JPH0244901A - Waveguide low pass filter - Google Patents
Waveguide low pass filterInfo
- Publication number
- JPH0244901A JPH0244901A JP19673088A JP19673088A JPH0244901A JP H0244901 A JPH0244901 A JP H0244901A JP 19673088 A JP19673088 A JP 19673088A JP 19673088 A JP19673088 A JP 19673088A JP H0244901 A JPH0244901 A JP H0244901A
- Authority
- JP
- Japan
- Prior art keywords
- waveguide
- flange
- pass filter
- harmonic
- standard
- 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
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、マイクロ波及びミリ波に使用される導波管低
域通過フィルタに関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a waveguide low-pass filter used for microwaves and millimeter waves.
従来の導波管低域通過フィルタは、マイクロ波及びミリ
波の基本周波数伝送帯域の例えば第2゜第3高調波等の
伝搬を阻止するために、導波管のE面方向の寸法を小さ
くし、かつ、この部分にE面の寸法を周期的に変化させ
て第2.第3の高調波を阻止し、この阻止領域より低い
周波数領域を基本周波数の通過領域とする導波管低域通
過フィルタが知られている。例えば電子通信学会編、電
子通信ハンドブック、第755頁オーム社(昭和54年
)参照。Conventional waveguide low-pass filters reduce the dimension of the waveguide in the E-plane direction in order to block the propagation of, for example, the 2nd and 3rd harmonics in the fundamental frequency transmission band of microwaves and millimeter waves. Then, the dimension of the E surface is periodically changed in this part to form the second. A waveguide low-pass filter is known that blocks the third harmonic and uses a frequency region lower than the third harmonic as a fundamental frequency pass region. For example, see Electronic Communication Handbook, edited by the Institute of Electronics and Communication Engineers, p. 755, Ohmsha (1978).
一方、この低域通過フィルタの前後に接続される入出力
導波管は標準導波管(例えばH面寸法とE面寸法の比が
2:1の導波管)で構成されるのが一般的である。しか
し、低域通過フィルタと標準導波管の入出力導波管とを
直接接続した場合インピーダンス不整合が生しる。イン
ピーダンス整合をとるためインピーダンス変換用の導波
管を有する構造となっていた。したかって、インピータ
ンス変換用の導波管を含め多くの導波管回路をフランジ
により接続していた。On the other hand, the input/output waveguides connected before and after this low-pass filter are generally constructed of standard waveguides (for example, waveguides with a ratio of H-plane dimensions to E-plane dimensions of 2:1). It is true. However, when the low-pass filter and the input/output waveguide of the standard waveguide are directly connected, an impedance mismatch occurs. The structure had a waveguide for impedance conversion to achieve impedance matching. Therefore, many waveguide circuits, including waveguides for impedance conversion, have been connected by flanges.
上述した従来の導波管低域通過フィルタは、低域通過フ
ィルタ部と、それに接続される入出力導波管とのインピ
ータンス整合をとるためのインピータンス変換部を含む
導波管低域通過フィルタの全長がインピーダンス変換部
の寸法分長くなり、又多数のフランジで接続しなければ
ならず、接続箇所1重量が増加するという欠点があった
。The conventional waveguide low-pass filter described above includes a low-pass filter section and an impedance conversion section for impedance matching between the input and output waveguides connected to the low-pass filter section. The overall length of the filter becomes longer by the dimension of the impedance converter, and it has to be connected with a large number of flanges, which has the disadvantage that the weight of each connection point increases.
本発明の目的は、標準導波管の2個のフランジに高調波
を開止する機能とインピータンス整合をとる機能とを組
込んだ小形で軽量な導波管低域通過フィルタを提供する
ことにある。An object of the present invention is to provide a small and lightweight waveguide low-pass filter that incorporates a harmonic blocking function and an impedance matching function into two flanges of a standard waveguide. It is in.
本発明の導波管低域通過フィルタは基本モードを伝搬す
る2個の導波管を接続する第1および第2のフランジの
それぞれにE面およびH面寸法を短縮した共振窓を設け
、この2つの共振窓の間に位置するE面方向の凹部を前
記第1または第2のフランジに設けている。The waveguide low-pass filter of the present invention has resonance windows with shortened E-plane and H-plane dimensions on each of the first and second flanges that connect two waveguides that propagate the fundamental mode. A recess in the E-plane direction located between the two resonance windows is provided in the first or second flange.
次にこの発明の一実施例を図面を用いて説明する。第1
図、第2図は、本発明の一実施例を構成する2個のフラ
ンジのそれぞれの正面図で、2個の導波管のそれぞれの
フランジ面から見た図である。第3図(a>、(b)は
本実施例の断面図てあり、第3図(a)は第1図および
第2図のAA縦断面図(E面の断面図)、第3図(1〕
)は第1図および第2図のB−B横断面図(H面断面図
)を示しており、両図面共に2個の導波管を接続した状
態を示している。Next, one embodiment of the present invention will be described with reference to the drawings. 1st
FIG. 2 is a front view of two flanges constituting an embodiment of the present invention, as viewed from the flange surfaces of two waveguides. 3(a) and 3(b) are cross-sectional views of this embodiment, and FIG. 3(a) is an AA vertical cross-sectional view (cross-sectional view of plane E) of FIGS. 1 and 2, and FIG. (1)
) shows a BB cross-sectional view (H-plane cross-sectional view) of FIGS. 1 and 2, and both drawings show a state in which two waveguides are connected.
