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JPS6156641B2 - - Google Patents
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JPS6156641B2 - - Google Patents

Info

Publication number
JPS6156641B2
JPS6156641B2 JP1616781A JP1616781A JPS6156641B2 JP S6156641 B2 JPS6156641 B2 JP S6156641B2 JP 1616781 A JP1616781 A JP 1616781A JP 1616781 A JP1616781 A JP 1616781A JP S6156641 B2 JPS6156641 B2 JP S6156641B2
Authority
JP
Japan
Prior art keywords
conductor
ultra
dielectric
coaxial resonator
center conductor
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
JP1616781A
Other languages
Japanese (ja)
Other versions
JPS57129505A (en
Inventor
Mitsuo Makimoto
Ko Kikuchi
Haruyoshi Endo
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 JP56016167A priority Critical patent/JPS57129505A/en
Publication of JPS57129505A publication Critical patent/JPS57129505A/en
Publication of JPS6156641B2 publication Critical patent/JPS6156641B2/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

Landscapes

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

Description

【発明の詳細な説明】 本発明は一端短絡、他端開放の4分の一波長超
高周波用同軸共振器に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a coaxial resonator for quarter-wave ultra-high frequencies with one end short-circuited and the other end open.

一端短絡、他端開放の4分の一波長超高周波同
軸型共振器は、円筒状外部導体中に棒状内部導体
の一端を固定させた共振器で小型、高Q、設計製
作の容易さもあり超高周波帯でしばしば用いられ
る共振器であるが、構造上中心導体が片持ばりと
なるため振動に対して特性が劣化しやすいという
欠点を持つている。
A quarter-wavelength ultra-high frequency coaxial resonator with one end short-circuited and the other end open is a resonator in which one end of a rod-shaped inner conductor is fixed in a cylindrical outer conductor, and it is small, has a high Q, and is easy to design and manufacture. Although this type of resonator is often used in high-frequency bands, it has the disadvantage that its characteristics tend to deteriorate due to vibration because the central conductor is cantilevered due to its structure.

このため従来は、中心導体先端部に、先端部を
外部導体に対して機械的に支持する誘電体円板を
挿入して耐振特性をもたせるようにしてきた。
For this reason, in the past, a dielectric disk was inserted into the tip of the center conductor to mechanically support the tip with respect to the outer conductor to provide vibration resistance.

第1図a,bに従来の中心導体の支持方法を示
す。101は共振器外部導体、102は中心導
体、103は誘電体による支持円板を示す。第2
図に誘電体円板103の構造を示し、201は中
心導体102に挿入するための穴である。
Figures 1a and 1b show a conventional method of supporting the center conductor. 101 is a resonator outer conductor, 102 is a center conductor, and 103 is a dielectric support disk. Second
The figure shows the structure of the dielectric disk 103, and 201 is a hole for inserting into the center conductor 102.

この方法により中心導体を支持する場合は、支
持自体には問題はないが、円板103を共振器に
挿入する際に円板103の外周がすべて外部導体
101内周に接するため摩擦が大きく指定された
位置に正しく挿入することが困難であること、ま
た誘電体円板103を中心導体102と外部導体
101間で容量を形成するため、誘電体損失に伴
う共振器無負荷Qが劣化するという問題を有して
いた。
When supporting the center conductor using this method, there is no problem with the support itself, but when inserting the disk 103 into the resonator, the entire outer periphery of the disk 103 touches the inner periphery of the outer conductor 101, resulting in large friction. In addition, since the dielectric disk 103 forms a capacitance between the center conductor 102 and the outer conductor 101, the no-load Q of the resonator deteriorates due to dielectric loss. I had a problem.

本発明はこのような欠点を除去せんとするもの
である。第3図および第4図に本発明による誘電
体支持板の構造を示す。第3図において301は
誘電体基板であり、その形状は、円板状誘電体よ
り円弧と弦で囲まれる3つの部分302〜304
を切断したものであり、残りの円周部306,3
07,308で外部導体と接する。305は中心
導体を通す穴を示す。また第4図は本発明の他の
実施例を示し、円板状の誘電体より、円弧と弦に
囲まれた4つの部分402〜405を切断した形
状をもつ誘電体板401を示し、穴406に中心
導体を通し、切断されて残つた4つの円周部で外
部導体と接し中心導体を支持するように用いられ
る。
The present invention seeks to eliminate these drawbacks. FIGS. 3 and 4 show the structure of a dielectric support plate according to the present invention. In FIG. 3, 301 is a dielectric substrate, and its shape consists of three parts 302 to 304 surrounded by arcs and chords from a disc-shaped dielectric.
is cut, and the remaining circumferential portion 306, 3
It contacts the outer conductor at 07,308. 305 indicates a hole through which the center conductor passes. FIG. 4 shows another embodiment of the present invention, and shows a dielectric plate 401 having a shape obtained by cutting four parts 402 to 405 surrounded by arcs and chords from a disc-shaped dielectric. The center conductor is passed through 406, and the four circumferential parts remaining after cutting are used to contact the outer conductor and support the center conductor.

