JPS6216003Y2 - - Google Patents
Info
- Publication number
- JPS6216003Y2 JPS6216003Y2 JP3233381U JP3233381U JPS6216003Y2 JP S6216003 Y2 JPS6216003 Y2 JP S6216003Y2 JP 3233381 U JP3233381 U JP 3233381U JP 3233381 U JP3233381 U JP 3233381U JP S6216003 Y2 JPS6216003 Y2 JP S6216003Y2
- Authority
- JP
- Japan
- Prior art keywords
- coupling
- bandpass
- duplexer
- input
- pass
- 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
Links
- 238000010168 coupling process Methods 0.000 description 56
- 230000008878 coupling Effects 0.000 description 51
- 238000005859 coupling reaction Methods 0.000 description 51
- 230000005684 electric field Effects 0.000 description 13
- 238000005192 partition Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 238000003780 insertion Methods 0.000 description 3
- 230000037431 insertion Effects 0.000 description 3
- 238000000926 separation method Methods 0.000 description 3
- 239000004020 conductor Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
Description
【考案の詳細な説明】
この考案は結合方式を互に異にする2種の帯域
通過波器それぞれの特性の相異を有効に利用し
て分波特性を改良した分波器に関する。[Detailed Description of the Invention] This invention relates to a duplexer that improves the demultiplexing characteristics by effectively utilizing the differences in the characteristics of two types of band-pass waveformers using different coupling methods.
従来の分波器は、結合方式を共に同一とした帯
域通過波器の組合せにより構成されていた。す
なわち従来の分波器は、入出力部の結合及び共振
素子間の結合がすべてループ等による磁界結合を
なす帯域通過波器の組合せによる構成、或いは
入出力部の結合及び共振素子間の結合がすべて先
端開放の結合用線又は容量板等による電界結合を
なす帯域通過波器の組合わせによる構成であつ
た。これらの分波器においては、分波すべき周波
数領域の減衰量を多くとるために、波器の段数
を増やしたり、或いはノツチフイルタを追加して
必要な減衰量を確保していた。しかしながらこの
ような接続構成にあつては通過域の挿入損失が従
らに増加し、分波器全体が大きなものとなり、取
扱いが不便で、しかも材料費や加工費の増加によ
るコスト高を招いていた。 A conventional duplexer is composed of a combination of bandpass duplexers that use the same coupling method. In other words, conventional duplexers are configured by a combination of band-pass waveformers in which the coupling between the input and output parts and the coupling between the resonant elements are all magnetic field coupling by a loop, or the coupling between the input and output parts and the coupling between the resonant elements is All of these configurations were composed of a combination of open-ended coupling wires or band-pass waveforms for electric field coupling using capacitive plates or the like. In these duplexers, in order to obtain a large amount of attenuation in the frequency range to be demultiplexed, the number of stages of the duplexer is increased or a notch filter is added to secure the necessary amount of attenuation. However, in such a connection configuration, the insertion loss in the passband increases accordingly, making the entire duplexer large and inconvenient to handle, and leading to higher costs due to increased material and processing costs. Ta.
この考案は上記実情に鑑みなされたもので、そ
の目的とするところは、分波すべき周波数領域に
おける減衰量を、通過域における挿入損失の増
加、更には分波器全体の構成の増大化等を招くこ
となく増大させることのできる分波効率の高い分
波器を提供することにある。 This idea was created in view of the above circumstances, and its purpose is to reduce the amount of attenuation in the frequency domain to be demultiplexed, increase the insertion loss in the passband, and further increase the overall configuration of the demultiplexer. The object of the present invention is to provide a duplexer with high demultiplexing efficiency that can be increased without causing problems.
