JPS6243909A - Resonator and filter using it - Google Patents

Resonator and filter using it

Info

Publication number
JPS6243909A
JPS6243909A JP18450885A JP18450885A JPS6243909A JP S6243909 A JPS6243909 A JP S6243909A JP 18450885 A JP18450885 A JP 18450885A JP 18450885 A JP18450885 A JP 18450885A JP S6243909 A JPS6243909 A JP S6243909A
Authority
JP
Japan
Prior art keywords
electrodes
spiral line
resonator
filter
line electrodes
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
Application number
JP18450885A
Other languages
Japanese (ja)
Inventor
Yohei Ishikawa
容平 石川
Jun Hattori
準 服部
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.)
Murata Manufacturing Co Ltd
Original Assignee
Murata Manufacturing 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 Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP18450885A priority Critical patent/JPS6243909A/en
Publication of JPS6243909A publication Critical patent/JPS6243909A/en
Pending legal-status Critical Current

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  • Filters And Equalizers (AREA)
  • Control Of Motors That Do Not Use Commutators (AREA)

Abstract

PURPOSE:To improve the Qo value and the electric characteristic, especially the insertion loss by connecting both spiral line electrodes electrically via a through hole provided to a dielectric base. CONSTITUTION:Two counter electrodes 7a, 7b are provided to both surfaces of a dielectric base 1 while interposing the base 1 in-between. Then spiral line electrodes 8a, 8b of, e.g., one turn wound in the same direction are connected respectively to the counter electrodes 7a, 7b and the tip of both the spiral line electrodes 8a, 8b is connected electrically via the through hole 9 provided to the dielectric base 1. A current flowing to the spiral line electrodes 8a, 8b is made the same direction between lines 81a and 81b and between lines 82a and 82b, they cause mutual inductance to attain magnetic field coupling. Since the increase in the stored magnetic field energy to the increase in the conductor loss is sufficiently larger than the case with a single line or one turn line electrode, resulting that the Qo of the resonance system is increased.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、誘電体基板の両表面に電極を形成して成る
共振器およびそれを用いたフィルタに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a resonator having electrodes formed on both surfaces of a dielectric substrate, and a filter using the resonator.

〔従来の技術とその問題点〕[Conventional technology and its problems]

従来、マイクロストリップラインフィルタやプリントフ
ィルタにおいてバンドパスフィルタラ構成する場合、小
形化に伴ってフィルタを構成する共振器(共振素子)の
Q、値が低下し、フィルタの挿入損失を増大させて電気
的特性を悪化させるという問題があった。
Conventionally, when using a bandpass filter configuration for a microstrip line filter or a printed filter, as the filter becomes smaller, the Q value of the resonator (resonant element) that makes up the filter decreases, increasing the insertion loss of the filter and causing electrical There was a problem of deteriorating the physical characteristics.

例えば、くシ形のマイクロストリップラインフィルタの
一例を示すと第6図のようなものであり、誘電体基板l
の一面にアース電極2を、他面に入出力電極3.5およ
び複数のくし形電極4を形成して成る。くし形電極4の
幅Wおよび誘電体基板lの厚みTは、例えば、それぞれ
1.0m−程度である。このようなマイクロストリップ
ラインフィルタにおいては、例えば、400MHzでQ
0値は100程度止りであった。また、誘電体基板に電
極パターンを印刷してフィルタを構成したブリントフィ
ルりにおいても、ao(直はこれとほぼ同程度である。
For example, an example of a comb-shaped microstrip line filter is shown in FIG.
A ground electrode 2 is formed on one side, and an input/output electrode 3.5 and a plurality of comb-shaped electrodes 4 are formed on the other side. The width W of the comb-shaped electrode 4 and the thickness T of the dielectric substrate 1 are each about 1.0 m, for example. In such a microstrip line filter, for example, Q at 400MHz is
The 0 value was only around 100. Furthermore, in the case of blind fill, in which a filter is constructed by printing an electrode pattern on a dielectric substrate, the ao (direction) is almost the same as this.

