JPS59117302A - Filter - Google Patents
FilterInfo
- Publication number
- JPS59117302A JPS59117302A JP22485582A JP22485582A JPS59117302A JP S59117302 A JPS59117302 A JP S59117302A JP 22485582 A JP22485582 A JP 22485582A JP 22485582 A JP22485582 A JP 22485582A JP S59117302 A JPS59117302 A JP S59117302A
- Authority
- JP
- Japan
- Prior art keywords
- coaxial
- electric field
- dielectric
- fundamental frequency
- harmonic
- 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.)
- Granted
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
Abstract
Description
【発明の詳細な説明】
(1)発明の技術分野
本発明は無線装置などに使用される帯域通過型フィルタ
(BPF)に関し、特に複数の共振器を有する多段同軸
型誘電体フィルタに関する。DETAILED DESCRIPTION OF THE INVENTION (1) Technical Field of the Invention The present invention relates to a bandpass filter (BPF) used in wireless devices, and more particularly to a multistage coaxial dielectric filter having a plurality of resonators.
(2)技術の背景
従来一般に、例えば車載無線や携帯無線などのVHF帯
、UHF帯の移動無線装置においてはBPFとして多段
同軸型フィルタが使用されている。多段同軸型フィルタ
には、キャビティ型をはじめとして数多くの種類がある
。近年は特に、小型軽量、温度特性が良好、低損失など
の特長を有する誘電体フィルタが多用されている。(2) Background of the Technology Conventionally, multi-stage coaxial filters are generally used as BPFs in VHF band and UHF band mobile radio devices such as in-vehicle radios and portable radios. There are many types of multistage coaxial filters, including cavity types. In recent years, dielectric filters, which have features such as small size, light weight, good temperature characteristics, and low loss, have come into widespread use.
しかるに、従来の同軸壓フィルタには後述するような問
題があり、その対策が要望されている。However, conventional coaxial filters have problems as described below, and countermeasures are desired.
(3)従来技術と問題点
第1図は従来の4段同軸型誘電体フィルタ(以下単に「
フィルタ」と略記)を示す。このフィルタは誘電体ブロ
ック1 (以下単に「ブロック」と略記)に4つの貫通
穴2を設け、ブロック1の外表面のうち1つの穴開口面
1a(図では上面)を除く他の5つの外表面ならびに穴
2の内表面に導体膜(図中、ハツチングで明示)全形成
(メタライズ)しである。これによりブロック外表面の
導体膜が外導体となり、また穴内表面の導体膜が内導体
となり、それぞれの穴2の内導体が穴の深さをZ波長と
する周波数で共振する共振器を構成する。従ってブロッ
ク1の両端全適当な励振体3(図示例ではメタライズさ
れた透体パターンによるCカップル)を介して外部回路
に接続すれば、フィルタはBPFとして動作する。(3) Prior art and problems Figure 1 shows a conventional four-stage coaxial dielectric filter (hereinafter simply "
(abbreviated as "filter"). This filter has four through holes 2 in a dielectric block 1 (hereinafter simply referred to as "block"), and the other five holes on the outer surface of the block 1 except for one hole opening surface 1a (top surface in the figure). A conductive film (indicated by hatching in the figure) is completely formed (metalized) on the surface and the inner surface of the hole 2. As a result, the conductive film on the outer surface of the block becomes the outer conductor, and the conductive film on the inner surface of the hole becomes the inner conductor, and the inner conductor of each hole 2 constitutes a resonator that resonates at a frequency whose Z wavelength is the depth of the hole. . Therefore, if both ends of the block 1 are connected to an external circuit via a suitable excitation body 3 (in the illustrated example, a C couple made of a metalized transparent pattern), the filter operates as a BPF.
