JPS59139701A - Comb-line type band-pass filter - Google Patents

Comb-line type band-pass filter

Info

Publication number
JPS59139701A
JPS59139701A JP58013360A JP1336083A JPS59139701A JP S59139701 A JPS59139701 A JP S59139701A JP 58013360 A JP58013360 A JP 58013360A JP 1336083 A JP1336083 A JP 1336083A JP S59139701 A JPS59139701 A JP S59139701A
Authority
JP
Japan
Prior art keywords
resonant
shaped
elements
housing
input
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
Application number
JP58013360A
Other languages
Japanese (ja)
Inventor
Hiroshi Hatanaka
博 畠中
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NIPPON DENGIYOU KOSAKU KK
Nihon Dengyo Kosaku Co Ltd
Original Assignee
NIPPON DENGIYOU KOSAKU KK
Nihon Dengyo Kosaku Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by NIPPON DENGIYOU KOSAKU KK, Nihon Dengyo Kosaku Co Ltd filed Critical NIPPON DENGIYOU KOSAKU KK
Priority to JP58013360A priority Critical patent/JPS59139701A/en
Publication of JPS59139701A publication Critical patent/JPS59139701A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/20Frequency-selective devices, e.g. filters
    • H01P1/201Filters for transverse electromagnetic waves
    • H01P1/205Comb or interdigital filters; Cascaded coaxial cavities

Abstract

PURPOSE:To attain an overall compact structure with simple control for a comb- line type band-pass filter by giving cuts to the wall of a housing and bending these cuts into the housing to control the resonance frequency. CONSTITUTION:A comb-line type band-pass filter contains a housing 1, dielectric materials 21-2n, resonance elements 31-3n, input/output coupling elements 40.1-4n.(n+1), input/output terminals 50.1-5n.(n+1), etc. In addition, resonance frequency fine adjustment elements 101-10n are provided to the band-pass filter by forming U-shaped similar cuts to the upper wall parts of the housing 1. Then the tongue-shaped areas of those cuts are bent downward to vary the mean distance between the elements 101-10n and 31-3n. In such a way, the fine adjustment is possible for the resonance frequency. Thus, the overall structure of a comb-line type band-pass filter with simple control is miniaturized.

Description

【発明の詳細な説明】 本発明は、超短波ないしマイクロ波用コムライン型帯域
通過ろ波器に関するものである。以下、帯域通過ろ波器
をBPFと略記する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a combline type bandpass filter for very high frequency waves or microwaves. Hereinafter, the bandpass filter will be abbreviated as BPF.

第1図は、本発明者がさきに提案しブこコムライン型B
PFの一例を示す断面図(第2図のB−8断面図)、第
2図は、第1図のA−A断面図で、両図において、1は
導体より成る筐体% 2tないし271(nはBPFの
次数)は誘電体で、例えばチタン酸バリウム磁器又はチ
タン酸マグネシウム磁器等より成る。31ないし3nは
共振素子で、各軸長を電気長で共振波長のほぼ14に形
成した棒状導体又は筒状導体より成り、誘電体2Iない
し2−ILに穿った挿入孔内に嵌入しである。尚、内部
導体3Iないし37Lを棒状導体を以て形成する代りに
誘電体21ないし2711m穿った挿入孔の内周面に銀
又は銅等の金属被膜を@着等の手段により付着せしめで
゛形成することも可能である。4o、r及び4n、(ユ
オリは入出力結合素子で、例えばコンデンサより成る。
Figure 1 shows the Bukocom line type B that the inventor proposed earlier.
A cross-sectional view showing an example of a PF (B-8 cross-sectional view in Figure 2), Figure 2 is a cross-sectional view along A-A in Figure 1, and in both figures, 1 is a casing made of a conductor. (n is the order of BPF) is a dielectric material made of, for example, barium titanate porcelain or magnesium titanate porcelain. 31 to 3n are resonant elements, which are made of rod-shaped or cylindrical conductors whose respective axial lengths are approximately 14 times the resonant wavelength in terms of electrical length, and are fitted into insertion holes drilled in the dielectrics 2I to 2-IL. . Incidentally, instead of forming the internal conductors 3I to 37L using rod-shaped conductors, a metal coating such as silver or copper may be attached to the inner circumferential surface of the insertion hole drilled in the dielectrics 21 to 2711m by means such as @ deposition. is also possible. 4o, r, and 4n (Yori are input/output coupling elements, such as capacitors.

