JPS6160601B2 - - Google Patents

Info

Publication number
JPS6160601B2
JPS6160601B2 JP20858781A JP20858781A JPS6160601B2 JP S6160601 B2 JPS6160601 B2 JP S6160601B2 JP 20858781 A JP20858781 A JP 20858781A JP 20858781 A JP20858781 A JP 20858781A JP S6160601 B2 JPS6160601 B2 JP S6160601B2
Authority
JP
Japan
Prior art keywords
conductor
dielectric material
dielectric
resonator
coaxial
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
JP20858781A
Other languages
Japanese (ja)
Other versions
JPS58108801A (en
Inventor
Jukichi Aihara
Toshiharu Noguchi
Mitsuo Makimoto
Sadahiko Yamashita
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 JP20858781A priority Critical patent/JPS58108801A/en
Publication of JPS58108801A publication Critical patent/JPS58108801A/en
Publication of JPS6160601B2 publication Critical patent/JPS6160601B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P7/00Resonators of the waveguide type
    • H01P7/04Coaxial resonators

Description

【発明の詳細な説明】 本発明は、同軸形誘電体共振器に関するもので
あり、小型で、耐振特性が優れ、製造バラツキの
少ない同軸形誘電体共振器を提供するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a coaxial dielectric resonator, and provides a coaxial dielectric resonator that is small in size, has excellent vibration resistance characteristics, and has little manufacturing variation.

従来、同軸形共振器として、高誘電率材料で波
長短絡されたλ/4又はλ/2同軸線路で共振器を構成
し たものがある。これらの共振器では、整数倍周波
数で高次スプリアス共振が顕著に現われるという
欠点を持つ。これを改善するため、従来では第1
図に示すように1/2共振器で誘電率の異なる誘電
体材料3及び4を、外導体2と内導体1との間に
設けることが試みられているが、このような構成
では、実際に共振器を組立てる際、異なる誘電体
相互の接着、固定が不確実なものとなり、また共
振周波数の調整や、共振器のより一層の小型化を
意図した場合は不利な点を有する。
Conventionally, as a coaxial resonator, there is a resonator configured with a λ/4 or λ/2 coaxial line whose wavelength is short-circuited using a high dielectric constant material. These resonators have the disadvantage that high-order spurious resonances appear prominently at integral multiple frequencies. In order to improve this, conventionally the first
As shown in the figure, an attempt has been made to provide dielectric materials 3 and 4 with different dielectric constants between the outer conductor 2 and the inner conductor 1 in a 1/2 resonator, but such a configuration is not practical. When assembling a resonator, the adhesion and fixing of different dielectrics to each other becomes uncertain, and there are also disadvantages when adjusting the resonant frequency or making the resonator more compact.

また他の従来例として第2図に示す如く、筒状
外導体6の中に中心導体5を一端開放、他端短絡
に形成し、開放端側の一部に誘電体材料4を装架
したものが考えられている。この方法では、上記
の問題点はほぼ解決しているものの、実際の組立
てには、バラツキを考慮して、材料にかなりの加
工精度を要求する。すなわち、内、外導体間に誘
電体を挿入するため、導体壁面と材料との間に僅
かな隙間が生じ、これが、共振周波数に大きな影
響を与え、また耐振特性、温度特性を不安定なも
のにする。本発明は、これらのさまざまな欠点を
除去する共振器を提供するものであり、更に、小
型化、高Q化という点で有利な共振器を提供する
ものである。
As another conventional example, as shown in FIG. 2, a center conductor 5 is formed in a cylindrical outer conductor 6 with one end open and the other end short-circuited, and a dielectric material 4 is mounted on a part of the open end side. Things are being thought of. Although this method largely solves the above problems, actual assembly requires consideration of variations and requires considerable machining accuracy of the material. In other words, since a dielectric material is inserted between the inner and outer conductors, a small gap is created between the conductor wall surface and the material, which has a large effect on the resonant frequency and also makes the vibration resistance and temperature characteristics unstable. Make it. The present invention provides a resonator that eliminates these various drawbacks, and further provides a resonator that is advantageous in terms of miniaturization and high Q.