しかるに、共振器2は、穴の深さをへ波長とする基本周
波数f。以外に、穴の深さを%、 5/4−1−−(
ルは奇数)波長とする奇数次の高調波成分” fO+
” fO、・・・、rLfoでも共振する性質を持って
いる。従ってフィルタの通過波は第2図に示す如くナル
。このようなフィルタを送信機のBPFとして用いた場
合、送信機のパワーアンプによって増幅された3fo、
sfo、・・・といった高調波成分もBPFを通過して
、アンテナから送出されるという問題がある。特に、3
foはエネルギーが大きく、非常に有害である。However, the resonator 2 has a fundamental frequency f whose wavelength is the depth of the hole. In addition, the depth of the hole is %, 5/4-1-(
is an odd number) harmonic component of an odd order with wavelength fO+
” fO, ..., rLfo also have the property of resonating.Therefore, the passing wave of the filter is null as shown in Figure 2.When such a filter is used as a BPF of a transmitter, the power amplifier of the transmitter 3fo amplified by
There is a problem in that harmonic components such as sfo, . . . also pass through the BPF and are sent out from the antenna. In particular, 3
fo has a large amount of energy and is extremely harmful.
(4)発明の目的
本発明の目的は、上記のような従来の多段同軸型フィル
タにおける問題を解決すること、すなわち基本周波数の
高調波成分、特にエネルギーの大きい3fo−’i有効
に減衰させ、実質上中心周波数f。のみを通過させ得る
ような高次スプリアス特性の良い誘電体フィルタを提供
することにある。(4) Purpose of the Invention The purpose of the present invention is to solve the problems in the conventional multistage coaxial filter as described above, namely, to effectively attenuate the harmonic components of the fundamental frequency, especially 3fo-'i, which have large energy; substantially the center frequency f. The object of the present invention is to provide a dielectric filter with good high-order spurious characteristics that allows only the above-mentioned spurious signals to pass through.
(5)発明の構成
本発明による多段同軸型防電体フィルタは、概略的には
、共振器どうしが基本周波数の高調波成分の電界分布の
最小点の位置で結合するように構成ちれたものである。(5) Structure of the Invention The multistage coaxial electric shield filter according to the present invention is generally configured such that the resonators are coupled to each other at the minimum point of the electric field distribution of harmonic components of the fundamental frequency. It is something.
(6)発明の実施例
以トー1本発明の実施例につき図面を参照して詳細に説
明する。(6) Embodiments of the Invention Embodiments of the present invention will be described in detail with reference to the drawings.
第3図は本発明によるフィルタの第1実施例を示す。こ
のフィルタは基本的には第1図に示した誘電体フィルタ
と同じものである。しかし、ブロック1を2個の部分I
A、IBに分割し、それらの間に導体の材料から成る遮
蔽板4を介在させてりる。第4図に示すように、遮蔽板
4には結合窓5を形成しである。結合窓5の位置は、第
5図に示す如く高調波成分3foの電界分布が最小とな
る点P。の位置、つまりブロック1の高さHとした場合
に底面からほぼV3・Hの位置としである。FIG. 3 shows a first embodiment of a filter according to the invention. This filter is basically the same as the dielectric filter shown in FIG. However, block 1 can be divided into two parts I
It is divided into A and IB, and a shielding plate 4 made of a conductive material is interposed between them. As shown in FIG. 4, a coupling window 5 is formed in the shielding plate 4. As shown in FIG. The position of the coupling window 5 is a point P where the electric field distribution of the harmonic component 3fo is minimum, as shown in FIG. , that is, when the height of the block 1 is H, the position is approximately V3·H from the bottom surface.
従って共振器2A、 2B (第3図)間では、中心周
波数f。は結合窓5を介して通過し得るが、3fOは結
合窓5をわずかしか通過できず、大幅に減衰される。こ
の結果、3foのスプリアス特性は第6図の如く改善さ
れる。この場合、5f0のスプリアス特性は改善されな
いが、そのエネルギーはかなり小さいので実用上問題と
なることは少ない。Therefore, between the resonators 2A and 2B (FIG. 3), the center frequency f. can pass through the coupling window 5, but 3fO can only pass through the coupling window 5 to a small extent and is greatly attenuated. As a result, the spurious characteristics of 3FO are improved as shown in FIG. In this case, the spurious characteristics of 5f0 are not improved, but since the energy thereof is quite small, it is unlikely to be a problem in practice.
