JPS6027217A - Composite type piezo-electric band pass filter - Google Patents
Composite type piezo-electric band pass filterInfo
- Publication number
- JPS6027217A JPS6027217A JP13470683A JP13470683A JPS6027217A JP S6027217 A JPS6027217 A JP S6027217A JP 13470683 A JP13470683 A JP 13470683A JP 13470683 A JP13470683 A JP 13470683A JP S6027217 A JPS6027217 A JP S6027217A
- Authority
- JP
- Japan
- Prior art keywords
- resonators
- filter
- resonator
- circuit
- mode
- 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
Links
- 239000002131 composite material Substances 0.000 title claims description 5
- 230000008878 coupling Effects 0.000 abstract description 3
- 238000010168 coupling process Methods 0.000 abstract description 3
- 238000005859 coupling reaction Methods 0.000 abstract description 3
- 238000004519 manufacturing process Methods 0.000 abstract description 2
- 230000005611 electricity Effects 0.000 abstract 1
- 238000010586 diagram Methods 0.000 description 5
- 238000000034 method Methods 0.000 description 5
- 230000009977 dual effect Effects 0.000 description 4
- 230000000694 effects Effects 0.000 description 2
- 239000013078 crystal Substances 0.000 description 1
- 238000011038 discontinuous diafiltration by volume reduction Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
- H03H9/46—Filters
- H03H9/54—Filters comprising resonators of piezoelectric or electrostrictive material
- H03H9/542—Filters comprising resonators of piezoelectric or electrostrictive material including passive elements
Landscapes
- Physics & Mathematics (AREA)
- Acoustics & Sound (AREA)
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は圧電帯域フィルタ、特に多重モード圧電共振子
と単一モードのそれと全複合した複合型圧電帯域フィル
タに関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a piezoelectric bandpass filter, and more particularly to a composite piezoelectric bandpass filter that is fully complexed with a multimode piezoelectric resonator and a single mode one.
水晶等の圧電共振子全利用して帯域フィルタ全構成する
場合、単1モードの共振子の組合せによる手法と多重モ
ード共振子を用いモノリシック・フィルりとして構成す
る方法の二つに大別できる。When all piezoelectric resonators such as crystals are used to construct a bandpass filter, there are two main methods: a method using a combination of single-mode resonators, and a method using a multi-mode resonator and configuring it as a monolithic filter.
この二つの方法を比較した場合、一般にモノリシック・
フィルタの方が価格、大きさ共にすぐれているが、多重
モード共振子の電極間隔についての設計上及び製造上の
制約が大きくフィルタのバンド幅に対する自由度が少な
いという欠点があった。When comparing these two methods, the monolithic
Although the filter is superior in terms of price and size, it has the disadvantage that there are large design and manufacturing constraints on the electrode spacing of the multimode resonator, and there is less freedom in the bandwidth of the filter.
本発明は上述の如き従来の多重モード共振子によるモノ
リシック・フィルタの欠点を除去しフィルタ特性につい
ての設計の自由度を高める為になされたものであって、
従属接続する複数個の多重モード圧′屯共振子の一部看
:単−モード圧電共撮子を使用するヤーマン回路に置換
した複合型圧電帯域フィルタを提供せんとするものであ
る。The present invention was made in order to eliminate the drawbacks of the conventional monolithic filter using a multi-mode resonator as described above and to increase the degree of freedom in designing filter characteristics.
It is an object of the present invention to provide a composite piezoelectric bandpass filter that replaces a Yarman circuit using a partial view of a plurality of multi-mode piezoelectric resonators connected in cascade: a single-mode piezoelectric co-resonator.
以下不発明を実施例に基づいて詳l!1IVc説明する
。Below is a detailed description of the invention based on examples! 1IVc Explain.
第1図は従来のフィルタの−?llヲ示す回路図である
がその近似特性は次数4の無極遅延最大平坦特性、中心
周波数(f o)−75MHz及び3dB低下の帯域幅
は40kHzである。Figure 1 shows the conventional filter -? The circuit diagram shown in FIG. 11 has an approximate characteristic of a 4th order non-polar delay maximum flatness characteristic, a center frequency (fo) of -75 MHz, and a bandwidth of 3 dB reduction of 40 kHz.
この場合、2重モード共振子Ql及びQ2の帯域幅はそ
れぞれ57 kI−Iz 、 29 kHzとなる。In this case, the bandwidths of dual mode resonators Ql and Q2 are 57 kI-Iz and 29 kHz, respectively.
