JP2002290152A - Voltage-controlled oscillator - Google Patents
Voltage-controlled oscillatorInfo
- Publication number
- JP2002290152A JP2002290152A JP2001093747A JP2001093747A JP2002290152A JP 2002290152 A JP2002290152 A JP 2002290152A JP 2001093747 A JP2001093747 A JP 2001093747A JP 2001093747 A JP2001093747 A JP 2001093747A JP 2002290152 A JP2002290152 A JP 2002290152A
- Authority
- JP
- Japan
- Prior art keywords
- voltage
- variable capacitance
- capacitance element
- controlled oscillator
- control voltage
- 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)
- Inductance-Capacitance Distribution Constants And Capacitance-Resistance Oscillators (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は電圧制御発振器を産
業上の技術分野とし、特に電圧可変容量素子に起因した
制御電圧Vcに対する周波数特性の非直線性を改善した
電圧制御発振器に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a voltage controlled oscillator as an industrial technical field, and more particularly to a voltage controlled oscillator having improved non-linear frequency characteristics with respect to a control voltage Vc caused by a voltage variable capacitor.
【0002】[0002]
【従来の技術】(発明の背景)電圧制御発振器はPLL
(PHASE LOCKED LOOP)回路や発振回路の温度補償機構
等に使用され、制御電圧Vcによって発振周波数を可変
するものとして知られている。通常では、発振閉ループ
に挿入された電圧可変容量素子に制御電圧Vcを印加し
て、端子間の容量変化によって発振周波数を可変する。
近年では、電圧可変容量素子による発振回路の制御電圧
−周波数特性の直線性を良好にしたものが望まれてい
る。2. Description of the Related Art A voltage controlled oscillator is a PLL.
(PHASE LOCKED LOOP) It is used as a temperature compensating mechanism of an oscillation circuit or the like, and is known to vary an oscillation frequency by a control voltage Vc. Normally, the control voltage Vc is applied to the voltage variable capacitance element inserted in the oscillation closed loop, and the oscillation frequency is varied by a change in capacitance between terminals.
In recent years, it has been desired to improve the linearity of a control voltage-frequency characteristic of an oscillation circuit using a voltage variable capacitance element.
【0003】(従来技術の一例)第4図は一従来例を説
明する電圧制御発振器の回路図である。電圧制御発振器
は、発振回路の閉ループ内に電圧可変容量素子1を挿入
してなる。発振回路は、例えばインダクタ成分とした水
晶振動子2とコンデンサ3及び電圧可変容量素子1から
共振回路を形成する。そして、水晶振動子2に並列接続
した帰還抵抗4を有するインバータ増幅素子5によって
共振周波数を帰還増幅する。電圧可変容量素子1はバリ
キャップダイオード(可変容量ダイオード1Aとする)
からなる。符号6は高周波阻止抵抗、同7は直流阻止コ
ンデンサである。FIG. 4 is a circuit diagram of a voltage controlled oscillator for explaining a conventional example. The voltage controlled oscillator has a voltage variable capacitance element 1 inserted in a closed loop of an oscillation circuit. The oscillation circuit forms a resonance circuit from, for example, the crystal resonator 2 having an inductor component, the capacitor 3, and the voltage variable capacitance element 1. Then, the resonance frequency is feedback-amplified by the inverter amplifying element 5 having the feedback resistor 4 connected in parallel to the crystal resonator 2. The voltage variable capacitance element 1 is a varicap diode (variable capacitance diode 1A)
Consists of Reference numeral 6 denotes a high-frequency blocking resistor, and reference numeral 7 denotes a DC blocking capacitor.
【0004】このようなものでは、高周波阻止抵抗6を
経て、可変容量ダイオード1Aに逆電圧となる制御電圧
Vcを印加すると、可変容量ダイオード1Aの端子間の
容量が変化する。したがって、水晶振動子2の両端子か
ら見た回路側の直列等価容量(所謂水晶振動子2の負荷
容量)が変化するので、発振周波数が変化する。In such a device, when a control voltage Vc, which is a reverse voltage, is applied to the variable capacitance diode 1A via the high-frequency blocking resistor 6, the capacitance between the terminals of the variable capacitance diode 1A changes. Accordingly, the series equivalent capacitance on the circuit side as viewed from both terminals of the crystal unit 2 (the so-called load capacitance of the crystal unit 2) changes, so that the oscillation frequency changes.
