JPH03143103A - Dielectric resonator - Google Patents
Dielectric resonatorInfo
- Publication number
- JPH03143103A JPH03143103A JP28246789A JP28246789A JPH03143103A JP H03143103 A JPH03143103 A JP H03143103A JP 28246789 A JP28246789 A JP 28246789A JP 28246789 A JP28246789 A JP 28246789A JP H03143103 A JPH03143103 A JP H03143103A
- Authority
- JP
- Japan
- Prior art keywords
- dielectric
- conductor
- hole
- throughhole
- 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.)
- Pending
Links
- 239000004020 conductor Substances 0.000 claims abstract description 39
- 239000003989 dielectric material Substances 0.000 claims abstract description 8
- 230000008878 coupling Effects 0.000 abstract description 7
- 238000010168 coupling process Methods 0.000 abstract description 7
- 238000005859 coupling reaction Methods 0.000 abstract description 7
- 230000002093 peripheral effect Effects 0.000 abstract description 3
- 230000002035 prolonged effect Effects 0.000 abstract 1
- 239000000919 ceramic Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000007423 decrease Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、誘電体共振器の構造に係るもので、特に小型
の誘電体フィルタを得るのに適した誘電体共振器に関す
るものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to the structure of a dielectric resonator, and particularly to a dielectric resonator suitable for obtaining a small dielectric filter.
マイクロ波帯域等の高周波領域で、誘電体セラミックを
用いた誘電体フィルタが用いられる。従来、円筒形の同
軸TEM共振器の内導体を容量結合させたものが一般的
であったが、第5図に示したようなブロック形の誘電体
フィルタも用いられるようになった。Dielectric filters using dielectric ceramics are used in high frequency regions such as microwave bands. Conventionally, a cylindrical coaxial TEM resonator in which the inner conductor is capacitively coupled has been common, but a block-shaped dielectric filter as shown in FIG. 5 has also come to be used.
これは、誘電体ブロック50に複数の貫通孔51を設け
、その貫通孔51内に導体膜を形成して内導体を形成し
、側面にも導体膜を形成して外導体を形成したものであ
る。誘電体ブロック50の下面の貫通孔の開口のある面
にも導体膜が形成され、短絡端面となっている。図の上
面は誘電体が露出して開放端面となっている。内導体と
外導体とで共振子ユニットが構成され、共振子ユニット
間の結合を調整するために、貫通孔52が貫通孔51間
に形成されている。In this structure, a plurality of through holes 51 are provided in a dielectric block 50, a conductor film is formed in the through holes 51 to form an inner conductor, and a conductor film is also formed on the side surface to form an outer conductor. be. A conductive film is also formed on the surface of the lower surface of the dielectric block 50 where the opening of the through hole is located, and serves as a short-circuit end surface. The top surface of the figure is an open end surface with exposed dielectric material. The inner conductor and the outer conductor constitute a resonator unit, and through holes 52 are formed between the through holes 51 in order to adjust the coupling between the resonator units.
[課題〕
このような誘電体フィルタを小型化して共振子ユニノI
・間の距離を小さくすることが望まれているが、結合調
整のために孔を形成しないと共振子ユニット間の結合が
大きくなりすぎて所望の特(?JEを青ることが雑しく
なる。[Challenge] Miniaturizing such a dielectric filter to create a resonator Unino I
・It is desired to reduce the distance between the resonator units, but unless holes are formed to adjust the coupling, the coupling between the resonator units will become too large and it will be difficult to achieve the desired characteristics (?JE). .
また、講雫体の内導体と外導体の距離が小さくなると掩
i1 萄Qが低下し、フィルタとしては損失が大きくな
る。Furthermore, when the distance between the inner conductor and the outer conductor of the droplet body becomes smaller, the covert i1 Q decreases, and the loss of the filter increases.
本発明は、このような問題を解決し、かつフィルタの小
型化の可能な誘電体共振器を提供するものである。The present invention provides a dielectric resonator that solves these problems and allows the filter to be made smaller.
本発明は、誘電体の内導体の形成される貫通孔の伸びる
方向に対して直角な方向の断面形状を長方形とすること
によって、上記の課題を解決するものである。The present invention solves the above-mentioned problems by making the cross-sectional shape in the direction perpendicular to the extending direction of the through hole in which the dielectric inner conductor is formed into a rectangular shape.
