JPH08250905A - Dielectric filter circuit and its configuration method - Google Patents

Dielectric filter circuit and its configuration method

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Publication number
JPH08250905A
JPH08250905A JP5268495A JP5268495A JPH08250905A JP H08250905 A JPH08250905 A JP H08250905A JP 5268495 A JP5268495 A JP 5268495A JP 5268495 A JP5268495 A JP 5268495A JP H08250905 A JPH08250905 A JP H08250905A
Authority
JP
Japan
Prior art keywords
attenuation
filter circuit
dielectric filter
attenuation pole
circuit elements
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
JP5268495A
Other languages
Japanese (ja)
Other versions
JP3467747B2 (en
Inventor
Takaya Noba
孝也 野場
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.)
Tokin Corp
Original Assignee
Tokin Corp
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 Tokin Corp filed Critical Tokin Corp
Priority to JP05268495A priority Critical patent/JP3467747B2/en
Publication of JPH08250905A publication Critical patent/JPH08250905A/en
Application granted granted Critical
Publication of JP3467747B2 publication Critical patent/JP3467747B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE: To suppress interference between circuit elements without the use of a special additional member and to obtain a further larger attenuation in excess of a noise level. CONSTITUTION: An attenuation pole circuit 12a(12c, 12b) forming an attenuation pole comprising a reactive element such as a capacitor or a coil and a dielectric resonator 11a(11c, 11b) is connected between coupling circuit elements 13a and 13b (between coupling circuit elements 13b and 13d and between coupling circuit elements 13c and 13b) which are components of the dielectric filter circuit consisting of the cascade connection of the four coupling circuit elements 13a, 13b, 13d and 13c in this order each being a reactive element such as a capacitor or a coil. Then the attenuation pole circuits 12a, 12b whose frequencies are close to each other are located apart among the attenuation pole circuits 12a, 12c and 12b.

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、主として通信用電子機
器等に用いられる誘電体フィルタ回路及びその構成方法
に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a dielectric filter circuit mainly used in electronic equipment for communication and the like and a method for constructing the same.

【0002】[0002]

【従来の技術】従来、この種の誘電体フィルタ回路は、
一般に通過帯域近接で大きな減衰を取るためのバンドパ
スフィルタとして使用される。このようなバンドパスフ
ィルタ用の誘電体フィルタ回路は、図3に示されるよう
に、コンデンサ又はコイルのリアクタンス素子を用いた
4個の結合回路素子13a,13b,13c,13d
(但し、各結合回路素子13a,13b,13cにはコ
ンデンサ,結合回路素子13dにはコイルを用いてい
る)がこの順で直列接続された各結合回路素子13a,
13b,13c,13dの隣接する相互間に対し、リア
クタンス素子及び誘電体同軸共振器11a,11b,1
1cから減衰極を成す3個の減衰極回路12a,12
b,12c(但し、減衰極回路12a,12bにはコン
デンサ,減衰極回路12cにはコイルを用いている)を
それぞれこの順に縦接続して構成されている。
2. Description of the Related Art Conventionally, this type of dielectric filter circuit has been
Generally, it is used as a bandpass filter to obtain large attenuation near the pass band. As shown in FIG. 3, a dielectric filter circuit for such a bandpass filter has four coupling circuit elements 13a, 13b, 13c, 13d using reactance elements of capacitors or coils.
(However, capacitors are used for the coupling circuit elements 13a, 13b, 13c, and coils are used for the coupling circuit element 13d), and the coupling circuit elements 13a, 13a are connected in series in this order.
Reactance elements and dielectric coaxial resonators 11a, 11b, 1 are provided between adjacent ones of 13b, 13c, 13d.
Three attenuation pole circuits 12a, 12 forming an attenuation pole from 1c
b and 12c (however, capacitors are used for the attenuation pole circuits 12a and 12b, and coils are used for the attenuation pole circuit 12c), which are vertically connected in this order.

【0003】図4は、このような回路構成を持つ誘電体
フィルタ回路の特性を周波数[MHz]と損失[dB]
との関係で示したものである。一般に誘電体フィルタ回
路の特性としては、信号通過域内では挿入損失がより小
さく、信号阻止域では大きな減衰を取れることが求めら
れる。
FIG. 4 shows the characteristics of a dielectric filter circuit having such a circuit structure as frequency [MHz] and loss [dB].
It is shown in the relationship with. In general, the dielectric filter circuit is required to have a smaller insertion loss in the signal pass band and a larger attenuation in the signal stop band.

