JPS59126302A - Dielectric filter - Google Patents
Dielectric filterInfo
- Publication number
- JPS59126302A JPS59126302A JP22485182A JP22485182A JPS59126302A JP S59126302 A JPS59126302 A JP S59126302A JP 22485182 A JP22485182 A JP 22485182A JP 22485182 A JP22485182 A JP 22485182A JP S59126302 A JPS59126302 A JP S59126302A
- Authority
- JP
- Japan
- Prior art keywords
- block
- filter
- dielectric
- input
- external 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.)
- 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
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】
(1)発明の技術分野
本発明は誘電体フィルタに関し、特に通堝帯竣外減衰特
性を改善するだめの改良構造に関するものである。DETAILED DESCRIPTION OF THE INVENTION (1) Technical Field of the Invention The present invention relates to a dielectric filter, and more particularly to an improved structure for improving the external attenuation characteristics of the filter.
(2)技術の背景
一般に、誘電体フィルタは、小型軽量かつ温度変化に対
する影、響が少い等の長所を有しているので、各種の通
信装置等に多用されている。特に、移動無線と呼ばれる
携帯無線装置や車載無線装置には、小型軽量かつ温度変
化に対する影響の少いフィルタが要求されるので、誘電
体フィルタが多用されている。(2) Background of the Technology In general, dielectric filters have the advantages of being small, lightweight, and less affected by temperature changes, and are therefore widely used in various communication devices. In particular, dielectric filters are frequently used in portable radio devices called mobile radio devices and in-vehicle radio devices, as they require filters that are small, lightweight, and less susceptible to temperature changes.
この種の誘電体フィルタは、一般に、直方体状の誘雷、
体プロ、りに複数個の貫通穴を設は該穴の内、共振素子
用貫通穴の内面をメタライズして内部導体膜を有する共
振用穴(共振素子)を形成し、かつ該ブロックの所要表
面をメタライズして外部導体膜を形成し、さらに該プロ
、り両端部に入出力用端子(励振体)を設けて、バンド
・ノ卆ス・フィルタ(BPF:帯域通過フィルタ)とし
て構成されている。そして、入出力用端子と共振素子、
及び共振素子相互が電磁界結合し、各共振素子が所定の
帯域に共振して該帯域が出力端子より外部回路に出力さ
れる。ととろが、入力用端子と共振素子間及び共振素子
相互間の青磁界エネルギーの一部が誘電体プロ、りの外
部に漏洩して出力端子と結合する場合や、入力用端子の
電磁界エネルギーの一部が空間を介して直接出力端子と
結合する場合があり、これらの現象はフィルタの通過帯
域外減衰特性(減衰帯域の減衰特性)に悪影響(特性の
劣化)を与えることになる。特に、共振素子の段数が少
い小型の誘電体フィルタは、入出力用端子間の距離が小
さいのでこの傾向が比較的強い。This type of dielectric filter generally has a rectangular parallelepiped lightning arrester,
To provide a plurality of through-holes in the block, the inner surface of the through-hole for a resonant element is metalized to form a resonant hole (resonant element) having an internal conductor film, and the required amount of the block is The surface is metallized to form an external conductive film, and input/output terminals (exciter) are provided at both ends of the filter to form a band pass filter (BPF). There is. Then, input/output terminals and resonant elements,
The resonant elements are electromagnetically coupled to each other, each resonant element resonates in a predetermined band, and the band is output from the output terminal to an external circuit. In some cases, a part of the celadon magnetic field energy between the input terminal and the resonant element or between the resonant elements leaks to the outside of the dielectric material and couples with the output terminal, or when the electromagnetic field energy of the input terminal A portion of the filter may be directly coupled to the output terminal through space, and these phenomena adversely affect (deteriorate the characteristics) the attenuation characteristics outside the passband (attenuation characteristics in the attenuation band) of the filter. This tendency is particularly strong in small dielectric filters with a small number of resonant element stages because the distance between the input and output terminals is small.
従って、このよう々現象を防止し得る構造の誘電体フィ
ルタが要望されている。Therefore, there is a need for a dielectric filter having a structure that can prevent such phenomena.
