JPS58146122A - Ladder type piezoelectric filter - Google Patents

Ladder type piezoelectric filter

Info

Publication number
JPS58146122A
JPS58146122A JP2921182A JP2921182A JPS58146122A JP S58146122 A JPS58146122 A JP S58146122A JP 2921182 A JP2921182 A JP 2921182A JP 2921182 A JP2921182 A JP 2921182A JP S58146122 A JPS58146122 A JP S58146122A
Authority
JP
Japan
Prior art keywords
filter
piezoelectric
ladder
frequency
vibrator
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
JP2921182A
Other languages
Japanese (ja)
Inventor
Takeshi Inoue
武志 井上
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.)
NEC Corp
Original Assignee
NEC Corp
Nippon Electric 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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP2921182A priority Critical patent/JPS58146122A/en
Publication of JPS58146122A publication Critical patent/JPS58146122A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/46Filters
    • H03H9/54Filters comprising resonators of piezo-electric or electrostrictive material
    • H03H9/58Multiple crystal filters
    • H03H9/60Electric coupling means therefor

Abstract

PURPOSE:To ensure the high reliability and to make the manufacture easy, by arranging piezoelectric oscillators of a ladder type piezoelectric filter so as to have resonance frequencies in order as increase or decrease, decrease after increase, or increase after decrease. CONSTITUTION:The resonance frequencies of the piezoelectric oscillators of the ladder type piezoelectric filter comprising the piezoelectric oscillators a1-a9 arranged in series and parallel capacitors C are arranged so as to be increased in order from the input terminal to the output terminal, allowing to realize the filter without large ripple and smooth pass band characteristics. Since the resonance frequencies of the oscillators have a tolerance at the manufacture in a prescribed range, the order of arrangement of the piezoelectric oscillators is selected to form the filter. The resonance frequencies can be reduced, reduced after increase, or increased after decrease in order. Thus, the process of the adjustment of frequency characteristics of the piezoelectric oscillators is omitted to manufacture the piezoelectric filter.

Description

【発明の詳細な説明】 本発明は梯子製圧電フィルタの構成に関するものであり
。梯子型圧電フィルタとして、第1図に示すよ5に直列
腕、並列11i1に各々圧W振動子な配置した4551
  中間周波フィルタがラジオ、トランシーバ用をはじ
め民生用に広く用いられている。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to the structure of a ladder piezoelectric filter. As a ladder type piezoelectric filter, as shown in Fig. 1, a 4551 with a series arm 5 and a pressure W oscillator arranged in parallel 11i1 is used.
Intermediate frequency filters are widely used in radios, transceivers, and other consumer applications.

このフィルタを構成する場合、まず直列腕に配置される
振動子11の共振周波数と、並列腕に配置される振動干
しの反共振周波数な一致させることが必要である。また
保証減衰量を大きくとるために振動子11は並列容量を
小さく、振動チルは逆に並列容量を大きくする必要があ
る。
When constructing this filter, it is first necessary to match the resonant frequency of the vibrator 11 arranged in the series arm with the anti-resonant frequency of the vibrator 11 arranged in the parallel arm. Further, in order to obtain a large guaranteed attenuation amount, the parallel capacitance of the vibrator 11 needs to be small, and the parallel capacitance of the vibrating chill needs to be large.

このため、保証減衰量に関し【、1種類の圧電材料でフ
ィルタを構成した場合には振動子の数が多くなりすぎる
ために、一般に互いKil電率の大幅に異なる2種類の
圧電材料が用いられている。
For this reason, regarding the guaranteed attenuation amount, if a filter is constructed from one type of piezoelectric material, the number of vibrators will be too large, so two types of piezoelectric materials with significantly different Kiloelectric constants are generally used. ing.

さらに、温度特性及びエージング特性において振動子1
1の共振周波数と振動子12の反共振周波数の動きが一
致し、かつその偏差の小さいことが必要であり、これら
の要求を満足させるような圧電材料が得られなければフ
ィルタの通過帯域内に9ツプルを生じる。
Furthermore, the temperature characteristics and aging characteristics of the resonator 1
It is necessary that the resonant frequency of the resonator 1 and the anti-resonant frequency of the vibrator 12 match and have a small deviation, and if a piezoelectric material that satisfies these requirements cannot be obtained, it is necessary to Generates 9-tuples.

