JPS61189701A - Band-pass filter - Google Patents

Band-pass filter

Info

Publication number
JPS61189701A
JPS61189701A JP2954485A JP2954485A JPS61189701A JP S61189701 A JPS61189701 A JP S61189701A JP 2954485 A JP2954485 A JP 2954485A JP 2954485 A JP2954485 A JP 2954485A JP S61189701 A JPS61189701 A JP S61189701A
Authority
JP
Japan
Prior art keywords
line
resonators
filter
width
resonator
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
JP2954485A
Other languages
Japanese (ja)
Other versions
JPH06101643B2 (en
Inventor
Mitsuo Makimoto
三夫 牧本
Morikazu Sagawa
守一 佐川
Sadahiko Yamashita
山下 貞彦
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP2954485A priority Critical patent/JPH06101643B2/en
Publication of JPS61189701A publication Critical patent/JPS61189701A/en
Publication of JPH06101643B2 publication Critical patent/JPH06101643B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime 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

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Control Of Motors That Do Not Use Commutators (AREA)

Abstract

PURPOSE:To obtain a wide band filter having a higher harmonic wave suppressing effect by using a 1/2 wavelength type strip line resonator having a linear taper part and an opened tip part and performing the connection between resonators and also between the input and the output with said taper part. CONSTITUTION:Resonators 101-103 have linear taper parts having large width at the center part and small width at the open end part respectively. Therefore the conductor loss can be reduced with these resonators since the line width is large at the center part where the current level is maximum and therefore applied suitably to a filter having low loss. Furthermore the higher harmonic wave suppressing effect is secured owing to the uneven line impedance, and a sufficiently large degree of bond is secured at the taper part. This attains a band-pass filter of a wide band. While resonators 201-203 have small width of line at the center part and large width at the open end part respectively. Thus the lengths of these resonators can be set shorter than the 1/2 wavelength.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、数百MHz 以上の周波数帯において、マイ
クロストリップあるいはストリップ線路を用いた帯域通
過フィルタに関するものであり、各種無線送受信機、計
測機器等に利用される。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a bandpass filter using a microstrip or strip line in a frequency band of several hundred MHz or higher, and is applicable to various wireless transceivers, measuring instruments, etc. used.

従来の技術 マイクロストリップ線路あるいはストリップ線路(以下
、ストリップ線路と総称する)共振器を用いた帯域通過
フィルタは、第3図に示すように構造が単純で製造が容
易であるためにマイクロ波帯およびその近傍の周波数帯
で賞月されている回路であシ、それの設計法もMicr
owave Filters。
BACKGROUND ART Band-pass filters using microstrip line or strip line (hereinafter collectively referred to as strip line) resonators have a simple structure and are easy to manufacture, as shown in Figure 3, so they are suitable for microwave bands and It is a circuit that has received awards in the nearby frequency band, and its design method is also based on Micr.
owave Filters.

Impedance Matching Networ
ks+ and CouplingStructure
s”(G、L+Mathaei、L、Young an
dE−M−T 、 7hones著、 MiGraw、
NewYork、1964 )に詳しく論じられている
Impedance Matching Network
ks+ and Coupling Structure
s” (G, L+Mathaei, L, Young an
dE-M-T, 7hones, MiGraw,
New York, 1964).

第3図において、301.302.303は二分の一波
長先端開放の一様線路共振器であシ、各恭振器は四分の
一波長で平行結合させたうえ、入出力線路304.30
5とも四分の一波長の線路で平行結合させて帯域通過フ
ィルタを構成している。しかしこのフィルタは、共振器
自体設計中心周波数を10とした場合、nfo(n=2
 、 s 、4.−・)にも共振点をもつため、通過域
がfoのみならず2f0,3f0,4f0・・・にも発
生するため、増力増巾器。
In Fig. 3, 301, 302, and 303 are uniform line resonators with half wavelength open ends, and each resonator is parallel coupled with a quarter wavelength, and input/output lines 304, 30
5 are coupled in parallel with a quarter wavelength line to form a bandpass filter. However, in this filter, when the design center frequency of the resonator itself is 10, nfo (n=2
, s, 4. -) also has a resonance point, so the passband occurs not only in fo but also in 2f0, 3f0, 4f0..., so it is a power amplifier.