(3)従来技術と問題点
第1図は従来の誘電体フィルタを説明するための図であ
り、(イ)は斜視図、←)は(イ)図の矢印A方向から
みた平面図、Cつけ(ロ)図のB−B’線に沿った側面
断面図である。同図において、符号10は誘雷、体フィ
ルタを示し、11は誘雷体ブロック、12゜13はプロ
、り11に形成された貫通穴、14゜15は入出力用端
子(金属棒からなる励振体)をそれぞれ示す。誘電体プ
ロ、り11は、その側面と下面の5面金てに、厚膜焼成
等の手法によりメタライズした外部導体膜16(図中ク
ロスハツチングで示す)が形成されている。貫通穴12
゜13それぞれの内面に前記と同様にメタライズした内
部導体膜12a、1’3aが設けられ、該内部導体膜1
2a、13aは下端が外部導体膜16と短絡され、上端
が開放されて形成されている。従って、貫通穴12.1
3は穴の深さく内部導体膜12a 、 13aの高さ)
を1/4波長(λ/4)とする周波数で共振する共振素
子(共振用穴)として形成されている。入出力用端子1
4.15はメタライズされていない穴17.18に嵌入
して取り付けられて励振体の役目を果すと共に外部回路
に接続される。このように、プロ、り11の上面がメタ
ライズされず開放された構造で少い段数(この場合、共
振素子が12と13から成る2段構成)で構成されたフ
ィルタは、入出力用端子14゜15間の距離が近くなる
ため、例えば符号14を入力用端子とすると、端子14
と共振素子12間、及び共振素子12.13間の電磁界
エネルギーの一部がブロック11の上面から外部に漏洩
して出力用端子15に結合する現象やまた入力用端子1
4の電磁界エネルギーの一部が空間を介して直接出力用
端子15に結合する現象が生じ易い。これらの現象によ
り、とのような従来のフィルタはその帯域外減衰特性が
劣化されるという問題がある0
(4)発明の目的
本発明の目的はJ記従来の問題点に鑑み、入力用端子と
共振素子間、及び共振素子間の電磁界エネルギーの漏洩
を抑制し、入出力用端子間の直接的雷、磁界エネルギー
の結合を抑制して、段数の少い小型のフィルタにおいて
も、フィルタの帯域外減衰特性の劣化を防止し得る誘電
体フィルタを提供することにある。(3) Prior art and problems Figure 1 is a diagram for explaining a conventional dielectric filter, where (A) is a perspective view, (←) is (A) a plan view seen from the direction of arrow A in the figure, and C is a diagram for explaining a conventional dielectric filter. It is a side sectional view along the BB' line of a (b) figure. In the same figure, reference numeral 10 indicates a lightning arrester and body filter, 11 indicates a lightning arrester block, 12° and 13 indicate through holes formed in the plate 11, and 14° and 15 indicate input/output terminals (made of metal rods). (excitation body) are shown respectively. The dielectric film 11 has an external conductor film 16 (indicated by crosshatching in the figure) metallized by a method such as thick film firing on its side and bottom surfaces. Through hole 12
Inner conductor films 12a and 1'3a which are metalized in the same manner as described above are provided on the inner surface of each of ゜13.
2a and 13a are formed such that their lower ends are short-circuited to the external conductor film 16 and their upper ends are open. Therefore, the through hole 12.1
3 is the depth of the hole and the height of the internal conductor films 12a and 13a)
It is formed as a resonant element (resonant hole) that resonates at a frequency of 1/4 wavelength (λ/4). Input/output terminal 1
4.15 is fitted in a non-metalized hole 17.18 and serves as an exciter and is connected to an external circuit. In this way, a filter configured with a structure in which the top surface of the filter 11 is not metalized and is open and has a small number of stages (in this case, a two-stage configuration consisting of resonant elements 12 and 13) is provided with the input/output terminal 14. Since the distance between ゜15 and ゜15 becomes close, for example, if the symbol 14 is used as an input terminal, the terminal 14
There is a phenomenon in which a part of the electromagnetic field energy between the resonant element 12 and the resonant elements 12 and 13 leaks to the outside from the top surface of the block 11 and is coupled to the output terminal 15.
