JPH0733441Y2 - High frequency filter - Google Patents
High frequency filterInfo
- Publication number
- JPH0733441Y2 JPH0733441Y2 JP15277386U JP15277386U JPH0733441Y2 JP H0733441 Y2 JPH0733441 Y2 JP H0733441Y2 JP 15277386 U JP15277386 U JP 15277386U JP 15277386 U JP15277386 U JP 15277386U JP H0733441 Y2 JPH0733441 Y2 JP H0733441Y2
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- inner conductor
- dielectric
- input
- frequency filter
- 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 - Lifetime
Links
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
Description
【考案の詳細な説明】 〔産業上の利用分野〕 この考案は比較的高周波帯、特にVHF帯、UHF帯およびマ
イクロ波帯で多く用いられる高周波ろ波器に関するもの
である。[Detailed Description of the Invention] [Industrial field of application] The present invention relates to a high-frequency filter which is often used in a relatively high frequency band, particularly in the VHF band, the UHF band and the microwave band.
第3図は例えば特開昭55-143801号に示された従来の高
周波ろ波器を示す図で、同図(a)は一部欠載した平面
図、同図(b)は縦断正面図である。図において、1,2
は外導体、3は内導体、4は周波数調整ネジ、5は誘電
体、6は入出力ループ、P1,P2は入出力端子である。FIG. 3 is a view showing a conventional high-frequency filter disclosed in, for example, Japanese Patent Laid-Open No. 55-143801, in which FIG. 3 (a) is a partially cutaway plan view and FIG. 3 (b) is a vertical front view. Is. In the figure, 1,2
Is an outer conductor, 3 is an inner conductor, 4 is a frequency adjusting screw, 5 is a dielectric, 6 is an input / output loop, and P 1 and P 2 are input / output terminals.
内導体3は一端が外導体1に接続されて短絡端となり、
他端は開放端となっており、周波数調整ネジ4によって
容量負荷が設けられている。静電容量の効果によって内
導体3の長さは1/4波長以下になっているので、内導体
3は主として磁界結合によって相互に結合している。結
合量は2つの内導体3間の距離によって調整される。
又、入出力ループ6は内導体3に平行して近接配置され
ており、その平行配置された区間の長さが1/4波長以下
であるのでその結合も主として磁界による結合となる。One end of the inner conductor 3 is connected to the outer conductor 1 to form a short-circuited end,
The other end is an open end, and a capacitive load is provided by the frequency adjusting screw 4. Since the length of the inner conductor 3 is not more than 1/4 wavelength due to the effect of electrostatic capacitance, the inner conductors 3 are mainly coupled to each other by magnetic field coupling. The amount of coupling is adjusted by the distance between the two inner conductors 3.
Further, since the input / output loop 6 is arranged in parallel with and close to the inner conductor 3 and the length of the section arranged in parallel is 1/4 wavelength or less, the coupling is mainly magnetic field coupling.
次に動作について説明する。今、内導体3の長さを調整
することによって全ての内導体3が同一周波数f0で共振
するものとすれば、周波数f0では共振状態にある内導体
3は相互に強く結合するとともに入出力ループ6とも強
く結合し、入出力端子P1への入射波は入出力端子P2に導
かれる。しかし、周波数f0以外の周波数では、内導体3
は相互の結合及び入出力ループ6との結合が非常に弱
く、入出力端子P1あるいはP2への入射波はほとんどの電
力が反射される。このように、第3図に示した従来の高
周波ろ波器は帯域通過フィルタとしての機能を有する。Next, the operation will be described. Now, assuming that all the inner conductors 3 resonate at the same frequency f 0 by adjusting the length of the inner conductors 3, the inner conductors 3 that are in a resonance state at the frequency f 0 are strongly coupled to each other and enter. It is also strongly coupled to the output loop 6, and the incident wave to the input / output terminal P 1 is guided to the input / output terminal P 2 . However, at frequencies other than the frequency f 0 , the inner conductor 3
Are very weakly coupled to each other and to the input / output loop 6, and most of the electric power of the incident wave to the input / output terminal P 1 or P 2 is reflected. As described above, the conventional high frequency filter shown in FIG. 3 has a function as a band pass filter.