以下、図面を参照しながら本発明の一実施例を
詳細に説明する。第3図および第4図は、本発明
の一実施例を示し、第3図の形状の誘電体材料3
と第4図の形状の誘電体材料4を別個に用意す
る。これらはプレス成形して焼結すれば、容易に
量産できる。そして、第3図に示す誘電体材料3
の凸部7に第4図に示す誘電体材料4をはめ込む
のであるが、その際、誘電体材料4の内周面には
導体層8を形成するべく銀ペースト等を塗布し、
それと接する誘電体材料3の凸部7の表面にも同
様な処理をして導体層9を設ける。第3図、第4
図に示す二つの誘電体材料3及び4を嵌合させた
本発明の共振器の構造を第5図に示す。この場
合、誘電体材料3及び4を嵌合後、誘電体材料3
及び4の外周に外部導体被膜を形成し外導体10
とし、誘電体材料3の内周面に内部導体被膜を形
成して内導体11とし、さらに一端面には導体被
膜12を形成して外部導体被膜10と内部導体被
膜11を接続し、他端面には内部導体被膜11と
導体層8または9とを接続するごとく導体被膜1
3を形成する。これら導体被膜としては銀ペース
ト等を使用し、塗布後高温炉で焼付けを行い電気
伝導度の良い導体被膜を形成する。導体層8及び
9を介して接する誘電体材料3と誘電体材料4と
の間の間隙は、スキンデプスの数倍以上あればよ
く、普通20μmから100μm位にとる。この場
合、組立てが容易であるのみならず、誘電体材料
3,4間に導体が充填されるので共振周波数バラ
ツキもない利点がある。また二つの誘電体材料が
堅固に接着固定される利点もある。
Hereinafter, one embodiment of the present invention will be described in detail with reference to the drawings. 3 and 4 show an embodiment of the present invention, in which a dielectric material 3 having the shape shown in FIG.
A dielectric material 4 having the shape shown in FIG. 4 is separately prepared. These can be easily mass-produced by press forming and sintering. Then, the dielectric material 3 shown in FIG.
The dielectric material 4 shown in FIG. 4 is fitted into the convex portion 7 of the dielectric material 4. At that time, a silver paste or the like is applied to the inner peripheral surface of the dielectric material 4 to form a conductive layer 8.
A conductor layer 9 is provided on the surface of the convex portion 7 of the dielectric material 3 in contact with the convex portion 7 by performing similar treatment. Figures 3 and 4
FIG. 5 shows the structure of the resonator of the present invention in which the two dielectric materials 3 and 4 shown in the figure are fitted together. In this case, after fitting dielectric materials 3 and 4, dielectric material 3
An outer conductor coating is formed on the outer periphery of the outer conductor 10 and 4.
Then, an inner conductor coating is formed on the inner peripheral surface of the dielectric material 3 to form an inner conductor 11, and a conductor coating 12 is further formed on one end surface to connect the outer conductor coating 10 and the inner conductor coating 11. A conductor film 1 is provided to connect the inner conductor film 11 and the conductor layer 8 or 9.
form 3. Silver paste or the like is used for these conductor coatings, and after application, baking is performed in a high temperature furnace to form a conductor coating with good electrical conductivity. The gap between the dielectric material 3 and the dielectric material 4, which are in contact with each other through the conductor layers 8 and 9, may be several times the skin depth or more, and is usually about 20 μm to 100 μm. In this case, there is an advantage that not only is assembly easy, but also there is no variation in resonance frequency since the conductor is filled between the dielectric materials 3 and 4. Another advantage is that the two dielectric materials are firmly bonded and fixed.

さらに本共振器は第5図にみられるように、誘
電体材料3と誘電体材料4との接着を導体層8及
び9を利用して行うため、結果的に二重同軸形共
振器となり、第1図に示した従来の共振器より大
巾な小型化が達成される。また、空間を最大限に
利用できるので、Qの劣化は少ない。誘電体材料
3としては誘電率は低けても誘電体損失のできる
だけ小さい材料がよい。アルミナやフオルステラ
イトのような安価で安定な材料が適する。一方、
誘電体材料4としては、使用する体積も小さく、
小型化をはかる為に誘電体材料3に比べて誘電率
が同じかそれ以上の材料が適する。共振条件は式
1で与えられる。
Furthermore, as shown in FIG. 5, this resonator uses conductor layers 8 and 9 to bond dielectric material 3 and dielectric material 4, resulting in a double coaxial resonator. A greater reduction in size than the conventional resonator shown in FIG. 1 is achieved. Further, since the space can be utilized to the maximum, there is little deterioration in Q. As the dielectric material 3, it is preferable to use a material that has as little dielectric loss as possible even if the dielectric constant is low. Cheap and stable materials such as alumina and forsterite are suitable. on the other hand,
As the dielectric material 4, the volume used is small,
In order to achieve miniaturization, a material having a dielectric constant equal to or higher than that of the dielectric material 3 is suitable. The resonance condition is given by Equation 1.

