JPH07154101A - Low pass filter - Google Patents

Low pass filter

Info

Publication number
JPH07154101A
JPH07154101A JP29638693A JP29638693A JPH07154101A JP H07154101 A JPH07154101 A JP H07154101A JP 29638693 A JP29638693 A JP 29638693A JP 29638693 A JP29638693 A JP 29638693A JP H07154101 A JPH07154101 A JP H07154101A
Authority
JP
Japan
Prior art keywords
pass filter
coaxial
low
low pass
section
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.)
Granted
Application number
JP29638693A
Other languages
Japanese (ja)
Other versions
JP2722166B2 (en
Inventor
Kiyotake Sasaki
清▲丈▼ 佐々木
Keiichi Umetsu
圭一 梅津
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Engineering Ltd
Original Assignee
NEC Engineering Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by NEC Engineering Ltd filed Critical NEC Engineering Ltd
Priority to JP5296386A priority Critical patent/JP2722166B2/en
Publication of JPH07154101A publication Critical patent/JPH07154101A/en
Application granted granted Critical
Publication of JP2722166B2 publication Critical patent/JP2722166B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To obtain the low pass filter with simple structure having a broad block band and excellent power resistant and general-purpose performance. CONSTITUTION:With a signal propagated to the low pass filter 1, the signal is propagated to a coaxial waveguide converter section 7a via a rectangular waveguide section 5a. The coaxial waveguide converter section 7a converts the mode of the signal propagated to the rectangular waveguide section 5 into the mode of a signal received by a coaxial low pass filter section 2. When the signal whose mode is converted by the coaxial waveguide converter section 7a is propagated to the coaxial low pass filter section 2, the coaxial low pass filter section 2 cuts off its high frequency component and provides a resulting output to a coaxial waveguide converter section 7b. The coaxial waveguide converter section 7b converts the mode of the signal outputted from the coaxial low pass filter section 2 into the mode of a signal propagated through a rectangular waveguide section 5b.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は低域通過ろ波器に関し、
特に広い阻止帯域を有しかつ耐電力性に優れた導波管型
低域通過ろ波器に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a low pass filter,
In particular, the present invention relates to a waveguide type low-pass filter having a wide stop band and excellent power resistance.

【0002】[0002]

【従来の技術】従来、この種の導波管型低域通過ろ波器
としては、コルゲート型とワッフルアイアン型とがあ
る。コルゲート型では矩形導波管の広幅面の電波伝搬方
向に沿って、その電波伝搬方向に直交する方向に延びる
隆起部と溝部とが交互に連続して設けられている。この
種のコルゲート型の低域通過ろ波器としては、特開昭6
3−166301号公報に開示された技術がある。
2. Description of the Related Art Heretofore, as a waveguide type low-pass filter of this type, there are a corrugated type and a waffle iron type. In the corrugated type, ridges and grooves extending in a direction orthogonal to the radio wave propagation direction are alternately and continuously provided along the radio wave propagation direction on the wide surface of the rectangular waveguide. A corrugated low pass filter of this type is disclosed in Japanese Patent Laid-Open No.
There is a technique disclosed in JP-A-3-166301.

【0003】また、ワッフルアイアン型は、図6に示す
ように、矩形導波管10の広幅面の電波伝搬方向及びこ
の電波伝搬方向に直交する方向に夫々沿って、隆起部1
1と溝部12とが交互に連続して設けられている。
Further, as shown in FIG. 6, the waffle iron type has a raised portion 1 along a radio wave propagation direction of a wide surface of a rectangular waveguide 10 and a direction orthogonal to the radio wave propagation direction.
1 and the groove part 12 are provided alternately and continuously.

【0004】この種のワッフルアイアン型の低域通過ろ
波器としては、実開昭57−202202号のマイクロ
フィルムや特開昭59−185403号公報に開示され
た技術がある。
As a waffle iron type low-pass filter of this type, there are the technique disclosed in Japanese Utility Model Laid-Open No. 57-202202 and Japanese Patent Laid-Open No. 59-185403.