【0004】そこで、この誘電体フィルタ回路におい
て、特性曲線Cに従って信号阻止域での規格線Aを達成
しようとする場合、二つの減衰極21a,21bを狭帯
域内に並べて配置させることによって各減衰極21a,
21bを合成し、信号阻止域での規格線Aを満足すべく
大きな減衰量を得ている。即ち、誘電体フィルタ回路で
はこのような条件を満足させるために通常減衰極21
a,21bを成す減衰極回路12a,12bが隣接して
配置される。
Therefore, in order to achieve the standard line A in the signal stop band in accordance with the characteristic curve C in this dielectric filter circuit, the two attenuation poles 21a and 21b are arranged side by side in a narrow band to reduce the attenuation. Pole 21a,
21b is combined to obtain a large amount of attenuation to satisfy the standard line A in the signal stop band. That is, in the dielectric filter circuit, in order to satisfy such a condition, the normal attenuation pole 21
Attenuation pole circuits 12a and 12b forming a and 21b are arranged adjacent to each other.

【0005】[0005]

【発明が解決しようとする課題】上述した誘電体フィル
タ回路の場合、ノイズレベルを超えて大きな減衰を要す
る条件下で使用すると、回路構成上充分な減衰量が得ら
れないことがある。
In the case of the dielectric filter circuit described above, if it is used under the condition that the noise level exceeds the noise level and large attenuation is required, a sufficient attenuation amount may not be obtained in terms of the circuit configuration.

【0006】図5は、図3に示した誘電体フィルタ回路
におけるノイズレベル特性を周波数[MHz]と減衰量
[dB]との関係で示したものである。ここではノイズ
レベルの減衰量は周波数によりその大きさが変化し、周
波数が高い程増加することが判る。因みに、一般にノイ
ズレベル特性は回路構成に使用する回路素子や誘電体同
軸共振器の特性等によって変化するもので、減衰量自体
は異なることが予想されるが、周波数との関係は概ね同
じ傾向を示す。
FIG. 5 shows the noise level characteristic of the dielectric filter circuit shown in FIG. 3 in terms of the relationship between frequency [MHz] and attenuation [dB]. Here, it can be seen that the amount of noise level attenuation changes depending on the frequency, and increases as the frequency increases. Incidentally, the noise level characteristics generally change depending on the characteristics of the circuit elements and dielectric coaxial resonators used in the circuit configuration, and it is expected that the amount of attenuation itself will differ, but the relationship with frequency shows a similar tendency. Show.

【0007】図6は、上述した誘電体フィルタ回路にお
けるノイズレベルを超えて大きな減衰を取る場合の特性
を実線で示す実測値の特性曲線C1と点線で示す理論値
の特性曲線C2との関係で示したものである。図6から
は減衰極21a,21bの比較において、特性曲線C2
では十分な減衰量が取れているが、特性曲線C1では実
際にそれが達成されていないことが判る。これはノイズ
レベルを超えて大きい減衰量を実現しようとした場合、
回路素子間に干渉が生じて大きな減衰量を得ることがで
きなくなっているためと類推される。
FIG. 6 shows the relationship between the characteristic curve C1 of the actual measurement value shown by the solid line and the characteristic curve C2 of the theoretical value shown by the dotted line, showing the characteristics of the above-mentioned dielectric filter circuit when a large attenuation is taken over the noise level. It is shown. From FIG. 6, in comparison of the attenuation poles 21a and 21b, the characteristic curve C2
It can be seen that in the characteristic curve C1, that is not actually achieved although the sufficient attenuation is obtained. If you try to achieve a large amount of attenuation above the noise level,
It is presumed that interference is caused between the circuit elements and a large amount of attenuation cannot be obtained.