導波管1と導波管5とはE面の寸法とH面の寸法か同一
の標準導波管であり、それぞれ阻止フィルタ付フランジ
2,3、共振窓イ」フランジ4を有している。導波管1
から基本周波数で基本モー1〜であるTE、oモードの
マイクロ波と基本周波数の例えば第2高調波を入力する
。まず、第3図(a)に示す阻止フィルタイイフランシ
2の共振窓3は、導波管1の標準寸法のH面寸法7を狭
くしてH面寸法8を形成し、第2高調波の高次モートの
発生を抑圧している。このH面寸法7とH面寸法8の不
連続により等測的に容量性サセプタンスとなるのて、こ
れを打消すための第3図(b )に示す誘導性サセプタ
ンスを有する誘導部8を形成してインピーダンス整合を
とっている。さらに、共振窓3の背面に共振窓付フラン
ジ4を接続した状態でE面とH面に対して凹部を形成し
、第2高調波を反射させている。この凹部の寸法は後述
する第2高調波の減衰特性を測定しながら決定される。The waveguide 1 and the waveguide 5 are standard waveguides with the same E-plane dimensions and H-plane dimensions, and each has flanges 2 and 3 with blocking filters and a resonant window I' flange 4. . waveguide 1
TE and o mode microwaves having fundamental frequencies of fundamental frequencies 1 to 1 and, for example, second harmonics of the fundamental frequencies are input. First, the resonant window 3 of the blocking filter efficiency 2 shown in FIG. It suppresses the generation of higher-order motes. This discontinuity between the H-plane dimension 7 and the H-plane dimension 8 results in isometric capacitive susceptance, and in order to cancel this, an inductive part 8 having an inductive susceptance as shown in FIG. 3(b) is formed. impedance matching is achieved. Furthermore, with the resonant window flange 4 connected to the back surface of the resonant window 3, recesses are formed on the E and H surfaces to reflect the second harmonic. The dimensions of this recess are determined while measuring the attenuation characteristics of the second harmonic, which will be described later.
また、共振窓付フランジ4の共振窓6は前述の共振窓3
と同様の機能と寸法を有している。このように、阻止フ
ィルタ付フランジ2と共振窓付フランジ4とが接続され
て、高調波阻止と基本波に対するインピーダンス整合が
実現てきる。例えは、第4図(a)、(b)の特性図の
それぞれに示すように、23.6 G Hzの第2高調
波に対して減衰し、11.8GHzの基本波に対して低
損失特性を有する導波管低域通過フィルタが得られる。Further, the resonant window 6 of the resonant window flange 4 is the resonant window 3 described above.
It has similar features and dimensions. In this way, the flange 2 with a blocking filter and the flange 4 with a resonance window are connected, and harmonic blocking and impedance matching for the fundamental wave are realized. For example, as shown in the characteristic diagrams in Figure 4 (a) and (b), the second harmonic of 23.6 GHz is attenuated, and the fundamental wave of 11.8 GHz has low loss. A waveguide low-pass filter having the following characteristics is obtained.
以上説明したように、本発明によれは導波管低域通過フ
ィルタが導波管フランジに組み込まれているため、その
重量および接続箇所が大幅に減少される。また、導波管
低域通過フィルタか2個のフランジに分割されているこ
とから製作、加工か容易となる効果がある。As explained above, according to the present invention, since the waveguide low-pass filter is incorporated into the waveguide flange, its weight and connection points are significantly reduced. Furthermore, since the waveguide low-pass filter is divided into two flanges, it has the advantage of being easy to manufacture and process.
第1図、第2図は本発明の一実施例の正面図、第3図(
a)、(b)は本実施例のそれぞれ縦断面図と横断面図
、第4図(a)、(b)は本実施例の特性図である。
1.5・・・導波管、2・・・阻止フィルタ付フランジ
、3.6・・・共振窓、4・・共振窓付フランジ、7,
8・・H面寸法、9・・・誘導部。Figures 1 and 2 are front views of one embodiment of the present invention, and Figure 3 (
4(a) and 4(b) are a longitudinal cross-sectional view and a cross-sectional view, respectively, of this embodiment, and FIGS. 4(a) and 4(b) are characteristic diagrams of this embodiment. 1.5...Waveguide, 2...Flange with blocking filter, 3.6...Resonance window, 4...Flange with resonance window, 7,
8...H surface dimension, 9...Guidance part.
Claims (1)
び第2のフランジのそれぞれにE面およびH面寸法を短
縮した共振窓を設け、この2つの共振窓の間に位置する
E面方向の凹部を前記第1または第2のフランジに設け
たことを特徴とする導波管低域通過フィルタ。A resonance window with shortened E-plane and H-plane dimensions is provided on each of the first and second flanges that connect two waveguides that propagate the fundamental mode, and an E-plane located between the two resonance windows is provided. A waveguide low-pass filter characterized in that a recess in the direction is provided in the first or second flange.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19673088A JPH0244901A (en) | 1988-08-05 | 1988-08-05 | Waveguide low pass filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19673088A JPH0244901A (en) | 1988-08-05 | 1988-08-05 | Waveguide low pass filter |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0244901A true JPH0244901A (en) | 1990-02-14 |
Family
ID=16362638
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19673088A Pending JPH0244901A (en) | 1988-08-05 | 1988-08-05 | Waveguide low pass filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0244901A (en) |
-
1988
- 1988-08-05 JP JP19673088A patent/JPH0244901A/en active Pending
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