JPS6242522B2 - - Google Patents

Info

Publication number
JPS6242522B2
JPS6242522B2 JP7145680A JP7145680A JPS6242522B2 JP S6242522 B2 JPS6242522 B2 JP S6242522B2 JP 7145680 A JP7145680 A JP 7145680A JP 7145680 A JP7145680 A JP 7145680A JP S6242522 B2 JPS6242522 B2 JP S6242522B2
Authority
JP
Japan
Prior art keywords
filter
frequency
attenuation
stub
wavelength
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
Application number
JP7145680A
Other languages
Japanese (ja)
Other versions
JPS56168401A (en
Inventor
Takao Shinkawa
Masaki Noda
Chuichi Sodeyama
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP7145680A priority Critical patent/JPS56168401A/en
Publication of JPS56168401A publication Critical patent/JPS56168401A/en
Publication of JPS6242522B2 publication Critical patent/JPS6242522B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/20Frequency-selective devices, e.g. filters
    • H01P1/201Filters for transverse electromagnetic waves
    • H01P1/203Strip line filters
    • H01P1/2039Galvanic coupling between Input/Output

Description

【発明の詳細な説明】 この発明は、マイクロストリツプ線路を用いて
構成したストリツプ線路フイルタに関するもので
ある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a stripline filter constructed using microstrip lines.

マイクロストリツプ線路を基本構成とするマイ
クロ波の平面回路において、第1図に示す帯域遮
断フイルタがよく使用される。これは、1/2波長の 長さの両端開放線路からなる共振器1の端から1/4 波長の長さの部分を伝送線路2に結合の空隙3を
設けて平行に接近させて構成するもので、共振器
1の共振周波数で大きな減衰が得られる帯域遮断
フイルタとなる。第2図に、このフイルタの特性
を示す。このフイルタは、結合の空隙3を小さく
することにより第2図の特性4のように減衰量を
大きくできるが、フイルタの結合帯域が広がつ
て、阻止したい周波数の減衰は大きくなる
が、阻止したくない周波数の減衰も増すとい
う欠点をもつている。そこで、このフイルタの設
計は、阻止したくない周波数で結合がなくな
る特性5を用いるが、この時阻止したい周波数
の減衰量も小さくなつてしまう。即ち、従来の
上記構成のフイルタでは、阻止周波数と阻止
しない周波数が近い場合、希望する減衰量が
作れないという欠点をもつていた。
In a microwave planar circuit whose basic configuration is a microstrip line, a band cutoff filter shown in FIG. 1 is often used. This is constructed by making a 1/4 wavelength portion from the end of a resonator 1 consisting of a 1/2 wavelength open line at both ends parallel to the transmission line 2 with a coupling gap 3 provided. This makes it a band-cut filter that can obtain large attenuation at the resonant frequency of the resonator 1. Figure 2 shows the characteristics of this filter. This filter can increase the amount of attenuation as shown in characteristic 4 in Figure 2 by reducing the coupling gap 3, but the coupling band of the filter expands and the attenuation of the frequency 1 that you want to block becomes large. This has the disadvantage that the attenuation of frequency 2 , which is not desired, also increases. Therefore, the design of this filter uses characteristic 5 where coupling disappears at frequency 2 , which is not desired to be blocked, but at this time, the frequency that is desired to be blocked is
The attenuation amount of 1 also becomes small. That is, the conventional filter having the above configuration has the disadvantage that when the blocking frequency 1 and the non-blocking frequency 2 are close to each other, the desired amount of attenuation cannot be produced.

この発明は、上述のような従来のストリツプ線
路フイルタの欠点を解決するためになされたもの
であり、従つてこの発明の目的は、通過帯域の減
衰が小さく、阻止帯域の減衰が大きいストリツプ
線路フイルタを提供することにある。従来のフイ
ルタ構成において、阻止帯域の減衰を大きくとる
と、通過帯域の減衰量が増した。これは、フイル
タを形成する共振器の残留容量と、残留インダク
タンスによるものであり、この発明ではこの残留
リアクタンスを打消すように構成したものであ
る。従つてこの発明の構成の要点は、1/2波長の長 さの終端開放線路の端から1/4波長の長さの部分を 伝送線路に平行に接近させ、該伝送線路におい
て、前記1/4波長の長さ部分の両端のどちらか一方 の位置に対すると共に、それとは反対の側にある
場所に、容量性あるいは誘導性のスタブを取り付
けることによりストリツプ線路フイルタを構成し
た点にある。
This invention was made in order to solve the above-mentioned drawbacks of the conventional stripline filter, and an object of the invention is to provide a stripline filter that has small attenuation in the passband and large attenuation in the stopband. Our goal is to provide the following. In conventional filter configurations, increasing the attenuation in the stopband increases the amount of attenuation in the passband. This is due to the residual capacitance and residual inductance of the resonator forming the filter, and the present invention is designed to cancel this residual reactance. Therefore, the main point of the configuration of the present invention is to bring a 1/4 wavelength portion from the end of the 1/2 wavelength open terminated line close to the transmission line in parallel, and to The stripline filter is constructed by attaching capacitive or inductive stubs to either end of a four-wavelength section and at the opposite end.