第5図a,bは、第3図の中心導体支持板30
1を用いて、中心導体102を支持するようにし
た本発明の一実施例における共振器の構造を示
す。
Figures 5a and 5b show the center conductor support plate 30 of Figure 3.
1 is used to illustrate the structure of a resonator in an embodiment of the present invention in which a center conductor 102 is supported.

第1図と比較すると容易に理解できるように、
支持板301は、同軸外導体101と接する部分
がきわめて小さくなるため、共振器に挿入する際
摩擦が小さくなり容易に装着、固定ができる。ま
た誘電体を介して、中心導体102と接地導体1
01間に成形される容量も第1図の場合に比して
著しく低減できるため、誘電体損失を伴う損失も
改善され、無負荷Qの劣化をほとんど無視できる
ようになる。一方耐振特性も第1図の場合と同等
に良好である。
As can be easily understood by comparing with Figure 1,
Since the portion of the support plate 301 in contact with the coaxial outer conductor 101 is extremely small, friction is reduced when inserting it into the resonator, and it can be easily mounted and fixed. In addition, the center conductor 102 and the ground conductor 1 are connected via a dielectric.
Since the capacitance formed between 01 and 01 can be significantly reduced compared to the case of FIG. 1, loss accompanying dielectric loss is also improved, and deterioration of no-load Q can be almost ignored. On the other hand, the vibration resistance characteristics are also as good as in the case shown in FIG.

なお第5図に示すように、中心導体102の先
端部の径w1を他の部分の径w2に比して小さくす
ると、誘電体板301の挿入位置を決めることが
容易に出来、作業性を高めることができる。
As shown in FIG. 5, if the diameter w 1 of the tip of the center conductor 102 is made smaller than the diameter w 2 of the other parts, the insertion position of the dielectric plate 301 can be easily determined and the work can be done easily. You can increase your sexuality.

なお、第5図の実施例では、第3図に示した略
三角形の形状をもつ誘電体板301を用いた場合
について説明したが、第4図に示す略四角形の形
状をもつ誘電体板を用いても同様の効果を持たせ
ることが可能である。また、この誘電体板301
の形状としては以上の実施例に限られず五角形、
六角形等の多角形でも同様の作用効果を呈する
が、角の数を増やすを誘電体の周囲部を切断する
面積が小さくなり円形に近づくので効果が小さく
なる。一般的には三角形〜六角形が適当である。
In the embodiment shown in FIG. 5, the dielectric plate 301 having the approximately triangular shape shown in FIG. It is possible to achieve the same effect by using In addition, this dielectric plate 301
The shape is not limited to the above examples, but may be pentagonal,
Although polygons such as hexagons exhibit similar effects, the effect becomes smaller as the number of corners increases, as the area for cutting the peripheral portion of the dielectric becomes smaller and the shape approaches a circle. Generally, a triangle to a hexagon is suitable.

また、誘電体板301の形状の対称性は特に特
性上問題とはならないが、加工の容易さ、ストレ
スの均一化等を考えると、中心に対して対称構造
の形状が望ましく、切断されずに残つた外周部が
略正多角形の角部に対応する形状が好ましい。
Furthermore, although the symmetry of the shape of the dielectric plate 301 does not pose any particular problem in terms of characteristics, in consideration of ease of processing, uniformity of stress, etc., it is desirable to have a symmetrical structure with respect to the center, so that it is not cut. It is preferable that the remaining outer peripheral portion corresponds to the corners of a substantially regular polygon.

