mode,
The rectangular waveguides 2, 2' transmit microwaves in TE 10 mode.
円筒可撓導波管を矩形可撓導波管と比較する
と、
機械的に強度である。 When comparing a cylindrical flexible waveguide with a rectangular flexible waveguide, it is mechanically stronger.
製作が容易である。 Easy to manufacture.
第3図bに示すようにあらゆる方向へ曲げる
ことができる。(矩形導波管では第3図aに示
すように矩形導波管の面と交差する方向に限定
される)。 It can be bent in any direction as shown in Figure 3b. (For a rectangular waveguide, it is limited to the direction intersecting the plane of the rectangular waveguide, as shown in FIG. 3a).
等の長所を有する。It has the following advantages.
また、第4図a,b及び第5図のように両端部
に矩形導波管有する可撓円筒導波管では出入口部
においてマイクロ波電界が一定方向となるので使
用上都合がよい。 Further, in a flexible cylindrical waveguide having rectangular waveguides at both ends as shown in FIGS. 4a, b and 5, the microwave electric field is in a fixed direction at the entrance and exit, which is convenient for use.
ところが、円筒可撓導波管は上記長所を有する
反面、曲げると第2図aで示すTE11oモードが励
振される。このTE11oモードは、遮断波長λcが第
2図bのTE11モードと同じで、電界方向がTE11
モードと直交する。なお、第2図a,bの図中の
点線矢印は電気力線を示す。上記TE11oモードは
例えば第4図a,b及び第5図の円筒可撓導波管
1,1′では遮断されることなく伝送されるが、
矩形導波管2,2′とは結合しないため、円筒可
撓導波管1,1′にトラツプされ、その間で共振
を起こす。そして、その共振周波数が使用帯域
に入るとマイクロ波損失の増大或いは導波管1,
1′でのマイクロ波電界の増大による放電等の現
象を引き起こし、導波管1,1′の使用が耐えら
れなくなる。
However, although the cylindrical flexible waveguide has the above-mentioned advantages, when it is bent, the TE 11o mode shown in FIG. 2a is excited. This TE 11o mode has the same cutoff wavelength λ c as the TE 11 mode shown in Figure 2b, and the electric field direction is TE 11
Orthogonal to the mode. Note that dotted arrows in FIGS. 2a and 2b indicate lines of electric force. The above-mentioned TE 11o mode is transmitted without being interrupted in the cylindrical flexible waveguides 1 and 1' shown in FIGS. 4a, b and 5, for example.
Since it is not coupled to the rectangular waveguides 2 and 2', it is trapped in the cylindrical flexible waveguides 1 and 1', causing resonance between them. When the resonant frequency enters the usage band, the microwave loss increases or the waveguide 1,
The increase in the microwave electric field at waveguide 1' causes phenomena such as discharge, and the use of waveguides 1 and 1' becomes unbearable.
そこで、この共振周波数を使用帯域から外す
ためには、円筒可撓導波管1,1′の長さlを調
整しなければならない。しかし、そのための設計
は円筒可撓導波管1,1′の管内波長λg、円筒
−矩形導波管変換器3の接合部の容量等の評価が
難しく、試行錯誤的に行なわざるを得ず、極めて
非能率的であつた。 Therefore, in order to remove this resonant frequency from the usable band, the length l of the cylindrical flexible waveguides 1 and 1' must be adjusted. However, this design has to be done by trial and error because it is difficult to evaluate the internal wavelength λg of the cylindrical flexible waveguides 1, 1', the capacity of the junction of the cylindrical-rectangular waveguide converter 3, etc. , was extremely inefficient.
本考案は上述の如き事情に鑑みてなされたもの
で導波管にトラツプされるTE11oモードの共振周
波数を使用帯域から極めて容易に外すことを可
能とした円筒可撓導波管を提供することである。 The present invention was made in view of the above-mentioned circumstances, and it is an object of the present invention to provide a cylindrical flexible waveguide that makes it possible to extremely easily remove the resonance frequency of the TE 11o mode trapped in the waveguide from the operating band. It is.
このために本考案のマイクロ波用導波管は、両
端に矩形導波管を有する円筒可撓導波管におい
て、
上記円筒可撓導波管の入口部又は出口部に、該
管内を伝送するTE11モードの電気力線と交差す
るように共振周波数調整ポストを取付けて構成し
た。
For this purpose, the microwave waveguide of the present invention is a cylindrical flexible waveguide having rectangular waveguides at both ends, and the microwave is transmitted through the tube to the entrance or exit of the cylindrical flexible waveguide. A resonant frequency adjustment post was installed to intersect the TE 11 mode electric field lines.
以下、本考案の実施例の円筒可撓導波管につい
て説明する。第1図において、4は左右両端部に
矩形導波管5,5′が連結された可撓円筒導波管
で、その入口部4aには内側に突出する共振周波
数調整ポスト6が取付けられている。該調整ポス
ト6は、TE11oモードの電気力線に対しては平行
に、伝送モードであるTE11モードの電気力線に
対しては交差(直交)するように配向され、その
挿入長hが調整できるように装着されている。
Hereinafter, a cylindrical flexible waveguide according to an embodiment of the present invention will be described. In FIG. 1, reference numeral 4 denotes a flexible cylindrical waveguide with rectangular waveguides 5, 5' connected to both left and right ends, and a resonant frequency adjustment post 6 protruding inward is attached to the entrance portion 4a of the flexible cylindrical waveguide. There is. The adjustment post 6 is oriented parallel to the lines of electric force in the TE 11o mode and intersects (orthogonal to) the lines of electric force in the TE 11 mode, which is the transmission mode, and its insertion length h is It is installed so that it can be adjusted.
