JPS631449Y2 - - Google Patents

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Publication number
JPS631449Y2
JPS631449Y2 JP7642182U JP7642182U JPS631449Y2 JP S631449 Y2 JPS631449 Y2 JP S631449Y2 JP 7642182 U JP7642182 U JP 7642182U JP 7642182 U JP7642182 U JP 7642182U JP S631449 Y2 JPS631449 Y2 JP S631449Y2
Authority
JP
Japan
Prior art keywords
dielectric block
dielectric
distributed constant
hole
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
Application number
JP7642182U
Other languages
Japanese (ja)
Other versions
JPS58178707U (en
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 filed Critical
Priority to JP7642182U priority Critical patent/JPS58178707U/en
Priority to US06/431,184 priority patent/US4464640A/en
Priority to GB08228112A priority patent/GB2109641B/en
Priority to DE19823236664 priority patent/DE3236664A1/en
Publication of JPS58178707U publication Critical patent/JPS58178707U/en
Application granted granted Critical
Publication of JPS631449Y2 publication Critical patent/JPS631449Y2/ja
Granted legal-status Critical Current

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Description

【考案の詳細な説明】 本考案は分布定数形フイルタ等に使用される誘
電体同軸共振器に関する。
[Detailed Description of the Invention] The present invention relates to a dielectric coaxial resonator used in distributed constant filters and the like.

従来、数100MHz域のフイルタとしては、LC共
振回路を用いたものや同軸共振器を用いたものが
あつたが、構造的に不安定あるいは複雑であつた
り、特性的に満足できない、調整に手間がかか
る、コストが引き下げられない、などの問題点が
あつた。
Conventionally, filters in the several 100 MHz range have used LC resonant circuits or coaxial resonators, but these were structurally unstable or complex, had unsatisfactory characteristics, and were difficult to adjust. There were problems such as the high cost and the inability to reduce costs.

このため、第1図および第2図に示すように、
誘電体ブロツク11に孔12,12を形成し、こ
の孔12,12の内周面に内導体13,13を形
成するとともに、上記孔12,12を囲む誘電体
ブロツク11の4つの外側面14,14および1
5,15に外導体16,16および17,17を
夫々形成し、これら内導体13,13と外導体1
6,16および17,17とを上記誘電体ブロツ
ク11の1方の端面に形成した短絡導体18で短
絡し、上記内導体13,13と、外導体16,1
6および17,17と、その間に介在する誘電体
ブロツク11とで一対の1/4波長共振ユニツトを
構成し、これら共振ユニツトの間に誘電結合度調
整のための空洞19を設け、さらに、図示しない
外部回路と上記共振ユニツトとを静電結合するた
めに、導線21,21に誘電体材料を被着してな
る誘電体ユニツト22,22を上記孔12,12
に夫々挿入した分布定数形フイルタがある。
For this reason, as shown in Figures 1 and 2,
Holes 12, 12 are formed in the dielectric block 11, inner conductors 13, 13 are formed on the inner peripheral surfaces of the holes 12, 12, and four outer surfaces 14 of the dielectric block 11 surrounding the holes 12, 12 are formed. , 14 and 1
Outer conductors 16, 16 and 17, 17 are formed on 5, 15, respectively, and these inner conductors 13, 13 and outer conductor 1
6, 16 and 17, 17 are short-circuited by a shorting conductor 18 formed on one end face of the dielectric block 11, and the inner conductors 13, 13 and the outer conductors 16, 1 are short-circuited.
6 and 17, 17 and the dielectric block 11 interposed between them constitute a pair of 1/4 wavelength resonant units, and a cavity 19 is provided between these resonant units for adjusting the degree of dielectric coupling. In order to electrostatically couple the above-mentioned resonant unit to an external circuit not connected to the resonant unit, a dielectric unit 22, 22, which is formed by coating the conductive wires 21, 21 with a dielectric material, is inserted into the above-mentioned holes 12, 12.
There is a distributed constant type filter inserted in each.

