JPS59110202A - Branching filter using band-pass filter - Google Patents

Branching filter using band-pass filter

Info

Publication number
JPS59110202A
JPS59110202A JP21991182A JP21991182A JPS59110202A JP S59110202 A JPS59110202 A JP S59110202A JP 21991182 A JP21991182 A JP 21991182A JP 21991182 A JP21991182 A JP 21991182A JP S59110202 A JPS59110202 A JP S59110202A
Authority
JP
Japan
Prior art keywords
resonator
input
bpf
branching
bpfs
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
Application number
JP21991182A
Other languages
Japanese (ja)
Other versions
JPH0452641B2 (en
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 JP21991182A priority Critical patent/JPS59110202A/en
Publication of JPS59110202A publication Critical patent/JPS59110202A/en
Publication of JPH0452641B2 publication Critical patent/JPH0452641B2/ja
Granted 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
    • H01P1/2056Comb 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)
  • Filters And Equalizers (AREA)

Abstract

PURPOSE:To decrease the number of parts by specifying geometric coefficients of BPFs equipped with input/output capacity-coupled devices forming a branching device and eliminating the need for a branching circuit. CONSTITUTION:Band-pass filters BPF1-BPF3 forming the branching device are comb line type BPFs each composed of a dielectric resonator. In this case, the decrease rate of geometric coefficients from the center resonator to the initial- stage resonator is set larger than that from the center resonator to the final- stage resonator. Further, capacity elements C1.0.1, C2.0.1, C3.0.1, and C4.0.1 which forms the input/output coupled circuits of the respective BPFs are coupled directly with branch points. Consequently, the need for a branching circuit is eliminated and the number of parts is decreased.

Description

【発明の詳細な説明】 本発明は、帯域通過ろ波器を用いた超短波ないしマイク
ロ波用分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。)従来、第1図又は第2図
に等価口路を示すよう(こ、入出力結合回路を容量結合
回路を以て形成したBPFを用いた超短波ないしマイク
ロ波用共用器が実用されでいる。第1図において、R1
ないしRn (nはBPFの次数)は共振回路、C1,
2、Oa、>、・・・・・・Ccn−弓、7?  は段
間結合容量、Cσ、l及びOn、tn−hりは入出力結
合容量である。第2図において、R1ないしRnは共振
回路、J、a、Ma、3 % ・・” ” M(71−
13,7Lは股間磁界結合係数、C6,1及びC,nc
n?すは入出力結合容量である。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a duplexer for very high frequency waves or microwaves using a bandpass filter. (Hereinafter, a bandpass filter is abbreviated as BPF.) Conventionally, as shown in FIG. or a microwave duplexer is in practical use.In Fig. 1, R1
or Rn (n is the order of BPF) is a resonant circuit, C1,
2, Oa, >,...Ccn-bow, 7? is the interstage coupling capacitance, and Cσ, l and On, tn−h are the input/output coupling capacitances. In Fig. 2, R1 to Rn are resonant circuits, J, a, Ma, 3%...''M(71-
13,7L is the crotch magnetic field coupling coefficient, C6,1 and C,nc
n? is the input/output coupling capacitance.

このようなりPFを用いた従来の共用器においては、B
PF’が等価長を有するために第3図示のようにアンテ
ナ等の外部回路を接続する分岐点BRNと中心周波数f
1なるBPF、及び中心周波数faなるBPF’、1の
各入出力端子間にセミリジットケーブル等より成る分岐
回路BC+及びBCaを介在せしめ、各電気長ノ。
In a conventional duplexer using such a PF, B
Since PF' has an equivalent length, the branch point BRN for connecting an external circuit such as an antenna and the center frequency f as shown in the third diagram.
Branch circuits BC+ and BCa made of semi-rigid cables are interposed between the input and output terminals of BPF 1 and BPF' with center frequency fa, respectively, and each electrical length is