すなわち、誘電体の側面に平行に伸びる貫通孔を有し、
該貫通孔に内導体が形成され、該側面に外導体が形成さ
れる誘電体共振器において、該貫通孔の伸びる方向に直
角な方向の該誘電体の断面形状が長方形であることに特
徴を有するものである。That is, it has a through hole extending parallel to the side surface of the dielectric,
A dielectric resonator in which an inner conductor is formed in the through hole and an outer conductor is formed on the side surface, characterized in that the cross-sectional shape of the dielectric in a direction perpendicular to the extending direction of the through hole is rectangular. It is something that you have.
更に、該誘電体の断面形状と該貫通孔の断面形状がほぼ
相似形であることに特徴を有するものである。その相似
比を3〜4とすると、無ft荷Qを高くすることができ
る。Furthermore, it is characterized in that the cross-sectional shape of the dielectric and the cross-sectional shape of the through hole are substantially similar. When the similarity ratio is set to 3 to 4, the no-ft load Q can be increased.
長方形として短辺方向に誘電体共振器を並べれば、誘電
体フィルタの全体の寸法を短くすることができる。By arranging the dielectric resonators in a rectangular shape along the shorter sides, the overall dimensions of the dielectric filter can be shortened.
配置方向に対して直角の方向の長さを大きくするにした
がって無i荷Qを大きくすることができる。The unloaded Q can be increased as the length in the direction perpendicular to the arrangement direction is increased.
また、実験の結果、誘電体を外周と内周の形状を相似形
としたとき、その比を3〜4としたときに無負荷Qが最
大になることが分かった。Additionally, as a result of experiments, it was found that when the outer and inner circumferences of the dielectric are made similar in shape, the no-load Q is maximized when the ratio is set to 3 to 4.
以下、図面を参照して、本発明の実施例について説明す
る。Embodiments of the present invention will be described below with reference to the drawings.
第1図は、本発明の実施例を示す斜視図で、直方体の誘
電体セラミック焼成体10には、貫通孔11が一表面か
ら対向する面へと伸びて形成されている。この貫通孔1
1内は表面に導体膜が形成されて内導体となっている。FIG. 1 is a perspective view showing an embodiment of the present invention. A rectangular parallelepiped dielectric ceramic fired body 10 has a through hole 11 extending from one surface to the opposite surface. This through hole 1
Inside 1, a conductive film is formed on the surface to serve as an inner conductor.
誘電体10の貫通孔11の開口しない外周面には導体膜
13が形成され、外導体となっている。下側の貫通孔の
開口のある面にも導体膜が形成されて内導体と外導体を
短絡した短絡端面となっているが、上面は誘電体の露出
した開放v:1;而となっている。A conductor film 13 is formed on the outer peripheral surface of the dielectric 10 on which the through hole 11 is not opened, and serves as an outer conductor. A conductive film is also formed on the surface where the opening of the lower through hole is, forming a short-circuited end surface that shorts the inner conductor and the outer conductor, but the upper surface is open with exposed dielectric material. There is.
開放端面の断面形状は第2図に示したように長方形とな
っている。すなわち、短辺の長さblと長辺の長さb2
とは異なっている。誘電体フィルタとして誘電体を配列
するときには、長さb2の長辺側で共振器同士を接触さ
せるとよい。The cross-sectional shape of the open end surface is rectangular as shown in FIG. That is, the short side length bl and the long side length b2
It is different from When arranging dielectrics as a dielectric filter, it is preferable that the resonators are brought into contact with each other on the long side of length b2.
内導体の形成される貫通孔11の形状は任意の形状とす
ることができるが、誘電体10の外形と相似形にするこ
とが望ましい。すなわち、貫通孔の短辺の長さalと長
辺の長さa2の比を等しくするとよい。Although the shape of the through hole 11 in which the inner conductor is formed can be any shape, it is desirable that the shape be similar to the outer shape of the dielectric 10. That is, it is preferable to make the ratio of the length a1 of the short side of the through hole equal to the length a2 of the long side.