【0008】具体的に云えば、図3に示した誘電体フィ
ルタ回路において、減衰極回路12a,12b間の干渉
は大きいが、減衰極回路12b,12c間の干渉と減衰
極回路12a,12c間の干渉とに関しては殆ど無視で
きる程小さい。即ち、干渉自体は3つの減衰極回路12
a,12b,12c間でそれぞれ生じているにも拘ら
ず、隣接配置された減衰極回路12a,12bに関して
狭帯域に配置された2つの減衰極21a,21bでは論
理値と実測値とが異なって干渉の影響が大きく出ている
のに対し、減衰極回路12cに関して通過帯域によって
隔てられて配置された減衰極21cでは理論値と実測値
とがほぼ一致しており、干渉の影響が小さくなってい
る。
Specifically, in the dielectric filter circuit shown in FIG. 3, although the interference between the attenuation pole circuits 12a and 12b is large, the interference between the attenuation pole circuits 12b and 12c and the interference between the attenuation pole circuits 12a and 12c. The interference is almost negligible. That is, the interference itself consists of three attenuation pole circuits 12
Despite the fact that they occur between a, 12b and 12c respectively, the two attenuation poles 21a and 21b arranged in a narrow band with respect to the adjacent attenuation pole circuits 12a and 12b have different logical values and measured values. While the influence of the interference is large, the theoretical value and the measured value are almost the same in the attenuation pole 21c arranged with the pass band separated in the attenuation pole circuit 12c, and the influence of the interference is small. There is.

【0009】又、こうした回路素子間の干渉は、図3に
示した誘電体フィルタ回路において、結合回路素子13
bを取り除いた場合に入力端子と出力端子との信号系が
途中で遮断されたことになって減衰量が無限大となる筈
であるにも拘らず、実際には空中を伝搬する電磁波の存
在によって無限大にはならないことからも判る。
Further, such interference between the circuit elements causes the coupling circuit element 13 in the dielectric filter circuit shown in FIG.
When b is removed, the signal system between the input terminal and the output terminal is cut off in the middle, and the attenuation should be infinite. However, the existence of electromagnetic waves that actually propagate in the air It can also be seen from the fact that it does not become infinite.

【0010】図7は、上述した誘電体フィルタ回路にお
いて回路素子間に干渉が生じた場合の等価回路を示した
ものである。即ち、この等価回路では実線で示した結合
の他に回路素子間の干渉によって点線で示したような結
合が生じている。
FIG. 7 shows an equivalent circuit in the case where interference occurs between circuit elements in the above-mentioned dielectric filter circuit. That is, in this equivalent circuit, in addition to the coupling shown by the solid line, the coupling shown by the dotted line occurs due to the interference between the circuit elements.

【0011】ところで、単に回路素子間の干渉を無くす
のであれば、例えば干渉し合っている回路素子同士の間
に金属板を設ける等の付加対策を施せば良いが、このよ
うな付加対策は有効である反面、他の基本的な回路素子
の配置が困難になるばかりでなく、大型化を招く要因に
なったり、或いは組み立てが複雑になって生産性が非常
に劣化してしまう等の弊害が多くなるため、回路素子間
の干渉対策としては好ましくない。
If the interference between the circuit elements is simply eliminated, additional measures such as providing a metal plate between the interfering circuit elements may be taken, but such additional measures are effective. On the other hand, it is not only difficult to arrange other basic circuit elements, but also causes a large size, or there is a problem that productivity is deteriorated due to complicated assembly. Since it increases, it is not preferable as a measure against interference between circuit elements.

【0012】本発明は、このような問題点を解決すべく
なされたもので、その技術的課題は、特別な付加部材を
用いること無く回路素子間の干渉を抑制し得ると共に、
ノイズレベルを越えて一層大きな減衰量を取得できる誘
電体フィルタ回路及びその構成方法を提供することにあ
る。
The present invention has been made to solve such a problem, and its technical problem is that interference between circuit elements can be suppressed without using a special additional member, and
It is an object of the present invention to provide a dielectric filter circuit that can obtain a larger amount of attenuation over a noise level and a method of configuring the dielectric filter circuit.