以下、この発明を図に示す実施例に従つて詳細
に説明する。第3図は、この発明の原理を説明す
るための説明図で、同図において端子6から伝送
線路2を見たインピーダンスと、端子7から伝送
線路2を見たインピーダンスは逆になる。即ち、
第4図のフイルタ特性説明図に示すように、帯域
阻止フイルタの中心周波数をより低い
周波数をLより高い周波数をHとすると
第3図において、端子6から見たインピーダンス
は、周波数Lで容量性、周波数で短絡、周
波数Hで誘導性のインピーダンスとなる。一
方、端子7から見たインピーダンスは、周波数
Lで誘導性、周波数で開放、周波数Hで容量
性となる。従つて、周波数Lでの減衰を小さく
するには、伝送線路2において共振器1の中心の
位置で、共振器1と反対側に、誘導性スタブある
いは、端子7側の共振器1の端に対応した位置に
容量性スタブを接続することにより、フイルタの
残留のインピーダンスを打消し、周波数Lでの
減衰を小さくする。また、周波数Hでの減衰を
小さくするには、周波数Lの場合と逆のスタブ
を接続することにより、残留のインピーダンスを
打消すことができる。
Hereinafter, the present invention will be explained in detail according to embodiments shown in the drawings. FIG. 3 is an explanatory diagram for explaining the principle of the present invention. In the figure, the impedance when viewing the transmission line 2 from the terminal 6 and the impedance when viewing the transmission line 2 from the terminal 7 are opposite. That is,
As shown in the filter characteristic diagram in Figure 4, if the center frequency of the band rejection filter is 0 , the frequency lower than 0 is L , and the frequency higher than 0 is H , the impedance seen from terminal 6 in Figure 3 is: At frequency L it becomes capacitive, at frequency 0 it becomes a short circuit, and at frequency H it becomes inductive impedance. On the other hand, the impedance seen from terminal 7 is the frequency
It is inductive at L , open at frequency 0 , and capacitive at frequency H. Therefore, in order to reduce the attenuation at frequency L , at the center of the resonator 1 in the transmission line 2, install an inductive stub on the side opposite to the resonator 1, or at the end of the resonator 1 on the terminal 7 side. By connecting a capacitive stub at the corresponding position, the residual impedance of the filter is canceled and the attenuation at frequency L is reduced. Furthermore, in order to reduce the attenuation at frequency H , residual impedance can be canceled by connecting a stub opposite to that for frequency L.

第5図は、この発明の一実施例を示す回路パタ
ーン図であり、同図において、伝送線路2で、共
振器1の端に対応する位置で、しかも共振器1の
反対側に容量性スタブ8を接続した実施例が示さ
れている。この実施例の減衰特性を第6図に示
す。第6図において、特性9は、スタブ8を接続
する前の特性、特性10は容量性スタブ8を接続
した時の特性で、中心周波数の減衰量は変わ
らずに、それより低い周波数Lの減衰量が大幅
に小さくなつている。なお、このスタブ線路は終
端を短絡したり、開放にしたり、また、長さを変
えることにより、容量性にも誘導性にもなること
はよく知られている。また、第5図のスタブ8を
誘導性スタブにすることにより、高い周波数H
の減衰を小さくできることは、上記説明より明ら
かである。
FIG. 5 is a circuit pattern diagram showing an embodiment of the present invention. In the figure, a capacitive stub is inserted in the transmission line 2 at a position corresponding to the end of the resonator 1 and on the opposite side of the resonator 1. An example in which 8 are connected is shown. The attenuation characteristics of this embodiment are shown in FIG. In Fig. 6, characteristic 9 is the characteristic before connecting the stub 8, and characteristic 10 is the characteristic when the capacitive stub 8 is connected . The amount of attenuation has become significantly smaller. It is well known that this stub line can be made capacitive or inductive by short-circuiting or opening its terminal ends, or by changing its length. In addition, by making the stub 8 in Fig. 5 an inductive stub, high frequency H
It is clear from the above explanation that the attenuation of can be reduced.