A phenomenon in which a part of the electromagnetic field energy of No. 4 is directly coupled to the output terminal 15 through space tends to occur. Due to these phenomena, there is a problem in that the out-of-band attenuation characteristics of conventional filters such as (4) Object of the Invention are deteriorated. By suppressing the leakage of electromagnetic field energy between the resonant element and the resonant element, and by suppressing the coupling of direct lightning and magnetic field energy between the input and output terminals, even in a small filter with a small number of stages, the filter An object of the present invention is to provide a dielectric filter that can prevent deterioration of out-of-band attenuation characteristics.
(5)発明の構成
そして、との目的を達成するために、本発明に依れば、
直方体状の誘電体ブロックに長手方向に沿って複数個の
貫通穴を所定間隔で形成し、該ブロックの両端部に入出
力端子を設け、前記貫通穴の内、共振素子用貫通穴のプ
ロ、り表面における両開口のいづれか一方の開口周辺部
と前記入出力用端子の周辺部とを非メタライズ部分とし
て形成し、とれらの非メタライズ部分を除くブロック表
面金てと前記共振素子用貫通穴の内面とをメタライズし
て形成したことを特徴とする誘電体フィルタが提供され
る。(5) Structure of the invention In order to achieve the objects of and, according to the present invention,
A plurality of through holes are formed at predetermined intervals along the longitudinal direction in a rectangular parallelepiped dielectric block, input/output terminals are provided at both ends of the block, and among the through holes, a through hole for a resonant element is formed; The surrounding area of either of the openings and the surrounding area of the input/output terminal on the surface of the block are formed as non-metallized parts, and the metal part of the block surface excluding these non-metallized parts and the through hole for the resonance element are formed. Provided is a dielectric filter characterized in that it is formed by metallizing the inner surface.
(6)発明の実施例
以下、本発明の実施例を図面に基づいて詳細に説明する
。(6) Embodiments of the invention Hereinafter, embodiments of the invention will be described in detail based on the drawings.
第2図から第4図は本発明の詳細な説明するまための図
である。FIGS. 2 to 4 are detailed illustrations of the present invention.
第2図は本発明の第1実施例を示す図で、(イ)は斜視
図、←)は(イ)図の矢印A方向からみた平面図、eつ
は←)図のB −B’線に沿った側面断面図、に)は(
つ図の矢印C方向からみた下面図である。同図において
、符号20は誘電体フィルタを示す。尚、同図において
、前出の第1図に示した従来例と同一部分又は同一部品
に対しては第1図と同一符号が付されている。従って、
符号11は誘電体ブロック、12.13は貫通穴(共振
素子)、12a、13aは内部導体膜、14.15は入
出力用端子(金属棒からなる励振体)、16はプロ、り
11の側面と下面に形成された外部導体膜、17.18
はメタライズされていない穴をそれぞれ示し、とれらは
第1図の場合と同様に形成されているのでその説明は省
略する。さて、符号19はプロ、り11の上面にメタラ
イズされた外部導体膜を示し、前出の外部体膜16と接
続して形成されている。また、符号20.21はブロッ
ク11上面における貫通穴(共振素子)12.13の開
口周辺部をメタライズしないで形成した非メタライズ部
分をそれぞれ示す。従って、この非メタライズ部分20
゜21は貫通穴12.13の穴径を内径とするリング状
に形成されている。同様に、符号22 、23は、プロ
、り11上面における入出力用端子14゜15の周辺部
をメタライズしないで形成した非メタライズ部分を示す
。とのように1この第1実施例は、前記非メタライズ部
分20.21,22゜23を除いたプロ、り11の上面
金てに外部導体膜19を形成することによシ、該外部導
体膜19と前記外部導体膜16とによってプロ、り11
の表面のほとんどが被覆されて形成されている。そして
、これらの外部導体膜16.19自体がシールドケース
の役割を兼有するように形成されている。従って、この
フィルタは、プロ、り11内部の結合電磁界エネルギー
が外部へ漏洩するのを良好に抑制し、きわめて電気的に
安定したフィルタとして形成されている。従って、この
ように形成(7)
することにより、段数の少い小型のフィルタにおいても
、入出力用端子間の直接的電磁界エネルギーの結合が抑
制されて、フィルタの帯域外減衰特性の劣化を防止する
ことが可能となり、この結果帯域外減衰特性の良好なフ
ィルタを実現することができる。非メタライズ部分20
.21の幅は非常にせまくてもよく、例えば、−例とし
て、プロ、り11の巾がl1mで、貫通穴12.13の
穴径が3簡の場合で非メタライズ部分20.21の幅を
1m程度にしてその外径を5−程度に形成してもよく、
さらにこの幅をせ寸<シて%0.11111程度に形成
してもよい。但し、この幅を非常にせまくするほど通過
帯域の周波数が変化する傾向にあるが、これはブロック
11の高さ寸法、す力わち内部導体膜12ILs13m
の高さを調整して所定の通過帯域を得ることが容易にで
きるので問題ない。次に、第5図を参照して、との実施