【0005】[0005]

【発明が解決しようとする課題】上述した従来の導波管
型低域通過ろ波器では、矩形導波管の広幅面に隆起部と
溝部とを交互に連続して設けているので、構造が複雑と
なり、コスト高になるという問題がある。
In the above-mentioned conventional waveguide type low pass filter, since the ridges and the grooves are alternately and continuously provided on the wide surface of the rectangular waveguide, the structure is However, there is a problem that it becomes complicated and the cost becomes high.

【0006】特に、特開昭63−166301号公報に
開示されたコルゲート型の低域通過ろ波器や特開昭59
−185403号公報に開示されたワッフルアイアン型
の低域通過ろ波器のように隆起部の高さを2種類にした
場合や、あるいは実開昭57−202202号のマイク
ロフィルムに開示されたワッフルアイアン型の低域通過
ろ波器のように隆起部の形状を変えた場合にはさらに構
造が複雑となる。
In particular, the corrugated low-pass filter disclosed in JP-A-63-166301 and JP-A-59
Waffle iron type low pass filter disclosed in Japanese Patent No. 185403, in which the height of the ridge is two, or in the waffle disclosed in Japanese Utility Model Publication No. 57-202202. The structure becomes more complicated when the shape of the ridge is changed like an iron type low-pass filter.

【0007】また、低域通過ろ波器を構成する導波管内
の隆起部と溝部とにおける上下の一致度、つまり加工精
度がわずかでも悪いと、図7に示すように、阻止帯域内
に共振が生じ、スプリアス特性が悪くなるという問題が
ある。
Further, if the up-and-down degree of coincidence between the raised portion and the groove portion in the waveguide forming the low-pass filter, that is, the processing accuracy is slightly poor, resonance occurs in the stop band as shown in FIG. Occurs, and the spurious characteristics deteriorate.

【0008】さらに、広い阻止帯域を実現するために
は、低域通過ろ波器を構成する導波管内の隆起部におけ
る上下の間隔を非常に狭くする必要があるが、この間隔
を狭くすると高電力用には適さなくなるという問題があ
る。
Further, in order to realize a wide stop band, it is necessary to make the upper and lower intervals in the ridges in the waveguide forming the low-pass filter very narrow. There is a problem that it is not suitable for electric power.

【0009】さらにまた、低域通過ろ波器を構成する導
波管内の隆起部及び溝部の寸法によって周波数特性が決
定されるため、異なった特性が要求される場合には隆起
部及び溝部の寸法をその特性に応じて変更しなければな
らないが、それら隆起部及び溝部とからなる矩形導波管
の構造が複雑であるので、容易に変更することが難し
い。
Furthermore, since the frequency characteristics are determined by the dimensions of the ridges and grooves in the waveguide forming the low-pass filter, the dimensions of the ridges and grooves are required when different characteristics are required. Must be changed according to its characteristics, but it is difficult to change easily because the structure of the rectangular waveguide including the ridge and the groove is complicated.

【0010】そこで、本発明の目的は上記の問題点を解
消し、構造を簡単にすることができ、広い阻止帯域を有
しかつ耐電力性及び汎用性に優れた低域通過ろ波器を提
供することにある。
Therefore, an object of the present invention is to solve the above-mentioned problems and to provide a low-pass filter which has a simple structure, has a wide stop band, and is excellent in power resistance and versatility. To provide.

【0011】[0011]

【課題を解決するための手段】本発明による低域通過ろ
波器は、矩形導波管からなる低域通過ろ波器であって、
前記矩形導波管内に設けられかつ高周波成分を除去する
同軸低域通過ろ波器と、前記矩形導波管内に設けられか
つ前記同軸低域通過ろ波器への入出力信号のモードを変
換する同軸導波管変換器とを備えている。
A low pass filter according to the present invention is a low pass filter comprising a rectangular waveguide,
A coaxial low-pass filter provided in the rectangular waveguide and removing high frequency components, and a mode of an input / output signal to / from the coaxial low-pass filter provided in the rectangular waveguide. And a coaxial waveguide converter.

