JPS6162203A - Microwave filter using dielectric resonator - Google Patents
Microwave filter using dielectric resonatorInfo
- Publication number
- JPS6162203A JPS6162203A JP18377084A JP18377084A JPS6162203A JP S6162203 A JPS6162203 A JP S6162203A JP 18377084 A JP18377084 A JP 18377084A JP 18377084 A JP18377084 A JP 18377084A JP S6162203 A JPS6162203 A JP S6162203A
- Authority
- JP
- Japan
- Prior art keywords
- dielectric
- resonator
- resonators
- coupling
- block
- 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
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/20—Frequency-selective devices, e.g. filters
- H01P1/201—Filters for transverse electromagnetic waves
- H01P1/205—Comb or interdigital filters; Cascaded coaxial cavities
- H01P1/2056—Comb filters or interdigital filters with metallised resonator holes in a dielectric block
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- 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)
この発明は誘電体共振器を用いたマイクロ波フィルタの
構造だ関する。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to the structure of a microwave filter using a dielectric resonator.
(従来の技術)
従来よシ、共振器に誘電体共振器すなわち高誘電率を有
する誘電体を用いた高周波フィルタが提案されている。(Prior Art) Conventionally, high frequency filters have been proposed in which a dielectric resonator, that is, a dielectric material having a high dielectric constant is used as a resonator.
誘電体共振器はストリップ線路共振器と同程度の大きさ
で共振器か実現出来、しかも無負荷Qは導波管共振器と
同程度のものが容易に得られるという利点がある。A dielectric resonator has the advantage that it can be realized with a size comparable to that of a strip line resonator, and that an unloaded Q of the same magnitude as a waveguide resonator can be easily obtained.
また、実際に製作する場合の加工工作もストリップ線路
共振器よシ複雑であるが、導波管共振器よシは容易であ
る。In addition, the actual manufacturing process is more complicated than that of a stripline resonator, but it is easier than that of a waveguide resonator.
しかし、誘電体共振器は温度特性が致命的に悪いという
欠点があったが、誘電体材料工学の進歩は、この問題を
解決しつつある。したがって、誘電体共振器を用いた誘
電体フィルタの重要性は優めて大きい。このような理由
から誘電体共振器を使用したフィルタは今後増々利用さ
れると思われる。However, dielectric resonators had the drawback of fatally poor temperature characteristics, but advances in dielectric material engineering are beginning to solve this problem. Therefore, dielectric filters using dielectric resonators are extremely important. For these reasons, filters using dielectric resonators are expected to be used more and more in the future.
このような、誘電体共振器を用いたフィルタとして、特
開昭54−3448号、特開昭55−68702号、特
開昭56−144602号のものが本願出願人によシ提
案されている。As such filters using dielectric resonators, filters disclosed in Japanese Patent Application Laid-open No. 54-3448, Japanese Patent Application Laid-Open No. 55-68702, and Japanese Patent Laid-Open No. 56-144602 have been proposed by the applicant of the present application. .
従来より、誘電体共振器を用いたマイクロ波フィルタの
構成例を第2図に示す。金属製ケースの両端に設けられ
た入出力端子1,2及びそれらに接続される伝送線路2
3.24が配量され、この伝送線路23.24間にコア
状又は角柱状の各々が分離した誘電体共振器25.26
,27.28が配列されている。フィルタを構成するば
ば、入出力の伝送線路23.24と誘電体共振器25゜
28との結合を所望の大きさに設定する。この結合の設
定は、共振器25.28と伝送線路2 、’l 。FIG. 2 shows an example of the configuration of a conventional microwave filter using a dielectric resonator. Input/output terminals 1 and 2 provided at both ends of the metal case and transmission line 2 connected to them
3.24 is arranged between the transmission lines 23 and 24, and dielectric resonators 25 and 26 each having a core shape or a prismatic shape are separated.