例の減衰特性について説明する。FIG. 2 is a diagram showing the first embodiment of the present invention, (A) is a perspective view, (←) is a plan view seen from the direction of arrow A in (A), and e is (←) B-B' in the figure. Side cross-section along the line, to) is (
FIG. 3 is a bottom view seen from the direction of arrow C in the figure. In the figure, reference numeral 20 indicates a dielectric filter. In this figure, the same parts or parts as those of the conventional example shown in FIG. 1 mentioned above are given the same reference numerals as in FIG. Therefore,
11 is a dielectric block, 12.13 is a through hole (resonant element), 12a, 13a are internal conductor films, 14.15 is an input/output terminal (exciter made of a metal bar), 16 is a professional, External conductor film formed on side and bottom surfaces, 17.18
1A and 1B respectively indicate holes that are not metalized, and since they are formed in the same manner as in FIG. 1, their explanation will be omitted. Now, reference numeral 19 indicates an external conductor film metallized on the upper surface of the plate 11, which is connected to the aforementioned external body film 16. Further, reference numerals 20 and 21 indicate non-metalized portions formed without metalizing the opening periphery of the through hole (resonant element) 12 and 13 on the upper surface of the block 11, respectively. Therefore, this non-metallized portion 20
21 is formed into a ring shape whose inner diameter is the diameter of the through hole 12.13. Similarly, reference numerals 22 and 23 indicate non-metalized portions formed around the input/output terminals 14 and 15 on the upper surface of the plate 11 without metallization. 1 In this first embodiment, the outer conductor film 19 is formed on the upper surface of the plate 11 excluding the non-metalized portions 20, 21, 22, and 23. The film 19 and the outer conductor film 16 cause the film 11 to
Most of the surface is coated. These outer conductor films 16 and 19 themselves are formed to also serve as a shield case. Therefore, this filter effectively suppresses leakage of the coupled electromagnetic field energy inside the filter 11 to the outside, and is formed as an extremely electrically stable filter. Therefore, by forming the filter in this way (7), even in a small filter with a small number of stages, the direct coupling of electromagnetic field energy between the input and output terminals is suppressed, and the deterioration of the filter's out-of-band attenuation characteristics is prevented. As a result, a filter with good out-of-band attenuation characteristics can be realized. Non-metalized part 20
.. The width of the non-metallized portion 20.21 may be very narrow, for example, if the width of the protrusion 11 is 11 m and the diameter of the through hole 12.13 is 3 mm, the width of the non-metallized portion 20.21 is It may be made to have an outer diameter of about 1 m and an outer diameter of about 5 mm.
Furthermore, this width may be formed to be approximately 0.11111%. However, as this width becomes very narrow, the frequency of the pass band tends to change.
There is no problem because it is easy to obtain a predetermined passband by adjusting the height of the passband. Next, with reference to FIG. 5, the attenuation characteristics of the embodiment will be explained.