そこでこの発明は、Q0埴を向l−させることによって
電気的特性、特に挿入ti失の改善を図った共振器およ
びそれを用いたフィルタを堤供することを目的とする。
SUMMARY OF THE INVENTION It is therefore an object of the present invention to provide a resonator and a filter using the resonator in which the electrical characteristics, particularly the insertion loss, are improved by changing the Q0 value.

〔問題点を解決するだめの手段〕[Failure to solve the problem]

この発明は、誘電体基板の両表面に対向電極およびそね
につながっていて互いに同方向に巻いたスパイラルライ
ン電極をそれぞれ設け、両スパイラルライン電極間を誘
電体基板に設けたスルーホールを介して電気的に接続し
て成ることを特徴とする共振器およびそわを用いたフィ
ルタである。
In this invention, counter electrodes and spiral line electrodes connected to each other and wound in the same direction are provided on both surfaces of a dielectric substrate, and a through hole provided in the dielectric substrate is provided between the two spiral line electrodes. This is a filter using a resonator and a warp, which are electrically connected to each other.

(作用〕 対向電極間で静電容量が形成され、両スパイラルライン
電極でインダクタンスが形成され、これによって並列1
. C共振回路が形成される。しかも、両スパイラルラ
イン電極を接続することによる導体111失の増加に比
べて蓄えられる磁界のエネルギーの増加の方が十分大き
いため、Q0値が向1−シ、それによって電気的特性、
特に挿入を置火の敗訴が図られる。
(Operation) Capacitance is formed between the opposing electrodes, and inductance is formed between both spiral line electrodes.
.. A C resonant circuit is formed. Moreover, since the increase in the energy of the stored magnetic field is sufficiently larger than the increase in the loss of conductor 111 due to the connection of both spiral line electrodes, the Q0 value increases in the 1- direction, thereby improving the electrical characteristics.
In particular, it is hoped that the case against the insertion will be defeated.

〔実施例〕〔Example〕

第1図は、この発明に係る共振器の・実施例を示す斜視
図である。誘電体基板1を挾んでその両表面に2つの対
向電極7aおよび7bが設けられている。当該対向電極
7a、7bの形状は、例えば図のように四角形でも、あ
るいは例えば円形のような他の形状でも良い。この対向
電極7a、7bの内の一方(例えば対向電極7b)は、
例えばアース電極とされる。そして、対向電極7a、7
bには、互いに同方向に巻いた例えば1ターンのスパイ
ラルライン電$Vi8a、8bがそれぞれつながってお
り、両スパイラルライン電極8a、8bの先端部は、誘
電体基板1に設けられたスルーポール9を介して電気的
に接続されている。このようにして共振器6が形成され
ている。
FIG. 1 is a perspective view showing an embodiment of a resonator according to the present invention. Two opposing electrodes 7a and 7b are provided on both surfaces of the dielectric substrate 1 with the dielectric substrate 1 in between. The shape of the opposing electrodes 7a and 7b may be, for example, a square as shown in the figure, or another shape such as a circle. One of the opposing electrodes 7a and 7b (for example, the opposing electrode 7b) is
For example, it is used as a ground electrode. And counter electrodes 7a, 7
For example, one-turn spiral line electrodes Vi8a and 8b wound in the same direction are connected to b, respectively, and the tips of both spiral line electrodes 8a and 8b are connected to through poles 9 provided on the dielectric substrate 1. electrically connected via. In this way, the resonator 6 is formed.

1−記共振器6においては、第2図に示すように、対向
電極7a、7b間で静電界¥Cが形成され、両スパイラ
ルライン電極8a、8bでインダクタンス1.が形成さ
れ、これによって並列L C共振回路が形成される。
1- In the resonator 6, as shown in FIG. 2, an electrostatic field C is formed between the opposing electrodes 7a and 7b, and an inductance of 1. is formed, thereby forming a parallel LC resonant circuit.