501.及び5n、(□71.は入出力端子% 61な
いし面は共振周波数微細調整素子で、共振素子31ない
し3nの開放端と対向して静電容量を形成する電極板及
びこの電極板と共振素子の開放端との間隔を良化せしめ
る調整ねじより成る。71ないし7n−/は段間結合調
整素子で、例えば容量性ねじより成る。8Iないし8n
は止めねじで、共振素子31ないし3□を所要位置に固
定する。共振素子31ないし3rLが筒状導体又は金属
被膜より成る場合には、止めねじ81ないし8ルによつ
で誘電体21ないし2nを固定するように形成しである
。9.ないし971M−1は誘電体間の2空隙である。
501. and 5n, (□71. is an input/output terminal %) 61 or the surface is a resonant frequency fine adjustment element, an electrode plate that faces the open end of the resonant elements 31 to 3n and forms a capacitance, and this electrode plate and the resonant element 71 to 7n-/ are interstage coupling adjustment elements, for example, capacitive screws. 8I to 8n
is a set screw to fix the resonant elements 31 to 3□ in a required position. When the resonant elements 31 to 3rL are made of a cylindrical conductor or a metal film, the dielectrics 21 to 2n are fixed by set screws 81 to 8L. 9. 971M-1 are two gaps between the dielectrics.

このBPF’においては共振素子3Iに共振電流が、′
M。
In this BPF', a resonant current flows through the resonant element 3I, '
M.

れると、第3図及び第4図に電界E及び磁界Hの各分布
を示すようなTFfVMモード波が共振素子31と筐体
1間に生ずる。このとき共振素子3Iには第15図に点
線を以て電圧分布を、1点鎖線を以て電流分布を示すよ
うな定在波が発生し、共振素子3Iがアンテナと同様に
作用してTEMモード波の磁界成分により共振素子3I
と3Q間の筐体1によって形成ぼれるカットオフ導波管
部を励振してHl−モード波を生せしめ、次設の共振素
子3aを励振する。尚、第5図においてiは共振電流、
iHは811モード波の電界、H)lはH1+モード波
の磁界で、このH++モード波の電磁界によって共振素
子31と32開の結合が行われることとなる。共振素子
3コ以下においても前記と同様にして信号の伝送が行わ
れる。
Then, a TFfVM mode wave is generated between the resonant element 31 and the housing 1, as shown in FIGS. 3 and 4, the distributions of the electric field E and the magnetic field H. At this time, a standing wave is generated in the resonant element 3I, as shown in FIG. 15, where the voltage distribution is shown by the dotted line and the current distribution is shown by the dashed-dotted line. Resonant element 3I depending on the component
The cut-off waveguide section formed by the housing 1 between and 3Q is excited to generate an Hl-mode wave, and the subsequent resonant element 3a is excited. In addition, in Fig. 5, i is the resonant current,
iH is the electric field of the 811 mode wave, H)l is the magnetic field of the H1+ mode wave, and the electromagnetic field of the H++ mode wave causes the resonant elements 31 and 32 to be coupled. Signal transmission is performed in the same manner as described above for three or less resonant elements.

各共振素子間における磁気結合損失(リアクタンス損失
)を表わす実験式、即5ち、共振素子の近くにおける電
磁界の乱れの影響を補償した実験式上記各式においで、 bcに、(K+Q  ;各共振素子間における磁気結合
損失k  =1. 2.    ・−・・・・nCd 
   C(I Cd = −十− 2 Cd −8共振素子の中心軸と誘電体の結合面との間隔(第2
図) Cjay、(に剰):空隙91ないし9nイ の各長さ
W:筐体1の横幅(第2図) ε:誘電体21ないし27の誘電早 入:伝送信号の自由空間波長で、周波数f (GHz)
との間に っである。
An experimental formula expressing the magnetic coupling loss (reactance loss) between each resonant element, that is, an experimental formula that compensates for the influence of disturbance of the electromagnetic field near the resonant element.In each of the above formulas, bc is (K+Q; Magnetic coupling loss between resonant elements k = 1. 2. ... nCd
C(I Cd = -10-2 Cd -8 Distance between the center axis of the resonant element and the coupling surface of the dielectric (second
(Fig.) Cjay, (remainder): Each length of the air gap 91 to 9n, W: Width of the housing 1 (Fig. 2) ε: Dielectric early entry of the dielectrics 21 to 27: Free space wavelength of the transmission signal, Frequency f (GHz)
It is between.