従って、ts1図のフィルタ構成で、民生品に比よ;上
゛2かに高信頼性が要求される搬送用フィルタを実現す
ることは材料の面で極めて困難である。
Therefore, it is extremely difficult in terms of materials to realize a conveyance filter that requires higher reliability than consumer products with the filter configuration shown in Figure ts1.

次に、第2図に示した梯子型フィルタは、上記欠点を解
消することができ、既に動作パラメータ法を用いた設計
で一部実用に供されている。しかし、動作パラメータ設
計を用いると多くの種類の異なる振動子A1〜A、h結
合容量01〜C,−、が必要となり製造コストが高くな
るといつた欠点がある。
Next, the ladder type filter shown in FIG. 2 can overcome the above-mentioned drawbacks, and some of the filters have already been put into practical use after being designed using the operating parameter method. However, when operating parameter design is used, many different types of oscillators A1 to A and h coupling capacitances 01 to C, - are required, resulting in an increase in manufacturing costs.

−一方、第2図に示したフィルタを影像パラメータ法で
設計した場合には振動子ム1〜A%の共振周波数fr及
び容量比lは等しく、両端の振動子ム、および4p並列
容量はこれ以外の振動子ム、〜Al&−tのそれぞれの
並列容量の24とし、また結合容量C1〜C,、はすべ
て等しくし−なければならない。従って並列容量の異な
る2種類の振動子と1m1tillの結合容量で実現で
きる長所を有する。しかしながら、振動子ム、〜入の共
振周波数をすべて等しくしなけければフィルタの通過域
に大きなリップルを生じるため、各振動子はあらかじめ
かなりの精度で周波数調整を行っておかなければならな
い欠点があった。
- On the other hand, when the filter shown in Fig. 2 is designed using the image parameter method, the resonant frequency fr and the capacitance ratio l of the oscillators 1 to A% are equal, and the oscillators at both ends and the 4p parallel capacitance are equal. 24 of the parallel capacitances of the vibrator elements ˜Al&-t, and the coupling capacitances C1 to C, , must all be equal. Therefore, it has the advantage that it can be realized with two types of vibrators with different parallel capacitances and a coupling capacitance of 1 ml till. However, if the resonant frequencies of the resonators are not all equalized, large ripples will occur in the passband of the filter, so each resonator has the disadvantage that the frequency must be adjusted with considerable precision in advance. Ta.

圧電材料では、原料や製造pットが変ると音速が若干変
化することが避けられないこと、また振動子の寸法の加
工精度でも共振周波数が若干変化するので、前述のよう
な周波数調整は必要不可欠の工程であると考えられてき
た。
With piezoelectric materials, it is unavoidable that the speed of sound changes slightly when the raw material or manufacturing point changes, and the resonant frequency changes slightly depending on the machining accuracy of the vibrator dimensions, so frequency adjustment as described above is necessary. It has been considered an essential process.

このような周波数v4整は多数の人手と設備が必要であ
り、量章時における障害になると同時に梯子型圧電フィ
ルタを高11i1cする大きな要因となっていた。
Such adjustment of the frequency v4 requires a large number of manpower and equipment, and is a major factor in increasing the height of the ladder-type piezoelectric filter to 11i1c, as well as being a hindrance during measurement.

本発明の目的は、高信頼性を有し、かつ製作容易で安価
な梯子型圧電フィルタを提供することKある。
An object of the present invention is to provide a ladder-type piezoelectric filter that has high reliability, is easy to manufacture, and is inexpensive.

j121El示した梯子聾圧電フィルタにおいて、電気
的Ki近1の振動子間では、共振周波数が若干異なって
も整合条件はあまり乱されない。
In the ladder-deaf piezoelectric filter shown in FIG. 121El, matching conditions are not disturbed much even if the resonant frequencies are slightly different between the vibrators whose electrical Ki is close to 1.

本発明楡、この性質を利用して第2図の示すllI接振
動子間で少しづつ共振周波数をずらせて多段接続構成し
、その結果全体としては共振周波数差が大きな振動子を
用いてフィルタな構成できるようKしたものである。
The present invention utilizes this property to construct a multi-stage connection structure in which the resonant frequency is slightly shifted between the I and I contact vibrators shown in Fig. 2, and as a result, the overall result is a filter using vibrators with a large difference in resonant frequency. It is designed so that it can be configured.