このように装着された調整ポスト6はTE11モ
ードにはほとんど影響を与えない。そして、ポス
ト6の挿入長hを変化させることにより、並列ア
ドミツタンスを変化させ、共振周波数r値を大き
く変化させることができる。 The adjustment post 6 mounted in this manner has almost no effect on the TE 11 mode. By changing the insertion length h of the post 6, the parallel admittance can be changed and the value of the resonant frequency r can be greatly changed.
この共振周波数rについては、設計段階で特に
考慮する必要はなく、製作後にポスト6の挿入長
hを変えることにより共振周波数rを可撓円筒導
波管4の使用帯域から外すことができる。 This resonant frequency r does not need to be particularly considered at the design stage, and by changing the insertion length h of the post 6 after manufacture, the resonant frequency r can be removed from the usable band of the flexible cylindrical waveguide 4.
なお、調整ポスト6の取付位置は可撓円筒導波
管4の出口部4bでもよい。 Note that the adjustment post 6 may be installed at the outlet portion 4b of the flexible cylindrical waveguide 4.
以上から本考案によれば、円筒可撓導波管の入
口部又は出口部に共振周波数調整ポストを取付け
たので、円筒可撓導波管の設計を複雑化させるこ
となく、また、煩雑な操作を要しないで、共振周
波数を可撓円筒導波管の使用帯域から外すことが
容易にできる。
From the above, according to the present invention, since the resonant frequency adjustment post is attached to the inlet or outlet of the cylindrical flexible waveguide, it is possible to avoid complicating the design of the cylindrical flexible waveguide, and to avoid complicated operations. The resonant frequency can be easily removed from the usage band of the flexible cylindrical waveguide.
第1図aは本考案の実施例の導波管の正面図、
第1図bはその断面図、第2図aはTE11oモード
が励振された導波管の断面図、第2図bはTE11
モードが励振された導波管の断面図、第3図aは
矩形可撓導波管の説明図、第3図bは円筒可撓導
波管の説明図、第4図a,bは従来の円筒可撓導
波管の正面図、第5図は従来の他の円筒可撓導波
管の正面図である。
4……可撓円筒導波管、4a……入口部、4b
……出口部、5,5′……矩形導波管、6……共
振周波数調整ポスト。
FIG. 1a is a front view of a waveguide according to an embodiment of the present invention;
Figure 1b is a cross-sectional view of the waveguide, Figure 2a is a cross-sectional view of the waveguide in which the TE 11o mode is excited, and Figure 2b is the TE 11
A cross-sectional view of the waveguide in which the mode is excited, Figure 3a is an explanatory diagram of a rectangular flexible waveguide, Figure 3b is an explanatory diagram of a cylindrical flexible waveguide, and Figures 4a and b are conventional FIG. 5 is a front view of another conventional cylindrical flexible waveguide. 4... Flexible cylindrical waveguide, 4a... Inlet section, 4b
...Exit part, 5, 5'...Rectangular waveguide, 6...Resonance frequency adjustment post.
Claims (1)
おいて、 上記円筒可撓導波管の入口部又は出口部に、
該管内を伝送するTE11モードの電気力線と交
差するように共振周波数調整ポストを取付けて
構成したことを特徴とするマイクロ波用導波
管。 (2) 上記共振周波数調整ポストを、上記円筒可撓
導波管内に突出する調整可能な棒状体で形成し
たことを特徴とする実用新案登録請求の範囲第
1項記載のマイクロ波用導波管。[Claims for Utility Model Registration] (1) In a cylindrical flexible waveguide having rectangular waveguides at both ends, at the entrance or exit of the cylindrical flexible waveguide,
A waveguide for microwaves, characterized in that a resonant frequency adjustment post is attached so as to intersect the lines of electric force of the TE 11 mode transmitted inside the pipe. (2) The microwave waveguide according to claim 1, wherein the resonant frequency adjustment post is formed of an adjustable rod-shaped body protruding into the cylindrical flexible waveguide. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15521287U JPH0434564Y2 (en) | 1987-10-09 | 1987-10-09 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15521287U JPH0434564Y2 (en) | 1987-10-09 | 1987-10-09 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0159303U JPH0159303U (en) | 1989-04-13 |
| JPH0434564Y2 true JPH0434564Y2 (en) | 1992-08-18 |
Family
ID=31432640
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15521287U Expired JPH0434564Y2 (en) | 1987-10-09 | 1987-10-09 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0434564Y2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP6707889B2 (en) * | 2016-02-17 | 2020-06-10 | 日立金属株式会社 | Waveguide communication system |
-
1987
- 1987-10-09 JP JP15521287U patent/JPH0434564Y2/ja not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0159303U (en) | 1989-04-13 |
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