発撮器等の出力に高いレベルの高調波成分を有する回路
の出力フィルタとして用いると高調波抑圧効果をもたな
いのみならず、損失、形状に対して設計の自由度が小さ
いという欠点ももつものである。
When used as an output filter for a circuit that has a high level of harmonic components in the output of an oscillator, etc., it not only has no harmonic suppression effect, but also has the disadvantage that there is little freedom in design regarding loss and shape. It is something.

これらの欠点を克服するため、第4図に示す非均−イン
ピーダンスをもつ共振器を共振素子に適用したストリッ
プ線路フィルタが考えられる。
In order to overcome these drawbacks, a strip line filter can be considered in which a resonator having an asymmetric impedance as shown in FIG. 4 is applied as a resonant element.

第4図において、401.402.403は共振器、4
04.405は入出力線路を示す。このフィルタで用い
る共振器は開放端近くの線路と中心部近くの線路の線路
巾をかえて線路インピーダンスと異なるようにしたもの
で(同図のものでは中央部の線路インビーダンスが低く
、開放端部は高い構造を示している。)、線路インピー
ダンスが一様でなくなるため、高次の共振点が基本波の
整数倍にはならない特性をもつ。そのため、高周波抑圧
効果をもつフィルタが実現可能となる。まだ低損失設計
が要求される場合は、線路中央部の線路巾を広くして設
計すればよい。また形状を小さく(共振器長を短かく)
設計する必要がある場合は、線路中央部を狭く設計する
ことで対応でき、設計の自由度が第3図の一様線路共振
器を用いたフィルタに比し大きいという特長をもってい
る。
In Fig. 4, 401.402.403 are resonators, 4
04.405 indicates an input/output line. The resonator used in this filter is one in which the line impedance is different from the line impedance by changing the line width of the line near the open end and the line near the center. ), the line impedance is no longer uniform, so the high-order resonance point is not an integral multiple of the fundamental wave. Therefore, a filter having a high frequency suppression effect can be realized. If a low-loss design is still required, the line width at the center of the line may be widened. Also, make the shape smaller (shorten the resonator length)
If it is necessary to design it, it can be done by designing the central part of the line to be narrow, and it has the advantage that the degree of freedom in design is greater than that of the filter using the uniform line resonator shown in FIG.

発明が解決しようとする問題点 ところが、このフィルタは、第4図からも理解できるよ
うに結合線路長を十分長くとることができないために、
結合度が大きくできず、狭帯域なフィルタにしか適用で
きないという欠点を有していた。
Problems to be Solved by the Invention However, as can be seen from FIG. 4, this filter cannot have a sufficiently long coupling line;
It has the disadvantage that the degree of coupling cannot be increased and it can only be applied to narrow band filters.

本発明は上記欠点に鑑み、通過帯域中の広い、高調波抑
圧効果をもつストリップ線路フィルタを実現しようとす
るものである。
In view of the above-mentioned drawbacks, the present invention aims to realize a strip line filter having a wide passband and having a harmonic suppressing effect.

問題点を解決するための手段 本発明では、非均−線路共撮器として直線状チー・(形
状を有する先端開放ストリップ線路共振器を用いて、前
記直線状テーパ部で共振器間および入出力結合を有する
ものである。
Means for Solving the Problems In the present invention, a linear strip line resonator having an open-ended tip is used as a non-uniform line co-optation device, and the linear tapered portion connects between the resonators and input/output. It has a bond.

作  用 直線状テーパを用いて線路インピーダンスを非均−にす
ることにより、ストリップ線路共振器の高次共振点は基
本共振点の整数倍よりずらすことが可能であり、また直
線状テーノ(部で結合させることにより結合長を十分長
くとることが実現できるため、結合度を強く設計でき通
過帯域中を拡大できる。
By making the line impedance non-uniform using a linear taper, the higher-order resonance point of the stripline resonator can be shifted from an integer multiple of the fundamental resonance point, and the linear taper By coupling, the coupling length can be made sufficiently long, so the degree of coupling can be designed to be strong and the passband can be expanded.

実施例 第1図に本発明の第1の実施例を示す。Example FIG. 1 shows a first embodiment of the present invention.

