JPH03220906A - Crystal oscillator - Google Patents
Crystal oscillatorInfo
- Publication number
- JPH03220906A JPH03220906A JP1643590A JP1643590A JPH03220906A JP H03220906 A JPH03220906 A JP H03220906A JP 1643590 A JP1643590 A JP 1643590A JP 1643590 A JP1643590 A JP 1643590A JP H03220906 A JPH03220906 A JP H03220906A
- Authority
- JP
- Japan
- Prior art keywords
- crystal
- inverter
- resistor
- output
- current flowing
- 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
Landscapes
- Oscillators With Electromechanical Resonators (AREA)
Abstract
Description
【発明の詳細な説明】
(発明の技術分野)
本発明は、動作が安定で正弦波状の出力波形を得ること
ができる水晶発振器に関する。DETAILED DESCRIPTION OF THE INVENTION (Technical Field of the Invention) The present invention relates to a crystal oscillator that operates stably and can obtain a sinusoidal output waveform.
(発明の技術的背景とその問題点)
従来第4図に示すようなインバータを用いた水晶発振回
路が多用されている。すなわちインバーところで近時、
特に半導体素子の性能向上が著しく高速動作の可能なデ
バイスが普及しつつある。(Technical background of the invention and its problems) Conventionally, a crystal oscillation circuit using an inverter as shown in FIG. 4 has been widely used. In other words, recently, invar
In particular, the performance of semiconductor elements has been significantly improved, and devices capable of high-speed operation are becoming widespread.
しかしてこのような高速動作の可能なデバイスを用いて
第4図に示すような水晶発振回路を製作すると、水晶振
動子に対する駆動レベルが大きすぎて過大な水晶電流が
流れる。このため、たとえば特性が飛躍するジャンプ現
象等を呈する問題があった。However, if a crystal oscillator circuit as shown in FIG. 4 is manufactured using such a device capable of high-speed operation, the drive level for the crystal resonator is too high and an excessive crystal current flows. For this reason, there is a problem in that, for example, a jump phenomenon occurs in which the characteristics jump.
(発明の目的)
本発明は、上記の事情に鑑みてなされたもので、安定な
正弦波状の水晶電流波形を得ることができる温度特性の
ジャンプもない水晶発振器を提供することを目的とする
ものである。(Object of the Invention) The present invention has been made in view of the above circumstances, and an object of the present invention is to provide a crystal oscillator that can obtain a stable sinusoidal crystal current waveform and has no jump in temperature characteristics. It is.
(発明の概要)
本発明は、インバータの入出力間に水晶振動子を接続し
た発振回路において、インバータの出力に水晶振動子を
流れる水晶電流を制限する抵抗を直列に介挿したこと特
徴とするものである。(Summary of the Invention) The present invention is characterized in that, in an oscillation circuit in which a crystal resonator is connected between the input and output of an inverter, a resistor is inserted in series at the output of the inverter to limit the crystal current flowing through the crystal resonator. It is something.
(実施例)
以下、本発明の一実施例を、第1図に示すブロック図を
参照して詳細に説明する。(Example) Hereinafter, an example of the present invention will be described in detail with reference to the block diagram shown in FIG.
図中11はインバータで、この人力と出力の間に水晶振
動子12及び帰還抵抗13を接続している。この帰還抵
抗13の値は水晶振動子12の周波数によって異なるが
一般に数百にΩないし数MΩである。そして、インバー
タ11の人力及び出力をそれぞれコンデンサ14.15
て接地している。このコンデンサ14.15の値も数P
Fないし百数十PFである。そして、インバータ11の
出力に水晶振動子12を流れる水晶電流を制限する抵抗
16を介挿している。この抵抗16の値は数百Ωないし
十数にΩで水晶振動子12を流れる水晶電流を適当な値
に調整する。In the figure, 11 is an inverter, and a crystal oscillator 12 and a feedback resistor 13 are connected between this human power and the output. The value of this feedback resistor 13 varies depending on the frequency of the crystal resonator 12, but is generally several hundred ohms to several Mohms. Then, the human power and output of the inverter 11 are connected to capacitors 14 and 15, respectively.
It is grounded. The value of this capacitor 14.15 is also several P
F to a hundred and several tens of PF. A resistor 16 is inserted into the output of the inverter 11 to limit the crystal current flowing through the crystal resonator 12. The value of this resistor 16 is from several hundred Ω to several tens of Ω, and adjusts the crystal current flowing through the crystal resonator 12 to an appropriate value.
このような構成であれば、インバータ11に高速動作の
ものを用いても水晶振動子12を流れる電流を抵抗16
によって制限することができ、たとえは第2図に示すよ
うに高調波の成分を含まず歪のない正弦波状の水晶電流
波形を得ることができる。With such a configuration, even if a high-speed operation type is used as the inverter 11, the current flowing through the crystal resonator 12 can be controlled by the resistor 16.
For example, as shown in FIG. 2, a sinusoidal crystal current waveform containing no harmonic components and no distortion can be obtained.
したがって、温度特性にジャンプ等を生しることもなく
、特に温度変化に応して周波数を一定値に維持するよう
に補償する温度補償発振器において良好な特性を得られ
る。Therefore, there is no jump or the like in the temperature characteristics, and good characteristics can be obtained especially in a temperature compensated oscillator that compensates to maintain the frequency at a constant value in response to temperature changes.