, 27.28 are arranged. The coupling between the input/output transmission lines 23, 24 and the dielectric resonators 25.degree. 28 constituting the filter is set to a desired magnitude. This coupling setup consists of a resonator 25.28 and a transmission line 2,'l.
24との間隔dを変えることによシ行っている。This is done by changing the distance d from 24.
すなわち、間隔dを狭くすれば結合が犬きくなシ、間隔
dを広げれば結合は小さくなる。寸だ誘電体共振器25
.2に 、27.28各々の間隔もフィルタの実現に際
して必゛〃な結合度をイ:1らルる様な間隔に選定する
必要がある。That is, if the spacing d is narrowed, the coupling becomes tighter, and if the spacing d is widened, the coupling becomes smaller. Dielectric resonator 25
.. Second, the intervals between 27 and 28 must be selected such that the required degree of coupling is 1:1 when realizing the filter.
この動作原理を111単に説明する。第3図は電流と磁
界の関係を示す図であり、29は導体である。The principle of this operation will be briefly explained. FIG. 3 is a diagram showing the relationship between current and magnetic field, and 29 is a conductor.
電磁気宇によると導体に電流工が流れると電磁界が発生
する。この電流によシ発生した電(磁界の大きさ1/i
4体からの距離が離れるに従って減少する。According to electromagnetism, when electric current flows through a conductor, an electromagnetic field is generated. The electric current generated by this current (magnetic field size 1/i
It decreases as the distance from the four increases.
誘電体共振器と伝送線路との結合は電磁界を介して行な
われるので、誘電体共振器と伝送線路の距濡を変えるこ
とにより結合量を変化させることができる。これが第2
図に示す従来のフィルタにおいて間隔を小さくすると結
合量が大きくなる理由である。Since the dielectric resonator and the transmission line are coupled through an electromagnetic field, the amount of coupling can be changed by changing the distance between the dielectric resonator and the transmission line. This is the second
This is the reason why in the conventional filter shown in the figure, the amount of coupling increases as the spacing decreases.
また、各々の誘電体共振器を個々に製造しないで、板状
の誘電体内の内心体間に溝または穴を設けたものとして
特開昭57−48801号として、本願出願人よシ出願
されている。In addition, the present applicant has filed an application as JP-A No. 57-48801 in which grooves or holes are provided between inner core bodies in a plate-shaped dielectric material without manufacturing each dielectric resonator individually. There is.
(発明が解決しようとする問題点)
このように、゛従来のフィルタがコア状又は角柱状の個
々の単一共振器を縦続接続して誘電体フィルタを実現し
ているが、下記の様な欠点をイ〕する。(Problems to be solved by the invention) In this way, conventional filters realize dielectric filters by cascading individual core-shaped or prismatic single resonators. A) to address the shortcomings.
(1) 各誘電体共振器を組立てる時、共振器の中心
からの距離即ち内導体間ピッチを精度良く配置すること
は難しく特性が変動しやすい。(1) When assembling each dielectric resonator, it is difficult to precisely arrange the distance from the center of the resonator, that is, the pitch between the inner conductors, and the characteristics tend to fluctuate.
(2)各々の誘電体共振器が単独で存在するために、フ
ィルタを構成するために必要な誘電体共振器を固定する
だめの方法が難しい。(2) Since each dielectric resonator exists independently, it is difficult to fix the dielectric resonators necessary to construct the filter.
(3) 急峻な特性を実現する際、誘電体共振器を多
く必要とするが、その際誘電体共振器を各々加 Jj
、 )、工するため誘電体共振器の単価が高価になり、
フィルタの価格も高価になる。(3) When realizing steep characteristics, many dielectric resonators are required, but in this case, each dielectric resonator is added.
), the unit cost of the dielectric resonator becomes expensive due to the
The price of the filter will also be high.