すなわち、本発明は直列に圧電振動子が配置され、並列
に容量が配置される梯子型圧電フィルタ忙おいて、圧電
振動子をその共振周波数が該フィルタの入力側から出力
*Kかげて願icj!&くなるように配置するか、ある
いはIjK低くなるように配置する構成、さらに圧電振
動子をその共振−周波数がフィルタの入力側から履に増
加してゆき途中から逆に減少してゆくように配置するか
、あるいは入力側からJ[k:減少してゆき途中から逆
kl[k増加してゆくように配置する構成を特徴とし【
いる。
That is, the present invention uses a ladder-type piezoelectric filter in which piezoelectric vibrators are arranged in series and capacitors are arranged in parallel, and the resonance frequency of the piezoelectric vibrators is output from the input side of the filter. ! A configuration in which the piezoelectric vibrator is arranged so that the resonance frequency increases from the input side of the filter to the input side of the filter, and conversely decreases from the middle of the input side of the filter. It is characterized by a configuration in which J[k: decreases from the input side and inversely increases kl[k] from the input side.
There is.

本発明に従えば、各圧電振動子の共振周波数が互いに異
なることが特徴である丸め、製造条件のばらつきkより
て生じる各振動子の共振周波数のばらつきは何等補正す
る必要がないばかりかむしろ好都合であり、上記従来フ
ィルタの欠点を除くことが可能となり、周波数調整とい
う面倒な工程は省略してフィルタを構成することができ
る。
According to the present invention, it is not necessary to correct variations in the resonance frequency of each piezoelectric vibrator caused by rounding and variations in manufacturing conditions, which are characterized by different resonance frequencies of each piezoelectric vibrator, but it is even convenient. Therefore, it is possible to eliminate the drawbacks of the conventional filter, and the filter can be constructed without the troublesome step of frequency adjustment.

以下、実施例に従って本発明のm明を行う。Hereinafter, the present invention will be explained according to Examples.

〔実施例1〕 中心周波数が564 KHzで、ジルコン・チタン酸鉛
系圧電セラミック材料からなる円板のラジアルそ−ド振
動子から構成した第3図に示すような9個の圧電振動子
と8個の容量からなる梯子製圧電フィルタを本発明の代
表例に選び説明する。
[Example 1] Nine piezoelectric vibrators as shown in FIG. A ladder-type piezoelectric filter having a capacitance of 1,000,000 is selected as a representative example of the present invention and will be explained.

第3Iiilで直列に配置される圧電振動子−〜a、は
並列容量c、が102〜105PF 、II量比lが5
.13〜5.27 。
The piezoelectric vibrators arranged in series in the third Iiiil have a parallel capacitance c of 102 to 105PF, and an II quantity ratio l of 5.
.. 13-5.27.

共振尖鋭度(は1920〜2060.またA端Ki1列
Ic&iifされる圧電振動子”、Lp a@はl及び
(は圧電振動子a、〜a、と同程度であるが並列容量C
en12倍の207〜211PFである。また結合容量
Cは1850〜1920PFに設定されている。
The resonance sharpness (is 1920~2060.Also, the A end Ki1 row Ic&iif of the piezoelectric vibrator", Lp a@ is l and (is about the same as the piezoelectric vibrator a, ~a, but the parallel capacitance C
It is 207 to 211PF, which is 12 times en1. Further, the coupling capacitance C is set to 1850 to 1920PF.

圧電振動子の形状については町及びa、は板厚0.65
闘、直径4,36關の全面電極構成、 a亡a、は板厚
0.80■p直径4.39 m y電極直径3.17i
nの部分電極構成である。そして圧電振動子の共振周波
数の設5゜を@4図に示すように定めた。即ち、フィル
タ・組み込むことが許される最低の共振周波数!567
.90KHzから300出おきK 56α6kkhまで
9区間のそれぞれの周波数範囲に属する振動子をそれぞ
れ順次18〜a、の圧電振動子として配置する。このう
ちa。
Regarding the shape of the piezoelectric vibrator, town and a are plate thickness 0.65.
Full-surface electrode configuration with a diameter of 4.36 cm, a plate thickness of 0.80 m, p diameter of 4.39 m, and y electrode diameter of 3.17 m.
n partial electrode configuration. Then, the resonance frequency of the piezoelectric vibrator was set at 5° as shown in Figure @4. In other words, the lowest resonant frequency that is allowed to be incorporated into the filter! 567
.. Vibrators belonging to each of nine frequency ranges from 90 KHz to 300 K 56α6 kkh are sequentially arranged as piezoelectric vibrators 18 to a. Of these a.