及びノコを、o<J!a<入1/4 及び  λフ/4
〈ノ、〈λt(勾は管内波長) I:選び・分岐・慨B
RN %ら分岐回路BCa側を見たインピーダンスを周
波数ffに対して無限大となし、分岐点BRNから分岐
回路Bet側を見たインピーダンスを周波数f、1に対
して無限大となしでf、及びfaが互に干渉することの
ないように構成する必要がある。このように第3図に示
した従来の共用器においては、分岐回路を必要とするた
め構成部品数が多くなり、全体の形状が複雑大形となる
と共に組立調整に比較的多くの時間と労力を要する等の
欠点がある。
and saw, o<J! a<in 1/4 and λf/4
〈ノ、〈λt (gradient is the wavelength within the jurisdiction) I: Selection, branching, outline B
The impedance viewed from the branch circuit BCa side from RN % is assumed to be infinite with respect to the frequency ff, and the impedance viewed from the branch point BRN to the branch circuit Bet side is assumed to be infinite and zero with respect to the frequency f, 1, and It is necessary to configure the fas so that they do not interfere with each other. In this way, the conventional duplexer shown in Figure 3 requires a branch circuit, which increases the number of component parts, makes the overall shape complex and large, and requires a relatively large amount of time and effort for assembly and adjustment. There are drawbacks such as the need for

本発明は、分岐点とBPFの入出力端子間に分岐回路を
介在せしめることなく BPPの入出力端子を分岐点に
直接結合することにより構成部品数が少なく、全体の形
状が簡潔小形で組立の容易な超短波ないしマイクロ波用
分波器を実現することを目的とする。
The present invention reduces the number of component parts by directly connecting the input/output terminals of the BPP to the branching point without intervening a branch circuit between the branching point and the input/output terminals of the BPF, and the overall shape is simple and small, making it easy to assemble. The purpose is to realize a simple duplexer for ultra-high frequency waves or microwaves.

第4図は本発明の一実施例を示す断面図、即ち第5図の
B−B断面図、第5図は第4図のA−A断面図で、両図
において、CASは導体より成る筐体、PARは導体よ
り成る隔壁、BPFIないしBPF4はそれぞれ誘電体
共振器より成るコムライン型BPF % Rr、+ない
しRrハ、R2,1ないしRJ、++シlないしR)■
及びR1/、1ないしR9,7Lはそれぞれ誘電体共振
器の構成素子で、例えば第6図に拡大断面図を示すよう
にチタン酸バリウム磁器等の誘電体より成る直方体りに
穿った孔隙H内に管内波長のりゆの軸長を有する棒状内
部導体Sを嵌入して成り、筐体CAS及び隔壁PARと
共に誘電体共振器を構成する。(1,+ないしOr、t
n−〇、(b、IないしGコ(71−1) % G3.
HないしG3fy+−++及びGEIないしG Q、(
’7L−r)は誘電体共振器間の空隙、SGR+、+な
いしSCR+11及び5CRa、/ないし5CRa、n
は誘電体共振器の構成素子Rr、+ないしRr、n及び
Ra、1ないしRj、%の止めねじで、図には示されて
いないが誘電体共振器の構成素子RJ、IないしR4,
n及びR9,lないしRqnもまた同様の止めねじによ
り筐体CAS内の所要位置に固定しであるo Ctn、
I % Ct、n、Cnpr)lICa、o、H% C
J−71,f7L−+) %03.11.1 % CJ
、n、tns) % CQ、n、+及び販n、(n啼)
は入出力結合容量素子で、適当なコンデンサ又は各初段
及び終段の誘電体共振器における内部導体との間に結合
容量を形成する電極板より成る。T、ないしT瞥は入出
力同軸端子、Tcは共通入出力同軸端子で、引出綿LO
T Th介して入出力結合容量素子Cto、+ % O
G01、cz、a、r及びCLt、olの分岐点に接続
しである。引出線LOT Iよ、特性インピーダンスが
共通入出力同軸端子に接続される外部回路の特性インピ
ーダンスに等し1\ストリツプライン又は同軸線等より
成る。
FIG. 4 is a sectional view showing one embodiment of the present invention, that is, BB sectional view in FIG. 5, and FIG. 5 is an AA sectional view in FIG. The housing, PAR is a partition wall made of a conductor, and BPFI to BPF4 are comline type BPFs each made of a dielectric resonator.
and R1/, 1 to R9, 7L are components of a dielectric resonator, for example, as shown in the enlarged cross-sectional view in FIG. A rod-shaped inner conductor S having an axial length equal to the tube wavelength is fitted into the inner conductor S, and together with the housing CAS and the partition wall PAR, a dielectric resonator is constructed. (1, + or Or, t
n-〇, (b, I to G (71-1) % G3.
H to G3fy+-++ and GEI to G Q, (
'7L-r) is the air gap between the dielectric resonators, SGR+, + to SCR+11 and 5CRa, / to 5CRa, n
are setscrews for the dielectric resonator components Rr, + to Rr, n and Ra, 1 to Rj, %, and are not shown in the figure for the dielectric resonator components RJ, I to R4,
o Ctn, and R9, l to Rqn are also fixed in position within the housing CAS by similar setscrews;
I%Ct,n,Cnpr)lICa,o,H%C
J-71, f7L-+) %03.11.1 % CJ
, n, tns) % CQ, n, + and sales n, (n啼)
is an input/output coupling capacitance element consisting of a suitable capacitor or an electrode plate that forms a coupling capacitance between it and the internal conductor of each initial stage and final stage dielectric resonator. T, or T is the input/output coaxial terminal, Tc is the common input/output coaxial terminal, and the drawn cotton LO
T Th via input/output coupling capacitive element Cto, +% O
It is connected to the branch point of G01, cz, a, r and CLt, ol. The leader line LOT I has a characteristic impedance equal to the characteristic impedance of the external circuit connected to the common input/output coaxial terminal, and is made of a strip line or coaxial line.