また、複数の共振器の内導体間に溝または穴を設けたも
のは、一つの誘電体でフィルタを構成しているため、誘
電体フィルタの歩留シが上がらないという欠点がある。Furthermore, in the case where grooves or holes are provided between the inner conductors of a plurality of resonators, the filter is made of a single dielectric material, so there is a drawback that the yield rate of the dielectric filter cannot be increased.
(問題点を解決するだめの手段)
本発明のフィルタは、複数の誘電体共振器を1グロ、り
とし、lブロックの当該誘電体共振器は一体の誘電体で
形成する。一体の誘電体内の個々の共振器は柱状であり
、従って個々の共振器間には溝が構成しており、誘電体
は一体であるから個々の共振器間はその一部を連続的に
形成しである。(Means for Solving the Problems) The filter of the present invention includes a plurality of dielectric resonators in one block, and the dielectric resonators in one block are formed of a single dielectric. The individual resonators within the integral dielectric are columnar, so grooves are formed between the individual resonators, and since the dielectric is integral, a portion of the resonators are continuously formed between the individual resonators. It is.
そして、複数の誘電体共振器を形成する各グロックの共
振器間を空間で完全に分離しである空間結合によシ複敢
個連結しである。The resonators of each Glock forming a plurality of dielectric resonators are completely separated by space and connected multiple times through spatial coupling.
(作 用)
印加された電気信号は、入力段の誘電体共振器により電
磁界を発生し、この電磁界は同一誘電体内の隣接する段
間誘電体共振器間に形成する溝の部分の結合部を介して
当該隣接の段間共振器へ電磁界をつたえる。股間共振器
4に達した電磁界は、前記誘電体が形成する第1のグロ
ックと、他の誘電体ブロックが形成する第2のグロ、り
の間に設けた空間結合部を介して第2のグロ、りに形成
された1段間共振器に伝えられる。順次このような動作
をくシ返しながら電気信号を最終段の誘電体共振器へ伝
える。(Function) The applied electric signal generates an electromagnetic field by the dielectric resonator of the input stage, and this electromagnetic field causes coupling between the grooves formed between adjacent interstage dielectric resonators in the same dielectric. The electromagnetic field is transmitted to the adjacent interstage resonator through the section. The electromagnetic field that has reached the groin resonator 4 is transmitted to the second groove through a spatial coupling section provided between the first groove formed by the dielectric and the second groove formed by another dielectric block. It is transmitted to the interstage resonator formed in the groove. The electric signal is transmitted to the final stage dielectric resonator by repeating this operation one after another.
各誘電体共振器間の結合は、電界結合と磁界結合との不
均質によりもたらされると推定されている。It is estimated that the coupling between each dielectric resonator is caused by inhomogeneity between electric field coupling and magnetic field coupling.
(実施例)
第1図はこの発明の実施例の樺造を説明するための斜視
図であって全体を覆う金属ケースは省略しである。第1
図において、1は入力端子、2は出力端子、3は入力段
の誘電体共振器、4,5は股間の誘電体共振器、6は出
力段の誘電体共振器。(Embodiment) FIG. 1 is a perspective view for explaining a birch construction according to an embodiment of the present invention, and a metal case covering the entire structure is omitted. 1st
In the figure, 1 is an input terminal, 2 is an output terminal, 3 is an input stage dielectric resonator, 4 and 5 are dielectric resonators between the legs, and 6 is an output stage dielectric resonator.
7.8はt117結合部、9は第1の誘電体フ゛0ツク
と第2の誘電体ブロックを結合する空間結合部である。7.8 is a t117 coupling portion, and 9 is a spatial coupling portion that couples the first dielectric block and the second dielectric block.
10は内導体、11は内導体10に接続する・ぐターン
で°ある。10 is an inner conductor, and 11 is a turn connected to the inner conductor 10.