〜a、までの7個の圧電振動子は製造ばらつきにより生
じた圧電振動子の共振周波数のばらつきを周波数選別1
1Kかげて分類した。この55&加〜5G0.20此ま
での21cHxの’+tらつきは′圧電振動子の通常の
製造方法によるばらつきKはぼ一致し、a、〜a畠まで
の圧電振動子は周波数調整の必要が全くない。
For the seven piezoelectric vibrators from ~a, frequency selection 1
Classified by 1K. The '+t fluctuation of 21cHx up to 55 & 5G0.20 is almost the same as the variation K due to the normal manufacturing method of piezoelectric vibrators, and the piezoelectric vibrators from a to a Hatake require frequency adjustment. Not at all.

本実施例におい【は、両端の11及びa、の圧電振動子
のみ周波数調整すれば良いわけである。
In this embodiment, it is only necessary to adjust the frequency of the piezoelectric vibrators 11 and a at both ends.

本発明のフィルタの通過域特性な菖5図に実線で示す。The passband characteristics of the filter of the present invention are shown by solid lines in Figure 5.

また同図の点線は、従来の影像パラメータ法で設計され
たフィルタ特性を示し、圧電振動チー〜a、までの共□
振周波数をすべて!59.25 k)h K周波wLI
Il−整を行ったものである1・峠いずれも滑らかな通
過域特性を示し【いること、がわかる。
In addition, the dotted line in the same figure shows the filter characteristics designed using the conventional image parameter method, and the common □
All vibration frequencies! 59.25 k)h K frequency wLI
It can be seen that both 1 and Toge, which were subjected to Il adjustment, exhibit smooth passband characteristics.

また、同図中一点鎖1は、各圧電振動子の並列容量Co
、容量比d、共振尖鋭度(が先の例と眸しいが、圧電振
動子11〜a9までの共振周波数を558.20kHz
〜560.20 kH/)範囲内にあるものを本発明の
構成に従わないでランダムに組み込んだものである。
In addition, the chain 1 in the same figure indicates the parallel capacitance Co of each piezoelectric vibrator.
, capacitance ratio d, resonance sharpness (This is similar to the previous example, but the resonance frequency of piezoelectric vibrators 11 to a9 is 558.20kHz.
~560.20 kHz/) were randomly incorporated without following the structure of the present invention.

内、終端インピーダンスは、いずれの場合も150Ωで
ある。
In each case, the terminal impedance is 150Ω.

以上の実施例から明らかなように5周波数の異なった圧
電振動子をランダムに![iみ合せれば、フィルタの通
過域特性が乱れ、大きなリップルが生ずる。これに対し
て、本発明のよ5に圧電fI勅子の共振周波数を入力側
から順に高(なるように配列を行うと通過域が乱れずに
各圧電振動子を厳密に調整した場合と全く同等の特性を
得ることができる。また本発明の原理から圧電振動子を
入力側からその共振周波数が順に減少するように配列し
ても実施例1.と同等の効果が得られることは明らかで
ある。
As is clear from the above examples, piezoelectric vibrators with 5 different frequencies are randomly placed! [If combined, the passband characteristics of the filter will be disturbed and large ripples will occur. On the other hand, if the resonant frequency of the piezoelectric vibrator is arranged so that it increases in order from the input side as in the present invention, the passband will not be disturbed and it will be completely different from the case where each piezoelectric vibrator is precisely adjusted. It is clear that the same effect as in Example 1 can be obtained from the principle of the present invention even if the piezoelectric vibrators are arranged so that their resonant frequencies decrease in order from the input side. be.

〔実施例2〕     、。[Example 2].

実施例1と同じ9個の圧電振動子と8個の容量からなる
梯子蓋フィルタの実施例である。実態lでは菖3図にお
いてfi動子1.〜a、の並列容量 が中央部分の振動
子12〜〜のそれぞれの並列容量のl。
This is an example of a ladder lid filter consisting of the same nine piezoelectric vibrators and eight capacitors as in Example 1. In reality l, in the irises 3 diagram, fi mover 1. The parallel capacitance of ~a is l of the parallel capacitance of each of the vibrators 12 ~ in the central portion.