(1)式の右辺第1項は誘電体部分に対応する筐体Iに
より形成されるカットオフ導波管部における損失量であ
り、第2項は誘電体間における空隙部分に対応する筐体
1により形成される力・/トオフ4波管部における損失
量である。
The first term on the right side of equation (1) is the amount of loss in the cutoff waveguide section formed by the housing I corresponding to the dielectric part, and the second term is the loss amount in the cutoff waveguide section formed by the housing I corresponding to the dielectric part. 1 is the amount of loss in the four-wave tube section.

誘電体間に空隙を設けることなく、共振素子間に誘電体
を一様に介在せしめた場合には共振素子の各中心間隔を
09に、(K÷I)とすると各共振素子間における磁気
結合損失Lcに、鴎やりの実験式は、で表わされる。
If the dielectric is uniformly interposed between the resonant elements without creating a gap between the dielectrics, and the center spacing of the resonant elements is 09, and (K÷I), the magnetic coupling between the resonant elements is The loss Lc is expressed by Kamoyari's empirical formula.

誘電体間に空隙を設けた場合にも空隙を設けていない場
合にも等価口路は第6図で示され、各段間の磁界結合係
数Ml、a 、M、、、  ・・・・・・M(n−1)
、W  を一般的にMK、(X++)とすると、各峻開
の磁界結合係数MK、(K刊)は1 で表ねされる。
The equivalent path is shown in Fig. 6 both with and without a gap between the dielectrics, and the magnetic field coupling coefficient between each stage is Ml,a,M,...・M(n-1)
, W is generally MK, (X++), then the magnetic field coupling coefficient MK, (K publication) of each sharp divergence is expressed as 1.

このBPFにおける伝達モードは前記のようにH1+モ
ード波であるから第7図(第1図におけるC−C部分の
切断部端面図)に示すように、筐体1の上壁から設問結
合調整素子71を811モード波の電界幅方向に挿入す
ることにより導波管BPFの場合と同様、素子71に電
界を集中せしめて電気力線を密ならしめ、その結果磁束
(HH) を密ならしめて股間結合度を大ならしめ得る
。したがって素子71の筐体1内への挿入長を変えるこ
とにより、挿入長が零の場合に比して結合度が高くなる
方向において結合度の調整が可能である。
Since the transmission mode in this BPF is the H1+ mode wave as described above, as shown in FIG. By inserting 71 in the electric field width direction of the 811 mode wave, the electric field is concentrated on the element 71 and the lines of electric force are made dense, as in the case of the waveguide BPF, and as a result, the magnetic flux (HH) is made dense and the groin The degree of coupling can be increased. Therefore, by changing the insertion length of the element 71 into the housing 1, it is possible to adjust the degree of coupling in a direction in which the degree of coupling becomes higher than when the insertion length is zero.

この段間結合調整素子は筐体外からの操作によって素子
の筐体内への挿入長を変化せしめて股間結合度を自在に
調整し得る利点を有する反面、素子の外端部が筐体外に
突出しているため、それだけ全体の形状を複雑大型なら
しめることとなり、誘電体共振器を用いて全体を小型し
ようとする目的を阻害することとなる。このことは共振
周波数微細調整素子6Iないし6rLにおいても同様で
、各素子の外端部が筐体1外に突出しているため全体の
小型化を阻害する欠点がある。
This interstage coupling adjustment element has the advantage that the insertion length of the element into the housing can be changed by operating from outside the housing, and the degree of joint coupling between the legs can be freely adjusted. However, the outer end of the element protrudes outside the housing. Therefore, the overall shape becomes complicated and large, which obstructs the purpose of using dielectric resonators to reduce the overall size. This also applies to the resonant frequency fine adjustment elements 6I to 6rL, and since the outer ends of each element protrude outside the housing 1, there is a drawback that it impedes overall miniaturization.