従来の高周波ろ波器は、以上のように構成されているの
で誘電体5として比誘電率の大きい誘電体を用い、周波
数調整ネジ4による容量負荷を設けることによって小形
化をはかっても、機械的に安定した構造とし、周波数調
整ネジを取りつけるためには外導体1,2に所定の肉厚が
必要であり、小形化するにはおのずと限度があり、ま
た、外導体1,2、内導体3、周波数調整ネジ4、誘電体
5等の個別の部品を組み立てて製造するものであるた
め、部品数が多く製造組立作業が煩雑になるという問題
点があった。Since the conventional high-frequency wave filter is configured as described above, a dielectric material having a large relative permittivity is used as the dielectric material 5 and a capacitive load is provided by the frequency adjusting screw 4 to reduce the size of the machine. The outer conductors 1 and 2 must have a certain thickness to mount the frequency adjustment screw, and there is a limit to the miniaturization. Since the individual components such as 3, the frequency adjusting screw 4, the dielectric 5 and the like are assembled and manufactured, there is a problem that the number of parts is large and the manufacturing and assembling work is complicated.
この考案は上記のような問題点を解消するためになされ
たもので、小形でかつ部品数が少なく、製造の容易な高
周波ろ波器を得ることを目的とする。The present invention has been made in order to solve the above problems, and an object thereof is to obtain a high-frequency filter which is small in size, has a small number of parts, and is easy to manufacture.
この考案に係る高周波ろ波器は、外導体を誘電体ブロッ
ク表面に密着した導体膜で形成し、内導体を誘電体ブロ
ックに所定間隔であけられた貫通孔の内周面に密着し、
一端で前記外導体に継目なく接続された導体膜で形成す
るとともに、前記内導体中にらせん状導線を挿入して筒
状誘電体で支持し、このらせん状導線の一端を前記内導
体の開放端側で前記外導体に接続したものである。The high frequency filter according to the present invention comprises an outer conductor formed of a conductive film adhered to the surface of a dielectric block, and an inner conductor adhered to the inner peripheral surface of through holes formed at predetermined intervals in the dielectric block,
It is formed of a conductor film that is seamlessly connected to the outer conductor at one end, and a spiral conductor is inserted into the inner conductor and supported by a tubular dielectric, and one end of the spiral conductor is opened to the inner conductor. It is connected to the outer conductor at the end side.
この考案における高周波ろ波器は、誘電体ブロックに比
誘電率の大きい誘電体を用いて波長を短縮し、内導体に
挿入されて筒状誘電体で支持されたらせん状導線で容量
負荷を設けて内導体の軸長を短縮するとともに、外導体
と内導体を誘電体ブロックに密着した導体膜で形成する
ことによって小形化をはかり、部品数を削減して製造組
立を容易化する。The high-frequency wave filter according to the present invention uses a dielectric block having a large relative permittivity to shorten the wavelength, and a capacitive load is provided by a spiral conductor wire inserted into an inner conductor and supported by a cylindrical dielectric body. In addition to shortening the axial length of the inner conductor, the outer conductor and the inner conductor are formed of a conductive film that is in close contact with the dielectric block to achieve miniaturization, reduce the number of parts, and facilitate manufacturing and assembly.
以下、この考案の一実施例を図について説明する。第1
図はこの考案の一実施例による高周波ろ波器の概略構成
を示すもので、同図(a)は斜視図、同図(b)はその
A−A線断面図である。図において、1は外導体、3は
内導体、5は誘電体ブロック、6a,6bは入出力内導体、
7は貫通孔、8はらせん状導線、9は筒状誘電体、10は
誘電体棒である。An embodiment of the present invention will be described below with reference to the drawings. First
FIG. 1 shows a schematic structure of a high frequency filter according to an embodiment of the present invention. FIG. 1A is a perspective view and FIG. 1B is a sectional view taken along the line AA. In the figure, 1 is an outer conductor, 3 is an inner conductor, 5 is a dielectric block, 6a and 6b are input / output inner conductors,
Reference numeral 7 is a through hole, 8 is a spiral conductive wire, 9 is a cylindrical dielectric, and 10 is a dielectric rod.