第3図は、前記のように誘電体の外形と貫通孔を相似に
形成したとき、その相似比を変えたときの無負荷Qの変
化を示したものである。第2図に示した短辺の長さす、
を4mm、7mm、 10mn+、 13mmとし、長
辺の長さb2をその1.5倍とし、貫通孔を相似形に形
成し、bi/a+(すなわちbz/az)の値を変化さ
せたときの無負荷Qの値の変化を示したものである。FIG. 3 shows the change in the no-load Q when the similarity ratio is changed when the outer shape of the dielectric and the through hole are formed to be similar as described above. The length of the short side shown in Figure 2,
are set to 4 mm, 7 mm, 10 mn+, and 13 mm, the length b2 of the long side is set to 1.5 times that length, the through holes are formed in similar shapes, and the values of bi/a+ (i.e. bz/az) are changed. It shows the change in the value of no-load Q.
曲線36.37.38.39は短辺の長さす、を4mm
、7mm、10mm、 13mn+としたときに対応し
ている。いずれもb / aが3〜4としたときに無負
荷Qの値が大きくなり、3.6としたときに最大値を示
していた。当然のことながら、全体の寸法が大きくなる
ほど無負荷Qの値も大きくなるが、寸法を小さくしたと
きにはこの範囲に寸法を選択することによって無負荷Q
の値を大きくすることができる。The length of the short side of curve 36, 37, 38, 39 is 4 mm.
, 7mm, 10mm, and 13mm+. In both cases, the no-load Q value increased when b/a was 3 to 4, and reached its maximum value when b/a was 3.6. Naturally, the larger the overall dimensions, the larger the value of the no-load Q will be, but when the dimensions are made smaller, the no-load Q
The value of can be increased.
本発明による誘電体共振器を内導体同士を容量結合さ・
已で用いることもできるが、第4図のように誘電体40
の貫通孔41に内導体を形成し、外周面に外導体43を
形成した共振器を接触配置させ、接触する側面の導体膜
の一部を除去して空洞44を形成し、共振器間を容量結
合と=F F結合で結合させることもできる。The dielectric resonator according to the present invention is capacitively coupled between inner conductors.
Although it can also be used with a dielectric material 40 as shown in FIG.
An inner conductor is formed in the through hole 41 of the resonator, and resonators with an outer conductor 43 formed on the outer peripheral surface are arranged in contact with each other, and a part of the conductor film on the contacting side surface is removed to form a cavity 44, and a cavity 44 is formed between the resonators. It is also possible to couple by capacitive coupling and =F F coupling.
この空洞の位置、面積を調整することによって結合状態
を変えることができる。したがって、小さい共振器の内
導体同士を近づLJでも、その結合を小さくすることが
でき小型化が容易となる。By adjusting the position and area of this cavity, the bonding state can be changed. Therefore, even if the inner conductors of a small resonator are brought close to each other at LJ, the coupling can be reduced, making it easy to downsize.
本発明によれば、共振器を組み合わせる誘電体フィルタ
の全体の寸法を大幅に減少させることが可能となる。According to the present invention, it is possible to significantly reduce the overall size of a dielectric filter in which a resonator is combined.
また、小型化しても無負荷Qの値を確保することが可能
となるので、フィルタとしての損失を少なくすることが
できる。Further, even if the filter is miniaturized, the no-load Q value can be maintained, so the loss as a filter can be reduced.
また、フィルタだけでなく、薄形化の要求される発振器
などに用いる誘電体共振器等にも利用することができる
。Moreover, it can be used not only for filters but also for dielectric resonators used in oscillators and the like that require thinning.
第1図は本発明の実施例を示す斜視図、第2図はその平
面図、第3図は寸法と特性の関係の説明図、第4図は本
発明の他の実施例を示す斜視図、笛5図は従来の誘電体
フィルタの斜視図である。
10.40・・・・誘電体
11、41・・・・貫通孔(内導体)
13.43・・・・外導体Fig. 1 is a perspective view showing an embodiment of the present invention, Fig. 2 is a plan view thereof, Fig. 3 is an explanatory diagram of the relationship between dimensions and characteristics, and Fig. 4 is a perspective view showing another embodiment of the invention. , Figure 5 is a perspective view of a conventional dielectric filter. 10.40...Dielectric 11, 41...Through hole (inner conductor) 13.43...Outer conductor
Claims (4)
通孔に内導体が形成され、該側面に外導体が形成される
誘電体共振器において、該貫通孔の伸びる方向に直角な
方向の該誘電体の断面形状が長方形であることを特徴と
する誘電体共振器。(1) In a dielectric resonator that has a through hole extending parallel to the side surface of the dielectric, an inner conductor is formed in the through hole, and an outer conductor is formed on the side surface, the dielectric resonator is perpendicular to the direction in which the through hole extends. 1. A dielectric resonator, wherein the dielectric has a rectangular cross-sectional shape in a direction.