2倍となっていたが、実施例2ではすべての振動子の並
列容量e、容量比α、共振尖鋭度(が実施例1の振動子
へ〜1.と全く同じである。
However, in Example 2, the parallel capacitance e, capacitance ratio α, and resonance sharpness (1) of all the vibrators are exactly the same as those of the vibrator in Example 1.

実施例2において、フィルタの入力側から出力側にかげ
て振動子を新たKa、、a、、−−一・、〜とし各共振
周波数の設定を第4図の如く行った。ここでフィルタに
組み込める振動子の共振周波数は557.90〜560
.60−まで2−7−の範囲にあり、しかも振動子は同
一形状で実現できるわもすであるからこの場合には全く
周波数調整の必要はない。製造した圧電振動子を300
 Hz毎に選別する周波数選別機Kかげて分類し、組み
込むだけで良いのである。
In Example 2, the oscillators were changed from the input side to the output side of the filter, and the resonant frequencies were set as shown in FIG. 4. Here, the resonant frequency of the vibrator that can be incorporated into the filter is 557.90 to 560.
.. 60- to 2-7-, and since the vibrator can be realized with the same shape, there is no need for frequency adjustment in this case. 300 manufactured piezoelectric vibrators
All that is required is to classify and incorporate a frequency sorter K that sorts by Hz.

このときの通過域動作減衰量特性をjI6図に示す。第
5図に示した本発明の実施例IK比べてf・±3.5k
Hz付近に小さなリップルが生じ【いる他は良好な特性
が得られていることがわかる。また、この程度のリップ
ルであれば一般に(例えば群搬供フィルタのようK)全
く問題にならないことが多い。
The passband operation attenuation characteristic at this time is shown in diagram jI6. f・±3.5k compared to the embodiment IK of the present invention shown in FIG.
It can be seen that other than a small ripple occurring around Hz, good characteristics are obtained. Further, ripples of this level generally do not pose a problem at all (for example, in a group carrier filter).

〔実施例3〕 実施例1及び2では圧電振動子の周波数分類数が9種類
であった。
[Example 3] In Examples 1 and 2, the number of frequency classifications of the piezoelectric vibrator was nine.

ここでは、$7図に示すように9個の圧電振動子と8個
の容量からなる構成で、圧電振動子を入j力側から順に
町1”*9”ly・・・・・・v m’sとする。そし
【、第8図に示すように共振周波数の設定を入力側から
次第に高くしていき、中央の振動子1.で最高の周波数
を設定し−〜〜にかげて今度は逆に次第に低く設定して
いく。振動子a、と1.は実施例1と同様に中央部分の
振動子a、〜a、の並列容量の2倍となりており、 a
;と、z、、Sとaz、  atと、;、<とべは同一
の周波数範囲に設定し、各周波数範囲を実施例1,20
倍の600)h毎にとりた。
Here, as shown in Figure 7, the configuration consists of 9 piezoelectric vibrators and 8 capacitors, and the piezoelectric vibrators are connected in order from the input side to 1"*9"ly...v Let's say m's. Then, as shown in FIG. 8, the resonance frequency setting is gradually increased from the input side, and the center vibrator 1. Set the highest frequency, and then gradually set it lower. vibrator a, and 1. As in Example 1, is twice the parallel capacitance of the central vibrators a, ~a, and a
;, z,, S, az, at, ;, <tobe are set to the same frequency range, and each frequency range is set to the same frequency range as in Examples 1 and 20.
The sample was taken every 600 hours.

このときの動作減衰量特性な籐9図に実線で示す。尚点
線は実施例1で示した影像パラメータ設計の特性である
。従って、実施例3を適用することにより実施例1に比
べ共振周波数の差の大きな圧電振動子を隣接させ【構成
しても良特性のフィルタが実現でき実施例1と同様に周
波数調整が必要なのは両端の振動子息r8とa−だげで
あり、中央部分の振動子4〜a%はこの必要がない。ま
た、実施例3の構成で9個の圧電振動子をすべて同じ並
列容量を持つものを用いても動作減衰量特性は良好であ
り、大きなリップルは現われない。
The operational attenuation characteristics at this time are shown in solid lines in Figure 9. Note that the dotted line is the characteristic of the image parameter design shown in the first embodiment. Therefore, by applying Embodiment 3, a filter with good characteristics can be realized even if piezoelectric vibrators with a large difference in resonance frequency are placed adjacent to each other compared to Embodiment 1. This is not necessary for the oscillators 4 to a% in the center, as the oscillators at both ends are separated by r8 and a-. Furthermore, even if all nine piezoelectric vibrators have the same parallel capacitance in the configuration of Example 3, the operation attenuation characteristics are good and large ripples do not appear.