外導体1は誘電体ブロック5の表面に密着して配置され
た導体膜によって形成されており、内導体3は、誘電体
ブロック5の一側面に所定間隔ずつ離して設けた複数個
の貫通孔7の内周面に密着して配置された導体膜によっ
て形成され、一端が前記外導体1と継目なく接続されて
短絡端となり、他端は開放端となっている。また、各内
導体3の中には、その開放端側より誘電体棒10に巻かれ
たらせん状導線8が挿入され、筒状誘電体9によって支
持されている。このらせん状導線8は、内導体3の開放
端側より導出された端部が外導体1に接続されている。The outer conductor 1 is formed of a conductor film which is arranged in close contact with the surface of the dielectric block 5, and the inner conductor 3 is formed with a plurality of through holes provided on one side surface of the dielectric block 5 at predetermined intervals. It is formed of a conductor film closely attached to the inner peripheral surface of 7, and has one end seamlessly connected to the outer conductor 1 to form a short-circuited end and the other end to an open end. A spiral conductor 8 wound around a dielectric rod 10 is inserted into each inner conductor 3 from its open end side, and is supported by a cylindrical dielectric 9. The spiral conductor 8 is connected to the outer conductor 1 at the end portion which is led out from the open end side of the inner conductor 3.
入出力内導体6a,6bは導体膜で形成されて外導体とは絶
縁されており、それぞれ両端の内導体3に接続され、当
該内導体3に流れる電流の一部を分流する形式の入出力
結合回路を形成している。The input / output inner conductors 6a, 6b are formed of a conductor film and are insulated from the outer conductor, are connected to the inner conductors 3 at both ends, respectively, and divide a part of the current flowing through the inner conductor 3 into the input / output. It forms a coupling circuit.
次に動作について説明する。第1図(b)の断面図で表
わされる共振器の等価回路は第2図のようになる。第2
図において、外導体1、内導体3の外周面、らせん状導
線8、内導体3の内周面は、それぞれ線路11、線路12、
線路13、線路14で表わされる。Next, the operation will be described. The equivalent circuit of the resonator shown in the sectional view of FIG. 1 (b) is as shown in FIG. Second
In the figure, the outer conductor 1, the outer peripheral surface of the inner conductor 3, the spiral conductor 8, the inner peripheral surface of the inner conductor 3, the line 11, the line 12, respectively.
It is represented by lines 13 and 14.
内導体3の開放端から見たらせん状導線8は、先端開放
のスタッブとなり、入力アドミッタンスYiは次式で表さ
れる。The spiral conductor 8 viewed from the open end of the inner conductor 3 is a stub with an open tip, and the input admittance Y i is expressed by the following equation.
Yi=j Y02tanθ (1) ここで、Y02はらせん状導線部の特性アドミッタンス、
θは電気長である。Y i = j Y 02 tan θ (1) where Y 02 is the characteristic admittance of the spiral conductor,
θ is an electrical length.
入力アドミッタンスYiは、電気長θがπ/2以下のとき容
量性サセプタンスとなり、θがπ/2に近づくほど大きな
値となる。従って、らせん状導線を用いた場合には、短
かい区間で長い線路を実現することができるので、θを
大きくして大きな静電容量を容量に得ることができ、共
振条件を満足するための内導体3の軸長を短縮すること
ができる。The input admittance Y i becomes a capacitive susceptance when the electrical length θ is π / 2 or less, and becomes larger as θ approaches π / 2. Therefore, when a spiral conductor is used, a long line can be realized in a short section, so that θ can be increased and a large capacitance can be obtained in the capacitance, so that the resonance condition is satisfied. The axial length of the inner conductor 3 can be shortened.
第1図(a)の高周波ろ波器において、内導体3の軸長
は上述のように1/4波長より短かくなつているので、主
として磁界によって相互に結合している。In the high-frequency wave filter of FIG. 1 (a), the axial length of the inner conductor 3 is shorter than 1/4 wavelength as described above, so that they are mutually coupled mainly by the magnetic field.
