JPS6322685B2 - - Google Patents
Info
- Publication number
- JPS6322685B2 JPS6322685B2 JP57015808A JP1580882A JPS6322685B2 JP S6322685 B2 JPS6322685 B2 JP S6322685B2 JP 57015808 A JP57015808 A JP 57015808A JP 1580882 A JP1580882 A JP 1580882A JP S6322685 B2 JPS6322685 B2 JP S6322685B2
- Authority
- JP
- Japan
- Prior art keywords
- dielectric
- conductor
- region
- coaxial
- 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.)
- Expired
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P7/00—Resonators of the waveguide type
- H01P7/04—Coaxial resonators
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
Description
【発明の詳細な説明】
本発明は、VHF〜UHF帯で用いられる同軸型
誘電体共振器さらに詳しくは、同軸線路の内外導
体間の空間に誘電体を充てんさせた構造の同軸型
誘電体共振器の改良に関するものである。Detailed Description of the Invention The present invention relates to a coaxial dielectric resonator used in the VHF to UHF band. It concerns the improvement of utensils.
従来用いられている誘電体を用いた同軸共振器
の例を第1図〜第3図に示す。第1図は最も良く
利用される4分の一波長形の共振器で、aは軸方
向の断面図、bはa図のA―A′における断面図
である。図において1は同軸構造の誘電体、2は
内部導体、3は外部(接地)導体、4は短絡部で
ある。通常内、外導体2,3および短絡部4は、
メツキあるいは焼付け等による低抵抗の導体膜で
形成される。 Examples of conventionally used coaxial resonators using dielectric materials are shown in FIGS. 1 to 3. FIG. 1 shows a quarter-wavelength resonator, which is the most commonly used resonator. A is a cross-sectional view in the axial direction, and b is a cross-sectional view taken along line A-A' in FIG. In the figure, 1 is a coaxial structure dielectric, 2 is an internal conductor, 3 is an external (ground) conductor, and 4 is a short circuit. Normally, the inner and outer conductors 2 and 3 and the short circuit part 4 are
It is formed from a low-resistance conductive film by plating or baking.
この構造は、構造が単純で無負荷Qもとれる
が、基本共振周波数0として、30,50等にも共
振点を持つため、高調波抑圧効果を持たない。こ
の欠点を改善するため、同一出願人が提案したの
が第2図、および第3図の構造の共振器である。
第2図及び第3図ともaが軸方向の断面図、bは
a図のA―A′における断面図である。これらの
共振器は、線路インピーダンスを部分的にかえる
ことにより、スプリアス共振周波数を基本共振周
波数の整数倍からずらすことを可能ならしめる。
第2図、および第3図において、1は誘電体、2
は内部導体、3は外部導体、4は短絡部、5は段
差部を示す。 This structure has a simple structure and can provide a no-load Q, but since the fundamental resonance frequency is 0 , it also has resonance points at 30 , 50, etc., so it does not have a harmonic suppression effect. In order to improve this drawback, the same applicant proposed resonators having the structures shown in FIGS. 2 and 3.
In both FIGS. 2 and 3, a is a sectional view in the axial direction, and b is a sectional view taken along line A-A' in FIG. These resonators make it possible to shift the spurious resonant frequency from an integer multiple of the fundamental resonant frequency by partially changing the line impedance.
In FIGS. 2 and 3, 1 is a dielectric, 2
3 indicates an inner conductor, 3 indicates an outer conductor, 4 indicates a short circuit portion, and 5 indicates a stepped portion.
この構造により、スプリアス特性の大巾な改善
が可能となるが、段差部5における不連続性が大
きな場合、この部分での電磁界の乱れが大きく、
無負荷Qが劣化する傾向にあり、また段差部5の
金属メツキあるいは焼付けの処理が困難であるこ
と、あるいは段差部5において金属のハク離を生
じやすい等欠点をもつ。 This structure makes it possible to greatly improve the spurious characteristics, but if the discontinuity in the stepped portion 5 is large, the disturbance of the electromagnetic field in this portion is large;
The unloaded Q tends to deteriorate, and there are other drawbacks such as difficulty in metal plating or baking of the stepped portion 5, or the tendency for metal flaking to occur in the stepped portion 5.
本発明は、この問題を解決するためになされた
ものであり、以下第4図〜第7図を用いてその一
実施例を説明する。 The present invention has been made to solve this problem, and one embodiment thereof will be described below with reference to FIGS. 4 to 7.