【0012】本発明による他の低域通過ろ波器は、上記
の構成のほかに、前記同軸低域通過ろ波器と前記同軸導
波管変換器との結合部分に設けられかつ前記同軸低域通
過ろ波器における高次モードの信号の発生を抑止するリ
ング部材を備えている。
In addition to the above structure, another low-pass filter according to the present invention is provided at a coupling portion between the coaxial low-pass filter and the coaxial waveguide converter and has the coaxial low-pass filter. A ring member for suppressing generation of higher-order mode signals in the pass filter is provided.

【0013】[0013]

【実施例】次に、本発明について図面を参照して説明す
る。
DESCRIPTION OF THE PREFERRED EMBODIMENTS Next, the present invention will be described with reference to the drawings.

【0014】図1は本発明の一実施例を示す構成図であ
る。図において、低域通過ろ波器1は同軸低域通過ろ波
器部2と、矩形導波管部5a,5bと、同軸導波管変換
器部7a,7bとから構成されている。
FIG. 1 is a block diagram showing an embodiment of the present invention. In the figure, a low-pass filter 1 comprises a coaxial low-pass filter section 2, rectangular waveguide sections 5a and 5b, and coaxial waveguide converter sections 7a and 7b.

【0015】同軸低域通過ろ波器部2は外導体3と、軸
径が細い軸径部分4aと軸径が太い軸径部分4bとがあ
る間隔で夫々複数個ずつ設けられた中心導体4とから構
成されている。ここで、中心導体4は矩形導波管部5
a,5bに夫々設けられたプローブ6a,6bに接着固
定されている。
The coaxial low-pass filter section 2 includes a plurality of outer conductors 3, a central shaft portion 4a having a small shaft diameter and a central shaft portion 4b having a large shaft diameter, and a plurality of central conductors 4 provided at intervals. It consists of and. Here, the central conductor 4 is the rectangular waveguide portion 5
It is adhered and fixed to probes 6a and 6b provided on a and 5b, respectively.

【0016】矩形導波管部5a,5bの一端には短絡面
が設けられており、また広幅面の中心にはプローブ6
a,6bが設けられている。尚、プローブ6a,6bは
中心導体4との結合部に発生する熱を矩形導波管部5
a,5bのケースに逃がす働きをする。
A short circuit surface is provided at one end of each of the rectangular waveguide portions 5a and 5b, and the probe 6 is provided at the center of the wide surface.
a and 6b are provided. It should be noted that the probes 6a and 6b apply heat generated at the joint with the central conductor 4 to the rectangular waveguide section 5.
It works to escape to the cases of a and 5b.

【0017】同軸導波管変換器部7a,7bは同軸低域
通過ろ波器部2と矩形導波管部5a,5bとの結合部
分、つまり同軸低域通過ろ波器部2の両端に夫々設けら
れ、中心導体4と矩形導波管部5a,5bとプローブ6
a,6bとによって形成されている。
The coaxial waveguide converter portions 7a and 7b are connected to the coaxial low-pass filter portion 2 and the rectangular waveguide portions 5a and 5b, that is, at both ends of the coaxial low-pass filter portion 2. The central conductor 4, the rectangular waveguide portions 5a and 5b, and the probe 6 are provided respectively.
It is formed by a and 6b.

【0018】低域通過ろ波器1に信号が伝搬されてくる
と、その信号は矩形導波管部5aを介して同軸導波管変
換器部7aに伝搬される。同軸導波管変換器部7aでは
矩形導波管部5aを伝搬される信号のモードを同軸低域
通過ろ波器部2に入力される信号のモードに変換する。
When a signal is propagated to the low pass filter 1, the signal is propagated to the coaxial waveguide converter portion 7a via the rectangular waveguide portion 5a. The coaxial waveguide converter unit 7a converts the mode of the signal propagated through the rectangular waveguide unit 5a into the mode of the signal input to the coaxial low-pass filter unit 2.