そして本発明分波器においては、各BPF lこお(す
る幾何係数を次のように定めである。即ち、一般にBP
F’の幾何係数は第7図(横軸はBPFの次数n1縦軸
は幾何係数の大きざg)Iこ実線を以て示すjうに、中
央の共振器から初段及び終段の共振器(こ到るにしたが
って漸次小となると共(こ初段側に到る減少状態と終段
側に到る減少状態が中心に対して対称となるように構成
するが、本発明分波器を構成する各BPFにおいては中
央部の共振器から分岐点側の初段共振器に到る各共振器
間の結合容量又は磁界結合係数を、中央部の共振器から
終段共振器1こ到る各共振器間の結合容量又は磁界結合
係数よりも適宜大ならしめる等の手段1こすり中央部の
共振器から初段共振器に到る各共振器に関連する幾何係
数を第7図に点線を以て示すように、中央部の共振器か
ら終段共振器に到る各共振器に関連する幾何係数に較べ
て小ならしめると共に、中央部の共振器から初段共振器
に到る各共振器に関連する幾何係数の減少の割合を適当
ならしめることによりBPF’lにおいては周波数f+
なる信号に対する結合特性を良好ならしめると共に、分
岐点からBPP+側を見たインピーダンスをノコないし
fQに対して無限大に近い状態となるように形成し、B
PFλにおいではfaに対する結合特性が良好でf(、
fa、f%に対するインピーダンスが無限大に近・IB
PFJにおいてはで3に対する結合特性が良好でfl、
、fax fg+に対するインピーダンスが無限大に近
< 、BPF9においてはflに対する結合特性が良好
でflないしfaに対するインピーダンスが無限大に近
い状態となるように形成しである。したがって分岐回路
を介することなく BPFrないしBPF’午を分岐点
に直接結合せしめてもflないしf%が互に干渉するこ
となく、f、ないしf、を各対応するBPFrないしB
PF’%に各別に分波結合せしめることが可能で、又、
分岐口路を必要としないからそれだけ全体の形状を簡潔
小形ならしめ得ると共に組立も容易である。
In the duplexer of the present invention, the geometric coefficients for each BPF are determined as follows. That is, in general, the BP
The geometric coefficients of F' are shown in Figure 7 (the horizontal axis is the order n of the BPF, the vertical axis is the size of the geometric coefficient g), and the distance from the central resonator to the first and final stage resonators (towards this point) is shown by the solid line. (The decreasing state reaching the first stage side and the decreasing state reaching the final stage side are configured to be symmetrical with respect to the center.) In , the coupling capacitance or magnetic field coupling coefficient between each resonator from the central resonator to the first stage resonator on the branch point side is calculated as Measures such as increasing the coupling capacitance or magnetic field coupling coefficient appropriately The geometric coefficients associated with each resonator from the central resonator to the first stage resonator are made smaller than the geometric coefficients associated with each resonator from the central resonator to the first stage resonator. By adjusting the ratio appropriately, the frequency f +
In addition to making the coupling characteristics good for the signals of
In PFλ, the coupling characteristics for fa are good, and f(,
Impedance for fa, f% is close to infinity/IB
In PFJ, the coupling characteristics for 3 are good, fl,
, fax fg+ is close to infinity.The BPF9 is formed so that the coupling characteristics to fl are good and the impedance to fl or fa is close to infinity. Therefore, even if BPFr to BPF' are directly connected to a branch point without going through a branch circuit, fl to f% will not interfere with each other, and f to f will be connected to each corresponding BPFr to B.
It is possible to perform demultiplexing and coupling to each PF'% separately, and
Since no branch passage is required, the overall shape can be made simple and compact, and assembly is easy.