本発明は、極めて簡単な構造で、筐体外への突出部分が
なく、筐体外からの操作によって共振周波数の微細調整
及び段間結合調整を行い得る調整素子を備えることによ
り全体を小型に構成し得る超短波ないしマイクロ波用コ
ムライン型BPFを実現することを目的とする。
The present invention has an extremely simple structure, has no protruding parts outside the casing, and has an adjustment element that can perform fine adjustment of the resonance frequency and interstage coupling adjustment by operating from outside the casing, making the entire structure compact. The purpose of this invention is to realize a combline type BPF for very short waves or microwaves.

第8図は、本発明の一実施例を示す断面図(第9図のB
−B断面図)、第9図は、第8図のA−A断面図で、両
図において、1は筐体、2.ないし2nは誘電体、3I
ないし3nは共振素子、4o、、及び4n、(n+υは
入出力結合素子% 5o、+及び571.(no+>は
入出力端子、8sないし、8ルは止めねじ、9tないし
9n−1は空隙で、これらは第1図及び第2図に示した
ものと同様である。10.ないし+Onは本発明σン要
旨たる共振周波数微細調整素子で、第10図2こ筐体1
の上壁の平面図を示すように、共振素子3tなし\し3
nの令 各開放端に対向する筐体lの上壁町こ設(すた1]字型
又はコの字型類似の切込みより成り、この切込みの舌状
部分を下方に(筐体内に−)屈曲せしめて素子+01な
いし10nと共振素子31ないし抛の各開放端との平均
間隔を変化せしめることにより、素子10Iないし+O
nと共振素子3Iないし3nの各開放端との間に形成さ
れる静電容量を変化せしめて共振周波数を微細に調整す
ることが出来る。111ないしIl、n−、ちまた本発
明の要旨たる段間結合調整素子で、共振素子31ないし
3.tの各開放端と対向する筐体1の土壁の中、共振素
子と共振素子との開(理想的にはFA接対向する共振素
子間隔の中心に対応する個所)に設けたU字型又はコの
字型類似の切込みより成り、こ・の切込みの舌状部分を
r方に(筐体内に)屈曲せしめてその屈曲角を変化せし
めることにより、筐体内への挿入長を変化せしめて従来
の容量性ねしより成る股間結合調整素子の場合と同様、
股間結合度を変化せしめることが出来る。
FIG. 8 is a sectional view (B in FIG. 9) showing one embodiment of the present invention.
9 is a sectional view taken along line A-A in FIG. 8, and in both figures, 1 is the housing, 2. or 2n is a dielectric, 3I
thru 3n are resonance elements, 4o, and 4n, (n+υ are input/output coupling elements %, 5o, + and 571.(no+> are input/output terminals, 8s and 8 are set screws, 9t and 9n-1 are air gaps. These are the same as those shown in Figs. 1 and 2. 10. to +On are resonant frequency fine adjustment elements which are the gist of the present invention.
As shown in the plan view of the upper wall of
The top wall of the casing l facing each open end of n consists of a notch shaped like a square or a U-shape, and the tongue-shaped part of this notch is placed downward (within the casing). ) By bending and changing the average distance between the elements +01 to +10n and the open ends of the resonant elements 31 to 31, the elements 10I to +O are bent.
The resonance frequency can be finely adjusted by changing the capacitance formed between n and each open end of the resonance elements 3I to 3n. 111 to Il, n-, which is also the gist of the present invention, is the interstage coupling adjustment element, and the resonant elements 31 to 3. In the earthen wall of the casing 1 facing each open end of t, a U-shape is provided between the resonant elements (ideally at a location corresponding to the center of the interval between the resonant elements facing each other in FA contact). Alternatively, it consists of a cut similar to a U-shape, and the length of insertion into the case is changed by bending the tongue-shaped part of this cut in the r direction (into the housing) and changing the bending angle. As in the case of the crotch joint adjustment element made of conventional capacitive screws,
It is possible to change the degree of groin connection.

尚、第10図には共振周波数微細調整素子10Iないし
IOF+及び股間結合調整素子111ないしlI?L−
1を形成する切込みの切込み方向を筐体1の長手方向に
一致せしめた場合を例示したが、筐体1の長手方向に対
して切込み方向を直角方向又は斜方向等任意の方向に選
んで本発明を実施することが出来る。
Incidentally, FIG. 10 shows resonant frequency fine adjustment elements 10I to IOF+ and crotch coupling adjustment elements 111 to 1I? L-
In this example, the cutting direction of the notch forming the casing 1 is made to coincide with the longitudinal direction of the casing 1. Able to carry out inventions.