以下図面を参照してこの考案の一実施例を説明
する。先ず具体的な構成例を説明するに際し、こ
の考案の概要を説明しておく。この考案において
は、入出力部の結合及び共振素子間の結合がすべ
て電界結合による帯域通過波器と、入出力部の
結合及び共振素子間の結合がすべて磁界結合によ
る帯域通過波器とを組合せて分波器を構成す
る。すなわち、上記電界結合による帯域通過波
器は、第1図aに示す如く、通過周波数の低い側
すなわち低域側の減衰特性が、より急峻(立上り
特性が優れている)であり、一方、上記電界結合
による帯域通過波器は、同図bに示す如く、通
過周波数の高い側すなわち高域側の減衰特性が、
より急峻であることに着目したもので、このよう
な各波器の特性を有効に利用し、周波数1,
2(1<2)を分波する場合、電界結合に
よる帯域通過波器を2用、磁界結合による帯
域通過波器を1用にすることにより、より分
離度の高い分波特性の良好な分波器を実現するこ
とができる。 An embodiment of this invention will be described below with reference to the drawings. First, before explaining a specific configuration example, an outline of this invention will be explained. This device combines a bandpass waver in which the coupling between the input and output parts and the coupling between the resonant elements is all based on electric field coupling, and a bandpass waver in which the coupling between the input and output parts and the coupling between the resonant elements is all based on magnetic field coupling. to configure a duplexer. In other words, as shown in FIG. 1a, the band-pass waver using electric field coupling has a steeper attenuation characteristic (excellent rise characteristic) on the lower side of the passing frequency, that is, on the low-frequency side. As shown in Figure b, a bandpass waveform using electric field coupling has an attenuation characteristic on the high pass frequency side, that is, on the high frequency side.
This method focuses on the steepness of the waveform, and effectively utilizes the characteristics of each waveform to achieve frequencies 1 , 2, and 3.
2 ( 1 < 2 ), by using a bandpass waver using electric field coupling for 2 and a bandpass waver using magnetic field coupling for 1 , it is possible to obtain good demultiplexing characteristics with a higher degree of separation. A duplexer can be realized.
次に第2図および第3図を参照してこの考案の
具体的な一実施例を説明する。第2図は一実施例
における分波器の構成を示すもので、図中、20
A,20Bはそれぞれ結合方式を異にする帯域通
過波器、21は入力端22に供給された信号を
上記各帯域通過波器20A,20Bに分配する
2分配器である。1及至9は上記帯域通過波器
20Aの各構成要素であり、1は周波数2の1/
4波長の長さの丸棒形状の共振素子、2は波器
20Aの外導体であるケース、3は各共振器間の
仕切板、4はこの仕切板3に設けられた結合用
窓、5は入出力部の結合板(又は結合線)、6,
7は共に共振器間の結合板(又は結合線)、8は
入力接栓、9は出力接栓である。この構成から明
らかな如く、帯域通過波器20Aは、入力部、
出力部、及び各共振器間の結合がすべて結合板
(又は結合線)5及至7によるもので、これらは
各共振器の電界の強い位置に設けられ、すべて電
界結合となつている。このような電界結合による
帯域通過波器20Aは、前述した如く、帯域通
過減衰特性の低域側における特性において優れて
いる。すなわち第1図aに示す如く低域側の立上
り特性が優れている。又、第2図において、11
及至19は上軌帯域通過波器20Bの各構成要
素であり、11は周波数1(1<2)の1/
4波長の長さの丸棒形状の共振素子、12は波
器20Bの外導体であるケース、13は各共振器
間の仕切板、14はこの仕切板13に設けられた
結合用窓、15は入出力部の結合ループ、16は
共振器間の結合ループ、18は入力接栓、19は
出力接栓である。この構成から明らかな如く、帯
域通過波器20Bは、入力部、出力部、及び各
共振器間の結合がすべて結合ループ15,16に
よるもので、これら結合ループは各共振器の磁界
の強い位置に設けられ、すべて磁界結合となつて
いる。このような磁界結合による帯域通過波器
20Bは、前述した如く、帯域通過減衰特性の高
域側における特性において優れている。すなわち
第1図bに示す如く高域側の立上り特性が優れて
いる。従つて、電界結合による帯域通過波器2
0Aを周波数2用、磁界結合による帯域通過
波器20Bを周波数1用として、これらを2分
配器21と組合わせ、周波数1と2の分波器
を構成すると、入力端22からの通過特性は第3
図の点線で示す特性ロの如くなる。すなわち周波
数2用の帯域通過波器20Aの1側、およ
び周波数1用の帯域通過波器20Bの2側
の減衰特性が共に急峻となり、減衰が多くとれる
ため、周波数1と2の分離度が、上記第3図
に実線で示す従来構成による特性イに比して大幅
に改善されたものとなる。 Next, a specific embodiment of this invention will be described with reference to FIGS. 2 and 3. Figure 2 shows the configuration of a duplexer in one embodiment.