第8図及び第9図は本発明分波器の等価回路図で、第8
図は各BPFを構成する各誘電体共振回路間を電界結合
せしめた場合で、R:、lないしR’+rIs R’2
.1ないしRJ、n、R’J、IないしRS、71x 
R’(IIないしR’vnは共振og各、C’t、a、
+、、C′+、n4n−+)、(4)、1%Ca、n、
+n+t+、C10,a、+、C’;、n、tnar)
 s C’17.6.1% O’et、n師qr)は入
力出結合容量、aS、>、c−91・・・・・・訃より
、rtは股間結合容量、T7ないしT−は入力端子、T
ユは共通入力端子である。
8 and 9 are equivalent circuit diagrams of the duplexer of the present invention.
The figure shows the case where electric field coupling is made between each dielectric resonant circuit configuring each BPF, R:, l or R'+rIs R'2
.. 1 to RJ, n, R'J, I to RS, 71x
R'(II to R'vn are resonances og each, C't, a,
+,,C'+,n4n-+),(4),1%Ca,n,
+n+t+,C10,a,+,C';,n,tnar)
s C'17.6.1% O'et, n 2 qr) is the input/output coupling capacity, aS, >, c-91... From the grave, rt is the groin coupling capacity, T7 or T- is Input terminal, T
Y is a common input terminal.

第9図は各BPFを構成する各誘電体共振回路間を磁界
結合せしめた場合で、MIJ % Ma、1・・・・・
・M(7L−1)乳は磁界結合係数で、他の符号は第8
図と同様である。
Figure 9 shows the case where the dielectric resonant circuits constituting each BPF are magnetically coupled, and MIJ % Ma, 1...
・M(7L-1) is the magnetic coupling coefficient, other signs are the 8th
It is similar to the figure.

本発明分波器を構成するBPFにおける誘電体共振器の
構成素子を第6図に示すように、誘電体りに穿った孔隙
H内に棒状導体Sを嵌入して形成する代りに、孔隙Hの
内壁面に銀又は銅等の金属被膜を付着せしめて内部導体
を形成してもよく、孔隙Hの内壁面に金属被膜を付着せ
しめ更にその内部に棒状導体を嵌入して内部導体を形成
してもよく、又、誘電体内にヘリカルコイルを埋込んで
内部導体としてもよい、誘電体りの形状を直方体に形成
する代りに円筒体に形成してもよく、又、隣接する誘電
体共振器間に空隙を設けることなく互に密着せしめるか
、筐体CAS内に誘電体を均一に充てんして誘電体共振
器より成るBPF’を構成してもよい。
As shown in FIG. 6, the constituent elements of the dielectric resonator in the BPF constituting the duplexer of the present invention are formed by inserting a rod-shaped conductor S into the hole H bored in the dielectric. The internal conductor may be formed by attaching a metal coating such as silver or copper to the inner wall surface of the hole H, or by attaching a metal coating to the inner wall surface of the hole H and further fitting a rod-shaped conductor into the inner wall surface of the hole H. Alternatively, a helical coil may be embedded in the dielectric material to serve as an internal conductor. The dielectric material may be formed into a cylindrical shape instead of a rectangular parallelepiped, or an adjacent dielectric resonator may be used as an internal conductor. A BPF' made of a dielectric resonator may be configured by making them closely contact each other without providing a gap therebetween, or by uniformly filling the casing CAS with a dielectric material.

誘電体共振器を以てBPFを構成する代りに多少全体の
形状が大形となるのを免れ得ないが、筐体CAS内の誘
電体を空気を以て置換し、棒状導体又は筒状導体等より
成る内部導体と筐体CAS及び隔壁PARとを以て共振
器を形成せしめるようにしてもよい。
Instead of configuring the BPF with a dielectric resonator, the overall shape will inevitably become somewhat larger, but the dielectric in the casing CAS is replaced with air, and the interior is made of a rod-shaped conductor or a cylindrical conductor. A resonator may be formed by the conductor, the casing CAS, and the partition wall PAR.

第4図及び第5図にはコムライン型BPFを用いた場合
を例示したが、入出力結合回路が容量結合回路より成る
インクディジタル型BPF を用いても本発明を実施す
ることが出来、又、一部のBPF 。
Although FIGS. 4 and 5 illustrate the case where a comline type BPF is used, the present invention can also be practiced using an ink-digital type BPF in which the input/output coupling circuit is a capacitive coupling circuit. , some BPF.