しかも上記共振器6においては、両面のスパイラルライ
ン電極8a、8bを接続することによって巻数が2倍(
この例では2ターン)になっているため大きなインダク
タンス1.を取ることができる。換言すれば、第3図を
参照して、スパイラルライン電極8a、8bを流れる電
流は、ライン81aと81bの間でおよびライン82a
と82bの間で同方向になり、それぞれが相互誘導を起
こして磁界結合する。なおMは磁力線を示す。そのため
、例えば単線とか1ターンの場合に比べて、導体損失の
増加(理論的には1ターンの2倍)に対して蓄えられる
磁界のエネルギーの増加(理論的には1ターンの4倍)
の方が十分大きいため、結果として共振系の00値が上
昇することになる。
Moreover, in the resonator 6, the number of turns can be doubled (
In this example, there are 2 turns), so there is a large inductance 1. can be taken. In other words, with reference to FIG. 3, the current flowing through spiral line electrodes 8a, 8b is between lines 81a and 81b and between lines
and 82b are in the same direction, causing mutual induction and magnetic field coupling. Note that M indicates lines of magnetic force. Therefore, compared to the case of a single wire or one turn, for example, the energy of the magnetic field stored increases (theoretically four times that of one turn) for an increase in conductor loss (theoretically twice that of one turn).
is sufficiently larger, and as a result, the 00 value of the resonance system increases.

実験的にも、単線を用いた場合と比べて約30%程度Q
0値が一ト昇することが確認された。従って上記のよう
な共振器6においては、従来のプリントフィルタに比べ
て同サイズのままで、電気的特性、特に挿入を置火を約
30%程度改善することが可能になる。このことは、言
ってみれば商品価値が高まり市場競争力が強化されるこ
とにもつながる。
Experimentally, the Q is about 30% compared to when using a single wire.
It was confirmed that the 0 value increased by one. Therefore, in the resonator 6 as described above, it is possible to improve the electrical characteristics, especially the insertion and setting, by about 30% while keeping the same size compared to the conventional printed filter. This means that product value increases and market competitiveness is strengthened.

また上記共振器6においては、インダクタンスI、を大
きく取れるため、同し共振周波数の場合でも静電容量C
を小さく、即ち対向電極7a、7bの寸法を小さくする
ことができ、それによって共振器6の寸法を小形にする
こともできる。更に、高誘電率の誘電体基板1を用いれ
ば、対向電極7a、7bの寸法、ひいては共振器6の寸
法を更に小さくすることもできる。
Furthermore, in the resonator 6, since the inductance I can be made large, even at the same resonant frequency, the capacitance C
In other words, the dimensions of the opposing electrodes 7a and 7b can be made small, and thereby the dimensions of the resonator 6 can also be made small. Furthermore, by using the dielectric substrate 1 with a high dielectric constant, the dimensions of the opposing electrodes 7a and 7b and, by extension, the dimensions of the resonator 6 can be further reduced.

第4図は、この発明に係るフィルタの一実施例を部分的
に示す平面図である。このフィルタにおいては、前述し
た共振器6を同一の誘電体基板1に複数(図では2つの
み示した)、互いの対向電極7a、7b同士を接近させ
て並べており、これによって隣り合う共振器6間を静電
容量C3で結合させている。それによって例えば第5図
に示すようなラダー形のバンドパスフィルタを形成して
いる。
FIG. 4 is a plan view partially showing an embodiment of the filter according to the present invention. In this filter, a plurality of the above-mentioned resonators 6 (only two are shown in the figure) are arranged on the same dielectric substrate 1 with their opposing electrodes 7a and 7b close to each other. 6 are coupled by capacitance C3. As a result, a ladder-shaped bandpass filter as shown in FIG. 5, for example, is formed.

この場合、各共振器6の配置の仕方および結合のさセか
たには図示のようなもの以外に種々のものが採り得る。
In this case, various ways of arranging and coupling the resonators 6 may be used in addition to those shown in the drawings.

