JPS59185402A - Waffle iron type filter - Google Patents
Waffle iron type filterInfo
- Publication number
- JPS59185402A JPS59185402A JP5955883A JP5955883A JPS59185402A JP S59185402 A JPS59185402 A JP S59185402A JP 5955883 A JP5955883 A JP 5955883A JP 5955883 A JP5955883 A JP 5955883A JP S59185402 A JPS59185402 A JP S59185402A
- Authority
- JP
- Japan
- Prior art keywords
- bosses
- wave
- order mode
- resonance
- mode wave
- 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
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
- H01P1/207—Hollow waveguide filters
- H01P1/211—Waffle-iron filters; Corrugated structures
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は方形導波管の幅広面の内壁に複数のボスを設
けたワツフルアイアン形ろ波器に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a Watsuful iron wave filter in which a plurality of bosses are provided on the inner wall of the wide side of a rectangular waveguide.
まず、第1図に示す従来のワツフルアイアン形ろ波器に
ついて簡単に説明する。第1図(a)はワツフルアイア
ン形ろ波器の部分切欠き斜視図、同図(b)は正面図で
ある。図中(1)は方形導波管、(2)は方形導波管(
1)の幅広面の内壁に設けた断面形状と高さの等しいボ
スである。First, the conventional Watsuful iron filter shown in FIG. 1 will be briefly explained. FIG. 1(a) is a partially cutaway perspective view of a Watsuful iron filter, and FIG. 1(b) is a front view. In the figure, (1) is a rectangular waveguide, and (2) is a rectangular waveguide (
This is a boss with the same height as the cross-sectional shape provided on the inner wall of the wide surface of 1).
このような構造のワツフルアイアン形ろ波器では、ボス
(2)の効果により波長が短縮されるためしゃ断層波数
が下がり、高次モード波が伝搬可能となる。In the Watsuful iron filter having such a structure, the wavelength is shortened by the effect of the boss (2), so the cutoff wave number is lowered, and higher-order mode waves can propagate.
従って、ろ波器の製作時にボス(2)の精度不足。Therefore, the boss (2) lacks precision when manufacturing the filter.
左右の非対称などが生じた場合には高次モード波が発生
して伝搬する。この高次モード波はう波器の両端に接続
される導波管でしゃ断となって反射され、ボス(2)の
形状、ろ波器の軸長で決まる周波数で閉じ込め共振を起
こす。When left-right asymmetry occurs, higher-order mode waves are generated and propagated. This higher-order mode wave is blocked and reflected by the waveguides connected to both ends of the filter, causing confined resonance at a frequency determined by the shape of the boss (2) and the axial length of the filter.
従来のワツフルアイアン形ろ波器では、この閉じ込め共
振が通過帯域内に生じた場合、ろ波器の特性を変化させ
ずに共振周波数を通過帯域外にすることができないとい
う欠点があった。Conventional Watsuful iron filters have the disadvantage that when this confined resonance occurs within the passband, the resonant frequency cannot be moved outside the passband without changing the characteristics of the filter.
この発明はこれらの欠点を除去するために、ボスの高さ
を不均一にしたもので、以下図面について詳細に説明す
る。In order to eliminate these drawbacks, the present invention makes the height of the boss non-uniform, and will be described in detail below with reference to the drawings.
第2図はこの発明の一実施例であり、同図(a)は部分
切欠き斜視図、同図(b)は正面図である。図中(1)
は方形導波管、(3)は必要なろ波特性を与える高さの
ボス、(4)はボス(3)とは高さの異るボスである。FIG. 2 shows an embodiment of the present invention, in which FIG. 2(a) is a partially cutaway perspective view and FIG. 2(b) is a front view. (1) in the diagram
is a rectangular waveguide, (3) is a boss with a height that provides the necessary filtering characteristics, and (4) is a boss with a different height from boss (3).
ボス(3)は方形導波管(1)の中央付近に、ボス(4
)は方形導波管(1)の幅の狭い面に近い位置に設げら
れている。The boss (3) is located near the center of the rectangular waveguide (1).
) is provided close to the narrow surface of the rectangular waveguide (1).
ボス(4)の位置では基本モード波の電界が小さいので
、ボス(4)はろ波器の通過特性にほとんど影響を与え
ない。しかし、高次モード波の電界はボス(4)の位置
では基本モード波の電界より太きいため波長短縮率が大
きくなり、高次モード波の共振周波数が大きく変化する
。従って、高次モード波による不要な共振を使用帯域外
にすることができ。Since the electric field of the fundamental mode wave is small at the position of the boss (4), the boss (4) has little effect on the passage characteristics of the filter. However, since the electric field of the higher-order mode wave is thicker than the electric field of the fundamental mode wave at the position of the boss (4), the wavelength shortening rate increases, and the resonant frequency of the higher-order mode wave changes significantly. Therefore, unnecessary resonance due to higher-order mode waves can be removed from the usable band.
良好な通過特性が得られるという利点がある。This has the advantage of providing good transmission characteristics.