第5図は本発明の第1実施例の減衰特性曲線を前出の従
来例(第1図)の減衰特性曲線と対比しく8)
て示した線図である。同図において、縦軸は減衰量(d
B)、横軸は周波数(イ)を示し、破線で示す曲線Eけ
従来例、そして実線で示す曲MFは第1実施例の減衰特
性曲線を示す。図中の曲線Eが示すように、従来のフィ
ルタは、前述したように人出用端子間における電磁界の
直接結合により、共振素子を通過せずに出力用端子に一
定レベルの伝送がすでになされているため、あるレベル
以上の減衰は望め力い。これに対して、曲線Fが示すよ
うに本実施例のフィルタは、との点が改善され、きわめ
て良好な減衰特性を示している。FIG. 5 is a diagram showing the attenuation characteristic curve of the first embodiment of the present invention in contrast to the attenuation characteristic curve of the prior art example (FIG. 1). In the figure, the vertical axis is the attenuation amount (d
B), the horizontal axis shows the frequency (a), the curve E shown by a broken line shows the conventional example, and the curve MF shown by a solid line shows the attenuation characteristic curve of the first embodiment. As shown by curve E in the figure, in the conventional filter, due to the direct coupling of the electromagnetic field between the output terminals as described above, a certain level of transmission has already been made to the output terminal without passing through the resonant element. Therefore, it is difficult to expect attenuation beyond a certain level. On the other hand, as shown by curve F, the filter of this embodiment has been improved in this respect and exhibits extremely good attenuation characteristics.
第3図は本発明の第2実施例を示す図で、(イ)は斜視
図、(ロ)は(イ)図の矢印A方向からみた上面図、&
)は((イ)図の矢印C方向からみた下面図である。同
図において、符号30は誘電体フィルタを示し、他の符
号全ては前出の第1実施例(第2図)と同一部分又は同
一部品を示す。従って、それらの説明は省略する。この
第2実施例は第1実施例と基板的には同様に構成された
ものである。第1実施例と異なる点は、非メタライズ部
分20と21をそれぞれブロック11の上面と下面に交
互に配設した点にある。とのように構成したこの第2実
施例も前述の第1実施例と同様な特性が得られる。FIG. 3 shows a second embodiment of the present invention, in which (A) is a perspective view, (B) is a top view seen from the direction of arrow A in FIG.
) is a bottom view seen from the direction of arrow C in figure (A). In the figure, numeral 30 indicates a dielectric filter, and all other numerals are the same as in the first embodiment (Fig. 2). The parts or the same parts are shown.Therefore, their explanations are omitted.This second embodiment has the same structure as the first embodiment in terms of the board.The only difference from the first embodiment is the following. The metallized portions 20 and 21 are arranged alternately on the upper and lower surfaces of the block 11, respectively.This second embodiment constructed as described above also provides the same characteristics as the first embodiment.
尚、この第2実施例は2段構成のフィルタを例示したが
、例えば、4段構成のフィルタの場合、第1番目と第3
番目の非メタライズ部分をブロック11の上面に、そし
て第2と第4番目の非メタライズ部分を下面に交互に配
設するととも、また、第1と第2番目の非メタライズ部
分を上面に、第3と第4番目の非メタライズ部分を下面
に交互に配設することもできる。さらに、他の多段構成
のフィルタにおいても、非メタライズ部分をプロ。Although this second embodiment illustrated a filter with a two-stage configuration, for example, in the case of a filter with a four-stage configuration, the first and third
The first and fourth non-metallized parts are alternately arranged on the top surface of the block 11 and the second and fourth non-metalized parts on the bottom surface, and the first and second non-metalized parts are arranged on the top surface of the block 11, and the second and fourth non-metalized parts are arranged on the top surface of the block 11 and It is also possible to alternately arrange the third and fourth non-metallized portions on the bottom surface. Furthermore, in other multi-stage configuration filters, the non-metallized parts are also processed.
り11の上下面に交互に配設する組合せは仕置にできる
。A combination of alternately disposed on the upper and lower surfaces of the ribs 11 can be used as a seclusion.
第4図は本発明の第3実施例を示す側面断面図である。FIG. 4 is a side sectional view showing a third embodiment of the present invention.