基本的な構造は、第2図、第3図のような段差
部5をなくし、開放端部に向かつてインピーダン
スが減少するようにテーパ状にゆるやかに変化す
るようにしたことにある。第4図、第5図は、誘
電体1に端部方向に向かつてテーパを形成し外部
導体3側にテーパ部6を設けた例で、第4図のも
のは一端開放、他端短絡の4分の一波長型の共振
器であり、第5図は両端開放の2分の一波長型の
共振器の例である。段差部をこのようなテーパ部
におきかえることにより、電磁界の分布を一様な
ものとし、Qの劣化を防ぎ、かつ導体膜の密着強
度も改善できる。(もちろんスプリアス特性の劣
化はない。)第4図、第5図においてaは軸方向
の断面形状を、bはa図のA−A′における断面
図であり、1は誘電体、2は内部導体、3は外部
導体、4は短絡部、6はテーパ部を示す。なおテ
ーパ部6は、線路全体にわたつて設けても良い
が、図に示す如く、開放端部分、短絡部分に近い
方は一様線路にする方が、電磁界の分布を一様な
ものにでき、かつ、共振器を他の筐体にマウント
する場合も好しい構造となる。テーパを設けるこ
とは一見工程が複雑に見えるが、誘電体1は通常
セラミツクであり、金型で成形したのち焼成して
作製するものであるから、金型の作製が多少複雑
になる程度で、工程は従来と全く同一である。第
6図、第7図は、本発明の他の実施例として内部
導体2側にテーパ部6を設けた例で、第6図は4
分の一波長型、第7図は2分の一波長型である。
なお図でaは軸方向の断面図、bはa図のA−
A′における断面形状であり、1は誘電体、2は
内部導体、3は外部導体、4は短絡部、6はテー
パ部を示す。この場合も第4図、第5図の場合と
まつたく同様の効果が得られる。本発明の場合、
開放端部に向かつてインピーダンスが減少するよ
うな構成であれば、内部導体、外部導体のいずれ
の側にテーパ部を形成しても同一の効果を奏す
る。 The basic structure is that the stepped portion 5 as shown in FIGS. 2 and 3 is eliminated, and the impedance gradually changes in a tapered shape so that the impedance decreases toward the open end. Figures 4 and 5 show examples in which the dielectric 1 is tapered toward the end, and a tapered part 6 is provided on the outer conductor 3 side. This is a quarter wavelength type resonator, and FIG. 5 is an example of a half wavelength type resonator with both ends open. By replacing the stepped portion with such a tapered portion, it is possible to make the distribution of the electromagnetic field uniform, prevent Q deterioration, and improve the adhesion strength of the conductor film. (Of course, there is no deterioration of the spurious characteristics.) In Figs. 4 and 5, a is the cross-sectional shape in the axial direction, b is a cross-sectional view taken along A-A' in Fig. a, 1 is the dielectric, and 2 is the inside. 3 is an outer conductor, 4 is a short-circuit portion, and 6 is a tapered portion. Note that the tapered portion 6 may be provided over the entire line, but as shown in the figure, it is better to make the line uniform near the open end portion and short-circuited portion to make the distribution of the electromagnetic field uniform. This is also a preferable structure when the resonator is mounted on another housing. Providing a taper may seem to be a complicated process at first glance, but since the dielectric 1 is usually made of ceramic and is produced by molding it in a mold and then firing it, it only makes the production of the mold a little more complicated. The process is exactly the same as before. 6 and 7 show examples in which a tapered portion 6 is provided on the inner conductor 2 side as another embodiment of the present invention, and FIG.
The wavelength type shown in FIG. 7 is a half wavelength type.
In the figure, a is a cross-sectional view in the axial direction, and b is a cross-sectional view in the A-
This is a cross-sectional shape at A', where 1 is a dielectric, 2 is an inner conductor, 3 is an outer conductor, 4 is a short circuit portion, and 6 is a tapered portion. In this case as well, the same effects as those shown in FIGS. 4 and 5 can be obtained. In the case of the present invention,
As long as the impedance decreases toward the open end, the same effect can be achieved regardless of whether the tapered portion is formed on either side of the inner conductor or the outer conductor.
以上のように、本発明は、従来の誘電体共振器
の内部導体、あるいは外部導体の外形を開放端部
に向かつてインピーダンスが漸次変化するように
テーパ状にすることにより、Qの劣化を防止し、
導体膜の密着強度を向上させることができ、その
工業的価値がきわめて大きいものである。 As described above, the present invention prevents Q deterioration by tapering the external shape of the internal conductor or external conductor of a conventional dielectric resonator so that the impedance gradually changes toward the open end. death,
The adhesion strength of the conductor film can be improved, and its industrial value is extremely large.