第3図はこの発明の他の実施例であり、同図(a)は部
分切欠き斜視図、同図(b)は正面図である。図中(1
)〜(4)は第2図と同じものである。FIG. 3 shows another embodiment of the present invention, in which FIG. 3(a) is a partially cutaway perspective view and FIG. 3(b) is a front view. In the figure (1
) to (4) are the same as in FIG.
ボス(4)は方形導波管(1)の幅の狭い面に近い位置
に4個だけ設けられている。Only four bosses (4) are provided at positions close to the narrow side of the rectangular waveguide (1).
この場合はボス(4)が高次モード波に対して集中定数
的なキャパシタンスとして働き、高次モード波の共振周
波数を変化させる。従って、第2図の場合と同様な利点
を有するが、第3図の場合は第2図の場合よりも共振周
波数の変化が小さいので閉じ込め共振の周波数を微調整
する場合に有効である。In this case, the boss (4) acts as a lumped constant capacitance for the higher-order mode waves, changing the resonance frequency of the higher-order mode waves. Therefore, although it has the same advantages as the case in FIG. 2, the change in the resonance frequency is smaller in the case in FIG. 3 than in the case in FIG. 2, so it is effective in finely adjusting the frequency of confined resonance.
なお9以上は角柱のボスを用いた場合について説明した
が、この発明はこれに限らず円柱のボスを用いた場合に
使用してもよい。Note that although the case in which a prismatic boss is used has been described in 9 and above, the present invention is not limited to this and may be used in a case where a cylindrical boss is used.
以上のようにこの発明に係るワツフルアイアン形ろ波器
では、ボスの高さを不均一にすることによって基本モー
ド波の通過特性にはほとんど影響をおよぼすことなく高
次モード波による共振を使用帯域外にすることができる
という利点がある。As described above, in the Watsuful iron filter according to the present invention, by making the height of the bosses non-uniform, resonance by higher-order mode waves is used with almost no effect on the passage characteristics of fundamental mode waves. It has the advantage of being able to go out of band.
第1図は従来のワツフルアイアン形ろ波器を示す図であ
り、同図(a)は部分切欠き斜視図、同図(b)は正面
図、第2図はこの発明の一実施例を示す図であり、同図
(a)は部分切欠き斜視図、同図(b)は正面図である
。第3図はこの発明の他の一実施例を示す図であり、同
図(a)は部分切欠き斜視図、同図(b)は正面図であ
る。
図中、(1)は方形導波管、(2)は断面形状と高さの
等しいボス、(3)は必要なろ波特性を与える高さのボ
ス、(4)はボス(3)とは高さの異るボスである。
なお9図中、同一あるいは相当部分には同一符号を付し
て示しである。
代理人大岩増雄
第1図
CI:))
第2図
rb)
第3図
(b)Fig. 1 is a diagram showing a conventional Watsuful iron filter, in which Fig. 1(a) is a partially cutaway perspective view, Fig. 2(b) is a front view, and Fig. 2 is an embodiment of the present invention. FIG. 3A is a partially cutaway perspective view, and FIG. 1B is a front view. FIG. 3 is a diagram showing another embodiment of the present invention, in which FIG. 3(a) is a partially cutaway perspective view and FIG. 3(b) is a front view. In the figure, (1) is a rectangular waveguide, (2) is a boss with the same cross-sectional shape and height, (3) is a boss with a height that provides the necessary filtering characteristics, and (4) is boss (3). are bosses of different heights. In FIG. 9, the same or corresponding parts are designated by the same reference numerals. Agent Masuo Oiwa Figure 1 CI:)) Figure 2 rb) Figure 3 (b)
Claims (1)
ボスを設けたワツフルアイアン形ろ波器において、上記
ボスの高さを不均一にしたことを特徴とするワツフルア
イアン形ろ波器。A Watsuful iron filter in which a plurality of prismatic or cylindrical bosses are provided on the inner wall of a wide surface of a rectangular waveguide, characterized in that the heights of the bosses are uneven. vessel.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5955883A JPS59185402A (en) | 1983-04-05 | 1983-04-05 | Waffle iron type filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5955883A JPS59185402A (en) | 1983-04-05 | 1983-04-05 | Waffle iron type filter |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59185402A true JPS59185402A (en) | 1984-10-22 |
Family
ID=13116695
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5955883A Pending JPS59185402A (en) | 1983-04-05 | 1983-04-05 | Waffle iron type filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59185402A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP3147994A1 (en) * | 2015-09-24 | 2017-03-29 | Gapwaves AB | Waveguides and transmission lines in gaps between parallel conducting surfaces |
-
1983
- 1983-04-05 JP JP5955883A patent/JPS59185402A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP3147994A1 (en) * | 2015-09-24 | 2017-03-29 | Gapwaves AB | Waveguides and transmission lines in gaps between parallel conducting surfaces |
WO2017050817A1 (en) * | 2015-09-24 | 2017-03-30 | Gapwaves Ab | Waveguides and transmission lines in gaps between parallel conducting surfaces |
CN108432037A (en) * | 2015-09-24 | 2018-08-21 | 加普韦夫斯公司 | Waveguide in gap between parallel conductive surfaces and transmission line |
US10892536B2 (en) | 2015-09-24 | 2021-01-12 | Gapwaves Ab | Waveguides and transmission lines in gaps between parallel conducting surfaces |
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