例えば、隣り合う対向電極7a間を学に接近させるだけ
でなく、図のように対向辺の一部または全部をくし形に
して対向面積を増大させると、上記静電容量C8をより
増大させることもできる。また、隣り合う共振器6にお
いて、一方の共振器6の一方の対向電極(例えば対向電
極7a>と他方の共振器6の他方の対向電極(例えば対
向電極7b)とを共に少し大きくして基板1を挟んで互
いに対向させることによって、それらの電極間における
静電容量で隣接する共振器6間を結合させることもでき
る。また、各共振器6は図示とは反対にスパイラルライ
ン電極8a18bが同じ側に来るように並べても良く、
その場合は主たる電界結合以外に、隣り合うスパイラル
ライン電極8a、8b間における磁界結合を起こさせる
こともできる。
For example, the capacitance C8 can be further increased by not only bringing the adjacent opposing electrodes 7a closer to each other, but also by combing part or all of the opposing sides as shown in the figure to increase the opposing area. You can also do it. In addition, in adjacent resonators 6, one counter electrode (for example, counter electrode 7a) of one resonator 6 and the other counter electrode (for example, counter electrode 7b) of the other resonator 6 are both slightly enlarged so that the substrate By arranging the resonators 6 to face each other across the electrodes, it is possible to couple adjacent resonators 6 by the capacitance between the electrodes.Also, contrary to the illustration, each resonator 6 has the same spiral line electrode 8a18b. You can also arrange them so that they are on the side.
In that case, in addition to the main electric field coupling, it is also possible to cause magnetic field coupling between the adjacent spiral line electrodes 8a and 8b.

上述のようなフィルタにおいても、前述した共振器6の
場合と同様の効果が得られる。即ち、Q0値の向上によ
って電気的特性、特に挿入損失が改善されると共に、寸
法も小形化される。
Even in the filter as described above, the same effect as in the case of the resonator 6 described above can be obtained. That is, by improving the Q0 value, the electrical characteristics, especially the insertion loss, are improved, and the dimensions are also reduced.

〔発明の効果〕〔Effect of the invention〕

以」−のようにこの発明に係る共振器およびそれを用い
たフィルタにおいては、QO(afの向上によって電気
的特性、特に挿入を置火が改善されると共に、寸法も小
形化される。
As described above, in the resonator according to the present invention and the filter using the same, the electrical characteristics, particularly the insertion and heating characteristics, are improved by improving the QO (af), and the size is also reduced.

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

第1図は、この発明に係る共振器の一実施例を示す斜視
図である。第2図は、第1図の共振器の等価回路図であ
る。第3図は、第1図の線m−mに沿う部分断面図であ
る。第4図は、この発明に係るフィルタの一実施例を部
分的に示す平面図である。第5図は、第4図のフィルタ
の等価回路図である。第6図(A)は従来のマイクロス
トリップラインフィルタの一例を示す平面図であり、第
6図(B)はその線B−Bに沿う断面図である。 1・・・誘電体基板、6・・・共振器、?a、7b・・
・対向電極、8a、8b・・・スパイラルライン電極、
9・・・スルーホール 第1図 第2図      第3図 A b 第4図 第5図
FIG. 1 is a perspective view showing an embodiment of a resonator according to the present invention. FIG. 2 is an equivalent circuit diagram of the resonator of FIG. 1. FIG. 3 is a partial cross-sectional view taken along line m--m in FIG. FIG. 4 is a plan view partially showing an embodiment of the filter according to the present invention. FIG. 5 is an equivalent circuit diagram of the filter of FIG. 4. FIG. 6(A) is a plan view showing an example of a conventional microstrip line filter, and FIG. 6(B) is a sectional view taken along the line BB. 1...Dielectric substrate, 6...Resonator, ? a, 7b...
- Counter electrode, 8a, 8b... spiral line electrode,
9...Through hole Figure 1 Figure 2 Figure 3 A b Figure 4 Figure 5

Claims (2)

