JPH02277302A - Magnetic field coupling loop - Google Patents

Magnetic field coupling loop

Info

Publication number
JPH02277302A
JPH02277302A JP9811189A JP9811189A JPH02277302A JP H02277302 A JPH02277302 A JP H02277302A JP 9811189 A JP9811189 A JP 9811189A JP 9811189 A JP9811189 A JP 9811189A JP H02277302 A JPH02277302 A JP H02277302A
Authority
JP
Japan
Prior art keywords
connector
dielectric resonator
magnetic field
conductor wire
coupling loop
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
JP9811189A
Other languages
Japanese (ja)
Inventor
Asao Ito
朝男 伊藤
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP9811189A priority Critical patent/JPH02277302A/en
Publication of JPH02277302A publication Critical patent/JPH02277302A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To change the distance between a magnetic field coupling loop and a dielectric resonator without moving the position of the dielectric resonator by using a conductor wire with an optional length so as to vary the coupling with the dielectric resonator. CONSTITUTION:One terminal of a conductor wire 5 is soldered to a fixture 4 and the other terminal is soldered to center conductor of a connector 3. The magnetic field coupling loop is formed by the center conductor 6, the conductor wire 5 and the fixture 4 and applies magnetic coupling to an electromagnetic wave inputted/outputted through the connector 3 to the dielectric resonator 2. In this case, when the conductor wire 5 with a long length is employed, the size of the magnetic field coupling loop is increased and the coupling is strengthened and when the conductor wire 5 with a short length is employed, the coupling is decreased. Thus, the coupling of the electromagnetic wave inputted/outputted through the connector 3 with the dielectric resonator 2 is varied optionally in any case by varying the length of the conductor wire 5.

Description

【発明の詳細な説明】 〔概要〕 誘電体フィルタなど金属ケースに内蔵された誘電体共振
器に、コネクタから入出力する電磁波を磁界結合させる
装置の磁界結合ループに関し、誘電体共振器の位置を動
かすことなしに磁界結合ループと誘電体共振器との間隔
を容易に変更することが出来て且つ外部からの振動にも
影響されない構造の磁界結合ループを目的とし、電磁波
を入出力するコネクタを、誘電体共振器を内蔵する金属
ケースに固定する半田付は可能な金具に、任意の長さの
導体線の一端を半田付けし、他端を該コネクタの中心導
体に半田付けするように構成する。
[Detailed Description of the Invention] [Summary] Regarding the magnetic field coupling loop of a device that magnetically couples electromagnetic waves input and output from a connector to a dielectric resonator built in a metal case such as a dielectric filter, the position of the dielectric resonator is determined. A connector that inputs and outputs electromagnetic waves is designed for the purpose of a magnetic coupling loop with a structure that allows the distance between the magnetic coupling loop and the dielectric resonator to be easily changed without moving it, and is not affected by external vibrations. One end of a conductor wire of any length is soldered to a metal fitting that can be soldered to fix it to a metal case containing a dielectric resonator, and the other end is soldered to the center conductor of the connector. .

〔産業上の利用分野〕[Industrial application field]

本発明は磁界結合する誘電体フィルタ等に係り、特にコ
ネクタから入出力する電磁波を誘電体フィルタ等の誘電
体共振器に磁界結合させる磁界結合ループに関する。
The present invention relates to a dielectric filter and the like that perform magnetic field coupling, and particularly to a magnetic field coupling loop that magnetically couples electromagnetic waves input and output from a connector to a dielectric resonator such as a dielectric filter.