通孔に内導体が形成され、該側面に外導体が形成される
誘電体共振器において、該貫通孔の伸びる方向に直角な
方向の該誘電体の断面形状が長方形であり、該誘電体の
断面形状と該貫通孔の断面形状がほぼ相似形であること
を特徴とする誘電体共振器。(2) A dielectric resonator having a through hole extending parallel to the side surface of the dielectric, an inner conductor formed in the through hole, and an outer conductor formed on the side surface, at right angles to the direction in which the through hole extends. 1. A dielectric resonator, wherein the dielectric has a rectangular cross-sectional shape in a direction, and the cross-sectional shape of the dielectric and the cross-sectional shape of the through hole are substantially similar.
4倍である請求項第2項記載の誘電体共振器。(3) The cross-sectional dimension of the dielectric is 3 or more of the cross-sectional dimension of the through hole.
3. The dielectric resonator according to claim 2, wherein the dielectric resonator is four times as large.
一部に外導体が形成されず、誘電体が露出する請求項第
1項記載の誘電体共振器。(4) The dielectric resonator according to claim 1, wherein the outer conductor is not formed on at least a portion of the side surface corresponding to the long side of the rectangle, and the dielectric material is exposed.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28246789A JPH03143103A (en) | 1989-10-30 | 1989-10-30 | Dielectric resonator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28246789A JPH03143103A (en) | 1989-10-30 | 1989-10-30 | Dielectric resonator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH03143103A true JPH03143103A (en) | 1991-06-18 |
Family
ID=17652809
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP28246789A Pending JPH03143103A (en) | 1989-10-30 | 1989-10-30 | Dielectric resonator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH03143103A (en) |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04292001A (en) * | 1991-03-20 | 1992-10-16 | Murata Mfg Co Ltd | Dielectric coaxial resonator |
JPH0521504U (en) * | 1991-08-30 | 1993-03-19 | 京セラ株式会社 | Dielectric filter |
JPH06252607A (en) * | 1993-02-17 | 1994-09-09 | Siemens Matsushita Components Gmbh & Co Kg | Adjusting method of resonance frequency for ceramic resonator |
JPH0865010A (en) * | 1994-08-22 | 1996-03-08 | Fuji Elelctrochem Co Ltd | Wide band dielectric filter |
JPWO2006137470A1 (en) * | 2005-06-23 | 2009-01-22 | 宇部興産株式会社 | Dielectric filter for base station communication equipment |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5442960A (en) * | 1978-08-18 | 1979-04-05 | Murata Manufacturing Co | Coaxial tem resonator |
JPS648807B2 (en) * | 1980-12-26 | 1989-02-15 | Matsushita Electric Ind Co Ltd | |
JPH0220103A (en) * | 1988-07-07 | 1990-01-23 | Matsushita Electric Ind Co Ltd | Coaxial type dielectric resonator |
-
1989
- 1989-10-30 JP JP28246789A patent/JPH03143103A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5442960A (en) * | 1978-08-18 | 1979-04-05 | Murata Manufacturing Co | Coaxial tem resonator |
JPS648807B2 (en) * | 1980-12-26 | 1989-02-15 | Matsushita Electric Ind Co Ltd | |
JPH0220103A (en) * | 1988-07-07 | 1990-01-23 | Matsushita Electric Ind Co Ltd | Coaxial type dielectric resonator |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04292001A (en) * | 1991-03-20 | 1992-10-16 | Murata Mfg Co Ltd | Dielectric coaxial resonator |
JPH0521504U (en) * | 1991-08-30 | 1993-03-19 | 京セラ株式会社 | Dielectric filter |
JPH06252607A (en) * | 1993-02-17 | 1994-09-09 | Siemens Matsushita Components Gmbh & Co Kg | Adjusting method of resonance frequency for ceramic resonator |
JPH0865010A (en) * | 1994-08-22 | 1996-03-08 | Fuji Elelctrochem Co Ltd | Wide band dielectric filter |
JPWO2006137470A1 (en) * | 2005-06-23 | 2009-01-22 | 宇部興産株式会社 | Dielectric filter for base station communication equipment |
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