Reference numerals A and 20B designate bandpass wavers having different coupling methods, and reference numeral 21 represents a two-way divider that distributes the signal supplied to the input terminal 22 to each of the bandpass waveformers 20A and 20B. 1 to 9 are each component of the bandpass waver 20A, and 1 is 1/1 of frequency 2 .
A resonant element in the shape of a round bar with a length of four wavelengths, 2 a case which is the outer conductor of the wave generator 20A, 3 a partition plate between each resonator, 4 a coupling window provided in this partition plate 3, 5 is the coupling plate (or coupling line) of the input/output section, 6,
7 is a coupling plate (or coupling line) between the resonators, 8 is an input connector, and 9 is an output connector. As is clear from this configuration, the bandpass waver 20A has an input section,
The output section and the coupling between each resonator are all provided by coupling plates (or coupling wires) 5 to 7, which are provided at a position of each resonator where the electric field is strong, and are all electrically coupled. As described above, the bandpass waveform generator 20A using such electric field coupling has excellent bandpass attenuation characteristics on the low frequency side. That is, as shown in FIG. 1a, the rise characteristics on the low frequency side are excellent. Also, in Figure 2, 11
to 19 are each component of the upper orbit bandpass transducer 20B, and 11 is 1/1 of frequency 1 ( 1 < 2 ).
A resonant element in the shape of a round bar with a length of four wavelengths, 12 a case which is the outer conductor of the wave transmitter 20B, 13 a partition plate between each resonator, 14 a coupling window provided in this partition plate 13, 15 16 is a coupling loop between the resonators, 18 is an input connector, and 19 is an output connector. As is clear from this configuration, in the band-pass waveform generator 20B, the input section, the output section, and the coupling between each resonator are all due to the coupling loops 15 and 16, and these coupling loops are located at the positions where the magnetic field of each resonator is strong. They are all magnetically coupled. As described above, the band-pass wave generator 20B using such magnetic field coupling has excellent band-pass attenuation characteristics on the high frequency side. That is, as shown in FIG. 1b, the rising characteristics on the high frequency side are excellent. Therefore, the bandpass wave generator 2 by electric field coupling
When 0A is used for frequency 2 and the bandpass waver 20B by magnetic field coupling is used for frequency 1 , and these are combined with the 2-way divider 21 to configure a duplexer for frequencies 1 and 2 , the pass characteristics from the input end 22 are as follows. Third
The characteristic will be as shown by the dotted line in the figure. In other words, the attenuation characteristics of the first side of the bandpass waveform generator 20A for frequency 2 and the second side of the bandpass waveform generator 20B for frequency 1 are both steep, and a large amount of attenuation can be obtained, so that the degree of separation between frequencies 1 and 2 is This is significantly improved compared to characteristic A of the conventional configuration shown by the solid line in FIG. 3 above.
尚、上記実施例において、各共振器間、及び入
出力部の結合をすべて電界結合又は磁界結合とし
たが、各共振器間の結合方式と入出力部の結合方
式とが異なつても、ある程度の効果は得られる。
例えば各共振器間の結合を電界結合とし、入出力
部の結合を磁界結合とした帯域通過波器と、各
共振器間の結合を磁界結合とし、入出力部の結合
を電界結合とした帯域通過波器との組合せによ
つても、ある程度の効果が得られる。又、上記実
施例においては同軸素子を用いた構成としている
が、素子形状はこれに限るものではなく、例えば
ヘリカル形、ストリツプライン形、又は誘電体形
等、何れであつてもよい。又、上記実施例におけ
る分波器は混合器として用いることもできる。 In the above embodiment, the coupling between each resonator and the input/output section is all electric field coupling or magnetic field coupling, but even if the coupling method between each resonator and the coupling method between the input/output section are different, the The effect can be obtained.