【0005】[0005]
【発明が解決しようとする課題】しかしながら、上記構
成の電圧制御発振器では、可変容量ダイオード1Aの電
圧−容量特性は、第5図に示したように制御電圧Vcに
対して指数関数的に容量が減少する。このため、制御電
圧Vcに対する発振周波数の周波数特性は直線的にはな
らず、非直線的になる。すなわち、制御電圧Vcに対し
て指数関数的に発振周波数が増加する特性となり(第6
図)、多くの場合は、制御電圧Vcの増加に従い発振周
波数fの制御電圧Vcに対する感度df/dVcが減少す
る。これにより、発振周波数を制御しにくく、設計を複
雑にする。However, in the voltage controlled oscillator having the above structure, the voltage-capacitance characteristic of the variable capacitance diode 1A has an exponentially increasing capacitance with respect to the control voltage Vc as shown in FIG. Decrease. For this reason, the frequency characteristic of the oscillation frequency with respect to the control voltage Vc is not linear but non-linear. In other words, the oscillation frequency increases exponentially with respect to the control voltage Vc (the sixth characteristic).
In many cases, the sensitivity df / dVc of the oscillation frequency f to the control voltage Vc decreases as the control voltage Vc increases. This makes it difficult to control the oscillation frequency and complicates the design.
【0006】特に、温度補償機構(発振器)に適用した
場合には、温度変化に対して制御電圧(温度補償電圧)
Vcが変化するが、可変容量ダイオード1Aによる非直
線性によって制御感度(Δf/V)も変化する。また、
自動周波数制御(AFC)回路によるAFC電圧を可変
容量ダイオード1Aに共用して印加する場合には、AF
C電圧による制御感度も変化する。In particular, when applied to a temperature compensating mechanism (oscillator), a control voltage (temperature compensating voltage) is applied to a temperature change.
Although Vc changes, the control sensitivity (Δf / V) also changes due to the non-linearity of the variable capacitance diode 1A. Also,
When the AFC voltage by the automatic frequency control (AFC) circuit is applied to the variable capacitance diode 1A in common, the AF
The control sensitivity by the C voltage also changes.
【0007】これらのことから、温度補償電圧及びAF
C電圧が相互に重畳して、非線形部分での独立的な制御
を困難にし、補償後の周波数温度特性を悪化させる問題
があった。特に、小電力化においては、可変容量ダイオ
ードの低域側での非直線性が問題となる。[0007] From these, the temperature compensation voltage and AF
There is a problem that the C voltages are superimposed on each other, making it difficult to perform independent control in the non-linear portion, and deteriorating the frequency temperature characteristics after compensation. In particular, in reducing the power, non-linearity of the variable capacitance diode on the low frequency side becomes a problem.
【0008】(発明の目的)本発明は、制御電圧に対す
る周波数変化特性の非直線性を改善した電圧制御発振器
を提供することを目的とする。(Object of the Invention) An object of the present invention is to provide a voltage controlled oscillator in which the nonlinearity of a frequency change characteristic with respect to a control voltage is improved.
【0009】[0009]
【課題を解決するための手段】(着目点)本発明では、
制御電圧Vcに対する周波数特性の非直線性は、可変容
量ダイオードの電圧−容量特性が非直線的であることに
起因することから、制御電圧Vcを補正制御電圧(補正
電圧とする)Vc′に変換し、結果として制御電圧Vcに
対する周波数特性に直線性を持たせる点に着目した。Means for Solving the Problems (Points of Interest) In the present invention,
The non-linearity of the frequency characteristic with respect to the control voltage Vc is caused by the non-linearity of the voltage-capacitance characteristic of the variable capacitance diode. As a result, attention has been paid to the point that the frequency characteristic with respect to the control voltage Vc has linearity.