近年、マイクロ波通信装置の小形化に伴い、マイクロ波
共振器は、空洞共振器から誘電体共振器へ移行し、複数
の共振器で構成されるフィルタも、誘電体共振器を用い
た誘電体フィルタが普及しつつある。誘電体フィルタで
は、入出力のコネクタから入出力される電磁波を誘電体
共振器に結合させる必要があるため、磁界結合ループが
用いられるが、この磁界結合ループは、誘電体フィルタ
の特性を所要特性に調整するため、結合ループの大きさ
を変更できるような構造になっている必要がある。
In recent years, with the miniaturization of microwave communication devices, microwave resonators have shifted from cavity resonators to dielectric resonators, and filters composed of multiple resonators have also changed to dielectric resonators using dielectric resonators. Filters are becoming popular. In dielectric filters, it is necessary to couple electromagnetic waves input and output from input and output connectors to dielectric resonators, so a magnetic coupling loop is used. The structure must be such that the size of the coupling loop can be changed in order to adjust the

〔従来の技術〕[Conventional technology]

この磁界結合ループは従来、第3図に示す如く、金属ケ
ースlに取付けられたコネクタ3から入出力する電磁波
を該コネクタの中心導体6と該中心導体の尖端を金属ケ
ース1に接続する金属棒7とからなる磁界結合ループに
よって、誘電体共振器2に磁界結合させる構造となって
いる。
As shown in FIG. 3, this magnetic field coupling loop conventionally connects electromagnetic waves input and output from a connector 3 attached to a metal case 1 to a center conductor 6 of the connector and a metal rod connecting the tip of the center conductor to the metal case 1. The dielectric resonator 2 is magnetically coupled to the dielectric resonator 2 by a magnetic coupling loop consisting of 7 and 7.

ところが、磁界結合ループの金属棒7は金属ケース1に
ネジ止めで接続されているため、磁界結合ループの大き
さが固定されてしまい、結合ルプの大きさの変更は困難
である。その結果、誘電体フィルタの特性を調整するた
め磁界結合ループと誘電体共振器2との間隔を変えるに
は、誘電体共振器2の位置を変えることが考えられるが
、誘電体フィルタは、一般に誘電体共振器の複数個を並
べた構造になっていて、それら複数個の誘電体共振器の
相互の間隔も、フィルタ特性の上から重要な要素である
ため変化させる必要があるが、個々の共振器の相互の間
隔を含めて誘電体共振器2の位置を動かして、磁界結合
ループとの間隔を変えることは事実」−は不可能である
However, since the metal rod 7 of the magnetic field coupling loop is screwed to the metal case 1, the size of the magnetic field coupling loop is fixed, and it is difficult to change the size of the coupling loop. As a result, in order to change the distance between the magnetic field coupling loop and the dielectric resonator 2 in order to adjust the characteristics of the dielectric filter, it is possible to change the position of the dielectric resonator 2. It has a structure in which multiple dielectric resonators are lined up, and the mutual spacing between these multiple dielectric resonators is also an important element in terms of filter characteristics, so it must be changed. In fact, it is not possible to change the position of the dielectric resonator 2, including the mutual spacing of the resonators, to change the spacing from the magnetic coupling loop.

また、磁界結合ループと誘電体共振器2との間隔を変え
られるような磁界結合ループの構造とするため、図示し
ないが金属棒7の代りに細い導体線を用い、その導体線
の一端をコネクタ3の中心導体6に半田付けし、他端は
固定せずに自由に動くようにした構造のものもあるが、
そのような構造の磁界結合ループは、外部からの振動に
影響され易く特性が安定し7ないという問題があった。
In addition, in order to create a magnetic field coupling loop structure in which the distance between the magnetic field coupling loop and the dielectric resonator 2 can be changed, a thin conductor wire (not shown) is used instead of the metal rod 7, and one end of the conductor wire is connected to a connector. There is also a structure in which the center conductor 6 of 3 is soldered and the other end is not fixed and can move freely.
A magnetic field coupling loop having such a structure has a problem in that it is easily influenced by external vibrations and its characteristics are unstable.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

本発明は、誘電体共振器の位置を動かずことなしに、磁
界結合ループと誘電体共振器との間隔を容易に変更する
ことが出来て、且つ外部からの振動にも影響されない構
造の磁界結合ループの提供を課題とする。
The present invention provides a magnetic field structure that allows the distance between the magnetic field coupling loop and the dielectric resonator to be easily changed without moving the position of the dielectric resonator, and that is not affected by external vibrations. The challenge is to provide a bonding loop.

