JPS61118001A - Crystal oscillation circuit - Google Patents

Crystal oscillation circuit

Info

Publication number
JPS61118001A
JPS61118001A JP23990784A JP23990784A JPS61118001A JP S61118001 A JPS61118001 A JP S61118001A JP 23990784 A JP23990784 A JP 23990784A JP 23990784 A JP23990784 A JP 23990784A JP S61118001 A JPS61118001 A JP S61118001A
Authority
JP
Japan
Prior art keywords
capacitance
emitter
capacitor
base
ambient temperature
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
JP23990784A
Other languages
Japanese (ja)
Inventor
Kazuhiro Honda
和博 本田
Toshio Abiko
安彦 利夫
Kuniharu Katazuki
堅月 邦治
Hiroshi Umeyama
梅山 寛
Minoru Kanda
実 神田
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.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works 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 Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP23990784A priority Critical patent/JPS61118001A/en
Publication of JPS61118001A publication Critical patent/JPS61118001A/en
Pending legal-status Critical Current

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  • Oscillators With Electromechanical Resonators (AREA)

Abstract

PURPOSE:To prevent fluctuation of an oscillating frequency against the change in ambient temperature by connecting a capacitive element having a temperature characteristic cancelling temperature change of a capacitance between an emitter and a base of an oscillation transistor (TR) between the emitter and base. CONSTITUTION:The capacitive element C having an opposite temperature characteristic to that of the emitter-base capacitance of the oscillation TR Q against ambient temperature is connected between the base and emitter. The capacitive element C consists of the 1st capacitor C1, the 2nd capacitor C2, a variable capacitor V, a thermister T and a resistor R. When ambient temperature rises, the resistance value of the thermister T is decreased and a voltage impressed to the variable capacitor V is lowered, then the capacitance of the variable capacitor V is decreased, resulting that the capacitance in a series circuit comprising the 1st capacitor C1, the 2nd capacitor C2 and the variable capacitor V is reduced, and the capacitance change in the series circuit is cancelled together with the emitter-base capacitance of the oscillation TR Q.

Description

【発明の詳細な説明】 [技術分野1 本発明は水晶発振回路、さらに詳しくは、水晶発振回路
において周囲温度の変化に対して発振周波数を安定化す
る技術に関す今ものである。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field 1] The present invention relates to a crystal oscillation circuit, and more particularly, to a technique for stabilizing the oscillation frequency against changes in ambient temperature in a crystal oscillation circuit.

[背景技術1 −1に第2図に示すようなエミッタホロワ形の水晶発振
回路において、エミッタ、ベース間容量は周囲温度が上
昇するとともに第3図のように比例して増大するもので
あり、このため水晶振動子Xに対する発振用トランジス
タQIllの負荷容量が変化することになり、1)14
図に示すように、周囲温度の上昇に伴なって発振周波数
が低下するという問題がある。したがって、水晶振動子
Xに温度安定性のよいものを用いても周囲温度の変化に
伴なって発振周波数が変動するものである。
[Background Art 1-1 In an emitter-follower type crystal oscillator circuit as shown in Fig. 2, the capacitance between the emitter and the base increases proportionally as the ambient temperature rises, as shown in Fig. 3. Therefore, the load capacitance of the oscillation transistor QIll with respect to the crystal resonator X changes, and 1) 14
As shown in the figure, there is a problem in that the oscillation frequency decreases as the ambient temperature increases. Therefore, even if a crystal resonator X with good temperature stability is used, the oscillation frequency will fluctuate as the ambient temperature changes.

[発明の目的1 本発明は上述の点に鑑みて為されたものであって、その
主な目的とするところは、発振用トランジスタのエミッ
タ、ベース間容量の温度特性を相殺する容量素子を発振
用トランジスタのエミ4り。
[Objective of the Invention 1 The present invention has been made in view of the above points, and its main purpose is to oscillate a capacitive element that cancels the temperature characteristics of the capacitance between the emitter and base of an oscillating transistor. Emitter 4 of the transistor for use.

ベース間に接続することにより、周囲温度が変化しても
発振周波数が変動しない水晶発振回路を提供することに
ある。
An object of the present invention is to provide a crystal oscillation circuit in which the oscillation frequency does not change even if the ambient temperature changes by connecting between the bases.

(発明の開示1 (実施例) 以下、本発明の実施例を図面に基づいて説明する0本実
施例においては第2図に示すように無調整回路に適用し
た例を示すが、二へに限定されるものではなく、ビアー
λ回路等の水晶発振回路にも適用でこるものである。
(Disclosure of the Invention 1 (Example) Examples of the present invention will be described below based on the drawings. In this example, an example in which the present invention is applied to a non-adjustable circuit as shown in FIG. 2 will be described. The invention is not limited to this, and can also be applied to crystal oscillation circuits such as via λ circuits.