例えばBPFr及びBPFaをコムライン型BPF’を
以て形成し、残りのBPFをインクディジタル型BPF
を以て形成しても本発明を実施することが出来る。
For example, BPFr and BPFa are formed using a comline type BPF', and the remaining BPF is formed using an ink digital type BPF.
The present invention can also be carried out by forming it using the following methods.

第10図は本発明の他の実施例を示す等価回路図で、B
PFr及びBPF4は第7図に実線を以て示した幾何係
数を有するBPF%LCは補償用インダクタンス、BR
Nは分岐点て、今、補償用インダクタンスLGを省いた
場合を検討すると、この場合にはapr、 (又はBP
F& )の入出力結合容量がBPF& (又はBPFE
)の入力端に並列接続された状態になり、電圧定在波比
特性及び伝送特性の劣化を来たすこととなる。然しなが
ら本実施例のように分岐点BRNに補償用インダクタン
スLCを並列に挿入するときは、分岐点BRNからBP
Pr又はBPF、を見た場合の非共振領域における容量
性アドミッタンスが補償用インダクタンスLCにより補
償だれて(この場合LCの太き任を適当に選23りこと
勿論である)、分岐点部分が低負荷Qの並列共振回路を
形成し、BPF’r及びBPF、間の干渉を生ずるおそ
れは全くない。したがって前実施例同様BPFと分岐点
間に分岐回路を介在せしめる必要なく、全体の形状が簡
潔小形で、組立を容易ならしめることが出来る。
FIG. 10 is an equivalent circuit diagram showing another embodiment of the present invention, and B
PFr and BPF4 have the geometric coefficients shown with solid lines in FIG. 7. BPF% LC is the compensation inductance, BR
N is the branch point, and if we now consider the case where the compensation inductance LG is omitted, in this case apr, (or BP
The input/output coupling capacitance of F& ) is BPF& (or BPFE
), resulting in deterioration of voltage standing wave ratio characteristics and transmission characteristics. However, when inserting the compensation inductance LC in parallel to the branch point BRN as in this embodiment, the BP
When looking at Pr or BPF, the capacitive admittance in the non-resonant region is compensated for by the compensating inductance LC (in this case, the thickness of LC should be selected appropriately23), and the branch point becomes low. A parallel resonant circuit of the load Q is formed, and there is no possibility of interference between BPF'r and BPF. Therefore, as in the previous embodiment, there is no need to interpose a branch circuit between the BPF and the branch point, and the overall shape is simple and compact, making assembly easy.

第4図及び第5図に示した実施例においてはBPFを4
個、第10図に示した実施例においではBPFを2−個
分岐点j:直接接続した場合を例示したが、何れの実施
例においても2以上任意複数個のBPFを用いて本発明
を実施することが出来る。
In the embodiment shown in FIGS. 4 and 5, the BPF is 4.
In the embodiment shown in FIG. 10, the case where two BPFs are directly connected to the branch point j is illustrated, but in any embodiment, the present invention can be implemented using any number of BPFs greater than or equal to two. You can.

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

第1図ないし第3図は従来の共用器を示す図、第4図及
び第5図は本発明の一実施例を示す断面図、第6図及び
第7図は本発明分波器を構成する帯域通過ろ波器の構成
を説明する図、第8図及び第9図は本発明分波器の等価
[88]路図、第10図]ま本発明の他の実施例を示す
等側口S各図で、BPF IないしBPF6 :帯域通
過ろ波器、BC+及びBCJ :分岐口路、BRN :
分岐点、CAS :筐体、PAR:隔壁、D:誘電体よ
り成る直方体、H:孔隙、S:棒A大内部導体、T1な
いしTφ:入出力同軸端子、TC:共通入出力同軸端子
、LOT :引出線、R11な(\しR+翫Ra、lな
り、%しRa、n % Ri、tないしRa、n及びR
qIなし% L、 Rq、x:共振器の構成素子、G+
、IないしG、促−〇−GaIなしゝしGコC丸−/)
、G3.IないしGj、(7L−1)及びGQ、fない
しG Ll、cqc−+) :空隙、SCR,、。 ないし5ORtTL及び5CRa、+ないし5CRr、
*:止めねじ、Ot、aへCt、n、(rL+g、OJ
、O,1JajyL、(ytx〕%CL’−1−G3.
’乙−Cnfυ、Cη、of及びCtAn、(fLtr
) ’入出力結合容量素子である。 第 第 第 第9図 第10図 M(71−1)、71
1 to 3 are diagrams showing a conventional duplexer, FIGS. 4 and 5 are sectional views showing an embodiment of the present invention, and FIGS. 6 and 7 are configurations of a duplexer according to the present invention. 8 and 9 are equivalent circuit diagrams of the duplexer according to the present invention, and FIG. 10 is an equivalent circuit diagram showing another embodiment of the present invention. In each figure, BPF I to BPF6: band pass filter, BC+ and BCJ: branch path, BRN:
Branch point, CAS: housing, PAR: partition wall, D: rectangular parallelepiped made of dielectric, H: hole, S: rod A large internal conductor, T1 to Tφ: input/output coaxial terminal, TC: common input/output coaxial terminal, LOT :Leader line, R11 (\shiR+翫Ra, l,%shiRa,n %Ri,t or Ra,n and R
No qI% L, Rq, x: Resonator components, G+
, I to G, prompt-〇-GaI, G-C-circle-/)
, G3. I to Gj, (7L-1) and GQ, f to G Ll, cqc-+): void, SCR, . to 5ORtTL and 5CRa, + to 5CRr,
*: Set screw, Ot, Ct, n, (rL+g, OJ
, O,1JajyL, (ytx]%CL'-1-G3.
'O-Cnfυ, Cη, of and CtAn, (fLtr
) 'It is an input/output coupling capacitive element. Figure 9 Figure 10 M (71-1), 71