【0019】同軸低域通過ろ波器部2は同軸導波管変換
器部7aでモードが変換された信号が伝搬されてくる
と、その高周波成分を切って同軸導波管変換器部7bに
出力する。同軸導波管変換器部7bでは同軸低域通過ろ
波器部2から出力される信号のモードを、矩形導波管部
5bで伝搬される信号のモードに変換する。
When the signal whose mode has been converted by the coaxial waveguide converter portion 7a is propagated to the coaxial low-pass filter portion 2, the high-frequency component is cut off to the coaxial waveguide converter portion 7b. Output. The coaxial waveguide converter unit 7b converts the mode of the signal output from the coaxial low-pass filter unit 2 into the mode of the signal propagated by the rectangular waveguide unit 5b.

【0020】図2は図1の低域通過ろ波器1における周
波数と減衰量との関係を示す図である。図においては、
低域通過ろ波器1を通常の電力用に形成した場合の周波
数と減衰量との関係を示している。
FIG. 2 is a diagram showing the relationship between the frequency and the amount of attenuation in the low pass filter 1 of FIG. In the figure,
The relationship between the frequency and the attenuation when the low-pass filter 1 is formed for normal power is shown.

【0021】この図2に示すように、低域通過ろ波器1
においては阻止帯域が通過周波数の3倍以上であって
も、その阻止帯域では図6に示す従来例のように阻止帯
域内に共振が生じることはなく、スプリアス特性が悪く
なることない。
As shown in FIG. 2, the low-pass filter 1
In the above, even if the stop band is 3 times or more of the pass frequency, resonance does not occur in the stop band in the stop band as in the conventional example shown in FIG. 6, and the spurious characteristic does not deteriorate.

【0022】よって、低域通過ろ波器1を高電力用に設
計することで、広い阻止帯域を有しかつ耐電力性に優れ
た低域通過ろ波器とすることができる。この場合、上述
の如く、構造が極めて単純であるため、低コスト化する
ことができる。
Therefore, by designing the low-pass filter 1 for high power, it is possible to obtain a low-pass filter having a wide stop band and excellent power resistance. In this case, since the structure is extremely simple as described above, the cost can be reduced.

【0023】また、阻止帯域は同軸線路の寸法によって
任意に選択することができる。また、同軸線路の寸法の
変更は中心導体4のみの交換で行えるため、汎用性に優
れた低域通過ろ波器を実現することができる。
The stop band can be arbitrarily selected depending on the size of the coaxial line. Further, since the size of the coaxial line can be changed by exchanging only the center conductor 4, it is possible to realize a low-pass filter having excellent versatility.

【0024】図3は図1の低域通過ろ波器1における周
波数と減衰量との関係を示す図である。図においては、
低域通過ろ波器1を高電力用に形成した場合の周波数と
減衰量との関係を示している。
FIG. 3 is a diagram showing the relationship between the frequency and the amount of attenuation in the low pass filter 1 of FIG. In the figure,
The relationship between the frequency and the attenuation when the low pass filter 1 is formed for high power is shown.

【0025】この図3に示すように、低域通過ろ波器1
においては高電力用に形成した場合、同軸低域通過ろ波
器部2の両端の径を大きくする必要がある。そのため、
阻止帯域が通過帯域の2倍程度であれば、図7に示す従
来例のように阻止帯域内に共振が生じることはなく、ス
プリアス特性が悪くなることもない。
As shown in FIG. 3, the low-pass filter 1
In the case of (1), when formed for high power, it is necessary to increase the diameter of both ends of the coaxial low-pass filter section 2. for that reason,
When the stop band is about twice the pass band, resonance does not occur in the stop band and the spurious characteristics do not deteriorate unlike the conventional example shown in FIG.