第2図に示すものは水晶振動子Xを備えrこ通常の無f
14整回路であって、同調回路を持たない水晶発振回路
である。この発振用トランツスタQのエミー/夕、ベー
ス間のコンデンサC0に代えて第1図に示すように、発
振用トランクスりQのエミッタ、ベース間容量の周囲温
度に対する変化と逆の温度特性を有した容量素子Cが接
続される。容量素子Cは第1のコンデンサC1、第2の
コンデンサC2、バリキャップV、サーミスタT、抵抗
Rにより構成さ八る。第1のコンデンサC1と、バリキ
ャップ■と、第2のコンデンサC2とは直列接aされ、
この直列回路が発振用1ランノスタQのエミッタ、ベー
ス間に挿入される。バリキャップ■にはサーミスタTと
抵抗Rとを抵抗Rを高圧量に接続して構r&された分圧
回路の出力電圧が印加さ八る。しかして、周囲温度が上
昇すると、サーミスタTの抵抗値が減少し、バリキャッ
プVへの印加電圧が低下するから、バリキャップ■の容
量が低下し、その結果、第1のコンデンサC,と第2の
コンデンサC2とバリキャップVとの直列回路の容量が
減少するらのであり、この直列回路の容量変化と発振用
Yランノ入りQのエミッタ、ベース間容量の変化とが相
殺することになる。すなわち、水晶発振子Xからみた負
荷容量は周囲温度が変化しても略一定値を保つことにな
り、発振周波数が安定するのである。ここで第1のコン
デンサC1と第2のコンデンサC,とは比較的容量の大
きなものが用いられ、バリキャップVを直流的1こ切り
離す上う(こしている。
The one shown in Figure 2 is equipped with a crystal oscillator
This is a crystal oscillation circuit that is a 14-channel rectifier circuit and does not have a tuning circuit. In place of the capacitor C0 between the emitter and the base of the oscillating transistor Q, as shown in Figure 1, a capacitor C0 having a temperature characteristic opposite to the change in the capacitance between the emitter and the base of the oscillating trunk Q with respect to the ambient temperature is used. Capacitive element C is connected. The capacitive element C is composed of a first capacitor C1, a second capacitor C2, a varicap V, a thermistor T, and a resistor R. The first capacitor C1, the varicap ■, and the second capacitor C2 are connected in series a,
This series circuit is inserted between the emitter and base of one oscillating runnostar Q. The output voltage of a voltage dividing circuit constructed by connecting a thermistor T and a resistor R to a high voltage is applied to the varicap (2). However, when the ambient temperature rises, the resistance value of the thermistor T decreases, and the voltage applied to the varicap V decreases, resulting in a decrease in the capacitance of the varicap The capacitance of the series circuit of the capacitor C2 and the varicap V of 2 is reduced, and the change in capacitance of this series circuit is offset by the change in the capacitance between the emitter and the base of the oscillating Y runno input Q. In other words, the load capacitance seen from the crystal oscillator X maintains a substantially constant value even if the ambient temperature changes, and the oscillation frequency is stabilized. Here, the first capacitor C1 and the second capacitor C have relatively large capacitances, and serve to isolate the varicap V by a single direct current.

[発明の効果J 本発明は上述のように、発振用トランクスりのエミッタ
、ベース間にエミッタ、ベースMtif!、の温度変化
を相殺する温度特性を有した容量素子を接続したので、
発振用トランツスタのエミッタ、ベース間の周囲温度に
対する容量変化が相殺され、周囲温度の変化に対して発
振周波数が変動しないという利点を有するものである。
[Effect of the Invention J] As described above, the present invention provides an emitter between the emitter and the base of the oscillation trunk, and the base Mtif! Since we connected a capacitive element with temperature characteristics that offset the temperature change of ,
This has the advantage that capacitance changes between the emitter and base of the oscillation transistor due to ambient temperature are canceled out, and the oscillation frequency does not vary with changes in ambient temperature.

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

第1図は本発明の一実施例を示す要部回路図、第2図は
本発明に係る水晶発振回路の一例を示す回路図、第3図
は発振用トランジスタの温度−容量特性を有する動作説
明図、tA4図は周囲温度に対士る発振周波数の変化を
示す動作説明図である。 Cは容量素子、C1、C2はコンデンサ、Tはサーミス
タ、■はバリキャップ、Xは水晶振動子である。
FIG. 1 is a circuit diagram of a main part showing an embodiment of the present invention, FIG. 2 is a circuit diagram showing an example of a crystal oscillation circuit according to the present invention, and FIG. 3 is an operation having temperature-capacitance characteristics of an oscillation transistor. The explanatory diagram, tA4, is an operation explanatory diagram showing changes in oscillation frequency with respect to ambient temperature. C is a capacitive element, C1 and C2 are capacitors, T is a thermistor, ■ is a varicap, and X is a crystal resonator.

Claims (1)

【特許請求の範囲】[Claims] (1)エミッタホロワ形の水晶発振回路において、発振
用トランジスタのエミッタ、ベース間にエミッタ、ベー
ス間容量の温度変化を相殺する温度特性を有した容量素
子を接続して成ることを特徴とする水晶発振回路。
(1) In an emitter follower type crystal oscillation circuit, a crystal oscillation circuit is characterized in that a capacitive element having temperature characteristics that cancels temperature changes in the capacitance between the emitter and the base is connected between the emitter and the base of the oscillation transistor. circuit.
JP23990784A 1984-11-14 1984-11-14 Crystal oscillation circuit Pending JPS61118001A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23990784A JPS61118001A (en) 1984-11-14 1984-11-14 Crystal oscillation circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23990784A JPS61118001A (en) 1984-11-14 1984-11-14 Crystal oscillation circuit

Publications (1)

Publication Number Publication Date
JPS61118001A true JPS61118001A (en) 1986-06-05

Family

ID=17051623

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23990784A Pending JPS61118001A (en) 1984-11-14 1984-11-14 Crystal oscillation circuit

Country Status (1)

Country Link
JP (1) JPS61118001A (en)

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