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JPS5814767B2 - Rejector circuit - Google Patents
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JPS5814767B2 - Rejector circuit - Google Patents

Rejector circuit

Info

Publication number
JPS5814767B2
JPS5814767B2 JP12322077A JP12322077A JPS5814767B2 JP S5814767 B2 JPS5814767 B2 JP S5814767B2 JP 12322077 A JP12322077 A JP 12322077A JP 12322077 A JP12322077 A JP 12322077A JP S5814767 B2 JPS5814767 B2 JP S5814767B2
Authority
JP
Japan
Prior art keywords
circuit
resonant frequency
rejector
sub
series arm
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
Application number
JP12322077A
Other languages
Japanese (ja)
Other versions
JPS5456749A (en
Inventor
奥田信也
角石光夫
吉川征
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP12322077A priority Critical patent/JPS5814767B2/en
Publication of JPS5456749A publication Critical patent/JPS5456749A/en
Publication of JPS5814767B2 publication Critical patent/JPS5814767B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic elements; Electromechanical resonators
    • H03H9/46Filters
    • H03H9/54Filters comprising resonators of piezoelectric or electrostrictive material
    • H03H9/542Filters 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)
  • Filters And Equalizers (AREA)

Description

【発明の詳細な説明】 本発明は振動素子に副共振が存在することによる特性劣
化を軽減したリジエクタ回路に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a resistor circuit that reduces characteristic deterioration due to the presence of sub-resonance in a vibrating element.

一般に信号伝送装置において、特定周波数成分を伝送さ
せないように水晶振動子または機械振動子を用いたリジ
エクタ回路が使用されている。
Generally, in signal transmission devices, a rejector circuit using a crystal resonator or a mechanical resonator is used so as not to transmit a specific frequency component.

第1図はこの種回路を示すブロック構成図で、直列腕を
形成する回路のインピーダンスをZA,並列腕を形成す
る回路のインピーダンスをZBとすると、従来のZA,
ZBは共に2次回路網となっている。
FIG. 1 is a block configuration diagram showing this type of circuit. If the impedance of the circuit forming the series arm is ZA, and the impedance of the circuit forming the parallel arm is ZB, then the conventional ZA,
Both ZBs are secondary circuit networks.

またZA−ZB−R2(たrLRは回路の特性インピー
ダンス)を満足している。
It also satisfies ZA-ZB-R2 (rLR is the characteristic impedance of the circuit).

従来のリジエクタ回路で水晶振動子XOを使用すると、
主共振周波数foに対し約1.1倍の所に最大副共振周
波数が存在することが多い。
When using a crystal oscillator XO in a conventional rejector circuit,
The maximum sub-resonant frequency often exists at about 1.1 times the main resonant frequency fo.

そのためリジエクタ回路の損失特性は第2図に示すよう
になる。
Therefore, the loss characteristics of the rejector circuit are as shown in FIG.

即ち副共振周波数においてリジエクタ回路の特性が大い
に劣化している。
That is, the characteristics of the resistor circuit are greatly degraded at the sub-resonant frequency.

第3図は水晶振動子の等価回路図を示し、Lo,co,
Roは主共振周波数foに対する値でfQ=1/2π■
の 関係にあり、LS,CS,RSは副共振周波数fsに対
する値でfs=1/2π■の関 係にある。
Figure 3 shows an equivalent circuit diagram of a crystal resonator, with Lo, co,
Ro is the value for the main resonant frequency fo, fQ=1/2π■
LS, CS, and RS have a relationship of fs=1/2π■ with respect to the subresonant frequency fs.

また等価抵抗ROの値が小さい程第2図の主共振周波数
foにおける減衰量が大となり、また等価インダクタン
スLoが小さい程減衰曲線の帯域が広い範囲で減衰量が
大となることが知られている。
It is also known that the smaller the value of the equivalent resistance RO, the greater the attenuation at the main resonant frequency fo shown in Figure 2, and the smaller the equivalent inductance Lo, the greater the attenuation in a wider range of the attenuation curve. There is.

そして副共振周波数fSにおける等価抵抗RSは大きい
程リジエクタとしては望ましい特性となることが判り、
従来この希望を満すため第1図に破線で示すように副共
振周波数が互いに少しずつ異なる複数の水晶振動子を並
列接続していた。
It was also found that the larger the equivalent resistance RS at the sub-resonant frequency fS, the more desirable the characteristics for the resistor.
Conventionally, in order to satisfy this desire, a plurality of crystal resonators having subresonant frequencies slightly different from each other were connected in parallel, as shown by the broken lines in FIG.

そのため主共振周波数fQにおける等価抵抗Roは総合
的に1個の値の略並列接続個数分の一に減少するので、
リジエクタ回路の特性は良好になるが、水晶振動子の選
別と接続後の調整が複雑となり、回路は大型化し且つ高
価になった。
Therefore, the equivalent resistance Ro at the main resonant frequency fQ is reduced to one value approximately divided by the number of parallel connections.
Although the characteristics of the resistor circuit were improved, selection of the crystal resonator and adjustment after connection became complicated, making the circuit larger and more expensive.