〔課題を解決するための手段〕[Means to solve the problem]

この課題は、第1図に示す如く、コネクタ3を金属ケー
ス1に半田付けが可能な金具4によゲで固定し、該金具
4に、任意の長さの導体線5の−・端を半田付けし、他
端を該コネクタの中心導体6に半田付けするように構成
した本発明の磁界結合ループによって解決される。
As shown in FIG. 1, this problem involves fixing a connector 3 to a metal case 1 with a metal fitting 4 that can be soldered, and attaching the negative end of a conductor wire 5 of an arbitrary length to the metal fitting 4. This is solved by the magnetic field coupling loop of the invention, which is configured to be soldered and the other end soldered to the center conductor 6 of the connector.

本発明の磁界結合ループの構成を示す第1図の原理図に
おいて、 1は、誘電体共振器2を内部に持ち、電磁波を人出力す
るコネクタ3を取り伺けた金属ケースである。
In the principle diagram of FIG. 1 showing the configuration of the magnetic field coupling loop of the present invention, 1 is a metal case that has a dielectric resonator 2 inside and has a connector 3 for outputting electromagnetic waves.

2は、金属ゲース1の内部に設LJられ、コネクタ3か
ら入出力する電磁波とループで磁界結合し、共振する誘
電体共振器である。
Reference numeral 2 denotes a dielectric resonator that is installed inside the metal gate 1, magnetically coupled with the electromagnetic waves input and output from the connector 3 through a loop, and resonates.

3は、金属ケース1に取り伺は固定され、誘電体共振器
2に磁界結合する電磁波を入出力するコネクタである。
Reference numeral 3 denotes a connector which is fixed to the metal case 1 and inputs and outputs electromagnetic waves that are magnetically coupled to the dielectric resonator 2.

4は、コネクタ3を金属ケース1に固定する半田付けが
可能な金具である。
Reference numeral 4 denotes a solderable metal fitting for fixing the connector 3 to the metal case 1.

5は、一端がコネクタ3の中心導体6に半田付けされ、
他端が金具4に半田付けされる長さが任意に設定される
導体線である。
5 has one end soldered to the center conductor 6 of the connector 3,
It is a conductor wire whose length is arbitrarily set and whose other end is soldered to the metal fitting 4.

6は、導体線5の一端が半田付けされるコネクタ3の中
心導体である。
6 is the center conductor of the connector 3 to which one end of the conductor wire 5 is soldered.

〔作用〕[Effect]

導体線5は、その長さが任意に設定され、その一端がコ
ネクタ3の中心導体6に半田付けされ、他端が金具4に
半田付けされるので、コネクタ3から入出力する電磁波
を誘電体共振器2に強く結合させる場合は、導体線5の
長さを長くしコネクタ3の中心導体6と金具4との間で
形成する導体線ループの大きさを大きくする。逆に誘電
体共振器2との結合を弱くする場合は、導体線5の長さ
を短くしコネクタ3の中心導体6と金具4との間で形成
する導体線ループの大きさを小さくする。
The length of the conductor wire 5 is arbitrarily set, and one end of the conductor wire 5 is soldered to the center conductor 6 of the connector 3, and the other end is soldered to the metal fitting 4, so that the electromagnetic waves input and output from the connector 3 are transferred to the dielectric. For strong coupling to the resonator 2, the length of the conductor wire 5 is increased to increase the size of the conductor wire loop formed between the center conductor 6 of the connector 3 and the metal fitting 4. Conversely, in order to weaken the coupling with the dielectric resonator 2, the length of the conductor wire 5 is shortened to reduce the size of the conductor wire loop formed between the center conductor 6 of the connector 3 and the metal fitting 4.