同図においてi叶符号40は誘電体フィルタを示す。符
号11から23は前出の第1実施例(第2図)と同一部
分又は同一部品を示す。従って、これらの説明は省略す
る。この第3実施例本基本構成は第1実施例と同様であ
る。さて、第4図において、符号24.25はっは何円
筒状金物を示し、とれらはそれぞれ入出力用端子14゜
15と同軸状に配置され、つば部分が外部導体膜19に
固着されている。そしてこの円筒状金物24.25にそ
れぞれ可撓性の金属チューブ26゜27が嵌着され、該
チューブ26.27の内部にはプラスチ、り等の樹脂系
材料が充填され、さらに同軸状に配置され入出力用端子
14.15にそれぞれ接続された導電線28.29が配
設されている。このように、との第3実施例は、入出力
用端子(励振体)14.15がブロック11から露出し
ている部分に電磁界遮蔽手段を設け、とれにより入出力
用端子14.15間の直接的電磁界結合を完全に遮断し
て、さらに一層良好外帯域外減衰特性が得られるように
形成されたフィルタである・
上記各実施例は1/4波長同軸誘電体フィルタの場合に
ついて例示したが、本発明は、勿論lk波長同軸誘電体
フィルタに対しても、上記実施例と同様な要領で適用す
ることができる。In the same figure, the reference numeral 40 indicates a dielectric filter. Reference numerals 11 to 23 indicate the same parts or components as those in the first embodiment (FIG. 2). Therefore, these descriptions will be omitted. The basic configuration of this third embodiment is the same as that of the first embodiment. Now, in FIG. 4, numerals 24 and 25 indicate cylindrical hardware, which are arranged coaxially with the input/output terminals 14 and 15, respectively, and whose flange portions are fixed to the external conductor film 19. There is. Flexible metal tubes 26 and 27 are fitted into the cylindrical metal fittings 24 and 25, respectively, and the tubes 26 and 27 are filled with a resin material such as plastic and resin, and are arranged coaxially. Conductive wires 28 and 29 respectively connected to the input and output terminals 14 and 15 are arranged. As described above, in the third embodiment, an electromagnetic field shielding means is provided in the portion where the input/output terminal (exciter) 14.15 is exposed from the block 11, and the gap between the input/output terminals 14.15 is provided. This filter is formed to completely block direct electromagnetic field coupling and obtain even better out-of-band attenuation characteristics. The above embodiments are exemplified for the case of a 1/4 wavelength coaxial dielectric filter. However, the present invention can of course be applied to the lk wavelength coaxial dielectric filter in the same manner as in the above embodiment.
(11)
また、本発明のフィルタの製造方法の一例として、予め
ブロック11の外面金てと、貫通穴12゜130内面と
を同時にメタライズ(但し、入出力用端子14.15の
取付穴17.18を除く)シて導体膜を形成し、その後
で、貫通穴12 、13周辺部の導体膜を、例えばテー
パーリーマ等で削り取る方法がある。この方法によれば
フィルタの製造工程を簡略化できるという利点がある。(11) As an example of the method for manufacturing the filter of the present invention, the outer surface of the block 11 and the inner surface of the through holes 12 and 130 are simultaneously metalized (however, the mounting holes 17 and 130 of the input/output terminals 14 and 15 are simultaneously metalized). There is a method of forming a conductive film (except for 18) and then scraping off the conductive film around the through holes 12 and 13 using, for example, a taper reamer. This method has the advantage of simplifying the filter manufacturing process.
尚、本発明は上記実施例に限定されるものではなく、例
えば、下記のような変形例を実施することも可能である
。It should be noted that the present invention is not limited to the above-mentioned embodiments, and for example, the following modifications can be implemented.
(イ)非メタライズ部分の外周形状を円形以外の形状、
例えば、角形等の形状に形成してもよい。(a) The outer circumferential shape of the non-metalized part is a shape other than circular,
For example, it may be formed into a rectangular shape or the like.
(ロ)入出力用端子14,15の配設位置を上記実施例
と異カる位置に配設することができる。例えば、第2図
において、端子14.15をブp。(b) The input/output terminals 14 and 15 can be arranged at different positions from those in the above embodiment. For example, in FIG. 2, terminals 14 and 15 are connected to bu p.