第7図は本発明の第2実施例を示す。この例ではブロッ
ク1を3つの部分LA、IB、ICに分割してそれぞれ
の間に第4図に示す如き遮蔽板4A。FIG. 7 shows a second embodiment of the invention. In this example, the block 1 is divided into three parts LA, IB, and IC, and a shielding plate 4A as shown in FIG. 4 is provided between each part.
4Bi介在させてあり、第3図の場合と比べて3foの
スプリアス特性は一層向上する。また、この実施例にお
いて中央のブロック部分IBも更に2分割してそれらの
間にも遮蔽板を介在させれば、3f0は共振器2の各結
合段ごとに減衰されることになり、極めて良好なスプリ
アス特性を実現できる。更に、この実施例において各遮
蔽板4A、 4B、・・・の結合窓5の位置を3foの
電界分布最小点、5f0の電界分布最小点というように
異なる位置に形成すれば、3foたけでなく5f0以上
の高次のスプリアス特性も改善きれる。4Bi is interposed, and the spurious characteristics of 3fo are further improved compared to the case of FIG. In addition, in this embodiment, if the central block portion IB is further divided into two and a shielding plate is interposed between them, 3f0 will be attenuated for each coupling stage of the resonator 2, which will be extremely effective. It is possible to realize spurious characteristics. Furthermore, in this embodiment, if the coupling windows 5 of each shielding plate 4A, 4B, . High-order spurious characteristics of 5f0 or higher can also be improved.
第8図は本発明の第3の実施例を示す。この実施例は前
述のような遮蔽板を用いずに、ブロック部分IBの側面
1bに、結合窓60部分を除いて導体膜を形成した構造
である。この場合も第3図に示す実施例と同様の効果が
得られる。FIG. 8 shows a third embodiment of the invention. This embodiment has a structure in which a conductive film is formed on the side surface 1b of the block portion IB except for the coupling window 60 portion, without using a shielding plate as described above. In this case as well, effects similar to those of the embodiment shown in FIG. 3 can be obtained.
尚、第3図及び第7図に示す第1および第2実施例の場
合、遮蔽板4. 4A、 4B、・・・を単独の部品と
せずに、ブロック1を収容する金属筐体と一体形成する
ことも可能である。In the case of the first and second embodiments shown in FIGS. 3 and 7, the shielding plate 4. It is also possible to form the blocks 4A, 4B, . . . not as independent parts, but integrally with the metal casing that houses the block 1.
(7)発明の効果
以上のように本発明によれば、通過させるべき基本周波
数以外の高調波成分を有効に減衰させ得る高次スプリア
ス特性のすぐれた多段同軸型フィルタを実現可能である
。(7) Effects of the Invention As described above, according to the present invention, it is possible to realize a multistage coaxial filter with excellent high-order spurious characteristics that can effectively attenuate harmonic components other than the fundamental frequency to be passed.