2重モード共振子は周知の如く、一枚の圧電板上に近接
する2個の電極を配置し、両者の音響的結合の結果生じ
る対称および反対称モードの二つの振動を利用して帯域
フィルり全構成するものであるが圧電材料として水晶を
用いた場合、電気−機械結合係数の大きさによる制約の
ため前記設計例に於いてはQ2は実現できるがQ、は前
記電極間隔が狭くなり実現困難であるフィルタを実現す
ることができない。As is well known, a dual mode resonator is a bandpass filter that uses two vibrations in symmetric and antisymmetric modes that are generated by acoustic coupling between two electrodes placed close to each other on a single piezoelectric plate. However, if quartz is used as the piezoelectric material, Q2 can be realized in the above design example due to restrictions due to the magnitude of the electro-mechanical coupling coefficient, but Q2 will result in a narrower electrode spacing. It is not possible to realize a filter that is difficult to realize.
このように2重モード共振子が実際には実現困難な場合
には第*回に示す如く単一モード共振子のみを用いるヤ
ーマン回路全縦続に接続してフィルり全構成するのが一
般的であった。If it is difficult to actually realize a dual mode resonator in this way, it is common to connect all the Yarman circuits in cascade using only single mode resonators to form a full configuration, as shown in Part *. there were.
しかしながら上述の如き手法でフィルりを構成する場合
、設計の自由度はあるが回路が複雑で部品も多く、価格
、大きさ共に第1図に示す回路に比べて不利であること
は明らかである。However, when constructing a fill using the method described above, although there is a degree of freedom in design, the circuit is complex and has many parts, and it is clear that it is disadvantageous in terms of cost and size compared to the circuit shown in Figure 1. .
これらの問題を解決する為、本発明に於いては第1図の
回路に於ける2重モード圧電共振子Q1及びQ2のうち
実現困難なQlf、(単1モード圧電共振子2ケを用い
たヤーマン回路で置換えたものであって第*回にその一
実施例を示す。In order to solve these problems, in the present invention, Qlf, which is difficult to realize among the dual mode piezoelectric resonators Q1 and Q2 in the circuit shown in FIG. This is replaced with a Yarman circuit, and an example of this is shown in Part *.
第4図に示す回路は第*回のそれに比べて圧電共振子が
1ケ少なくてすみ、より安価で小型のフィルタとなるこ
とが理解されよう。It will be understood that the circuit shown in FIG. 4 requires one less piezoelectric resonator than the one in the *th circuit, resulting in a cheaper and smaller filter.
一方、本発明による回路構成を採用した結果、そのフィ
ルタ特性にも改善がみられる。第各図フィルタの減衰特
性を示す図であるが両者を比較すれば明らかな如く中心
周波数f o (−75MH2)近傍のスプリアスを見
るに、既ね8d13の向上が見られると共に、例えば減
衰量40’ d Bのライン金横切るスプリアスの数を
比l咬すると従来の回路構成によれば6個存在するのに
対し、本発明によればわずか2個に減少していることが
判る。。。理由。第蕃図。フイ7゜2構成、よる場合単
1モード共振子Q3乃至Q6に発生する副共振の周波数
が同じ位11tに重なって減衰量が大きく低下するのに
対し、第*回のそれでは2重モード共振子Q2と単1モ
ード共振子Q3及びQ4の副共振周波数が同じ位置に重
なる確率が低くなってスプリアス減衰量が向上するから
でおる。On the other hand, as a result of employing the circuit configuration according to the present invention, the filter characteristics are also improved. Fig. 7 is a diagram showing the attenuation characteristics of each filter.As is clear from comparing the two, when looking at the spurious near the center frequency f o (-75MH2), an improvement of 8d13 can already be seen, and for example, the attenuation amount is 40 Comparing the number of spurious components across the line metal of 'dB, it can be seen that while there are six spurious components in the conventional circuit configuration, this number has been reduced to only two in the present invention. . . reason. Part 3. In the case of the F7゜2 configuration, the frequency of the sub-resonance generated in the single mode resonators Q3 to Q6 overlaps with 11t to the same extent, resulting in a large decrease in attenuation, whereas in the case of the This is because the probability that the sub-resonant frequencies of Q2 and the single mode resonators Q3 and Q4 overlap at the same position is reduced, and the amount of spurious attenuation is improved.