以上説明した通りであるから、この発明によれ
ば、1/2波長共振器の1/4波長部分を伝送線路に接
近さ せて構成する帯域阻止フイルタにおいて、上記フ
イルタ回路が形成された伝送線路の両端のどちら
か一方に容量性あるいは誘導性スタブを接続する
ことにより、阻止帯域の減衰量を変えることなく
阻止帯域に近い通過帯域の減衰量を小さくできる
という利点がある。
As explained above, according to the present invention, in a band rejection filter configured by bringing a 1/4 wavelength portion of a 1/2 wavelength resonator close to a transmission line, the transmission line on which the filter circuit is formed is By connecting a capacitive or inductive stub to either end, there is an advantage that the amount of attenuation in the pass band near the stop band can be reduced without changing the amount of attenuation in the stop band.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、従来のストリツプ線路フイルタの回
路パターンを示す平面図、第2図は、従来のフイ
ルタの特性を示す特性図、第3図は、この発明の
原理を説明するための説明図、第4図はフイルタ
特性の説明図、第5図はこの発明の一実施例を示
す平面図、第6図はこの発明によるフイルタの特
性例を示す特性図、である。 図において、1は1/2波長共振器、2は伝送線 路、3は空隙、8はスタブ、を示す。
FIG. 1 is a plan view showing the circuit pattern of a conventional strip line filter, FIG. 2 is a characteristic diagram showing the characteristics of the conventional filter, and FIG. 3 is an explanatory diagram for explaining the principle of the present invention. FIG. 4 is an explanatory diagram of filter characteristics, FIG. 5 is a plan view showing an embodiment of the present invention, and FIG. 6 is a characteristic diagram showing an example of the characteristics of the filter according to the present invention. In the figure, 1 is a 1/2 wavelength resonator, 2 is a transmission line, 3 is a gap, and 8 is a stub.

Claims (1)

【特許請求の範囲】 1 マイクロストリツプ線路を用いて構成したス
トリツプ線路フイルタであつて、1/2波長の長さの 終端開放線路の端から1/4波長の長さの部分を伝送 線路に平行に接近させ、該伝送線路において、前
記1/4波長の長さ部分の両端のどちらか一方の位置 に対すると共に、それとは反対の側にある場所
に、容量性あるいは誘導性のスタブを取り付けて
成ることを特徴とするストリツプ線路フイルタ。
[Scope of Claims] 1. A strip line filter configured using a microstrip line, in which a 1/4 wavelength portion from the end of a 1/2 wavelength open terminated line is used as a transmission line. A capacitive or inductive stub is installed in the transmission line at a position on either end of the 1/4 wavelength length portion and at a location on the opposite side thereof. A strip line filter characterized by comprising:
JP7145680A 1980-05-30 1980-05-30 Strip line filter Granted JPS56168401A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7145680A JPS56168401A (en) 1980-05-30 1980-05-30 Strip line filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7145680A JPS56168401A (en) 1980-05-30 1980-05-30 Strip line filter

Publications (2)

Publication Number Publication Date
JPS56168401A JPS56168401A (en) 1981-12-24
JPS6242522B2 true JPS6242522B2 (en) 1987-09-09

Family

ID=13461087

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7145680A Granted JPS56168401A (en) 1980-05-30 1980-05-30 Strip line filter

Country Status (1)

Country Link
JP (1) JPS56168401A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3422899A1 (en) * 1984-06-20 1986-01-02 Siemens AG, 1000 Berlin und 8000 München Planar circuit structure constructed as a filter circuit
JPH05299712A (en) * 1992-04-22 1993-11-12 Sumitomo Electric Ind Ltd Microwave part
JPH09326602A (en) * 1996-06-04 1997-12-16 Atr Kodenpa Tsushin Kenkyusho:Kk High frequency filter circuit
US6792299B2 (en) * 2001-03-21 2004-09-14 Conductus, Inc. Device approximating a shunt capacitor for strip-line-type circuits

Also Published As

Publication number Publication date
JPS56168401A (en) 1981-12-24

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