本発明においても設問結合調整素子11.ないしIIy
L−、の゛筐体1内への挿入長が大となるにしたがって
設問結合が密となるから、BPFの設計に際して股間結
合度が所要値よりも低くなるように共振素子の間隔を定
め、組立に際して股間結合調整索−子11+ないし目に
−1の筐体内への屈曲角度を適当ならしめることにより
段間結合度を所要値に正確に一致せしめることが出来る
Also in the present invention, the question coupling adjustment element 11. Or IIy
As the insertion length of L- into the housing 1 increases, the coupling becomes denser, so when designing the BPF, determine the spacing between the resonant elements so that the degree of coupling between the legs is lower than the required value. During assembly, by appropriately bending the groin connection adjustment cables 11+ to 11-1 into the housing, the degree of interstage connection can be made to accurately match the required value.

設計に際して股間結合度が所要値よりも低くなるように
共振素子の間隔を定める代りに、共振素子の間隔を所要
値よりも小ならしめ、第11図Cご要部断面図(第12
図のB−8断面図)を、第12図に第11図のA−A断
面図を示すように、各誘電体2.ないし2□の結合面1
こ、共振素子と同方向の結合窓を形成する金属被膜12
11及びI 21J (12rt又は12ノコの何れか
一方のみでもよい)ないし12tn−0,r及び12t
n−n、、rを付着せしめるか、第13図に要部断面図
(第14図のB−8断面図)を、第14図に第13図の
A−A断面図を示すように、共振素子3.ないし3rL
の各中間部に結合窓を形成する導体板132.及び+3
1コ(+ 3.、又は132.の何れか一方を省いても
よい)ないしl 3<n−z)、を及び13(71−υ
、コを介在せしめて股間結合度を低下せしめ、組立に際
して股間結合調整素子I+、ないし目、−1−の筐体内
への屈曲角度を適当ならしめることにより設問結合度を
所要値に正確に一致せしめるように構成してもよく、金
属被膜又は導体板により形成される結合窓を設ける代り
に共振素子間に導体より成る誘導性結合阻止棒を介在せ
しめでもよく、何れの場合にも共振素子間隔を比較的小
ならしめ得るから全体を小型化することが可能となる。
Instead of determining the spacing between the resonant elements so that the degree of crotch coupling is lower than the required value during design, the spacing between the resonant elements is made smaller than the required value, and
As shown in FIG. 12, which is a sectional view taken along line A-A in FIG. 11, each dielectric 2. or 2□ bonding surface 1
This metal coating 12 forms a coupling window in the same direction as the resonant element.
11 and I 21J (either 12rt or 12 saws may be used) or 12tn-0, r and 12t
As shown in FIG. 13 is a cross-sectional view of the main part (B-8 cross-sectional view in FIG. 14), and FIG. 14 is a cross-sectional view taken along A-A in FIG. 13. Resonant element 3. or 3rL
conductor plates 132 . and +3
1 (either + 3. or 132. may be omitted) or l 3 < n-z), and 13 (71-υ
, and to lower the degree of crotch connection, and by adjusting the bending angle of the groin connection adjustment elements I+, -1-, and -1- into the housing to an appropriate value during assembly, the degree of connection can be accurately matched to the required value. Alternatively, instead of providing a coupling window formed by a metal film or a conductive plate, an inductive coupling blocking rod made of a conductor may be interposed between the resonant elements, and in either case, the resonant element spacing may be can be made relatively small, making it possible to downsize the whole.

尚、本発明BPFの等価回路及び伝送特性は第1図及び
第2図に示したBPFと同様である。
The equivalent circuit and transmission characteristics of the BPF of the present invention are the same as those of the BPF shown in FIGS. 1 and 2.

以上は各共振素子の周りに誘電体を設けて誘電体共振器
を構成することにより全体を小型ならしめた場合を例示
したが、誘電体を省いても本発明を実施し得ること勿論
である。
The above example illustrates a case in which the entire structure is made smaller by providing a dielectric material around each resonant element to form a dielectric resonator, but it is of course possible to implement the present invention even if the dielectric material is omitted. .