第1図は従来の同軸型誘電体フィルタの一例の概略斜視
図、第2図は第1図のフィルタの特性を示すグラフ、第
3図は本発明による同軸型誘電体フィルタの第1実施例
の概略斜視図、第4図は遮蔽板の側面図、第5図は誘電
体フィルタの電界分布説明図、第6図は第1実施例の特
性を示すグラフ、第7図は本発明の第2実施例の概略斜
視図、第8図は本発明の第3実施例の概略斜視図である
。
1・・・誘電体ブロック、
]、A、IB、IC・・・ブロック部分、1a・・・穴
開口面、
2、2A、 2B・・・穴(共振器)、 3・・・励振
体、4.4A、4B・・・遮蔽板、5.6・・・結合窓
。
特許出願人
富士通株式会社
特許出願代理人
弁理士青水 朗
弁理士西舘和之
弁理士 内 1)辛 男
弁理士 山 口 昭 之
第1図
第 2図
f、 J io づ10周波数第3図
第4図
ム
第6図
@7図
8図FIG. 1 is a schematic perspective view of an example of a conventional coaxial dielectric filter, FIG. 2 is a graph showing the characteristics of the filter shown in FIG. 1, and FIG. 3 is a first embodiment of a coaxial dielectric filter according to the present invention. 4 is a side view of the shielding plate, FIG. 5 is an explanatory diagram of the electric field distribution of the dielectric filter, FIG. 6 is a graph showing the characteristics of the first embodiment, and FIG. 7 is a diagram showing the characteristics of the first embodiment. FIG. 8 is a schematic perspective view of the second embodiment of the invention, and FIG. 8 is a schematic perspective view of the third embodiment of the present invention. 1... Dielectric block, ], A, IB, IC... Block part, 1a... Hole opening surface, 2, 2A, 2B... Hole (resonator), 3... Exciter, 4.4A, 4B... Shielding plate, 5.6... Combined window. Patent Applicant Fujitsu Limited Patent Application Agent Patent Attorney Akira Aomi Patent Attorney Kazuyuki Nishidate Patent Attorney 1) Shino Patent Attorney Akiyuki Yamaguchi Figure 1 Figure 2 f, Jio 10 Frequency Figure 3 Figure 4 Figure 6 @ Figure 7 Figure 8
Claims (1)
おいて、共振器どうしが基本周波数の高調波成分の電界
分布の最小点の位置で結合するように構成されたことを
特徴とするフィルタ。1. A multistage coaxial dielectric filter having a plurality of resonators, characterized in that the resonators are coupled to each other at the minimum point of the electric field distribution of harmonic components of the fundamental frequency.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP22485582A JPS59117302A (en) | 1982-12-23 | 1982-12-23 | Filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP22485582A JPS59117302A (en) | 1982-12-23 | 1982-12-23 | Filter |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS59117302A true JPS59117302A (en) | 1984-07-06 |
JPH0417481B2 JPH0417481B2 (en) | 1992-03-26 |
Family
ID=16820217
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP22485582A Granted JPS59117302A (en) | 1982-12-23 | 1982-12-23 | Filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59117302A (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6258701A (en) * | 1985-09-06 | 1987-03-14 | Alps Electric Co Ltd | Waveguide filter |
JPS63142901A (en) * | 1986-12-05 | 1988-06-15 | Murata Mfg Co Ltd | Dielectric coaxial resonator |
JPH0250502A (en) * | 1988-08-11 | 1990-02-20 | Tdk Corp | Dielectric filter |
JPH0356203U (en) * | 1989-10-05 | 1991-05-30 | ||
JPH03136402A (en) * | 1989-10-20 | 1991-06-11 | Toko Inc | Dielectric filter |
US5319328A (en) * | 1991-06-25 | 1994-06-07 | Lk-Products Oy | Dielectric filter |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS549014A (en) * | 1977-06-22 | 1979-01-23 | Aoki Metal | Method of connecting tap lead pipe |
JPS57133101U (en) * | 1981-02-16 | 1982-08-19 |
-
1982
- 1982-12-23 JP JP22485582A patent/JPS59117302A/en active Granted
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS549014A (en) * | 1977-06-22 | 1979-01-23 | Aoki Metal | Method of connecting tap lead pipe |
JPS57133101U (en) * | 1981-02-16 | 1982-08-19 |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6258701A (en) * | 1985-09-06 | 1987-03-14 | Alps Electric Co Ltd | Waveguide filter |
JPS63142901A (en) * | 1986-12-05 | 1988-06-15 | Murata Mfg Co Ltd | Dielectric coaxial resonator |
JPH0250502A (en) * | 1988-08-11 | 1990-02-20 | Tdk Corp | Dielectric filter |
JPH0356203U (en) * | 1989-10-05 | 1991-05-30 | ||
JPH03136402A (en) * | 1989-10-20 | 1991-06-11 | Toko Inc | Dielectric filter |
US5319328A (en) * | 1991-06-25 | 1994-06-07 | Lk-Products Oy | Dielectric filter |
Also Published As
Publication number | Publication date |
---|---|
JPH0417481B2 (en) | 1992-03-26 |
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