【0013】[0013]

【課題を解決するための手段】本発明によれば、直列接
続された複数の結合回路素子と、複数の結合回路素子の
隣接するものの相互間にそれぞれ縦接続されると共に、
誘電体共振器を含んで減衰極を成す複数の減衰極回路と
を含む誘電体フィルタ回路において、複数の減衰極回路
は、周波数の近接するもの同士がそれぞれ離間されてい
る誘電体フィルタ回路が得られる。
According to the present invention, a plurality of coupling circuit elements connected in series and a plurality of coupling circuit elements adjacent to each other are vertically connected to each other, and
In a dielectric filter circuit that includes a plurality of attenuation pole circuits that include a dielectric resonator and that form an attenuation pole, a plurality of attenuation pole circuits can be obtained by a dielectric filter circuit in which adjacent frequencies are separated from each other. To be

【0014】一方、本発明によれば、誘電体共振器を含
んで減衰極を成す複数の減衰極回路をそれぞれ直列接続
された複数の結合回路素子の隣接するものの相互間に縦
接続して誘電体フィルタ回路を成す誘電体フィルタ回路
の構成方法において、複数の減衰極回路のうちの周波数
の近接するもの同士をそれぞれ離間させる誘電体フィル
タ回路の構成方法が得られる。
On the other hand, according to the present invention, a plurality of attenuation pole circuits each including a dielectric resonator and forming an attenuation pole are vertically connected between adjacent ones of a plurality of series-connected coupling circuit elements. In a method of configuring a dielectric filter circuit that forms a body filter circuit, a method of configuring a dielectric filter circuit that separates adjacent ones of frequencies of a plurality of attenuation pole circuits from each other is obtained.

【0015】[0015]

【作用】一般に減衰極を成す減衰極回路同士が互いに干
渉する現象は、近接する周波数で減衰極を構成した場合
に大きく現われるが、特性的に信号通過帯域を隔てて配
置された減衰極との間の干渉は殆ど無視できる。そこ
で、本発明の誘電体フィルタ回路の構成方法では、これ
に着目して各減衰極回路のうちの周波数の近接するもの
同士をそれぞれ離間させている。こうした場合、各減衰
極回路の近接するもの同士間では回路素子間の干渉が生
じるが、各々減衰極が通過帯域を挾んで近接した周波数
に配置されていないため、干渉の影響が無視できる程小
さくなる。この結果、誘電体フィルタ回路では各回路素
子間の干渉を無視できるようになり、周波数が近接した
減衰極同士が合成されてノイズレベルを越えて充分に大
きな減衰量を取得できる。
In general, the phenomenon that the attenuation pole circuits forming the attenuation poles interfere with each other greatly appears when the attenuation poles are formed at frequencies close to each other. However, the characteristic of the attenuation poles separated from the signal pass band is characteristic. Interference between them is almost negligible. Therefore, in the method of constructing the dielectric filter circuit of the present invention, attention is paid to this, and those of the respective attenuation pole circuits whose frequencies are close to each other are separated from each other. In such a case, interference between circuit elements occurs between adjacent ones of the respective attenuation pole circuits, but since the attenuation poles are not placed at frequencies close to each other across the pass band, the influence of interference is small enough to be ignored. Become. As a result, in the dielectric filter circuit, the interference between the respective circuit elements can be ignored, and the attenuation poles whose frequencies are close to each other are combined to exceed the noise level and a sufficiently large attenuation amount can be obtained.

【0016】[0016]

【実施例】以下に実施例を挙げ、本発明の誘電体フィル
タ回路及びその構成方法について、図面を参照して詳細
に説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The dielectric filter circuit of the present invention and the method of constructing the same will be described in detail below with reference to the drawings.

【0017】最初に、本発明の誘電体フィルタ回路の構
成方法について、その概要を簡単に説明する。この誘電
体フィルタ回路の構成方法は、誘電体共振器を含んで減
衰極を成す複数の減衰極回路をそれぞれ直列接続された
複数の結合回路素子の隣接するものの相互間に縦接続し
て誘電体フィルタ回路を成す点は従来通りであるが、本
発明では各減衰極回路のうちの周波数の近接するもの同
士をそれぞれ離間させて回路構成する。
First, the outline of the method of constructing the dielectric filter circuit of the present invention will be briefly described. This dielectric filter circuit is constructed by connecting a plurality of attenuation pole circuits, each including a dielectric resonator and forming an attenuation pole, vertically between adjacent ones of a plurality of coupling circuit elements connected in series. Although the point of forming a filter circuit is the same as that of the conventional one, in the present invention, the circuits of the respective attenuation pole circuits whose frequencies are close to each other are separated from each other.