以上の説明から明らかなように、本発明BPFにおける
共振周波数微細調整素子io+ないし1o+1及び段間
結合調整素子+1+ないしI覇−Iは何れも筐体壁に設
けたU字型又はコの字型類似の切込みょ9成り、この切
込みを筐体内へ屈曲せしめて共振周波数及び段間結合度
を調整するように構成しであるから筐体外への突出部は
全くなく、それだけ全体の形状を簡潔小型ならしめ得る
と共に、切込みの屈曲角度を筐体外からの掃作によって
自在に変化せしめ得るから調整も極めて容易で、又、各
素子の構造も極めて簡単で量産に好適である等の特長を
有するもので、実用上の効果甚だ大である。
As is clear from the above description, the resonant frequency fine adjustment elements io+ to 1o+1 and the interstage coupling adjustment elements +1+ to Ih-I in the BPF of the present invention are both U-shaped or U-shaped provided on the housing wall. There are 9 similar notches, and this notch is bent into the housing to adjust the resonance frequency and inter-stage coupling, so there is no protrusion outside the housing, making the overall shape simpler and smaller. In addition, the bending angle of the cut can be freely changed by sweeping from outside the casing, making adjustment extremely easy. Also, the structure of each element is extremely simple, making it suitable for mass production. The practical effect is enormous.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図及び第2図は、従来の帯域通過ろ波器を示す断面
図、第3図ないし第5図及び第7図は、その作動説明図
、第6図は、その等価回路図、第8図及び第9図は、本
発明の一実施例を示す断面図、第10図は、その要部構
成の一例を示す平面図、第11図ないし第14図は、他
の実施例の要部を示す断面図で、1:筐体、21ないし
2n:g%誘電体3Iないし3yL:共振素子、4a、
1及び4n、(n+す:入出力結合素子、5a、1及び
5 n、(nヤリ:入出力端子、6Iないし6n及び1
0.ないし10n:共振周波数微細調整素子、71ない
し7ト、及び111ないしlIn−、:段間結合調整素
子、8Iないし8yL=止めねじ、9.ないし9n−t
 :空隙、+ 2/l及び12/コニ結合窓を形成する
金属被膜、+3/l及び13/コニ結合窓を形成する導
体板である。 第1図 第3図   第4図 第5図 第6図 第7図 第8図 第9図  II
1 and 2 are cross-sectional views showing a conventional bandpass filter, FIGS. 3 to 5, and 7 are explanatory diagrams of its operation, and FIG. 6 is its equivalent circuit diagram. 8 and 9 are cross-sectional views showing one embodiment of the present invention, FIG. 10 is a plan view showing an example of the main structure, and FIGS. 11 to 14 are main views of other embodiments. 1: housing, 21 to 2n: g% dielectric 3I to 3yL: resonant element, 4a,
1 and 4n, (n+su: input/output coupling element, 5a, 1 and 5 n, (n spear: input/output terminal, 6I to 6n and 1
0. to 10n: resonant frequency fine adjustment element, 71 to 7t, and 111 to lIn-,: interstage coupling adjustment element, 8I to 8yL = set screw, 9. or 9nt
: air gap, metal coating forming +2/l and 12/coni bond windows, conductor plate forming +3/l and 13/coni bond windows. Figure 1 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 Figure 8 Figure 9 II

Claims (1)