【0026】しかしながら、上記の低域通過ろ波器1で
は阻止帯域が通過帯域の3倍以上になると、図3に示す
ように、阻止帯域内に共振が生じ、スプリアス特性が悪
くなる。このスプリアス特性が悪くなる原因としては、
同軸低域通過炉波器部2が高電力用に形成されているた
めに生ずる高次モードの発生がある。
However, in the low pass filter 1 described above, when the stop band is three times or more of the pass band, resonance occurs in the stop band as shown in FIG. 3 and the spurious characteristics deteriorate. The causes of the spurious characteristics are:
Since the coaxial low-pass reactor wave section 2 is formed for high power, there is generation of a higher mode.

【0027】同軸線路中はTEM波であり、最初の高次
モードはTE11モードである。このTE11モードの発生
する周波数fは外導体3の半径をaとし、中心導体4の
半径をbとすると、 f=300/π(a+b) という式で表される。
The coaxial line is a TEM wave, and the first higher order mode is the TE 11 mode. When the radius of the outer conductor 3 is a and the radius of the central conductor 4 is b, the frequency f of the TE 11 mode is expressed by the following formula: f = 300 / π (a + b)

【0028】このTE11モードの発生を抑圧すること
で、さらに広い阻止帯域を実現することができる。
By suppressing the occurrence of the TE 11 mode, a wider stop band can be realized.

【0029】図4は本発明の他の実施例を示す構成図で
ある。図において、本発明の他の実施例による低域通過
ろ波器8は同軸低域通過ろ波器部2と同軸導波管変換器
部7a,7bとの結合部分にリング部材9a,9bを設
けた以外は図1に示す本発明の一実施例と同様の構成と
なっており、同一構成要素には同一符号を付してある。
また、それら同一構成要素の動作は本発明の一実施例と
同様である。
FIG. 4 is a block diagram showing another embodiment of the present invention. In the figure, a low-pass filter 8 according to another embodiment of the present invention includes ring members 9a and 9b at the coupling portion between the coaxial low-pass filter unit 2 and the coaxial waveguide converter units 7a and 7b. The configuration is the same as that of the embodiment of the present invention shown in FIG. 1 except that it is provided, and the same reference numerals are given to the same components.
The operation of those same constituent elements is similar to that of the embodiment of the present invention.

【0030】低域通過ろ波器8では同軸低域通過ろ波器
部2と同軸導波管変換器部7a,7bとの結合部分にリ
ング部材9a,9bを取付けることによって、同軸低域
通過ろ波器部2でのTE11モードの発生を抑圧するよう
にしている。
In the low-pass filter 8, the coaxial low-pass filter is attached to the coupling portion between the coaxial low-pass filter section 2 and the coaxial waveguide converter sections 7a and 7b. The generation of the TE 11 mode in the filter unit 2 is suppressed.

【0031】図5は図1の低域通過ろ波器8における周
波数と減衰量との関係を示す図である。図においては、
低域通過ろ波器8を高電力用に形成した場合の周波数と
減衰量との関係を示している。
FIG. 5 is a diagram showing the relationship between frequency and attenuation in the low pass filter 8 of FIG. In the figure,
The relationship between the frequency and the attenuation amount when the low-pass filter 8 is formed for high power is shown.

【0032】この図に示すように、低域通過ろ波器8に
おいては同軸低域通過ろ波器部2を高電力用に形成した
場合、通過帯域の3倍以上の阻止帯域、つまり通過帯域
が5850〜6425MHzであれば17.475〜1
9.35GHzの阻止帯域において、図7に示す従来例
や図3に示す本発明の一実施例のように阻止帯域内に共
振が生じることはなく、スプリアス特性が悪くなること
はない。
As shown in this figure, in the low-pass filter 8, when the coaxial low-pass filter section 2 is formed for high power, the stop band which is three times or more of the pass band, that is, the pass band is used. Is 5.850-6425 MHz, 17.475-1
In the stop band of 9.35 GHz, resonance does not occur in the stop band as in the conventional example shown in FIG. 7 and the embodiment of the present invention shown in FIG. 3, and spurious characteristics do not deteriorate.