K3=tanβ1l1+(K2・sinβ1l2 /cosβl1)・tanβ3l3 …(1) 但し β:位相定数 β=2πo√r1/c β=2πo√r2/c (o:共振周波数、c:光速度) ここで、誘電体材料3,4の比誘電率をεr1
εr2とし、誘電体材料3の内導体半径γa、誘電
体材料4の内導体半径をγb1、外導体半径をγb
としている。
K 3 = tanβ 1 l 1 + (K 2・sinβ 1 l 2 /cosβl 1 )・tanβ 3 l 3 …(1) However, β: Phase constant β=2πo√ r1 /c β=2πo√ r2 /c (o: resonance frequency, c: speed of light) Here, the relative permittivity of the dielectric materials 3 and 4 is ε r1 ,
ε r2 , the inner conductor radius of dielectric material 3 is γa, the inner conductor radius of dielectric material 4 is γb 1 , and the outer conductor radius is γb.
It is said that

これによれば、例えば、誘電体材料3にフオル
ステライト(εr=6)を用い、誘電体材料4に
高誘電率材料(εr=85)を用いれば、共振器長
を1/10以下に短縮することができる。
According to this, for example, if forsterite (εr=6) is used as the dielectric material 3 and a high permittivity material (εr=85) is used as the dielectric material 4, the resonator length can be reduced to 1/10 or less. can do.

第4図に本発明の他の実施例を示す、これは誘
電体材料4を△lだけ長めに形成したもので、こ
の部分を研摩等によつて変化させることにより、
共振器を高温銀焼き付け完成後でも、共振周波数
を調整することができる。
FIG. 4 shows another embodiment of the present invention, in which the dielectric material 4 is made longer by Δl, and by changing this part by polishing or the like,
The resonant frequency can be adjusted even after the resonator has been baked with high-temperature silver.

以上述べたように、本発明によれば、整数倍高
次スプリアスのない小型、高Qの共振器を再現性
よく、容易な組立て法で構成できる。本発明は二
重同軸形共振器という、性能は優れてはいるがや
や複雑な構成をもつ共振器を、二種頼の誘電体の
接着固定の作用と同時に実現しており、極めて有
益な共振器を提供するものである。
As described above, according to the present invention, a small, high-Q resonator free of integer multiple higher-order spurious can be constructed with good reproducibility and by an easy assembly method. The present invention realizes a double coaxial resonator, which has excellent performance but has a slightly complicated structure, at the same time as the effect of adhesion and fixation of two types of dielectric materials, and extremely useful resonance. It provides equipment.

なお、上記実施例では、軸に垂直な断面は円形
と仮定したが、矩形でも同様な効果が得られるの
は言う迄もない。
In the above embodiment, it is assumed that the cross section perpendicular to the axis is circular, but it goes without saying that the same effect can be obtained even if the cross section is rectangular.

本発明による共振器は、あらゆる電気通信機器
などにおいて、利用することができる。特に最近
の機器の小型化の趨勢に呼応して、フイルタ、発
振器等に応用され、量産効果も期待され、工業上
極めて有益である。
The resonator according to the present invention can be used in all kinds of telecommunication equipment. In particular, in response to the recent trend of miniaturization of equipment, it is applied to filters, oscillators, etc., and is expected to be effective in mass production, making it extremely useful industrially.