【特許請求の範囲】[Claims] (1)誘電体基板の両表面に対向電極およびそれにつな
がっていて互いに同方向に巻いたスパイラルライン電極
をそれぞれ設け、両スパイラルライン電極間を誘電体基
板に設けたスルーホールを介して電気的に接続して成る
ことを特徴とする共振器。
(1) A counter electrode and spiral line electrodes connected to it and wound in the same direction are provided on both surfaces of the dielectric substrate, and electrical connection is made between both spiral line electrodes via a through hole provided in the dielectric substrate. A resonator characterized by being connected to each other.
(2)誘電体基板の両表面に対向電極およびそれにつな
がっていて互いに同方向に巻いたスパイラルライン電極
をそれぞれ設け、両スパイラルライン電極間を誘電体基
板に設けたスルーホールを介して電気的に接続して成る
共振器を同一の誘電体基板に複数形成し、隣り合う共振
器間を少なくとも静電容量で結合させて成ることを特徴
とするフィルタ。
(2) A counter electrode and spiral line electrodes connected to it and wound in the same direction are provided on both surfaces of the dielectric substrate, and electrical connection is made between both spiral line electrodes via a through hole provided in the dielectric substrate. A filter characterized in that a plurality of connected resonators are formed on the same dielectric substrate, and adjacent resonators are coupled by at least capacitance.
JP18450885A 1985-08-22 1985-08-22 Resonator and filter using it Pending JPS6243909A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18450885A JPS6243909A (en) 1985-08-22 1985-08-22 Resonator and filter using it

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18450885A JPS6243909A (en) 1985-08-22 1985-08-22 Resonator and filter using it

Publications (1)

Publication Number Publication Date
JPS6243909A true JPS6243909A (en) 1987-02-25

Family

ID=16154417

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18450885A Pending JPS6243909A (en) 1985-08-22 1985-08-22 Resonator and filter using it

Country Status (1)

Country Link
JP (1) JPS6243909A (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0410406U (en) * 1990-05-15 1992-01-29
JPH05338581A (en) * 1992-02-27 1993-12-21 Bg Innovation Sarl Gear shifting device for cycle having chain and pinion transmission
US5365432A (en) * 1990-11-30 1994-11-15 Atsugi Unisia Corporation System and method for optimally controlling damping force characteristics of front and rear suspension units of four-wheeled vehicle
US5425436A (en) * 1992-08-26 1995-06-20 Nippondenso Co., Ltd. Automotive suspension control system utilizing variable damping force shock absorber
EP1168483A2 (en) * 2000-06-26 2002-01-02 Murata Manufacturing Co., Ltd. Resonator, filter, duplexer, and communication device
JP2009055161A (en) * 2007-08-24 2009-03-12 Panasonic Corp Resonator, and filter and electronic apparatus using same
JP2010232765A (en) * 2009-03-26 2010-10-14 Fujikura Ltd Electric circuit equipped with inductor and capacitor
JP2019186696A (en) * 2018-04-06 2019-10-24 株式会社村田製作所 Electronic component

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0410406U (en) * 1990-05-15 1992-01-29
US5365432A (en) * 1990-11-30 1994-11-15 Atsugi Unisia Corporation System and method for optimally controlling damping force characteristics of front and rear suspension units of four-wheeled vehicle
JPH05338581A (en) * 1992-02-27 1993-12-21 Bg Innovation Sarl Gear shifting device for cycle having chain and pinion transmission
US5425436A (en) * 1992-08-26 1995-06-20 Nippondenso Co., Ltd. Automotive suspension control system utilizing variable damping force shock absorber
EP1168483A2 (en) * 2000-06-26 2002-01-02 Murata Manufacturing Co., Ltd. Resonator, filter, duplexer, and communication device
EP1168483A3 (en) * 2000-06-26 2003-08-06 Murata Manufacturing Co., Ltd. Resonator, filter, duplexer, and communication device
JP2009055161A (en) * 2007-08-24 2009-03-12 Panasonic Corp Resonator, and filter and electronic apparatus using same
JP2010232765A (en) * 2009-03-26 2010-10-14 Fujikura Ltd Electric circuit equipped with inductor and capacitor
JP2019186696A (en) * 2018-04-06 2019-10-24 株式会社村田製作所 Electronic component

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