【0033】これはリング部材9a,9bによって同軸
低域通過ろ波器部2でのTE11モードの発生を抑圧して
いるので、同軸低域通過ろ波器部2を高電力用に形成し
ても阻止帯域内に共振が生じることがないためである。
Since the ring members 9a and 9b suppress the occurrence of the TE 11 mode in the coaxial low pass filter section 2, the coaxial low pass filter section 2 is formed for high power. However, resonance does not occur in the stop band.

【0034】よって、低域通過ろ波器8を高電力用に設
計することで、広い阻止帯域を有しかつ耐電力性に優れ
た低域通過ろ波器とすることができる。この場合、上述
の如く、構造が極めて単純であるため、低コスト化する
ことができる。
Therefore, by designing the low-pass filter 8 for high power, a low-pass filter having a wide stop band and excellent in power resistance can be obtained. In this case, since the structure is extremely simple as described above, the cost can be reduced.

【0035】また、阻止帯域は同軸線路の寸法によって
任意に選択することができる。また、同軸線路の寸法の
変更は中心導体4のみの交換で行えるため、汎用性に優
れた低域通過ろ波器を実現することができる。
The stop band can be arbitrarily selected depending on the size of the coaxial line. Further, since the size of the coaxial line can be changed by exchanging only the center conductor 4, it is possible to realize a low-pass filter having excellent versatility.

【0036】しかも、低域通過ろ波器8では阻止帯域が
通過帯域の3倍以上になっても、リング部材9a,9b
によって同軸低域通過ろ波器部2でのTE11モードの発
生が抑圧されるので、阻止帯域内に共振が生じることは
なく、スプリアス特性が悪くなることもない。
Moreover, in the low-pass filter 8, even if the stop band is three times the pass band or more, the ring members 9a, 9b
Since the TE 11 mode is suppressed from being generated in the coaxial low-pass filter section 2, resonance does not occur in the stop band and spurious characteristics do not deteriorate.

【0037】このように、低域通過ろ波器1に伝搬され
てきた信号を同軸導波管変換器部7aで矩形導波管部5
aを伝搬される信号のモードを同軸低域通過ろ波器部2
に入力される信号のモードに変換し、このモードが変換
された信号の高周波成分を同軸低域通過ろ波器部2で切
って同軸導波管変換器部7bに出力して矩形導波管部5
bで伝搬される信号のモードに変換することによって、
構造を簡単にすることができ、広い阻止帯域を有しかつ
耐電力性及び汎用性に優れた低域通過ろ波器を提供する
ことができる。
In this way, the signal propagated to the low pass filter 1 is guided by the coaxial waveguide converter section 7a to the rectangular waveguide section 5a.
The mode of the signal propagated through a is the coaxial low-pass filter unit 2
To the coaxial waveguide converter unit 7b by converting the high-frequency component of the signal converted into the mode into a mode of the signal input to the coaxial waveguide low-pass filter unit 2 and outputting it to the coaxial waveguide converter unit 7b. Part 5
By converting to the mode of the signal propagated in b,
It is possible to provide a low-pass filter having a simple structure, a wide stop band, and excellent power resistance and versatility.

【0038】また、同軸低域通過ろ波器部2と同軸導波
管変換器部7a,7bとの結合部分に取付けたリング部
材9a,9bで同軸低域通過ろ波器部2でのTE11モー
ドの発生を抑圧することによって、通過帯域の3倍以上
の阻止帯域で共振が発生するのを防止することができ、
スプリアス特性の悪化を防止することができる。
Further, the ring member 9a, 9b attached to the coupling portion between the coaxial low-pass filter unit 2 and the coaxial waveguide converter units 7a, 7b is used to connect the coaxial low-pass filter unit 2 to the TE. By suppressing the generation of 11 modes, it is possible to prevent resonance from occurring in the stop band which is three times as large as the pass band,
It is possible to prevent deterioration of spurious characteristics.