なお、上記実施例のようにインバータの出力に抵抗16
を介挿すると第3図に示す周波数と負性抵抗値の関係を
示すグラフのように、負性抵抗を示す領域を低周波数域
に移動させることができる。In addition, as in the above embodiment, a resistor 16 is connected to the output of the inverter.
By inserting , it is possible to move the region exhibiting negative resistance to a lower frequency region, as shown in the graph showing the relationship between frequency and negative resistance value shown in FIG.
すなわち第3図において曲線Aは第4図に示すような従
来の発振回路における負性抵抗の特性である。そして曲
線Bは抵抗16として比較的小さな抵抗値のものを介挿
した時の特性、曲線Cは抵抗16として比較的大きな抵
抗値のものを介挿した時の特性である。すなわち抵抗1
6として比較的大きな抵抗値のものをインバータ11の
出力に介挿すれば発振回路は高い周波数の負性抵抗を抑
圧し、それによってオーバートーンの共振を抑圧して基
本波周波数の発振出力を確実に得ることができる。That is, in FIG. 3, curve A is the characteristic of negative resistance in a conventional oscillation circuit as shown in FIG. Curve B shows the characteristics when a resistor 16 with a relatively small resistance value is inserted, and curve C shows the characteristics when a resistor 16 with a relatively large resistance value is inserted. i.e. resistance 1
By inserting a relatively large resistance value as 6 into the output of the inverter 11, the oscillation circuit suppresses the negative resistance at high frequencies, thereby suppressing overtone resonance and ensuring the oscillation output at the fundamental frequency. can be obtained.
なお、本発明は上記実施例に限定されるものではなく、
たとえは上記実施例ではコンデンサ14.15は固定コ
ンデンサとして説明したが、その−方または両方を電圧
容量変換素子として、その印加電圧を制御して温度補償
を行うものにも適用することができることは勿論である
。Note that the present invention is not limited to the above embodiments,
For example, in the above embodiment, the capacitors 14 and 15 were explained as fixed capacitors, but it is also possible to use one or both of them as voltage-capacitance conversion elements to control the applied voltage and perform temperature compensation. Of course.
(発明の効果)
以上詳述したように、本発明によれは安定な正弦波状の
水晶電流波形を得られ温度特性のジャンプもなく特に温
度補償に適する水晶発振器を提供することができる。(Effects of the Invention) As detailed above, according to the present invention, it is possible to provide a crystal oscillator which can obtain a stable sinusoidal crystal current waveform and is particularly suitable for temperature compensation without jumps in temperature characteristics.
第1図は本発明の一実施例を示すブロック図、第2図は
本発明の上記実施例の水晶電流波形を示す図、
第3図は本発明の周波数と負性抵抗との関係を示す図、
第4図は従来の水晶発振器の一例を示すブロック図、
第5図は従来の水晶発振器の水晶電流波形の一例を示す
図である。
1 l ・
l 2 ・
l 3 ・
14、
l 6 ・
・・・インバータ
・・・水晶振動子
・・・帰還抵抗
15・コンデンサ
・・・抵抗
′:A212]
第3閏
集4回
第5図FIG. 1 is a block diagram showing one embodiment of the present invention, FIG. 2 is a diagram showing the crystal current waveform of the above embodiment of the present invention, and FIG. 3 is a diagram showing the relationship between frequency and negative resistance of the present invention. 4 is a block diagram showing an example of a conventional crystal oscillator, and FIG. 5 is a diagram showing an example of a crystal current waveform of the conventional crystal oscillator. 1 l ・ l 2 ・ l 3 ・ 14, l 6 ・ ... Inverter ... Crystal oscillator ... Feedback resistor 15, Capacitor ... Resistor': A212] 3rd Leap Collection 4th Figure 5
Claims (1)
において、 上記インバータの出力に上記水晶振動子を流れる水晶電
流を制限する抵抗を直列に介挿したことを特徴とする水
晶発振器。[Scope of Claims] An oscillation circuit in which a crystal resonator is connected between the input and output of an inverter, characterized in that a resistor is inserted in series to the output of the inverter to limit the crystal current flowing through the crystal resonator. crystal oscillator.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1643590A JPH03220906A (en) | 1990-01-26 | 1990-01-26 | Crystal oscillator |
| US07/644,614 US5081431A (en) | 1990-01-26 | 1991-01-23 | Digital temperature-compensated oscillator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1643590A JPH03220906A (en) | 1990-01-26 | 1990-01-26 | Crystal oscillator |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH03220906A true JPH03220906A (en) | 1991-09-30 |
Family
ID=11916156
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1643590A Pending JPH03220906A (en) | 1990-01-26 | 1990-01-26 | Crystal oscillator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH03220906A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2005168066A (en) * | 2002-01-11 | 2005-06-23 | Piedekku Gijutsu Kenkyusho:Kk | Electronic equipment |
-
1990
- 1990-01-26 JP JP1643590A patent/JPH03220906A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2005168066A (en) * | 2002-01-11 | 2005-06-23 | Piedekku Gijutsu Kenkyusho:Kk | Electronic equipment |
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