ところで、上記の分布定数形フイルタでは、誘
電体ブロツク11のコーナ部23,……,23は
直角になつていた。このため、誘電体ブロツク1
1の成型時に上記コーナ部23,……,23にカ
ケが発生したり、電気特性的にも、上記コーナ部
23,……,23で電磁界の分布に乱れが生じ、
共振ユニツトのQが低下する問題があつた。
Incidentally, in the above-mentioned distributed constant type filter, the corner portions 23, . . . , 23 of the dielectric block 11 are at right angles. Therefore, dielectric block 1
1, chips may occur in the corner portions 23, .
There was a problem that the Q of the resonance unit decreased.

本考案は上記問題を解消すべくなされたもので
あつて、その目的は、誘電体同軸共振器の誘電体
ブロツクのコーナに丸みを設けて、誘電体ブロツ
クのカケを無くすとともに、誘電体ブロツク内で
の電磁界の乱れをなくして共振器のQを大きくす
ることである。
The present invention was devised to solve the above problem, and its purpose is to round the corners of the dielectric block of a dielectric coaxial resonator to eliminate chipping of the dielectric block, and to prevent the inside of the dielectric block from being chipped. The aim is to increase the Q of the resonator by eliminating disturbances in the electromagnetic field.

以下、添付図面を参照して本考案の実施例を説
明する。
Hereinafter, embodiments of the present invention will be described with reference to the accompanying drawings.

本考案においては、第3図に示すように、第1
図と全く同一の構成を有する分布定数形フイルタ
において、誘電体ブロツク11′の外側面14,
14および15,15を含むコーナ部23,…
…,23に丸みを付けるようにしている。
In this invention, as shown in FIG.
In a distributed constant filter having exactly the same configuration as shown in the figure, the outer surface 14 of the dielectric block 11',
The corner portion 23 including 14 and 15, 15,...
..., 23 is rounded.

上記丸みの曲率半径Rは、誘電体ブロツク1
1′の厚みをLとすると、R/L=0.2〜0.5とな
るように選択することが好ましい。R/Lが0.2
より小さいと効果がない。R/Lが0.5を越える
と従来と同様に電磁界の乱れが生じ始める。
The radius of curvature R of the above roundness is the dielectric block 1
If the thickness of 1' is L, it is preferable to select so that R/L=0.2 to 0.5. R/L is 0.2
If it is smaller, it will have no effect. When R/L exceeds 0.5, disturbances in the electromagnetic field begin to occur as in the conventional case.

上記のようにすれば、誘電体ブロツク11′は
そのコーナ部23,……,23に丸みを有してい
るため、誘電体ブロツク11′にカケ等が発生す
ることはなくなる。
By doing the above, since the dielectric block 11' has rounded corners 23, . . . , 23, chips and the like will not occur in the dielectric block 11'.

また、誘電体ブロツク11内の電磁界は、第4
図に示すように、誘電体ユニツト22に関して電
界31および磁界32がいずれもほゞ対称な形と
なつて乱れがほとんどなくなり、共振ユニツトの
Qが従来のものに比較して約10パーセント向上す
る。なお、上記実施例は1/4波長共振器を用いた
場合についてであるが、1/2波長共振器を用いて
も本発明は実施できる。
Furthermore, the electromagnetic field within the dielectric block 11 is
As shown in the figure, both the electric field 31 and the magnetic field 32 are almost symmetrical with respect to the dielectric unit 22, and there is almost no disturbance, and the Q of the resonant unit is improved by about 10% compared to the conventional one. Note that although the above embodiments are based on the case where a 1/4 wavelength resonator is used, the present invention can also be implemented using a 1/2 wavelength resonator.