【0039】[0039]

【発明の効果】以上説明したように本発明の低域通過ろ
波器によれば、矩形導波管内に高周波成分を除去する同
軸低域通過ろ波器と、同軸低域通過ろ波器への入出力信
号のモードを変換する同軸導波管変換器とを備えること
によって、構造を簡単にすることができ、広い阻止帯域
を有しかつ耐電力性及び汎用性に優れた低域通過ろ波器
を提供することができるという効果がある。
As described above, according to the low pass filter of the present invention, a coaxial low pass filter for removing high frequency components in a rectangular waveguide and a coaxial low pass filter are provided. And a coaxial waveguide converter for converting the mode of the input / output signal of the above, the structure can be simplified and the low pass filter has a wide stop band and is excellent in power resistance and versatility. There is an effect that a wave instrument can be provided.

【0040】また、本発明の他の低域通過ろ波器によれ
ば、同軸低域通過ろ波器と同軸導波管変換器との結合部
分に、同軸低域通過ろ波器における高次モードの信号の
発生を抑止するリング部材を備えることによって、構造
を簡単にすることができ、通過帯域の3倍以上の広い阻
止帯域を有しかつ耐電力性及び汎用性に優れた低域通過
ろ波器を提供するという効果がある。
Further, according to another low-pass filter of the present invention, a high-order filter in the coaxial low-pass filter is provided at a coupling portion between the coaxial low-pass filter and the coaxial waveguide converter. By providing a ring member that suppresses the generation of mode signals, the structure can be simplified, and the low pass band has a wide stop band that is three times the pass band or more and is excellent in power resistance and versatility. The effect is to provide a filter.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の一実施例を示す構成図である。FIG. 1 is a configuration diagram showing an embodiment of the present invention.

【図2】図1の低域通過ろ波器における周波数と減衰量
との関係を示す図である。
FIG. 2 is a diagram showing a relationship between a frequency and an attenuation amount in the low pass filter shown in FIG.

【図3】図1の低域通過ろ波器における周波数と減衰量
の関係を示す図である。
FIG. 3 is a diagram showing the relationship between frequency and attenuation in the low pass filter shown in FIG.

【図4】本発明の他の実施例を示す構成図である。FIG. 4 is a configuration diagram showing another embodiment of the present invention.

【図5】図4の低域通過ろ波器における周波数と減衰量
との関係を示す図である。
5 is a diagram showing a relationship between a frequency and an attenuation amount in the low pass filter of FIG.

【図6】従来例を示す構成図である。FIG. 6 is a configuration diagram showing a conventional example.

【図7】図6の低域通過ろ波器における周波数と減衰量
との関係を示す図である。
7 is a diagram showing the relationship between frequency and attenuation in the low pass filter of FIG.

【符号の説明】[Explanation of symbols]

1,8 低域通過ろ波器 2 同軸低域通過ろ波器部 3 外導体 4 中心導体 4a 細い軸径部分 4b 太い軸径部分 5a,5b 矩形導波管 6a,6b プローブ 7a,7b 同軸導波管変換器部 9a,9b リング部材 1,8 low-pass filter 2 coaxial low-pass filter 3 outer conductor 4 center conductor 4a thin shaft diameter part 4b thick shaft diameter part 5a, 5b rectangular waveguide 6a, 6b probe 7a, 7b coaxial conductor Wave tube converter section 9a, 9b Ring member