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

第1図および第2図aは従来の同軸型誘電体共
振器の縦断面図、同b図は同横断面図、第3図及
び第4図aは本発明の同軸型誘電体共振器に使用
される部品の縦断面図、同bは同横断面図、第5
図Aは本発明の第1の実施例における誘電体共振
器の縦断面図、同bは同横断面図、第6図は本発
明の他の実施例を示す縦断面図である。 3,4……誘電体材料、8,9……導体層、1
0……外導体、11……内導体、12,13……
導体被膜。
Figures 1 and 2a are vertical cross-sectional views of a conventional coaxial dielectric resonator, Figures 2b and 4a are cross-sectional views of the same, and Figures 3 and 4a are views of the coaxial dielectric resonator of the present invention. A vertical cross-sectional view of the parts used, b is a cross-sectional view of the same, No.
Figure A is a longitudinal cross-sectional view of a dielectric resonator according to a first embodiment of the present invention, Figure B is a cross-sectional view thereof, and Figure 6 is a vertical cross-sectional view showing another embodiment of the present invention. 3, 4... Dielectric material, 8, 9... Conductor layer, 1
0... Outer conductor, 11... Inner conductor, 12, 13...
conductor coating.

Claims (1)

【特許請求の範囲】 1 内導体を有する第1の誘電体材料の開放端部
が突出部を有しており、前記突出部に、導体層を
介して嵌合されるリング状の第2の誘電体材料を
設け、前記第1及び第2の誘電体材料の外周部に
外導体が形成されており、前記外導体と内導体と
が短絡端面に設けられた導体被膜により接続され
ており、さらに前記導体層と内導体とが開放端面
に設けられた導体被膜により接続されていること
を特徴とする同軸型誘電体共振器。 2 第1の誘電体材料の突出部とリング状の第2
の誘電体材料の内周面との嵌合部に設けられた導
体層がスキンデプスより充分厚い銀ペースト等の
良導体で形成されていることを特徴とする特許請
求の範囲第1項記載の同軸型誘電体共振器。 3 第2の誘電体材料の誘電率が、第1の誘電体
材料のそれより同じか、それ以上の大なる値にし
たことを特徴とする特許請求の範囲第1項または
第2項記載の同軸型誘電体共振器。 4 第2の誘電体材料の軸方向の端面を、第1の
誘電体材料の開放端面より突出させたことを特徴
とする特許請求の範囲第1項または第2項記載の
同軸型誘電体共振器。
[Claims] 1. An open end of a first dielectric material having an inner conductor has a protrusion, and a ring-shaped second material is fitted into the protrusion through a conductor layer. A dielectric material is provided, an outer conductor is formed on the outer periphery of the first and second dielectric materials, and the outer conductor and the inner conductor are connected by a conductor coating provided on the shorted end surface, Furthermore, the coaxial dielectric resonator is characterized in that the conductor layer and the inner conductor are connected by a conductor coating provided on the open end surface. 2 The protrusion of the first dielectric material and the ring-shaped second
The coaxial according to claim 1, wherein the conductive layer provided at the fitting portion with the inner circumferential surface of the dielectric material is formed of a good conductor such as silver paste which is sufficiently thicker than the skin depth. type dielectric resonator. 3. Claims 1 or 2, characterized in that the dielectric constant of the second dielectric material is equal to or greater than that of the first dielectric material. Coaxial dielectric resonator. 4. Coaxial dielectric resonance according to claim 1 or 2, characterized in that the axial end face of the second dielectric material projects from the open end face of the first dielectric material. vessel.
JP20858781A 1981-12-22 1981-12-22 Coaxial type dielectric resonator Granted JPS58108801A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20858781A JPS58108801A (en) 1981-12-22 1981-12-22 Coaxial type dielectric resonator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20858781A JPS58108801A (en) 1981-12-22 1981-12-22 Coaxial type dielectric resonator

Publications (2)

Publication Number Publication Date
JPS58108801A JPS58108801A (en) 1983-06-29
JPS6160601B2 true JPS6160601B2 (en) 1986-12-22

Family

ID=16558653

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20858781A Granted JPS58108801A (en) 1981-12-22 1981-12-22 Coaxial type dielectric resonator

Country Status (1)

Country Link
JP (1) JPS58108801A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0793527B2 (en) * 1990-11-30 1995-10-09 富士電気化学株式会社 Coaxial dielectric resonator
JP2008136686A (en) * 2006-12-01 2008-06-19 Pentax Corp Oct probe
JP5188242B2 (en) 2008-03-31 2013-04-24 テルモ株式会社 In vivo insertion probe
CN103930044B (en) 2012-03-08 2016-05-18 奥林巴斯株式会社 guide sheath and medical system

Also Published As

Publication number Publication date
JPS58108801A (en) 1983-06-29

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