For example, there is a bandpass waver in which the coupling between each resonator is electric field coupling and the coupling in the input/output part is magnetic field coupling, and the other is a band pass waver in which the coupling between each resonator is magnetic field coupling and the coupling in the input/output part is electric field coupling. A certain degree of effect can also be obtained by combining it with a passing wave device. Further, although the above embodiment uses a coaxial element, the shape of the element is not limited to this, and may be of any type, such as a helical type, a stripline type, or a dielectric type. Moreover, the duplexer in the above embodiment can also be used as a mixer.
以上詳記したようにこの考案によれば、入出力
部及び各共振器間の結合がすべて電界結合にによ
る帯域通過波器と、入出力部及び各共振器間の
結合がすべて磁界結合による帯域通過波器とを
組合わせて分波器を構成することにより、従来の
分波器のように従らに段数を増加することなく、
又、ノツチフイルタ等を付加することなく、分離
度を容易に改善することができる。すなわち挿入
損失の増加や分波器全体の構成増大等を招くこと
なく、分波器の特性を改善することができ、従つ
て経済的に有利で、かつ取扱いの容易な分波器が
実現できる。 As detailed above, according to this invention, the coupling between the input/output section and each resonator is entirely based on electric field coupling, and the coupling between the input/output section and each resonator is entirely based on magnetic field coupling. By configuring a duplexer by combining it with a pass waver, there is no need to increase the number of stages as in conventional duplexers.
Furthermore, the degree of separation can be easily improved without adding a notch filter or the like. In other words, it is possible to improve the characteristics of the duplexer without increasing insertion loss or increasing the overall configuration of the duplexer, and therefore it is possible to realize a duplexer that is economically advantageous and easy to handle. .
第1図aは電界結合による帯域通過波器の特
性を示す図、同図bは磁界結合による帯域通過
波器の特性を示す図、第2図はこの考案の一実施
例における構成を示す図、第3図は上記実施例に
おける分波器の特性を従来の構成による分波器の
特性を対比して示す図である。
1,11……共振素子、2,12……ケース、
3,13……仕切板、5,6,7……結合板(又
は結合線)、8,18……入力接栓、9,19…
…出力接栓、20A,20B……帯域通過フイル
タ、21……2分配器、22……入力端。
Figure 1a is a diagram showing the characteristics of a bandpass waver using electric field coupling, Figure 1b is a diagram showing the characteristics of a bandpass waver using magnetic field coupling, and Figure 2 is a diagram showing the configuration of an embodiment of this invention. FIG. 3 is a diagram showing the characteristics of the duplexer in the above embodiment in comparison with the characteristics of a duplexer with a conventional configuration. 1, 11... Resonant element, 2, 12... Case,
3, 13... Partition plate, 5, 6, 7... Connection plate (or connection line), 8, 18... Input connector, 9, 19...
...output connector, 20A, 20B...bandpass filter, 21...2 divider, 22...input end.
Claims (1)
波器と、共振器間をすべて磁界結合してなる帯域
通過波器とを組合わせて構成したことを特徴と
する分波器。 A duplexer characterized in that it is constructed by combining a band-pass waveformer in which all resonators are electrically coupled and a band-pass waveform in which all resonators are magnetically coupled.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3233381U JPS6216003Y2 (en) | 1981-03-09 | 1981-03-09 |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3233381U JPS6216003Y2 (en) | 1981-03-09 | 1981-03-09 |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS57146404U JPS57146404U (en) | 1982-09-14 |
JPS6216003Y2 true JPS6216003Y2 (en) | 1987-04-23 |
Family
ID=29829731
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3233381U Expired JPS6216003Y2 (en) | 1981-03-09 | 1981-03-09 |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6216003Y2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2790612B2 (en) * | 1994-07-26 | 1998-08-27 | 日本電業工作株式会社 | Antenna system common equipment |
-
1981
- 1981-03-09 JP JP3233381U patent/JPS6216003Y2/ja not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS57146404U (en) | 1982-09-14 |
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