【0018】図1は、この誘電体フィルタ回路の構成方
法を適用した本発明の一実施例に係る誘電体フィルタ回
路の基本構成を示したものである。
FIG. 1 shows the basic structure of a dielectric filter circuit according to an embodiment of the present invention to which this method of forming a dielectric filter circuit is applied.

【0019】この誘電体フィルタ回路は、コンデンサ又
はコイルのリアクタンス素子を用いた4個の結合回路素
子13a,13b,13d,13c(但し、ここでも各
結合回路素子13a,13b,13cにはコンデンサ,
結合回路素子13dにはコイルを用いている)と、コン
デンサ又はコイルのリアクタンス素子及び誘電体同軸共
振器11a,11c,11bから減衰極を成すと共に、
この順で直列接続された各結合回路素子13a,13
b,13d,13cの隣接するものの相互間に対して順
次縦接続された3個の減衰極回路12a,12c,12
b(但し、ここでも減衰極回路12a,12bにはコン
デンサ,減衰極回路12cにはコイルを用いている)と
から構成されており、各減衰極回路12a,12c,1
2bにおいては周波数の近接するもの同士である各減衰
極回路12a,12bが離間された構成となっている。
In this dielectric filter circuit, four coupling circuit elements 13a, 13b, 13d and 13c using reactance elements such as capacitors or coils (however, here as well, each coupling circuit element 13a, 13b, 13c has a capacitor,
A coil is used as the coupling circuit element 13d), a reactance element of a capacitor or a coil, and dielectric coaxial resonators 11a, 11c, and 11b form an attenuation pole, and
Each coupling circuit element 13a, 13 connected in series in this order
b, 13d, 13c, three attenuation pole circuits 12a, 12c, 12 which are vertically connected in series with each other.
b (however, a condenser is used for the attenuation pole circuits 12a and 12b, and a coil is used for the attenuation pole circuit 12c here as well), and each of the attenuation pole circuits 12a, 12c, 1
In 2b, the attenuation pole circuits 12a and 12b, which have frequencies close to each other, are separated from each other.

【0020】因みに、この誘電体フィルタ回路は400
MHz帯のバンドパスフィルタ用のもので、400MH
zにおけるノイズレベルの減衰量は図5に示したノイズ
レベル特性に従った45dBとなっている。
Incidentally, this dielectric filter circuit has 400
400MHz for band pass filter of MHz band
The noise level attenuation amount at z is 45 dB according to the noise level characteristic shown in FIG.

【0021】この誘電体フィルタ回路では、近接した周
波数で減衰極を成す減衰極回路12aと減衰極回路12
bとを隔てるように減衰極回路12cが中央に配置され
ている。このため、減衰極回路12a,12c間と減衰
極回路12c,12b間とでは回路素子間の干渉が生じ
るが、各減衰極回路12a,12c,12bにおける各
々減衰極が通過帯域を挾んで近接した周波数に配置され
ていないため、干渉の影響が無視できる程小さくなる。
In this dielectric filter circuit, the attenuation pole circuit 12a and the attenuation pole circuit 12 which form attenuation poles at frequencies close to each other.
An attenuation pole circuit 12c is arranged in the center so as to separate it from b. Therefore, interference occurs between the circuit elements between the attenuation pole circuits 12a and 12c and between the attenuation pole circuits 12c and 12b, but the attenuation poles of the attenuation pole circuits 12a, 12c, and 12b are close to each other across the pass band. Since it is not placed in frequency, the effect of interference is negligible.

【0022】図2は、この誘電体フィルタ回路において
ノイズレベルを超えて大きな減衰を取る場合の特性(実
線で特性曲線C3として示す)を図3に示す従来の誘電
体フィルタ回路における特性(点線で特性曲線C4とし
て示す)と比較して周波数[MHz]と損失[dB]と
の関係で示したものである。
FIG. 2 shows the characteristics of the conventional dielectric filter circuit shown in FIG. 3 (shown by the solid line as a characteristic curve C3) when the dielectric filter circuit has a large attenuation exceeding the noise level (indicated by the dotted line). This is shown by the relationship between the frequency [MHz] and the loss [dB] in comparison with the characteristic curve C4).