り11の上面で対角線状に配置、また該端子14゜15
の一方をブロック11の上面に、そして他方を下面に配
置、さらに該端子14.15をブロック11の側面11
a(又はこれの対向側面)に直(12)
立して配置、さらにまた、該端子14.15の一方を前
記側面11mに、そして他方を側面11mの対向側面に
配置することもできる。The terminals 14 and 15 are arranged diagonally on the upper surface of the terminal 11.
one is placed on the top surface of the block 11 and the other is placed on the bottom surface, and the terminals 14 and 15 are placed on the side surface 11 of the block 11.
a (or the opposite side thereof), and it is also possible to arrange one of the terminals 14.15 on the side surface 11m and the other on the opposite side of the side surface 11m.
(7)発明の効果
以上、詳細に説明したように、本発明の誘電体フィルタ
は、誘電体ブロックの貫通穴(共振用穴)周辺部と入出
力端子周辺部とに非メタライズ部分を設け、他の全ての
表面にメタライズした外部導体膜を設けることにより、
段数の少い小型のフィルタの場合でも、簡易構造で帯域
外減衰特性を向上させ得るといった効果大なるものがあ
る。(7) Effects of the Invention As explained in detail above, the dielectric filter of the present invention provides non-metalized portions around the through holes (resonance holes) of the dielectric block and around the input/output terminals, By providing a metalized external conductor film on all other surfaces,
Even in the case of a small filter with a small number of stages, there is a great effect that the out-of-band attenuation characteristic can be improved with a simple structure.
第1図は従来の誘電体フィルタの斜視図、平面図及び側
面断面図を示す図、第2図は本発明の第1実施例の刺視
図、平面図、側面断面図及び下面図を示すV1第3図は
本発明の第2実施例の斜視図、上面図及び下面図を示す
図、第4図は本発明の第3実施例の側面断面図を示す図
、第5図は前記第1実施例の帯域外減衰特性曲線を従来
例の特性曲線と対比して示した線図である。
エO;・・従来の誘電体フィルタ、20.30.40・
・・本発明に依る誘電体フィルタ、11・・・誘電体ブ
ロック、11L・・・ブロック11の側面、12.13
・・・貫通穴(共振用穴、共振素子) 、121L、1
31L・・・内部導体膜、14.15・・・入出力用端
子(励振体)、16,19・・・外部導体膜、20.2
1゜22.23・・・非メタライズ部分、24.25・
・・つば付置筒状金物、26.27・・・可撓性金属チ
ューブ、28.29・・・導電線。
特許出願人
富士通株式会社
特許出願代理人
弁理士 青 木 朗
弁理士西舘和之
弁理士 内 1)幸 男
弁理士 山 口 昭 之
(15)
第1図
゛°七済思窄叱n
第3図
(ハ)FIG. 1 is a perspective view, a top view, and a side sectional view of a conventional dielectric filter, and FIG. 2 is a perspective view, a top view, a side sectional view, and a bottom view of a first embodiment of the present invention. V1 FIG. 3 is a perspective view, top view, and bottom view of the second embodiment of the present invention, FIG. 4 is a side sectional view of the third embodiment of the present invention, and FIG. FIG. 3 is a diagram showing an out-of-band attenuation characteristic curve of one embodiment in comparison with a characteristic curve of a conventional example. E;...Conventional dielectric filter, 20.30.40.
...Dielectric filter according to the present invention, 11...Dielectric block, 11L...Side surface of block 11, 12.13
...Through hole (resonance hole, resonance element), 121L, 1
31L...Inner conductor film, 14.15...Input/output terminal (exciter), 16,19...Outer conductor film, 20.2
1゜22.23...Non-metalized part, 24.25.