第1図において、101,102,103は共振器、1
04,105は入出力結合線路である。共振器101.
102.103は線路中央部で線路巾が広く、開放端で
狭い構造の直線状チー・くを有する共振器である。この
共振器101,102゜103は、電流が最大となる線
路中央部の線路巾が大きいため導体損失が低減でき、低
損失のフィルタに適している。また線路インピーダンス
が非均−であるためフィルタとして高調波抑圧効果も備
えているとともに、直線状チー・4部で十分太きな結合
度が得られるため、広帯域な帯域通過フィルタを実現で
きる0 次に、他の実施例について説明する。
In FIG. 1, 101, 102, 103 are resonators, 1
04 and 105 are input/output coupling lines. Resonator 101.
102 and 103 are resonators having a linear channel with a wide line width at the center of the line and a narrow structure at the open end. These resonators 101, 102, and 103 have a large line width at the center of the line where the current is maximum, so that conductor loss can be reduced, making them suitable for low-loss filters. In addition, since the line impedance is non-uniform, it also has a harmonic suppression effect as a filter, and since a sufficiently thick coupling degree can be obtained with the four linear channels, a zero-order Next, another embodiment will be described.

第2図は本発明の第2の実施例である。FIG. 2 shows a second embodiment of the invention.

第2図において、201.202.203は共振器、2
04.205は入出力結合線路である。
In Figure 2, 201.202.203 are resonators, 2
04.205 is an input/output coupling line.

本実施例では共振器201.202.203の中央部の
線路巾が狭く、開放端が広くなっている非均−インピー
ダンスを有する共振器となっているため、第1図のもの
と同様にフィルタとして高調波抑圧効果を持つ。この構
造の共振器は、共振器長を二分の画性長より短かく設計
できるため小型化に適する。
In this example, the resonators 201, 202, and 203 have a narrow line width at the center and a wide open end, which is a resonator with nonuniform impedance. It has a harmonic suppression effect. A resonator with this structure is suitable for miniaturization because the resonator length can be designed to be shorter than the half-scale length.

なお本実施例の説明では、共振器3ケを用いた3段フィ
ルタを示したが、段数(共振器の数)は任意に選ぶこと
ができることは言うまでもない。
In the description of this embodiment, a three-stage filter using three resonators is shown, but it goes without saying that the number of stages (number of resonators) can be arbitrarily selected.

発明の効果 以上述べたように本発明は直線状テーパ部を有する先端
開放二分の画性長形ストリップ線路共振器を用い、その
テーパ部で共振器間および入出力結合を行わせて、フィ
ルタとして高調波抑圧効果をもった広帯域フィルタを実
現することができ、その工業的価値はきわめて大きい。
Effects of the Invention As described above, the present invention uses a bipartite open-ended long strip line resonator having a linear tapered portion, and uses the tapered portion to perform inter-resonator and input/output coupling, so that it can be used as a filter. A broadband filter with harmonic suppression effect can be realized, and its industrial value is extremely large.

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

第1図は本発明の第1の実施例における帯域通過フィル
タの平面図、第2図は本発明の第2の実施例における帯
域通過フィルタの平面図、第3図は従来のストリップ線
路共振器の平面図、第4図は高調波抑圧効果をもつ従来
のストリップ線路共振器の平面図である。 101.102,103:201.202゜203・・
・・・・共振器、104,105 ;204゜205・
・・・・・入出力結合線路。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 貫2因 第 3 図
FIG. 1 is a plan view of a band-pass filter according to a first embodiment of the present invention, FIG. 2 is a plan view of a band-pass filter according to a second embodiment of the present invention, and FIG. 3 is a plan view of a conventional strip line resonator. FIG. 4 is a plan view of a conventional strip line resonator having a harmonic suppression effect. 101.102,103:201.202゜203...
...Resonator, 104,105 ;204°205・
...Input/output coupling line. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Zukan 2nd cause 3rd figure

Claims (2)