【0023】図2からは、信号通過帯域の挿入損失域で
の規格線Bが3dB,信号阻止域での規格線Aが63d
Bである場合、従来の特性では特性曲線C4から規格線
Aを達成できていないのに対し、本実施例の特性では特
性曲線C3から規格線Aを達成できていることが判る。
From FIG. 2, the standard line B in the insertion loss region of the signal pass band is 3 dB, and the standard line A in the signal stop band is 63 d.
In the case of B, it can be seen that the characteristic curve C4 cannot achieve the standard line A in the conventional characteristic, whereas the characteristic curve C3 can achieve the standard line A in the characteristic of the present embodiment.

【0024】尚、実施例の誘電体フィルタ回路では、4
個の結合回路素子13a,13b,13d,13cと3
個の減衰極回路12a,12c,12bとから成る構成
を説明したが、これらの各回路素子の数はそれ以上であ
っても良い。
In the dielectric filter circuit of the embodiment, 4
3 coupling circuit elements 13a, 13b, 13d, 13c and 3
Although the configuration including the individual attenuation pole circuits 12a, 12c, 12b has been described, the number of each of these circuit elements may be greater than that.

【0025】[0025]

【発明の効果】以上に説明した通り、本発明の誘電体フ
ィルタ回路及びその構成方法によれば、ノイズレベルを
超えて大きな減衰が必要とされる場合でも、各回路素子
間の干渉が無視できるようになるため、減衰極を複数配
置して信号阻止域での大きな減衰量を取得できるように
なる。特に、金属板等の特別な付加部材を用いること無
く基本的な回路素子だけの構成で回路素子間の干渉を抑
制し得るため、誘電体フィルタ回路の大型化や生産性の
劣化等を生じないという長所を奏する。
As described above, according to the dielectric filter circuit and the method of constructing the same of the present invention, the interference between the respective circuit elements can be ignored even when a large attenuation is required beyond the noise level. Therefore, it is possible to obtain a large amount of attenuation in the signal stop band by disposing a plurality of attenuation poles. In particular, since interference between circuit elements can be suppressed by the configuration of only basic circuit elements without using a special additional member such as a metal plate, the dielectric filter circuit does not become large and productivity is not deteriorated. It has the advantage.

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

【図1】本発明の一実施例に係るバンドパスフィルタ用
の誘電体フィルタ回路の基本構成を示したものである。
FIG. 1 shows a basic configuration of a dielectric filter circuit for a bandpass filter according to an embodiment of the present invention.

【図2】図1に示す誘電体フィルタ回路においてノイズ
レベルを超えて大きな減衰を取る場合の特性を図3に示
す従来の誘電体フィルタ回路における特性と比較して周
波数[MHz]と損失[dB]との関係で示したもので
ある。
2 is a graph showing characteristics of the dielectric filter circuit shown in FIG. 1 when a large attenuation is taken over a noise level, as compared with the characteristics of the conventional dielectric filter circuit shown in FIG. 3, in frequency [MHz] and loss [dB]. ] Is shown in the relationship with.

【図3】従来のバンドパスフィルタ用の誘電体フィルタ
回路の基本構成を示したものである。
FIG. 3 shows a basic configuration of a conventional dielectric filter circuit for a bandpass filter.

【図4】図3に示す誘電体フィルタ回路の特性を周波数
[MHz]と損失[dB]との関係で示したものであ
る。
FIG. 4 shows the characteristics of the dielectric filter circuit shown in FIG. 3 in terms of the relationship between frequency [MHz] and loss [dB].

【図5】図3に示す誘電体フィルタ回路におけるノイズ
レベル特性を周波数[MHz]と減衰量[dB]との関
係で示したものである。
5 shows the noise level characteristic of the dielectric filter circuit shown in FIG. 3 as a relationship between frequency [MHz] and attenuation [dB].

【図6】図3に示す誘電体フィルタ回路におけるノイズ
レベルを超えて大きな減衰を取る場合の特性を実測値と
理論値との関係で示したものである。
FIG. 6 is a graph showing the characteristics of the dielectric filter circuit shown in FIG. 3 when a large attenuation is achieved in excess of the noise level, in terms of the relationship between measured values and theoretical values.