【特許請求の範囲】 (1)電気長で共振波長σ月Jぼ14の軸長を有し、同
一極性を以て複数個配設された棒状又は筒状導体より成
る共振素子と、この複数個の共振素子の各周りに設けた
。J電体と、前記複数個の共振素子の各開放端と対向す
る筐体壁部分lこ設けられ、筐体内へ屈曲せしめられる
u′:i−型又はコの字型類似の切込みより成る共振周
波数の微細調整素子と、前記複数個の共振素子の中、初
段及び終段共振素子と入出力端子゛との開に介在する入
出力結合素子とより成ることを特徴とするコムライン型
帯域通過ろ、皮脂。 (2ン電気長で共振波長のほぼ14の軸長を有し、同一
極性を以て複数個配設された棒状又は筒状導体より成る
共振素子と、この複数個の共振素子の各周りに設けた誘
電体と、前記複数個の共振素子の各開放端と対向する筐
体壁の中、各共振素子間に対応する筐体壁部分に設けら
れ、筐体内へ屈曲せしめられるU字型又はコの字型類似
の切込みより成る股間結合調整素子と、前記複数個の共
振素子の中、初段及び終段共振素子と入出力端子との間
に介在する入出力結合素子とより成ることを特徴とする
コムライン型帯域通過ろ波器。 (3)電気長で共拡波長のほぼ1/4の軸長を有し、同
一極性を以て複数個配設された棒状又は筒状導体まり成
る共振素子と、この複数個の共振素子の各周りに設けた
誘電体と、前記複数個の共振素子の各開放端と対向する
筐体壁部分に設けられ、筐体内へ屈曲せしめられるU字
型又はコの字型類似の切込みより成る共振周波数微細調
整素子と、この共振周波数微細調整素子を設けた筐体壁
の中、前記複数個の共振素子間に対応する筐体壁部分に
設けられ、筐体内へ屈曲せしめられる0字型」又はコの
字型類似の切込みより成る段間結合A整累子と、前記複
数個の共振素子の中、初段及び終段共振素子と入出力端
子との開に介在する入出力結合素子とより成ることを1
.′徴とするコムライン型帯助通過ろ波器。 (4)誘電体を空気を以て置換した特許請求の範囲第1
項ないし第3項の何れかに記載のコムライン型帯域通過
ろ波器。
[Scope of Claims] (1) A resonant element consisting of a plurality of rod-shaped or cylindrical conductors arranged with the same polarity and having an electrical length and an axial length of a resonant wavelength σ14; provided around each resonant element. J electric body and a resonator consisting of an i-shaped or U-shaped notch provided on the housing wall portion facing each open end of the plurality of resonant elements and bent into the housing. A combline type band pass characterized by comprising a frequency fine adjustment element and an input/output coupling element interposed between the first and final stage resonant elements and the input/output terminal among the plurality of resonant elements. Wow, sebum. (A resonant element consisting of a plurality of rod-shaped or cylindrical conductors with an electrical length of 2 mm and an axial length of approximately 14 resonant wavelengths and arranged with the same polarity, and a resonant element provided around each of the plurality of resonant elements. A U-shaped or U-shaped U-shaped or U-shaped U-shaped or U-shaped U-shaped or U-shaped dielectric, which is provided in the housing wall facing each of the open ends of the plurality of resonant elements and between each of the resonant elements, and is bent into the housing. It is characterized by comprising a crotch coupling adjustment element made of a cut similar to a letter shape, and an input/output coupling element interposed between the first and final stage resonance elements and the input/output terminal among the plurality of resonance elements. Combline type bandpass filter. (3) A resonant element consisting of a plurality of rod-shaped or cylindrical conductors arranged with the same polarity and having an axial length that is approximately 1/4 of the co-spreading wavelength in terms of electrical length; A dielectric material provided around each of the plurality of resonant elements and a U-shaped or U-shaped part provided on the casing wall portion facing each open end of the plurality of resonant elements and bent into the casing. A resonant frequency fine adjustment element consisting of a notch similar to the type, and a resonant frequency fine adjustment element provided in the housing wall portion corresponding to the plurality of resonant elements in the housing wall in which this resonant frequency fine adjustment element is provided, and bent into the housing. interstage coupling A commutator consisting of a "0-shaped" or U-shaped similar notch, interposed between the first and final stage resonant elements and the input/output terminals among the plurality of resonant elements; 1 consists of an input/output coupling element.
.. A combline-type band pass filter with the following characteristics: (4) Claim 1 in which the dielectric is replaced with air
The combline type bandpass filter according to any one of Items 1 to 3.
JP58013360A 1983-01-30 1983-01-30 Comb-line type band-pass filter Pending JPS59139701A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58013360A JPS59139701A (en) 1983-01-30 1983-01-30 Comb-line type band-pass filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58013360A JPS59139701A (en) 1983-01-30 1983-01-30 Comb-line type band-pass filter

Publications (1)

Publication Number Publication Date
JPS59139701A true JPS59139701A (en) 1984-08-10

Family

ID=11830929

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58013360A Pending JPS59139701A (en) 1983-01-30 1983-01-30 Comb-line type band-pass filter

Country Status (1)