【特許請求の範囲】[Claims] (1)共振線路中央部の線路巾が広く、2つの開放端部
の線路巾が狭くなっている直線状テーパ形状のストリッ
プあるいはマイクロストリップ線路共振器を単数あるい
は複数用い、前記共振器間および入出力線路と共振器の
結合を直線状テーパ部で平行結合させた帯域通過フィル
タ。
(1) Using one or more linear tapered strip or microstrip line resonators with a wide line width at the center of the resonant line and narrow line widths at the two open ends, A bandpass filter in which the output line and resonator are coupled in parallel through a linear taper.
(2)共振線路中央部の線路巾が狭く、2つの開放端部
の線路巾が広くなっている直線状テーパ形状のストリッ
プあるいはマイクロストリップ線路共振器を単数あるい
は複数用い、前記共振器間および入出力線路と共振器の
結合を直線状テーパ部で平行結合させた帯域通過フィル
タ。
(2) Using one or more linear tapered strip or microstrip line resonators with a narrow line width at the center of the resonant line and wide line widths at the two open ends, A bandpass filter in which the output line and resonator are coupled in parallel through a linear taper.
JP2954485A 1985-02-18 1985-02-18 Bandpass filter Expired - Lifetime JPH06101643B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2954485A JPH06101643B2 (en) 1985-02-18 1985-02-18 Bandpass filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2954485A JPH06101643B2 (en) 1985-02-18 1985-02-18 Bandpass filter

Publications (2)

Publication Number Publication Date
JPS61189701A true JPS61189701A (en) 1986-08-23
JPH06101643B2 JPH06101643B2 (en) 1994-12-12

Family

ID=12279064

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2954485A Expired - Lifetime JPH06101643B2 (en) 1985-02-18 1985-02-18 Bandpass filter

Country Status (1)

Country Link
JP (1) JPH06101643B2 (en)

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02272802A (en) * 1989-04-13 1990-11-07 Matsushita Electric Ind Co Ltd Resonator
JPH04284003A (en) * 1991-03-13 1992-10-08 Matsushita Electric Ind Co Ltd Planar dielectric filter
JPH0548304A (en) * 1991-08-12 1993-02-26 Matsushita Electric Ind Co Ltd Band pass filter
JPH06204702A (en) * 1992-12-28 1994-07-22 Japan Energy Corp Microwave filter
US5334961A (en) * 1991-08-12 1994-08-02 Matsushita Electric Industrial Co., Ltd. Strip-line type bandpass filter
JP2005045447A (en) * 2003-07-25 2005-02-17 Tdk Corp Laminate bandpass filter
US7378924B2 (en) 2004-02-03 2008-05-27 Ntt Docomo, Inc. Filter with improved capacitive coupling portion
RU2677103C1 (en) * 2017-12-18 2019-01-15 Федеральное государственное бюджетное образовательное учреждение высшего образования "Сибирский государственный университет науки и технологий имени академика М.Ф. Решетнева" (СибГУ им. М.Ф. Решетнева) Microstrip low-pass filter
CN117477195A (en) * 2023-12-27 2024-01-30 成都宏科电子科技有限公司 Broadband parallel coupling filter for inhibiting 2-frequency multiplication harmonic wave

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02272802A (en) * 1989-04-13 1990-11-07 Matsushita Electric Ind Co Ltd Resonator
JPH04284003A (en) * 1991-03-13 1992-10-08 Matsushita Electric Ind Co Ltd Planar dielectric filter
JPH0548304A (en) * 1991-08-12 1993-02-26 Matsushita Electric Ind Co Ltd Band pass filter
US5334961A (en) * 1991-08-12 1994-08-02 Matsushita Electric Industrial Co., Ltd. Strip-line type bandpass filter
JPH06204702A (en) * 1992-12-28 1994-07-22 Japan Energy Corp Microwave filter
JP2005045447A (en) * 2003-07-25 2005-02-17 Tdk Corp Laminate bandpass filter
US7378924B2 (en) 2004-02-03 2008-05-27 Ntt Docomo, Inc. Filter with improved capacitive coupling portion
RU2677103C1 (en) * 2017-12-18 2019-01-15 Федеральное государственное бюджетное образовательное учреждение высшего образования "Сибирский государственный университет науки и технологий имени академика М.Ф. Решетнева" (СибГУ им. М.Ф. Решетнева) Microstrip low-pass filter
CN117477195A (en) * 2023-12-27 2024-01-30 成都宏科电子科技有限公司 Broadband parallel coupling filter for inhibiting 2-frequency multiplication harmonic wave

Also Published As

Publication number Publication date
JPH06101643B2 (en) 1994-12-12

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