【図7】図3に示す誘電体フィルタ回路において回路素
子間に干渉が生じた場合の等価回路を示したものであ
る。
7 shows an equivalent circuit in the case where interference occurs between circuit elements in the dielectric filter circuit shown in FIG.

【符号の説明】[Explanation of symbols]

11a,11b,11c 誘電体同軸共振器 12a,12b,12c 減衰極回路 13a,13b,13c,13d 結合回路素子 21a,21b,21c 減衰極 A 信号阻止域での規格線 B 挿入損失域での規格線 11a, 11b, 11c Dielectric coaxial resonator 12a, 12b, 12c Attenuation pole circuit 13a, 13b, 13c, 13d Coupling circuit element 21a, 21b, 21c Attenuation pole A Standard line at signal stop band B Standard at insertion loss band line

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 直列接続された複数の結合回路素子と、
前記複数の結合回路素子の隣接するものの相互間にそれ
ぞれ縦接続されると共に、誘電体共振器を含んで減衰極
を成す複数の減衰極回路とを含む誘電体フィルタ回路に
おいて、前記複数の減衰極回路は、周波数の近接するも
の同士がそれぞれ離間されていることを特徴とする誘電
体フィルタ回路。
1. A plurality of coupling circuit elements connected in series,
A plurality of attenuating poles, each of which is vertically connected between adjacent ones of the plurality of coupling circuit elements and includes a plurality of attenuating pole circuits which form attenuating poles by including a dielectric resonator. The circuit is a dielectric filter circuit characterized in that those having frequencies close to each other are separated from each other.
【請求項2】 誘電体共振器を含んで減衰極を成す複数
の減衰極回路をそれぞれ直列接続された複数の結合回路
素子の隣接するものの相互間に縦接続して誘電体フィル
タ回路を成す誘電体フィルタ回路の構成方法において、
前記複数の減衰極回路のうちの周波数の近接するもの同
士をそれぞれ離間させることを特徴とする誘電体フィル
タ回路の構成方法。
2. A dielectric which forms a dielectric filter circuit by vertically connecting a plurality of attenuation pole circuits including a dielectric resonator and forming an attenuation pole between adjacent ones of a plurality of coupling circuit elements connected in series. In the method of constructing the body filter circuit,
A method of constructing a dielectric filter circuit, characterized in that among the plurality of attenuation pole circuits, those having a close frequency are separated from each other.
JP05268495A 1995-03-13 1995-03-13 Dielectric filter circuit and configuration method thereof Expired - Fee Related JP3467747B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP05268495A JP3467747B2 (en) 1995-03-13 1995-03-13 Dielectric filter circuit and configuration method thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP05268495A JP3467747B2 (en) 1995-03-13 1995-03-13 Dielectric filter circuit and configuration method thereof

Publications (2)

Publication Number Publication Date
JPH08250905A true JPH08250905A (en) 1996-09-27
JP3467747B2 JP3467747B2 (en) 2003-11-17

Family

ID=12921723

Family Applications (1)

Application Number Title Priority Date Filing Date
JP05268495A Expired - Fee Related JP3467747B2 (en) 1995-03-13 1995-03-13 Dielectric filter circuit and configuration method thereof

Country Status (1)

Country Link
JP (1) JP3467747B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6593816B2 (en) * 2000-11-21 2003-07-15 Darfon Electronics Corp. Balanced input/output filter circuit and device
WO2012164264A1 (en) * 2011-06-01 2012-12-06 Filtronic Wireless Ltd A band combining filter
US8686808B2 (en) 2011-06-01 2014-04-01 Filtronic Wireless Ltd Band combining filter

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6593816B2 (en) * 2000-11-21 2003-07-15 Darfon Electronics Corp. Balanced input/output filter circuit and device
WO2012164264A1 (en) * 2011-06-01 2012-12-06 Filtronic Wireless Ltd A band combining filter
US8686808B2 (en) 2011-06-01 2014-04-01 Filtronic Wireless Ltd Band combining filter

Also Published As

Publication number Publication date
JP3467747B2 (en) 2003-11-17

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