今、らせん状導線8の挿入長を調整することによってす
べての内導体が同一周波数f0で共振するものとすれば、
周波数f0では共振状態にある内導体3は相互に強く結合
するとともに入出力内導体6a,6bとも強く結合し、入出
力内導体6aに接続される入出力端子への入射波は入出力
内導体6bに接続される入出力端子に導かれる。しかし、
周波数f0以外の周波数では内導体3は相互の結合及び入
出力内導体6a,6bとの結合が非常に弱く、入出力内導体6
a,6bに接続される入出力端子への入射波はほとんどの電
力が反射される。このように、この実施例の高周波ろ波
器は帯域通過フィルタとしての機能を有する。Now, assuming that all the inner conductors resonate at the same frequency f 0 by adjusting the insertion length of the spiral conductor wire 8,
At the frequency f 0 , the inner conductors 3 in the resonance state are strongly coupled to each other and also strongly coupled to the input / output inner conductors 6a and 6b, so that the incident wave to the input / output terminal connected to the input / output inner conductor 6a is It is led to an input / output terminal connected to the conductor 6b. But,
At frequencies other than the frequency f 0 , the inner conductors 3 are very weakly coupled to each other and the input / output inner conductors 6a and 6b.
Almost all the power of the incident wave to the input / output terminals connected to a and 6b is reflected. Thus, the high frequency filter of this embodiment has a function as a band pass filter.
なお、上記実施例では、内導体の数が3本の場合につい
て述べたが、内導体の数が2本の場合および4本以上の
場合にも適用することができる。また、入出力結合回路
として内導体に流れる電流を一部分流する場合について
述べたが、磁界あるいは静電容量による結合を用いても
よく、上記実施例と同等の効果を奏する。In addition, in the said Example, although the case where the number of inner conductors was three was described, it is applicable also when the number of inner conductors is two, and when it is four or more. Further, the case where a part of the current flowing through the inner conductor is used as the input / output coupling circuit has been described, but coupling by a magnetic field or electrostatic capacitance may be used, and an effect equivalent to that of the above-described embodiment is obtained.
以上のように、この考案によれば、外導体及び内導体を
誘電体ブロックの表面あるいは貫通孔の内周面に密着し
た導体膜で形成し、内導体内に筒状誘電体で支持された
らせん状導線を挿入して、その一端を内導体の開放端側
で外導体に接続する構成としたので、外導体、内導体が
極めて薄形化され、比誘電率の大きな誘電体ブロックに
よって波長が短縮される一方でらせん状導線によって大
きな容量負荷が実現されて内導体の軸長が短縮されるた
め大幅な小形化が可能となるばかりか、らせん状導線が
内導体中に設けた筒状誘電体で支持されていて外部に支
持機構が不要であり、外導体、内導体が誘電体ブロック
に密着した導体膜であるため、部品数も少なく、製造組
立の容易な高周波ろ波器が得られる効果がある。As described above, according to the present invention, the outer conductor and the inner conductor are formed by the conductor film adhered to the surface of the dielectric block or the inner peripheral surface of the through hole, and the inner conductor is supported by the cylindrical dielectric. Since the conductor is inserted and one end of the conductor is connected to the outer conductor at the open end side of the inner conductor, the outer conductor and inner conductor are extremely thin, and the dielectric block with a large relative dielectric constant While the spiral lead wire realizes a large capacitive load and the axial length of the inner conductor is shortened, the size can be greatly reduced, and the spiral lead wire is provided inside the inner conductor. Since it is supported by a dielectric and no external support mechanism is required, and the outer and inner conductors are conductor films that are in close contact with the dielectric block, the number of parts is small and a high-frequency filter that is easy to manufacture and assemble can be obtained. It is effective.
第1図(a)はこの考案の一実施例による高周波ろ波器
の概略構成を示す斜視図、第1図(b)は第1図(a)
のA−A線断面図、第2図はその動作を説明するための
等価回路図、第3図(a)は従来の高周波ろ波器の概略
構成を示す一部切載平面図、第3図(b)は第3図
(a)の縦断正面図である。 1は外導体、3は内導体、5は誘電体ブロック、7は貫
通孔、8はらせん状導線、9は筒状誘電体、10は誘電体
棒。 なお、図中、同一符号は同一、又は相当部分を示す。FIG. 1 (a) is a perspective view showing a schematic configuration of a high frequency filter according to an embodiment of the present invention, and FIG. 1 (b) is FIG. 1 (a).