以上のように、本発明は一端短絡、一端開放の
4分の一波長同軸共振器の中心導体を機械的に支
持するために、円板状誘電体の周辺部の一部を切
断して略多角形としたものを支持板として中心導
体の先端部に挿入するようにした同軸共振器であ
る。この支持板は、同軸外部導体に接する部分の
面積が小さいので、摩擦も少なく取付けの作業性
が著しく改善される。また、無負荷Qの劣化をほ
とんど無視することができ、超高周波用の耐振特
性のすぐれた同軸共振器を得ることができる。
As described above, in order to mechanically support the center conductor of a quarter-wavelength coaxial resonator with one end short-circuited and one end open, a portion of the peripheral portion of the disc-shaped dielectric material is cut off. This is a coaxial resonator in which a polygonal support plate is inserted into the tip of the center conductor. Since this support plate has a small area in contact with the coaxial outer conductor, there is little friction and the workability of installation is significantly improved. Moreover, the deterioration of the no-load Q can be almost ignored, and a coaxial resonator with excellent vibration resistance characteristics for ultra-high frequencies can be obtained.

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

第1図a,bは従来の超高周波用同軸共振器の
一例を示す断面側面図およびそのA−A′線断面
図、第2図は第1図における超高周波用同軸共振
器に使用される中心導体支持用の誘電体円板の平
面図、第3図および第4図はそれぞれ本発明によ
る超高周波用同軸共振器に使用される中心導体支
持用の誘電体板の実施例を示す平面図、第5図
a,bは本発明による超高周波用同軸共振器の実
施例を示す断面側面図およびそのA−A′線断面
図である。 101……外部導体、102……中心導体、3
01,401……誘電体基板。
Figures 1a and b are a cross-sectional side view and a cross-sectional view taken along the line A-A' of an example of a conventional coaxial resonator for ultra-high frequencies, and Figure 2 is a coaxial resonator used for the ultra-high frequency coaxial resonator in Figure 1. A plan view of a dielectric disk for supporting a center conductor, and FIGS. 3 and 4 are plan views showing examples of a dielectric plate for supporting a center conductor used in an ultra-high frequency coaxial resonator according to the present invention, respectively. , FIGS. 5a and 5b are a cross-sectional side view and a cross-sectional view taken along the line A-A' of the embodiment of the ultra-high frequency coaxial resonator according to the present invention. 101...Outer conductor, 102...Center conductor, 3
01,401...Dielectric substrate.

Claims (1)

【特許請求の範囲】 1 円筒状外部導体内に略同軸に棒状内部導体の
一端を固定し、内部導体の他端に、上記外部導体
の内径に等しい直径の誘電体円板の外周部の一部
を3ケ所以上残して切断した支持板を挿入したこ
とを特徴とする超高周波用同軸共振器。 2 支持板の切断されずに残された外周部が略正
多角形の角部に対応するように形成された特許請
求の範囲第1項記載の超高周波用同軸共振器。 3 正多角形が正三角形乃至正六角形である特許
請求の範囲第2項記載の超高周波用同軸共振器。
[Scope of Claims] 1. One end of a rod-shaped internal conductor is fixed substantially coaxially within a cylindrical external conductor, and at the other end of the internal conductor, a part of the outer peripheral portion of a dielectric disk having a diameter equal to the internal diameter of the external conductor is attached. A coaxial resonator for ultra-high frequencies, characterized in that a supporting plate is inserted with parts left in three or more places. 2. The ultra-high frequency coaxial resonator according to claim 1, wherein the outer peripheral portion of the support plate that remains uncut is formed so as to correspond to the corners of a substantially regular polygon. 3. The ultra-high frequency coaxial resonator according to claim 2, wherein the regular polygon is a regular triangle or a regular hexagon.
JP56016167A 1981-02-04 1981-02-04 Coaxial resonator for superhigh frequency Granted JPS57129505A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56016167A JPS57129505A (en) 1981-02-04 1981-02-04 Coaxial resonator for superhigh frequency

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56016167A JPS57129505A (en) 1981-02-04 1981-02-04 Coaxial resonator for superhigh frequency

Publications (2)

Publication Number Publication Date
JPS57129505A JPS57129505A (en) 1982-08-11
JPS6156641B2 true JPS6156641B2 (en) 1986-12-03

Family

ID=11908944

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56016167A Granted JPS57129505A (en) 1981-02-04 1981-02-04 Coaxial resonator for superhigh frequency

Country Status (1)

Country Link
JP (1) JPS57129505A (en)

Also Published As

Publication number Publication date
JPS57129505A (en) 1982-08-11

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