Country Link
JP (1) JPS59139701A (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03125507U (en) * 1990-04-02 1991-12-18
EP0508733A2 (en) * 1991-04-12 1992-10-14 Lk-Products Oy Adjustable ceramic filter
EP0663702A1 (en) * 1994-01-18 1995-07-19 Lk-Products Oy A dielectric resonator
EP0712177A1 (en) * 1994-11-11 1996-05-15 Murata Manufacturing Co., Ltd. Antenna device
JP2015510353A (en) * 2012-02-27 2015-04-02 ケーエムダブリュ・インコーポレーテッド Radio frequency filter with cavity structure
JP2015192452A (en) * 2014-03-28 2015-11-02 インナートロン インコーポレイテッド Resonator and filter having the same
JPWO2014049922A1 (en) * 2012-09-26 2016-08-22 ノキア ソリューションズ アンド ネットワークス オサケユキチュア Semi-coaxial resonator
GB2555180A (en) * 2016-07-29 2018-04-25 Radio Design Ltd Filter apparatus and method of use thereof

Cited By (14)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03125507U (en) * 1990-04-02 1991-12-18
EP0508733A2 (en) * 1991-04-12 1992-10-14 Lk-Products Oy Adjustable ceramic filter
EP0508733A3 (en) * 1991-04-12 1993-01-13 Lk-Products Oy Adjustable ceramic filter
EP0663702A1 (en) * 1994-01-18 1995-07-19 Lk-Products Oy A dielectric resonator
US5550519A (en) * 1994-01-18 1996-08-27 Lk-Products Oy Dielectric resonator having a frequency tuning element extending into the resonator hole
EP0712177A1 (en) * 1994-11-11 1996-05-15 Murata Manufacturing Co., Ltd. Antenna device
JP2015510353A (en) * 2012-02-27 2015-04-02 ケーエムダブリュ・インコーポレーテッド Radio frequency filter with cavity structure
US9716301B2 (en) 2012-02-27 2017-07-25 Kmw Inc. Radio frequency filter having a hollow box with a wrinkle structure and including a resonance element disposed therein which is short-circuited to the box by a pin
US10090572B1 (en) 2012-02-27 2018-10-02 Kmw Inc. Radio frequency filter having a hollow box with a resonance element disposed therein and a depression with dot peen structures therein
JPWO2014049922A1 (en) * 2012-09-26 2016-08-22 ノキア ソリューションズ アンド ネットワークス オサケユキチュア Semi-coaxial resonator
US9595746B2 (en) 2012-09-26 2017-03-14 Nokia Solutions And Networks Oy Semi-coaxial resonator comprised of columnar shaped resonant elements with square shaped plates, where vertical screw holes are disposed in the square shaped plates
JP2015192452A (en) * 2014-03-28 2015-11-02 インナートロン インコーポレイテッド Resonator and filter having the same
GB2555180A (en) * 2016-07-29 2018-04-25 Radio Design Ltd Filter apparatus and method of use thereof
GB2555180B (en) * 2016-07-29 2021-06-09 Radio Design Ltd Filter apparatus and method of use thereof

Similar Documents

Publication Publication Date Title
US4963844A (en) Dielectric waveguide-type filter
US4996506A (en) Band elimination filter and dielectric resonator therefor
US4179673A (en) Interdigital filter
JP4710174B2 (en) Balanced LC filter
JPS6123881B2 (en)
JP2000114807A (en) Filter device, duplexer and communication equipment device
KR20010030828A (en) Multi surface coupled coaxial resonator
JPS59139701A (en) Comb-line type band-pass filter
JP3797273B2 (en) Band stop filter and communication device
US6924718B2 (en) Coupling probe having an adjustable tuning conductor
JP2630387B2 (en) Dielectric filter
KR19990030945A (en) High Frequency Filter with Citron Resonator
EP1191625A2 (en) High-pass filter
JPS595701A (en) Comb line type band-pass filter
KR100388067B1 (en) Dielectric Filters
JPS628601A (en) Comb-line type band pass filter
JP2516857B2 (en) Ring resonator and filter using the ring resonator
US5859575A (en) Dielectric filter
KR100258788B1 (en) Microwave band pass filters made with an half-cut coaxial resonators
JPH08321702A (en) Dielectric filter and adjustment method for its frequency band with
JPS5952841B2 (en) Dielectric line type filter
JP2012205096A (en) Band pass filter
JPS62181504A (en) Filter
JPH08293708A (en) Resonator and filter composed of the same
JPH0467361B2 (en)