さらにこの実施例において圧電振動子なその共振周波数
が11から願に減少するようK a/、で最小にし、a
%からInk増加するように配置しても良好な特性が得
られることは本発明のJ[J!から明らかである。さら
にこれらの振動子の配列中において最大あるいは最小の
共振周波数を持つ圧電振動子がフィルタ内の全圧電振動
子の配列の中央に位置する必要はなく、その位置が入力
側あるいは出力側に片寄っていても設計が多少難しくな
るほかは動作減衰量特性はほば同等のものが得られる。
Further, in this embodiment, the resonance frequency of the piezoelectric vibrator is minimized by Ka/, so that the resonance frequency is decreased from 11 to 1, and a
The J[J! It is clear from this. Furthermore, the piezoelectric vibrator with the maximum or minimum resonant frequency in the array of these vibrators does not have to be located in the center of the array of all piezoelectric vibrators in the filter, and its position may be biased toward the input side or output side. However, the operational attenuation characteristics are almost the same, except that the design is somewhat more difficult.

以上の実施例はフィルタの入力側及び出力側が共に1端
の場合について述べ友が、第10図に示すよ5に入力側
、出力側がともにπ端である梯子歴圧電フィルタにも、
第uIllで示すように入力側あるいは出力側のいずれ
か一方が1端で他方はぎ端であるような梯子搬圧電フィ
ルタにも本発明がそのまま適用できることは言うまでも
ない。
The above embodiments have been described for the case where both the input side and the output side of the filter are one end, but as shown in FIG.
It goes without saying that the present invention can also be applied as is to a ladder-carried piezoelectric filter in which either the input side or the output side is one end and the other is a stripped end, as shown in No. uIll.

なお、本発明のフィルタにおいて並列の位置に配置され
る結合容量は設計値から±5−程度のバラツキは許され
る。またフィルタKI!求される規格値によっては、こ
の結合容量のバラツキや圧電振動子の選別幅な実施例の
値より大きくすることができることは明らかである。
In addition, in the filter of the present invention, the coupling capacitances arranged in parallel positions are allowed to vary by about ±5- from the designed value. Filter KI again! It is clear that depending on the required standard value, the variation in coupling capacitance and the selection range of piezoelectric vibrators can be made larger than the values in the embodiments.

以上詳述した如く本発明に従えば、梯子型圧電フィルタ
に組み込む圧電振動子の周波数範囲をかなり広い範囲ま
で許すことができる。
As detailed above, according to the present invention, the frequency range of the piezoelectric vibrator incorporated in the ladder-type piezoelectric filter can be allowed to be quite wide.

従って、本発明に従えば圧電振動子の周波数特性調整の
工程を省略して圧電フィルタが製造可能となりその工業
的価値は極めて大きいものがある。
Therefore, according to the present invention, a piezoelectric filter can be manufactured without the step of adjusting the frequency characteristics of a piezoelectric vibrator, and its industrial value is extremely large.