このマイクロ波フィルタの動作は入力端子より印加され
た電気信号は第1の誘電体グロ、り内に設けられた人力
段の誘電体共振2:’r 、7により′電磁界を発生し
この電磁界は隣接の段間共振器4間に設けられた溝加工
された結合部7を介して段間共振器4へ電磁界をつたえ
る。段間共振器4に達した電磁界は誘電体ブロック1と
誘電体グロック2の間に設けられた空間結合部9を介し
て誘電体ブロック2に形成された段間共振器5に電磁界
を伝える。順次このような動作をくり返しながら電気信
号を誘電体フィルタの出力に設けられた負荷へ電気エイ
・ルギーを供給するものである。The operation of this microwave filter is such that an electric signal applied from the input terminal generates an electromagnetic field due to the dielectric resonances 2:'r and 7 of the manual stage provided in the first dielectric group. The electromagnetic field is transmitted to the interstage resonators 4 via grooved coupling portions 7 provided between adjacent interstage resonators 4. The electromagnetic field that has reached the interstage resonator 4 is transmitted to the interstage resonator 5 formed in the dielectric block 2 via the spatial coupling section 9 provided between the dielectric block 1 and the dielectric Glock 2. tell. While repeating such operations one after another, an electric signal is supplied to a load provided at the output of the dielectric filter.
次に、ここに設けられた各誘電体共振器の共振周波数は
誘電体共振器の高さく内導体1oの高さ)及び周波数1
!l整・やターン11等により決定され、この調整は機
械的な工法または光学的な工法により行なうことが可能
である。Next, the resonant frequency of each dielectric resonator provided here is determined by the height of the dielectric resonator (the height of the inner conductor 1o) and the frequency 1
! It is determined by the adjustment, turn 11, etc., and this adjustment can be performed by a mechanical method or an optical method.
結合部は誘電体ブロックに設けられた溝の幅。The joint part is the width of the groove provided in the dielectric block.
深さ等により決定され、誘電体グロ、り間の結合はグo
yり間の間隔により決定することが出来、フィルタを構
成するために必要な結合度を得る長さに合わせる。Determined by the depth etc., the coupling between the dielectric grooves and grooves is determined by the depth etc.
It can be determined by the spacing between the y-rings, and the length is adjusted to obtain the degree of coupling necessary to construct the filter.
(発明の効果)
この発明は以上説明したように誘電体プロ、夕に複数個
の円柱形状の中心導体を設は誘電体共振器を実現し、こ
れらの誘電体共振器を用いフィルタを構成するために、
これら誘電体共振器間の距離はフィルタを実現するため
に必要な結合度を得るために必要な溝の寸法により決ま
る。また各々の誘電体ブロックの間隔はフィルタを構成
するために必要な結合度を得る長さに合わせる。(Effects of the Invention) As explained above, this invention realizes a dielectric resonator by providing a plurality of cylindrical center conductors using a dielectric material, and constructs a filter using these dielectric resonators. for,
The distance between these dielectric resonators is determined by the dimensions of the grooves necessary to obtain the degree of coupling necessary to realize the filter. Further, the spacing between each dielectric block is adjusted to a length that provides the degree of coupling necessary to construct the filter.
従ってこの発明の誘電体フィルタは誘電体ブロックに円
柱形状の中心導体を設は誘電体共振器を実現し、共振器
間に溝を設けて結合を得る構造のブロックを組み合わせ
てマイクロ波フィルタを実現するもので、誘電体材料の
大きさに自由度をもたせることが出来、この種のフィル
タの構成ておいて最も特性変動の大きい中心導体間距離
も組立 lて時変動することが少く、また組立て法は
誘電体 5(iが一体となっているために取り付けが
簡単である等の利点を有している。Therefore, in the dielectric filter of this invention, a dielectric resonator is realized by providing a cylindrical center conductor in a dielectric block, and a microwave filter is realized by combining blocks with a structure in which grooves are provided between the resonators to obtain coupling. This allows flexibility in the size of the dielectric material, and the distance between the center conductors, which has the largest characteristic variation in this type of filter configuration, does not vary much during assembly. This method has advantages such as easy installation because the dielectric 5 (i) is integrated.