以上詳述したことからも明らかなように、本考
案は、誘電体同軸共振器において誘電体ブロツク
のコーナ部に丸みを設けるようにしたから、誘電
体ブロツクのコーナ部にカケが発生することがな
く、誘電体ブロツクの金型成型が容易で成型の能
率が向上する一方、誘電体ブロツク内での電磁界
の乱れが少くなり、共振器のQを高くすることが
できる。
As is clear from the above detailed description, in the present invention, the corner portions of the dielectric block in the dielectric coaxial resonator are rounded, so that chipping does not occur at the corner portions of the dielectric block. Therefore, it is easy to mold the dielectric block with a mold, improving molding efficiency, and at the same time, the disturbance of the electromagnetic field within the dielectric block is reduced, making it possible to increase the Q of the resonator.

また、誘電体ブロツクのコーナ部に丸みを付け
ることにより、誘電体ブロツクの使用材料を削減
することができる利点もある。
Further, by rounding the corners of the dielectric block, there is an advantage that the material used for the dielectric block can be reduced.

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

第1図および第2図は夫々従来の分布定数形フ
イルタの縦断面図よび平面図、第3図は本考案に
係る分布定数形フイルタの一実施例の平面図、第
4図は第3図の分布定数形フイルタの誘電体ブロ
ツク内の電磁界の説明図である。 11,11′……誘電体ブロツク、12……孔、
13……内導体、16,17……外導体、18…
…短絡導体、23……コーナ部、31……電界、
32……磁界。
1 and 2 are a vertical cross-sectional view and a plan view of a conventional distributed constant filter, respectively, FIG. 3 is a plan view of an embodiment of a distributed constant filter according to the present invention, and FIG. 4 is a plan view of a conventional distributed constant filter. FIG. 2 is an explanatory diagram of an electromagnetic field within a dielectric block of a distributed constant type filter. 11, 11'...dielectric block, 12...hole,
13... Inner conductor, 16, 17... Outer conductor, 18...
... Short circuit conductor, 23 ... Corner part, 31 ... Electric field,
32...Magnetic field.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 誘電体ブロツクに筒状の孔を形成し、この孔の
内周面に内導体を形成するとともに、上記孔を囲
む誘電体ブロツクの4つの外側面に外導体を形成
した誘電体同軸共振器において、誘電体ブロツク
のコーナ部に夫々丸みを付け、これらの丸みの曲
率半径Rと上記誘導体ブロツクの厚みLとの比
R/Lが0.2から0.5の範囲となるようにしたこと
を特徴とする誘電体同軸共振器。
In a dielectric coaxial resonator, a cylindrical hole is formed in a dielectric block, an inner conductor is formed on the inner peripheral surface of the hole, and outer conductors are formed on four outer surfaces of the dielectric block surrounding the hole. A dielectric characterized in that the corner portions of the dielectric block are each rounded, and the ratio R/L of the radius of curvature R of these roundness and the thickness L of the dielectric block is in the range of 0.2 to 0.5. Body coaxial resonator.
JP7642182U 1981-10-02 1982-05-24 dielectric coaxial resonator Granted JPS58178707U (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP7642182U JPS58178707U (en) 1982-05-24 1982-05-24 dielectric coaxial resonator
US06/431,184 US4464640A (en) 1981-10-02 1982-09-30 Distribution constant type filter
GB08228112A GB2109641B (en) 1981-10-02 1982-10-01 Distributed constant type filter
DE19823236664 DE3236664A1 (en) 1981-10-02 1982-10-04 DISTRIBUTION CONSTANT TYPE FILTER

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7642182U JPS58178707U (en) 1982-05-24 1982-05-24 dielectric coaxial resonator

Publications (2)

Publication Number Publication Date
JPS58178707U JPS58178707U (en) 1983-11-30
JPS631449Y2 true JPS631449Y2 (en) 1988-01-14

Family

ID=30085736

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7642182U Granted JPS58178707U (en) 1981-10-02 1982-05-24 dielectric coaxial resonator

Country Status (1)

Country Link
JP (1) JPS58178707U (en)

Also Published As

Publication number Publication date
JPS58178707U (en) 1983-11-30

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