第1図aは従来から用いられている誘電体を利
用した同軸共振器の軸方向断面図、同bは同横断
面図、第2図a及び第3図aはスプリアス特性を
改善した従来の同軸型誘電体共振器の軸方向断面
図、同bは同横断面図、第4図aは外部導体にテ
ーパを設けた本発明の一実施例における1/4波長
同軸型誘電体共振器の軸方向断面図、同bは同横
断面図、第5図aは外部導体にテーパを設けた本
発明の一実施例における1/2波長同軸型誘電体共
振器の軸方向断面図、同bは同横断面図、第6図
aは内部導体にテーパ部を設けた本発明の一実施
例における1/4波長同軸型誘電体共振器の軸方向
断面図、同bは同横断面図、第7図aは内部導体
にテーパ部を設けた本発明の一実施例における1/
2波長同軸型誘電体共振器の軸方向断面図、同b
は同横断面図である。
1…誘電体、2…内部導体、3…外部導体、4
…短絡部、6…テーパ部。
Figure 1a is an axial cross-sectional view of a conventionally used coaxial resonator using a dielectric, Figure 1b is a cross-sectional view of the same, and Figures 2a and 3a are conventional coaxial resonators with improved spurious characteristics. FIG. 4A is an axial cross-sectional view of a coaxial dielectric resonator, FIG. Figure 5a is an axial cross-sectional view of a 1/2 wavelength coaxial dielectric resonator according to an embodiment of the present invention in which the outer conductor is tapered; 6A is a cross-sectional view of the same, FIG. FIG. 7a shows 1/1/2 in an embodiment of the present invention in which the internal conductor is provided with a tapered portion.
Axial cross-sectional view of a two-wavelength coaxial dielectric resonator, same b
is a cross-sectional view of the same. 1...Dielectric, 2...Inner conductor, 3...Outer conductor, 4
...Short circuit part, 6...Taper part.
Claims (1)
面に設けられた内部導体と、前記誘電体の外周部
に設けられた外部導体と、少なくとも1つの開放
端部とを備え、前記内部導体の外形、もしくは外
部導体の外形の少なくとも一方が、前記開放端部
に向かつてインピーダンスが漸次減少する領域を
有するごとくテーパ状に構成されていることを特
徴とする同軸型誘電体共振器。 2 インピーダンスが漸次減少する領域は先端部
にまではおよばず、先端部近傍にインピーダンス
の均一な領域を設けた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 インピーダンスが漸次減少する領域が、誘電
体の外周部の径をテーパ状に変化させたものであ
る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 インピーダンスが漸次減少する領域が、誘電
体の中空部内周面の径をテーパ状に変化させたも
のである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。[Scope of Claims] 1. A hollow dielectric, an internal conductor provided on the inner circumferential surface of the hollow portion of the dielectric, an external conductor provided on the outer circumference of the dielectric, and at least one open end. a coaxial type, characterized in that at least one of the outer shape of the inner conductor and the outer shape of the outer conductor is tapered so as to have a region where the impedance gradually decreases toward the open end. dielectric resonator. 2. The coaxial dielectric resonator according to claim 1, wherein the region where the impedance gradually decreases does not extend to the tip, but a region with uniform impedance is provided near the tip. 3. The coaxial dielectric resonator according to claim 1 or 2, wherein the region where the impedance gradually decreases is formed by tapering the diameter of the outer circumference of the dielectric material. . 4. A coaxial dielectric according to claim 1 or 2, wherein the region where the impedance gradually decreases is formed by tapering the diameter of the inner peripheral surface of the hollow portion of the dielectric. resonator.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57015808A JPS58133002A (en) | 1982-02-02 | 1982-02-02 | Coaxial dielectric resonator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57015808A JPS58133002A (en) | 1982-02-02 | 1982-02-02 | Coaxial dielectric resonator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58133002A JPS58133002A (en) | 1983-08-08 |
| JPS6322685B2 true JPS6322685B2 (en) | 1988-05-12 |
Family
ID=11899141
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57015808A Granted JPS58133002A (en) | 1982-02-02 | 1982-02-02 | Coaxial dielectric resonator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58133002A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63187901A (en) * | 1987-01-30 | 1988-08-03 | Murata Mfg Co Ltd | Dielectric filter |
| JPH06303006A (en) * | 1993-04-14 | 1994-10-28 | Matsushita Electric Ind Co Ltd | Dielectric filter |
| WO2025211317A1 (en) * | 2024-03-31 | 2025-10-09 | キーコム株式会社 | Transmission line and resonator |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4893747U (en) * | 1972-02-16 | 1973-11-09 | ||
| JPS5286044A (en) * | 1976-01-12 | 1977-07-16 | Nippon Telegr & Teleph Corp <Ntt> | Branching filter using dielectric resonator |
-
1982
- 1982-02-02 JP JP57015808A patent/JPS58133002A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58133002A (en) | 1983-08-08 |
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