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

絡1図は直列腕及び並列腕に各々圧電振動子を配置した
梯子屋圧電フィルタな示す。 籐2図は直列腕に圧電振動子、並列腕に容量を配置した
高安定形梯子聾圧電フィルタ。 第3図は実施例の梯子産圧電フィルタの構成、84図は
本発明の実施例に従った振動子の周波数設定を示す図で
ある。 第5図の実線はフィルタの通過域特性を示す。 第6図は、本発明の実施例のフィルタの通過域特性であ
る。第7図は本発明の実施例における梯子屋フィルタの
構成であり、#E8図はその周波数第10図は人、出力
端がともにπ端である梯子臘圧電フィルタ、第11図は
、入力あるいは出力側のいずれか一方がT端で、他方か
に端である梯子型圧電フイ〃りの構成を示す。 図において、11 、12 、ム1@4p〜、・・・−
g AIL−IAla、、 a、、 &、、 a4. 
a、、 a、 a、、 a、、 a、、 a、。 al、畠、、 a4. l、、 l、、 a、、 a、
、 IL、は圧電振動子、CIt C,、C,# +−
・・−* c、−ffi、 c、−1,cは容量を示す
。 第1 図 °) 楽乙図 卒B図 準5 図 −6−4−2几    子2    す4    +4
闇 渡 叡 (充H,) 嘉ム図 −6−4−2ム    +?    す4−   +ろ
R弓  シベ乙  壇ルニ  ((リイ乙)亮 q 区 −ろ   −4−2f、    +;l     十4
   −+6m5!I己0  (イトH乙) 歪ち lO図
Figure 1 shows a ladder piezoelectric filter in which piezoelectric vibrators are arranged in each of the series arm and the parallel arm. Figure 2 shows a highly stable ladder deaf piezoelectric filter with a piezoelectric vibrator in the series arm and a capacitor in the parallel arm. FIG. 3 is a diagram showing the configuration of the ladder-type piezoelectric filter according to the embodiment, and FIG. 84 is a diagram showing the frequency setting of the vibrator according to the embodiment of the present invention. The solid line in FIG. 5 shows the passband characteristics of the filter. FIG. 6 shows the passband characteristics of the filter according to the embodiment of the present invention. FIG. 7 shows the configuration of a ladder filter in an embodiment of the present invention. This figure shows the configuration of a ladder-type piezoelectric fiber in which one of the output sides is a T end and the other is a right end. In the figure, 11, 12, mu1@4p~,...-
g AIL-IAla, a, &, a4.
a,, a, a,, a,, a,, a,. al, Hatake,, a4. l,, l,, a,, a,
, IL, is a piezoelectric vibrator, CIt C,, C, # +-
...-*c, -ffi, c, -1, c indicates capacity. Figure 1 °) Raku-otzu Graduation B Standard 5 Figure-6-4-2 几子2 Su4 +4
Yami Wataru Akira (Mitsuru H,) Kamu Figure -6-4-2mu +? Su4- +RoR Bow Shibeotsu Danruni ((Riiiot) Ryo q Ku-ro -4-2f, +;l 14
-+6m5! I Self 0 (It H Otsu) Distortion lO figure

Claims (2)

【特許請求の範囲】[Claims] (1)  直列腕に圧電振動子、並列腕に容量を配置し
た梯子型圧電フィルタにおい″C%前記圧電振動子をそ
の共振周波数が入力端から出力端にかげて順に増加する
ように配置するか、あるいは順に減少するように配置す
ることを特徴とする梯子型圧電フィルタ。
(1) In a ladder-type piezoelectric filter in which a piezoelectric vibrator is placed in a series arm and a capacitor is placed in a parallel arm, is the piezoelectric vibrator arranged so that its resonant frequency increases in order from the input end to the output end? , or a ladder-type piezoelectric filter characterized in that the filters are arranged in decreasing order.
(2)直列腕に圧電振動子、並列腕に容量を配置した梯
子型圧電フィルタにおいて、前記圧電振動子をその共振
・周波数が入力端から順に増加して行き、途中から逆に
願に減少して〜1くように配置するか、あるいは入力端
からJ[k減少していき途中から逆KIIIK増加して
いくように配置することを特徴とする梯子型圧電フィル
タ。
(2) In a ladder-type piezoelectric filter in which a piezoelectric vibrator is placed in the series arm and a capacitor is placed in the parallel arm, the resonance/frequency of the piezoelectric vibrator increases sequentially from the input end and decreases in the opposite direction. A ladder-type piezoelectric filter characterized in that it is arranged so that J[k decreases from the input end and increases inversely KIIIK from the middle.
JP2921182A 1982-02-25 1982-02-25 Ladder type piezoelectric filter Pending JPS58146122A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2921182A JPS58146122A (en) 1982-02-25 1982-02-25 Ladder type piezoelectric filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2921182A JPS58146122A (en) 1982-02-25 1982-02-25 Ladder type piezoelectric filter

Publications (1)

Publication Number Publication Date
JPS58146122A true JPS58146122A (en) 1983-08-31

Family

ID=12269851

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2921182A Pending JPS58146122A (en) 1982-02-25 1982-02-25 Ladder type piezoelectric filter

Country Status (1)

Country Link
JP (1) JPS58146122A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5291159A (en) * 1992-07-20 1994-03-01 Westinghouse Electric Corp. Acoustic resonator filter with electrically variable center frequency and bandwidth

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5291159A (en) * 1992-07-20 1994-03-01 Westinghouse Electric Corp. Acoustic resonator filter with electrically variable center frequency and bandwidth

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