以上本発明の実施例および効果を次数4の回路について
のみ説明したが、本発明が更に次数の大きいフィルり回
路にも応用可能であることはいうまでもない。Although the embodiments and effects of the present invention have been described above only for circuits of order 4, it goes without saying that the present invention can be applied to fill circuits of even higher orders.
又、本発明の実施例に於ては2重モード圧電共振子と単
1モード圧電共振子全使用したが、2重モード共振子の
かわりに3重モード以上の多重モード共振子を用いるこ
とも可能である。Further, in the embodiments of the present invention, a double mode piezoelectric resonator and a single mode piezoelectric resonator are all used, but a triple mode or more multimode resonator may be used instead of the double mode resonator. It is possible.
本発明は以上説明した如く構成しかつ機能するものであ
るからフィルタの設計の自由度を大きくすると共にその
減衰量金も売女に確保することができるのみならずコス
ト、容積の低減にも著しい効果を奏するものである。Since the present invention is configured and functions as explained above, it not only allows greater freedom in designing the filter and also secures the attenuation amount for the prostitute, but also has a remarkable effect on cost and volume reduction. It is something that plays.
第1図は2重モード圧電共振子を2ケ縦絖した圧電帯域
フィルりの構成例を示す回路図、第2図は従来一般に使
用されてきた単lモード圧電共振子用いたヤーマン回路
全2セクション縦続に接続した圧電帯域フィルりの構成
例を示す回路図、第3図は本発明に係る複合型圧電帯域
〆
フィルタの1実施例を示す回路図、第*回お上び第6図
は夫々従来の回路構成によるフィルりの特性および本発
明に係るフィルタの特性を示す(2)である。
QlおよびQ22重モード圧電共振子
Q3の至Q6 単1モード圧11C共振子特許出願人
東洋通信機株式会社Figure 1 is a circuit diagram showing a configuration example of a piezoelectric band fill using two double-mode piezoelectric resonators vertically, and Figure 2 is a total of two Yarman circuits using single-mode piezoelectric resonators that have been commonly used in the past. A circuit diagram showing an example of the configuration of a piezoelectric band filter connected in cascade of sections, FIG. 3 is a circuit diagram showing one embodiment of a composite piezoelectric band filter according to the present invention, (2) shows the fill characteristics of the conventional circuit configuration and the characteristics of the filter according to the present invention, respectively. Ql and Q2 double mode piezoelectric resonator Q3 to Q6 single mode pressure 11C resonator patent applicant
Toyo Tsushinki Co., Ltd.
Claims (1)
接続した帯域フィルりに於いて、前記複数個の多重モー
ド・モノリシック圧電共振子の一部全単一モード圧電゛
共振子を使用するヤーマン回路に置換したことを特徴と
する複合型圧電帯域フィルタ。In a bandpass filter in which a plurality of multimode monolithic piezoelectric resonators are connected in series, a Yarman circuit uses all single mode piezoelectric resonators as part of the plurality of multimode monolithic piezoelectric resonators. A composite piezoelectric bandpass filter characterized by replacing the .
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13470683A JPS6027217A (en) | 1983-07-22 | 1983-07-22 | Composite type piezo-electric band pass filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13470683A JPS6027217A (en) | 1983-07-22 | 1983-07-22 | Composite type piezo-electric band pass filter |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6027217A true JPS6027217A (en) | 1985-02-12 |
Family
ID=15134691
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP13470683A Pending JPS6027217A (en) | 1983-07-22 | 1983-07-22 | Composite type piezo-electric band pass filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6027217A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6181016A (en) * | 1984-09-28 | 1986-04-24 | Nippon Dempa Kogyo Co Ltd | Piezoelectric filter |
JPH0480125U (en) * | 1990-11-27 | 1992-07-13 |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58134707A (en) * | 1982-02-05 | 1983-08-11 | Kuraray Co Ltd | Manufacture for composite-hardened product |
-
1983
- 1983-07-22 JP JP13470683A patent/JPS6027217A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58134707A (en) * | 1982-02-05 | 1983-08-11 | Kuraray Co Ltd | Manufacture for composite-hardened product |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6181016A (en) * | 1984-09-28 | 1986-04-24 | Nippon Dempa Kogyo Co Ltd | Piezoelectric filter |
JPH0480125U (en) * | 1990-11-27 | 1992-07-13 |
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