何れにしても誘電体共振器2を動かずことなくコネクタ
3から入出力する電磁波の1六重体共振器2への結合を
任意に変えられ、且つ両端が半rII付けで固定される
ので外部からの振動の影響は少なくて問題は解決される
In any case, the coupling of the electromagnetic waves input and output from the connector 3 to the hexaplex resonator 2 can be changed arbitrarily without moving the dielectric resonator 2, and since both ends are fixed with half-rII connections, it is possible to control the connection from the outside. The problem is solved because the influence of vibration is small.

〔実施例〕〔Example〕

第1図の原理図は、そのまま本発明の実施例の磁界結合
ループの構成を示す断面図であり、第2図はその側面図
である。
The principle diagram in FIG. 1 is a sectional view showing the configuration of a magnetic field coupling loop according to an embodiment of the present invention, and FIG. 2 is a side view thereof.

図中、従来例の第3図で示したものと同一のものは、同
一記号で示してあり、■は金属ケース、2は誘電体共振
器、3はコネクタであって、例えば小形のSMA型同軸
コネクタ、4は半田付は可能な金具、5は長さが任意に
設定される導体線、6はコネクタ3の中心導体である。
In the figure, the same parts as those shown in FIG. 3 of the conventional example are indicated by the same symbols, and ■ is a metal case, 2 is a dielectric resonator, and 3 is a connector, such as a small SMA type. The coaxial connector includes a metal fitting 4 that can be soldered, a conductor wire 5 whose length can be arbitrarily set, and a center conductor 6 of the connector 3.

金具4は、金属ケース1の内側からコネクタ3をネジ止
めし、また金具4には導体線5の一端が半田付けされて
いる。導体線5の他端はコネクタ3の中心導体6に半田
付けされている。
The connector 3 is screwed to the metal fitting 4 from inside the metal case 1, and one end of a conductor wire 5 is soldered to the metal fitting 4. The other end of the conductor wire 5 is soldered to the center conductor 6 of the connector 3.

中心導体6と導体線5と金具4とにより磁界結合ループ
が形成され、コネクタ3を通して入出力される電磁波を
、金属ケース1に接着剤などで接着されている誘電体共
振器2に、磁界結合させる働きをする。
A magnetic field coupling loop is formed by the center conductor 6, the conductor wire 5, and the metal fitting 4, and the electromagnetic waves input and output through the connector 3 are magnetically coupled to the dielectric resonator 2 bonded to the metal case 1 with adhesive or the like. It works to make things happen.

この時、導体線5として長さの長いものを用いれば、磁
界結合ループは大きくなり、誘電体共振器2に近づくの
で、結合は強くなり、逆に、導体線5として長さの短い
ものを用いれば、磁界結合ループは小さくなり、誘電体
共振器2から遠のくので、結合は弱くなる。
At this time, if a long wire is used as the conductor wire 5, the magnetic field coupling loop will be large and it will come closer to the dielectric resonator 2, so the coupling will be stronger; conversely, if a wire with a short length is used as the conductor wire 5. If used, the magnetic field coupling loop becomes smaller and moves away from the dielectric resonator 2, so that the coupling becomes weaker.

何れにしても誘電体共振器2を動かすことなくコネクタ
3から入出力される電磁波の誘電体共振器2への結合を
導体線5の長さを変えて任意に変えられるし、且つ導体
線5の両端が半田付けで固定されるので、外部からの振
動で影響されることが少なくて特性は安定するので問題
は無い。
In any case, the coupling of electromagnetic waves input and output from the connector 3 to the dielectric resonator 2 can be changed arbitrarily by changing the length of the conductor wire 5 without moving the dielectric resonator 2. Since both ends are fixed by soldering, there is no problem because it is less affected by external vibrations and the characteristics are stable.