Claims (2)

【特許請求の範囲】[Claims] (1)中央部の共振器から初段共振器に到る各共振器に
関連する幾何係数の減少の割合を、中央部の共振器から
終段共振器に到る各共振器に関連する幾何係数の減少の
割合に牝し大ならしめると共に、入出力結合回路を容量
結合口路を以て形成した複数個の帯域通過ろ波器の各初
段共振器側の入出力結合回路を分岐点に直接結合して成
ることを特徴とする帯域通過ろ波器を用いた分波器。
(1) The rate of decrease in the geometric coefficient associated with each resonator from the central resonator to the first stage resonator is calculated by the geometric coefficient associated with each resonator from the central resonator to the final stage resonator. In addition to increasing the rate of decrease in A duplexer using a bandpass filter characterized by comprising:
(2)入出力結合回路を容量結合回路を以て形成した複
数個の帯域通過ろ波器の各一方の入出力結合回路を分岐
点に直接結合すると共に前記分岐点に補償用インダクタ
ンス素子を並列接続して成ることを特徴とする帯域通過
ろ波器を用いた分波器。
(2) One input/output coupling circuit of each of a plurality of bandpass filters formed using capacitive coupling circuits is directly coupled to a branch point, and a compensating inductance element is connected in parallel to the branch point. A duplexer using a bandpass filter characterized by comprising:
JP21991182A 1982-12-15 1982-12-15 Branching filter using band-pass filter Granted JPS59110202A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21991182A JPS59110202A (en) 1982-12-15 1982-12-15 Branching filter using band-pass filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21991182A JPS59110202A (en) 1982-12-15 1982-12-15 Branching filter using band-pass filter

Publications (2)

Publication Number Publication Date
JPS59110202A true JPS59110202A (en) 1984-06-26
JPH0452641B2 JPH0452641B2 (en) 1992-08-24

Family

ID=16742947

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21991182A Granted JPS59110202A (en) 1982-12-15 1982-12-15 Branching filter using band-pass filter

Country Status (1)

Country Link
JP (1) JPS59110202A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2632123A1 (en) * 1988-05-27 1989-12-01 Alcatel Thomson Faisceaux MULTIPLEX FILTER IN HYPERFREQUENCE, AND METHOD FOR ADJUSTING SUCH FILTER
JP2007174519A (en) * 2005-12-26 2007-07-05 Mitsubishi Electric Corp Microwave circuit

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5657302A (en) * 1979-10-15 1981-05-19 Murata Mfg Co Ltd Microwave device using coaxial resonator

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5657302A (en) * 1979-10-15 1981-05-19 Murata Mfg Co Ltd Microwave device using coaxial resonator

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2632123A1 (en) * 1988-05-27 1989-12-01 Alcatel Thomson Faisceaux MULTIPLEX FILTER IN HYPERFREQUENCE, AND METHOD FOR ADJUSTING SUCH FILTER
JP2007174519A (en) * 2005-12-26 2007-07-05 Mitsubishi Electric Corp Microwave circuit

Also Published As

Publication number Publication date
JPH0452641B2 (en) 1992-08-24

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