また、この誘電体フィルタの特徴は誘電体フィルタを数
個の誘電体共振器のグa2りに分割して構成することに
ある。Further, the feature of this dielectric filter is that the dielectric filter is divided into several groups a2 of dielectric resonators.
これによシ誘電体共振器の円柱形状の中心導体間の間隔
を精密に設定する数が減少し誘電体フィルタの歩留りが
向上することにある。This reduces the number of times to precisely set the spacing between the cylindrical center conductors of the dielectric resonator, and improves the yield of dielectric filters.
第1図は本発明の一実施例を説明するための斜視図、第
2図は従来の誘電体フィルタの平面図、8g3図は電流
と磁界の関係を示す図である。
3.4,5.6・・・誘電体共振器、7,8・・・溝結
合部、9・・・空間績−訃部。
特許出願人 沖電気工業株式会社
第1図
第2図FIG. 1 is a perspective view for explaining an embodiment of the present invention, FIG. 2 is a plan view of a conventional dielectric filter, and FIG. 8g3 is a diagram showing the relationship between current and magnetic field. 3.4, 5.6... Dielectric resonator, 7, 8... Groove coupling portion, 9... Spatial connection-end portion. Patent applicant: Oki Electric Industry Co., Ltd. Figure 1 Figure 2
Claims (1)
電体共振器を構成する誘電体と一体で連続に形成した前
記共振器を複数個空間結合により連結したことを特徴と
する誘電体共振器を用いたマイクロ波フィルタ。A plurality of columnar dielectric resonators each having a groove between them and a part of which is continuously formed integrally with a dielectric constituting the dielectric resonator are connected by spatial coupling. A microwave filter using a dielectric resonator.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18377084A JPS6162203A (en) | 1984-09-04 | 1984-09-04 | Microwave filter using dielectric resonator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18377084A JPS6162203A (en) | 1984-09-04 | 1984-09-04 | Microwave filter using dielectric resonator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6162203A true JPS6162203A (en) | 1986-03-31 |
Family
ID=16141653
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP18377084A Pending JPS6162203A (en) | 1984-09-04 | 1984-09-04 | Microwave filter using dielectric resonator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6162203A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4837534A (en) * | 1988-01-29 | 1989-06-06 | Motorola, Inc. | Ceramic block filter with bidirectional tuning |
EP0322780A2 (en) * | 1987-12-28 | 1989-07-05 | Oki Electric Industry Company, Limited | Dielectric filter with attenuation pole |
JPH06252607A (en) * | 1993-02-17 | 1994-09-09 | Siemens Matsushita Components Gmbh & Co Kg | Adjusting method of resonance frequency for ceramic resonator |
EP0774798A3 (en) * | 1995-11-16 | 1997-06-11 | Ngk Spark Plug Co |
-
1984
- 1984-09-04 JP JP18377084A patent/JPS6162203A/en active Pending
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0322780A2 (en) * | 1987-12-28 | 1989-07-05 | Oki Electric Industry Company, Limited | Dielectric filter with attenuation pole |
US4837534A (en) * | 1988-01-29 | 1989-06-06 | Motorola, Inc. | Ceramic block filter with bidirectional tuning |
JPH06252607A (en) * | 1993-02-17 | 1994-09-09 | Siemens Matsushita Components Gmbh & Co Kg | Adjusting method of resonance frequency for ceramic resonator |
EP0774798A3 (en) * | 1995-11-16 | 1997-06-11 | Ngk Spark Plug Co | |
US5841332A (en) * | 1995-11-16 | 1998-11-24 | Ngk Spark Plug Co., Ltd. | Dielectric filter and method of adjusting central frequency of the same |
EP1119070A1 (en) * | 1995-11-16 | 2001-07-25 | NGK Spark Plug Co. Ltd. | Dielectric filter and method of adjusting central frequency of the same |
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