〔発明の効果〕〔Effect of the invention〕

以上説明した如く、本発明によれば、誘電体共振器を動
かすことなく、入出力する電磁波の誘電体共振器への結
合を任意の長さの導体線の半田付けで簡単に変えられる
ので、誘電体共振器を用いた誘電体フィルタを所要特性
に調整する作業が容易となり、かつ導体線の両端が半1
月伺すなので外部からの振動に強くなり、誘電体フィル
タの特性の向上と製造コストの低減の効果がある。
As explained above, according to the present invention, the coupling of input and output electromagnetic waves to the dielectric resonator can be easily changed by soldering conductor wires of arbitrary length without moving the dielectric resonator. It is easy to adjust the dielectric filter using a dielectric resonator to the required characteristics, and both ends of the conductor wire are
Since it is made of a lunar metal, it is resistant to external vibrations, which improves the characteristics of the dielectric filter and reduces manufacturing costs.

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

第1図は本発明の磁界結合ループの構成を示す原理図、 第2図は本発明の実施例の磁界結合ループの構成を示す
側面図、 第3図は従来の磁界結合ループの構成を示す断面図であ
る。 図において、 1は金属ケース、2は誘電体共振器、3はコネクタ、4
は金具、5ば導体線、6は中心導体、7は金属棒である
。 (断面間) 猪 1 口 (第10め縄界粘合ゾループのイ則面M)第 従天の磁界銘菅ループめ構成友亦T断面図部 3図
Figure 1 is a principle diagram showing the configuration of the magnetic field coupling loop of the present invention, Figure 2 is a side view showing the configuration of the magnetic field coupling loop of the embodiment of the present invention, and Figure 3 is a diagram showing the configuration of the conventional magnetic field coupling loop. FIG. In the figure, 1 is a metal case, 2 is a dielectric resonator, 3 is a connector, and 4
5 is a metal fitting, 5 is a conductor wire, 6 is a center conductor, and 7 is a metal rod. (Between cross-sections) Boar 1 Mouth (I-law surface M of the 10th menawakai cohesive sol loop) Magnetic field signature of the 1st subtenth Suga loop me configuration friend T cross-sectional view part 3

Claims (1)

【特許請求の範囲】  金属ケース(1)の内部に設けられた誘電体共振器(
2)に、コネクタ(3)から入出力する電磁波を磁界結
合させる装置において、 該コネクタを該金属ケースに固定する半田付け可能な金
具(4)に、任意の長さの導体線(5)の一端を半田付
けし、他端を該コネクタの中心導体(6)に半田付けし
たことを特徴とした磁界結合ループ。
[Claims] A dielectric resonator (
2) In a device that magnetically couples electromagnetic waves input and output from a connector (3), a conductor wire (5) of any length is attached to a solderable metal fitting (4) that fixes the connector to the metal case. A magnetic coupling loop characterized in that one end is soldered and the other end is soldered to the central conductor (6) of the connector.
JP9811189A 1989-04-18 1989-04-18 Magnetic field coupling loop Pending JPH02277302A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9811189A JPH02277302A (en) 1989-04-18 1989-04-18 Magnetic field coupling loop

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9811189A JPH02277302A (en) 1989-04-18 1989-04-18 Magnetic field coupling loop

Publications (1)

Publication Number Publication Date
JPH02277302A true JPH02277302A (en) 1990-11-13

Family

ID=14211214

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9811189A Pending JPH02277302A (en) 1989-04-18 1989-04-18 Magnetic field coupling loop

Country Status (1)

Country Link
JP (1) JPH02277302A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5457087A (en) * 1992-08-21 1995-10-10 E. I. Du Pont De Nemours And Company High temperature superconducting dielectric resonator having mode absorbing means
US6239673B1 (en) 1995-03-23 2001-05-29 Bartley Machines & Manufacturing Dielectric resonator filter having reduced spurious modes

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5457087A (en) * 1992-08-21 1995-10-10 E. I. Du Pont De Nemours And Company High temperature superconducting dielectric resonator having mode absorbing means
US5563505A (en) * 1992-08-21 1996-10-08 E. I. Du Pont De Nemours And Company Apparatus for characterizing high temperature superconducting thin film
US6239673B1 (en) 1995-03-23 2001-05-29 Bartley Machines & Manufacturing Dielectric resonator filter having reduced spurious modes

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