...Tubular hardware with collar, 26.27...Flexible metal tube, 28.29...Conductive wire. Patent Applicant: Fujitsu Limited Patent Attorney: Akira Aoki, Patent Attorney: Kazuyuki Nishidate, Patent Attorney: 1) Yukio, Patent Attorney: Akira Yamaguchi (15) Figure 1. (c)
Claims (1)
個の貫通穴を所定間隔で形成し、該ブロックの両端部に
入出力端子を設け、前記貫通穴の内、共振素子用貫通穴
のプロ、り表面における両開口のいづれか一方の開口周
辺部と前記入出力用端子の周辺部とを非メタライズ部分
として形成し、これらの非メタライズ部分を除くプロ、
り表面全てと前記共振素子用貫通穴の内面とをメタライ
ズして形成したことを特徴とする誘電体フィルタ。 2、前記共振素子用貫通穴開口周辺部の非メタライズ部
分すべてを、前記誘電体ブロックの前記開口を含む一表
面に配列して形成したことを特徴とする特許請求の範囲
第1項に記載の誘電体フィルタ。 3、前記共振素子用貫通穴開口周辺部の非メタライズ部
分を、前記誘電体ブロックの前記開口を含む一表面と他
表面とに交互に配列して形成したことを特徴とする特許
請求の範囲第1項に記載の誘電体フィルタ。 4、前記人出用端子に電磁界辿蔽手段を設けたことを特
徴とする特許請求の範囲第1項から第3項のいずれかに
記載の誘電体フィルタ。[Claims] 1. A rectangular parallelepiped dielectric block is provided with a plurality of through holes at predetermined intervals along its longitudinal direction, input/output terminals are provided at both ends of the block, and Among them, the part of the through hole for the resonant element, the peripheral part of one of the openings on the surface and the peripheral part of the input/output terminal are formed as non-metallized parts, and these non-metalized parts are excluded,
A dielectric filter characterized in that the entire surface of the filter and the inner surface of the through hole for the resonant element are formed by metallizing. 2. All of the non-metallized portions around the opening of the resonant element through-hole are arranged and formed on one surface of the dielectric block including the opening. Dielectric filter. 3. The non-metalized portions around the opening of the resonant element through-hole are arranged alternately on one surface including the opening and the other surface of the dielectric block. The dielectric filter according to item 1. 4. The dielectric filter according to any one of claims 1 to 3, characterized in that the terminal for attendance is provided with an electromagnetic field tracing means.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP22485182A JPS59126302A (en) | 1982-12-23 | 1982-12-23 | Dielectric filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP22485182A JPS59126302A (en) | 1982-12-23 | 1982-12-23 | Dielectric filter |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS59126302A true JPS59126302A (en) | 1984-07-20 |
JPH043122B2 JPH043122B2 (en) | 1992-01-22 |
Family
ID=16820154
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP22485182A Granted JPS59126302A (en) | 1982-12-23 | 1982-12-23 | Dielectric filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59126302A (en) |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61139002U (en) * | 1985-02-18 | 1986-08-28 | ||
JPS61140606U (en) * | 1985-02-22 | 1986-08-30 | ||
JPS62154801A (en) * | 1985-12-26 | 1987-07-09 | Fuji Elelctrochem Co Ltd | Dielectric filter |
JPS62109502U (en) * | 1985-12-26 | 1987-07-13 | ||
US4742562A (en) * | 1984-09-27 | 1988-05-03 | Motorola, Inc. | Single-block dual-passband ceramic filter useable with a transceiver |
JPS63109601A (en) * | 1986-10-28 | 1988-05-14 | Toshiba Corp | Filter |
JPH07158156A (en) * | 1993-12-06 | 1995-06-20 | Shinko Kozai Kk | Side ditch |
-
1982
- 1982-12-23 JP JP22485182A patent/JPS59126302A/en active Granted
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4742562A (en) * | 1984-09-27 | 1988-05-03 | Motorola, Inc. | Single-block dual-passband ceramic filter useable with a transceiver |
JPS61139002U (en) * | 1985-02-18 | 1986-08-28 | ||
JPS61140606U (en) * | 1985-02-22 | 1986-08-30 | ||
JPS62154801A (en) * | 1985-12-26 | 1987-07-09 | Fuji Elelctrochem Co Ltd | Dielectric filter |
JPS62109502U (en) * | 1985-12-26 | 1987-07-13 | ||
JPH032964Y2 (en) * | 1985-12-26 | 1991-01-25 | ||
JPS63109601A (en) * | 1986-10-28 | 1988-05-14 | Toshiba Corp | Filter |
JPH07158156A (en) * | 1993-12-06 | 1995-06-20 | Shinko Kozai Kk | Side ditch |
Also Published As
Publication number | Publication date |
---|---|
JPH043122B2 (en) | 1992-01-22 |
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