2 is a sectional view taken along the line AA of FIG. 2, FIG. 2 is an equivalent circuit diagram for explaining the operation, and FIG. 3 (a) is a partially cutaway plan view showing a schematic configuration of a conventional high-frequency filter. FIG. 3B is a vertical sectional front view of FIG. 1 is an outer conductor, 3 is an inner conductor, 5 is a dielectric block, 7 is a through hole, 8 is a spiral conductor, 9 is a cylindrical dielectric, and 10 is a dielectric rod. In the drawings, the same reference numerals indicate the same or corresponding parts.
フロントページの続き (72)考案者 武田 文雄 神奈川県鎌倉市大船5丁目1番1号 三菱 電機株式会社情報電子研究所内 (56)参考文献 特開 昭60−254802(JP,A) 実開 昭57−11802(JP,U) 実開 昭61−50302(JP,U)Front page continuation (72) Creator Fumio Takeda 5-1-1, Ofuna, Kamakura-shi, Kanagawa Mitsubishi Electric Corporation Information & Electronics Laboratory (56) Reference JP-A-60-254802 (JP, A) -11802 (JP, U) Actually open Sho 61-50302 (JP, U)
Claims (1)
定の間隔で複数個あけられた誘電体ブロックと、前記各
貫通孔の内周面に密着して配された導体膜で形成される
内導体と、前記誘電体ブロックの表面に密着して配され
た導体膜で形成され、前記各内導体の一方の端部が継目
なく接続されている外導体と、前記内導体中に挿入され
て筒状誘電体で支持され、前記内導体の開放端より導出
された端部が前記外導体に接続されたらせん状導線とを
備えた高周波ろ波器。1. A dielectric block having a plurality of through holes penetrating from one side surface to a back surface thereof at a predetermined interval, and a conductor film closely attached to an inner peripheral surface of each of the through holes. An inner conductor, and an outer conductor formed by a conductor film closely attached to the surface of the dielectric block, one end of each inner conductor being seamlessly connected, and inserted into the inner conductor. A high-frequency filter provided with a spiral conductor wire which is supported by a cylindrical dielectric and whose end portion led out from the open end of the inner conductor is connected to the outer conductor.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15277386U JPH0733441Y2 (en) | 1986-10-02 | 1986-10-02 | High frequency filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15277386U JPH0733441Y2 (en) | 1986-10-02 | 1986-10-02 | High frequency filter |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6359403U JPS6359403U (en) | 1988-04-20 |
JPH0733441Y2 true JPH0733441Y2 (en) | 1995-07-31 |
Family
ID=31071054
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP15277386U Expired - Lifetime JPH0733441Y2 (en) | 1986-10-02 | 1986-10-02 | High frequency filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0733441Y2 (en) |
-
1986
- 1986-10-02 JP JP15277386U patent/JPH0733441Y2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPS6359403U (en) | 1988-04-20 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
EP0005525B1 (en) | High frequency wave guide filter | |
JPH0230883Y2 (en) | ||
US4996506A (en) | Band elimination filter and dielectric resonator therefor | |
JPH0697721B2 (en) | Ceramic filter | |
US4276525A (en) | Coaxial resonator with projecting terminal portion and electrical filter employing a coaxial resonator of that type | |
JPS61161806A (en) | High frequency filter | |
JPS638641B2 (en) | ||
JPH0255402A (en) | Dielectric filter | |
JP2630387B2 (en) | Dielectric filter | |
JPH0733441Y2 (en) | High frequency filter | |
JPH0671165B2 (en) | Dielectric filter | |
JP2511907Y2 (en) | High frequency filter | |
JPH0546322Y2 (en) | ||
JPS633220Y2 (en) | ||
JPS5881302A (en) | Coaxial resonance circuit | |
JPS6110323Y2 (en) | ||
JPH0526802Y2 (en) | ||
JPS59161B2 (en) | Filter using coaxial resonator | |
JPS6390202A (en) | High-frequency filter | |
JPH0633684Y2 (en) | Dielectric filter | |
JPS6055702A (en) | High frequency filter | |
JPS6336722Y2 (en) | ||
JPH0323001B2 (en) | ||
JPH0624283B2 (en) | Dielectric filter | |
JPH032966Y2 (en) |