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 矩形導波管からなる低域通過ろ波器であ
って、前記矩形導波管内に設けられかつ高周波成分を除
去する同軸低域通過ろ波器と、前記矩形導波管内に設け
られかつ前記同軸低域通過ろ波器への入出力信号のモー
ドを変換する同軸導波管変換器とを含むことを特徴とす
る低域通過ろ波器。
1. A low-pass filter comprising a rectangular waveguide, wherein the coaxial low-pass filter is provided in the rectangular waveguide and removes high-frequency components, and in the rectangular waveguide. And a coaxial waveguide converter provided for converting a mode of an input / output signal to / from the coaxial low-pass filter.
【請求項2】 前記同軸低域通過ろ波器と前記同軸導波
管変換器との結合部分に設けられかつ前記同軸低域通過
ろ波器における高次モードの信号の発生を抑止するリン
グ部材を有することを特徴とする請求項1記載の低域通
過ろ波器。
2. A ring member which is provided at a coupling portion between the coaxial low pass filter and the coaxial waveguide converter and which suppresses generation of a higher-order mode signal in the coaxial low pass filter. The low-pass filter according to claim 1, further comprising:
【請求項3】 前記同軸低域通過ろ波器は、互いに異な
る少なくとも2種類の軸径部分を含む中心導体と、前記
中心導体との間に間隙をもって前記中心導体の外周部分
に周設された外導体とから構成されたことを特徴とする
請求項1または請求項2記載の低域通過ろ波器。
3. The coaxial low-pass filter is provided around an outer peripheral portion of the center conductor with a gap between the center conductor and at least two types of shaft diameter portions different from each other. The low pass filter according to claim 1 or 2, wherein the low pass filter comprises an outer conductor.
【請求項4】 前記同軸低域通過ろ波器は、高電力用に
形成されたことを特徴とする請求項1から請求項3のい
ずれか記載の低域通過ろ波器。
4. The low pass filter according to claim 1, wherein the coaxial low pass filter is formed for high power.
【請求項5】 前記リング部材は、その内径が前記同軸
低域通過ろ波器を構成する外導体の内径よりも小さいこ
とを特徴とする請求項1から請求項4のいずれか記載の
低域通過ろ波器。
5. The low band according to claim 1, wherein the ring member has an inner diameter smaller than an inner diameter of an outer conductor forming the coaxial low pass filter. Passing filter.
JP5296386A 1993-11-26 1993-11-26 Low-pass filter Expired - Lifetime JP2722166B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5296386A JP2722166B2 (en) 1993-11-26 1993-11-26 Low-pass filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5296386A JP2722166B2 (en) 1993-11-26 1993-11-26 Low-pass filter

Publications (2)

Publication Number Publication Date
JPH07154101A true JPH07154101A (en) 1995-06-16
JP2722166B2 JP2722166B2 (en) 1998-03-04

Family

ID=17832881

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5296386A Expired - Lifetime JP2722166B2 (en) 1993-11-26 1993-11-26 Low-pass filter

Country Status (1)

Country Link
JP (1) JP2722166B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2005104293A1 (en) * 2004-04-21 2005-11-03 Matsushita Electric Industrial Co., Ltd. Photonic crystal device
WO2012101699A1 (en) * 2011-01-25 2012-08-02 日本電気株式会社 Coaxial waveguide tube converter, and ridge waveguide tube
CN104617362A (en) * 2015-01-30 2015-05-13 东莞鸿爱斯通信科技有限公司 Low-pass filter with transmission zero

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59119607U (en) * 1983-01-31 1984-08-13 富士通株式会社 Coaxial waveguide conversion structure
JPH01107204U (en) * 1988-01-12 1989-07-19

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59119607U (en) * 1983-01-31 1984-08-13 富士通株式会社 Coaxial waveguide conversion structure
JPH01107204U (en) * 1988-01-12 1989-07-19

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2005104293A1 (en) * 2004-04-21 2005-11-03 Matsushita Electric Industrial Co., Ltd. Photonic crystal device
US7280736B2 (en) 2004-04-21 2007-10-09 Matsushita Electric Industrial Co., Ltd. Photonic crystal device
US7574098B2 (en) 2004-04-21 2009-08-11 Panasonic Corporation Photonic crystal device
US7764861B2 (en) 2004-04-21 2010-07-27 Panasonic Corporation Photonic crystal device
WO2012101699A1 (en) * 2011-01-25 2012-08-02 日本電気株式会社 Coaxial waveguide tube converter, and ridge waveguide tube
US9118098B2 (en) 2011-01-25 2015-08-25 Nec Corporation Coaxial waveguide converter and ridge waveguide
CN104617362A (en) * 2015-01-30 2015-05-13 东莞鸿爱斯通信科技有限公司 Low-pass filter with transmission zero
CN104617362B (en) * 2015-01-30 2017-11-28 东莞鸿爱斯通信科技有限公司 Low pass filter with transmission zero

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