本発明は簡易な構成の回路を使用して調整が容易で且つ
特性の良好なリジエクタ回路を得ることを目白勺とする
The aim of the present invention is to obtain a resistor circuit that is easy to adjust and has good characteristics using a circuit with a simple configuration.

以下図面に示す本発明の実施例について説明する。Embodiments of the present invention shown in the drawings will be described below.

第4図に示す回路図において、直列腕、並列腕中1点鎖
線で囲んだ部分が各腕をそれぞれ4次全域通過回路網と
するため付加したインダクタンス素子・容量素子を示す
In the circuit diagram shown in FIG. 4, the parts surrounded by one-dot chain lines in the series and parallel arms indicate inductance elements and capacitance elements added to make each arm a fourth-order all-pass circuit network.

そして付加した素子による共振周波数を第2図における
副共振周波数fSに一致させ、且つ |ZA(fo)l>|ZA(fS)| となるよう素子の値を選定する。
Then, the values of the elements are selected so that the resonant frequency of the added element matches the sub-resonant frequency fS in FIG. 2 and that |ZA(fo)l>|ZA(fS)|.

たゞしZA(fo)は主共振周波数fOにおける直列腕
のインピーダンス、ZA(fs)は副共振周波数fsに
おける直列腕のインピーダンスを示す。
ZA(fo) indicates the impedance of the series arm at the main resonant frequency fO, and ZA(fs) indicates the impedance of the series arm at the sub-resonant frequency fs.

第5図に直列腕インピーダンスZAの総合周波数特性を
示す。
FIG. 5 shows the overall frequency characteristics of the series arm impedance ZA.

第5図から判るようにZAの次数は4次で零点と極が2
次の場合より各1個多くなっている。
As can be seen from Figure 5, the order of ZA is 4th, with 2 zeros and 2 poles.
There are one more each than in the following cases.

fo,fs附近の曲線勾配が急であるため両者の減衰量
に大きな差が生じ、リジエクタ回路として副共振の影響
が少なくなる。
Since the slopes of the curves near fo and fs are steep, there is a large difference in the amount of attenuation between the two, which reduces the influence of sub-resonance as a rejector circuit.

特に|ZA(fo)|が大きい程広帯域に亘り大きな減
衰量の得られることが計算の結果判明しているので、前
述の素子の選定を行なえばより良い効果が得られる。
In particular, it has been found from calculations that the larger |ZA(fo)|, the greater the attenuation over a wider band can be obtained, so better effects can be obtained by selecting the above-mentioned elements.

このようにして本発明によれば構成が簡易で調整が容易
で且つ特性が良好な回路を安価に得ることができる。
In this way, according to the present invention, a circuit with a simple configuration, easy adjustment, and good characteristics can be obtained at low cost.

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

第1図は従来のリジエクタ回路を示す図、第2図は第1
図の損失特性を示す図、第3図は水晶振動子の等価回路
図、第4図は本発明実施例を示す図、第5図はインピー
ダンスZAの周波数特性を示す図である。 XO・・・・・・水晶振動子。
Figure 1 shows a conventional resistor circuit, and Figure 2 shows a conventional resistor circuit.
3 is an equivalent circuit diagram of a crystal resonator, FIG. 4 is a diagram showing an embodiment of the present invention, and FIG. 5 is a diagram showing frequency characteristics of impedance ZA. XO...Crystal oscillator.

Claims (1)

【特許請求の範囲】[Claims] 1 全域通過回路網の直列腕に振動素子を接続し該振動
素子の共振周波数を阻止域としたリジエクタ回路におい
て、前記直列腕及び並列腕にインダクタンス素子・容量
素子の組合せ回路を更に付加し、振動素子を除く直列腕
及び並列腕をそれぞれ4次全域通過回路網とし、付加し
た回路の共振周波数を振動素子の副共振周波数としたこ
とを特徴とするリジエクタ回路。
1. In a rejector circuit in which a resonant element is connected to the series arm of the all-pass circuit network and the resonant frequency of the resonant element is used as a stop band, a combination circuit of an inductance element and a capacitance element is further added to the series arm and the parallel arm, and vibration 1. A rejector circuit characterized in that the series arm and the parallel arm excluding the element are each made into a fourth-order all-pass circuit network, and the resonant frequency of the added circuit is set as the sub-resonant frequency of the vibrating element.
JP12322077A 1977-10-14 1977-10-14 Rejector circuit Expired JPS5814767B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12322077A JPS5814767B2 (en) 1977-10-14 1977-10-14 Rejector circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12322077A JPS5814767B2 (en) 1977-10-14 1977-10-14 Rejector circuit

Publications (2)

Publication Number Publication Date
JPS5456749A JPS5456749A (en) 1979-05-08
JPS5814767B2 true JPS5814767B2 (en) 1983-03-22

Family

ID=14855164

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12322077A Expired JPS5814767B2 (en) 1977-10-14 1977-10-14 Rejector circuit

Country Status (1)

Country Link
JP (1) JPS5814767B2 (en)

Also Published As

Publication number Publication date
JPS5456749A (en) 1979-05-08

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