【0010】(解決手段)本発明は、電圧可変容量素子
の端子間に定電圧源(電圧E)、ダイオード及び抵抗の
直列回路を接続して、制御電圧Vcを電圧可変容量素子
と直列回路の接続点に印加したことを基本的な解決手段
とする。(Solution) According to the present invention, a series circuit of a constant voltage source (voltage E), a diode and a resistor is connected between terminals of a voltage variable capacitance element to control a control voltage Vc of the voltage variable capacitance element and the series circuit. The application to the connection point is a basic solution.
【0011】[0011]
【作用】本発明では、定電圧源(電圧E)、ダイオード
及び抵抗による直列回路の端子間に高周波阻止抵抗を経
て制御電圧Vcが印加されると、直列回路の端子間電圧
即ち補正電圧Vc′は、次になる。すなわち、ダイオー
ドには印加電圧が約0.7V以下では殆ど電流は流れず、
0.7V以上になると指数関数的に電流が増大する。した
がって、制御電圧VcがE−0.7(V)以下になると補正
電圧Vc′は指数関数的に減少する。これらのことか
ら、制御電圧Vcは直線的でも補正電圧Vc′をE−0.7
(V)以下で曲線的にするので、補正電圧Vc′が印加
される可変容量ダイオードの電圧−容量特性及び周波数
特性を直線的にする。以下、本発明の一実施例を説明す
る。According to the present invention, when a control voltage Vc is applied between the terminals of a series circuit composed of a constant voltage source (voltage E), a diode and a resistor via a high-frequency blocking resistor, the voltage between the terminals of the series circuit, that is, the correction voltage Vc '. Becomes That is, almost no current flows through the diode when the applied voltage is about 0.7 V or less,
When the voltage exceeds 0.7 V, the current increases exponentially. Therefore, when the control voltage Vc falls below E-0.7 (V), the correction voltage Vc 'decreases exponentially. From these facts, even if the control voltage Vc is linear, the correction voltage Vc 'is changed to E-0.7.
(V) Since the curve is formed below, the voltage-capacitance characteristic and the frequency characteristic of the variable capacitance diode to which the correction voltage Vc 'is applied are linearized. Hereinafter, an embodiment of the present invention will be described.
【0012】[0012]
【実施例】第1図は本発明の一実施例を説明する電圧制
御発振器の回路図である。なお、前従来例図と同一部分
には同番号を付与してその説明は簡略又は省略する。電
圧制御発振器は、前述したように、水晶振動子1、電圧
可変容量素子1(可変容量ダイオード1A)、コンデン
サ3(ab)、及び帰還抵抗4を有するインバータ増幅
素子5からなる。なお、符号6は高周波阻止抵抗、同7
は直流阻止抵抗である。FIG. 1 is a circuit diagram of a voltage controlled oscillator for explaining an embodiment of the present invention. The same parts as those in the prior art are denoted by the same reference numerals, and description thereof will be simplified or omitted. As described above, the voltage controlled oscillator includes the crystal resonator 1, the voltage variable capacitance element 1 (variable capacitance diode 1A), the capacitor 3 (ab), and the inverter amplification element 5 having the feedback resistor 4. Reference numeral 6 denotes a high-frequency blocking resistor, and reference numeral 7 denotes
Is a DC blocking resistance.
【0013】そして、この実施例では、可変容量ダイオ
ード1Aの端子間即ちカソードとアース電位との間に、
アース側から定電圧源(電圧E)8、ダイオード9及び
抵抗10とした直列回路11を接続してなる。In this embodiment, between the terminals of the variable capacitance diode 1A, that is, between the cathode and the ground potential.
A constant voltage source (voltage E) 8, a diode 9, and a series circuit 11 including a resistor 10 are connected from the ground side.
【0014】このようなものでは、制御電圧Vcが高周
波阻止抵抗6を経て直列回路11に印加されると、直列
回路11の端子間電圧Vc′は次になる。すなわち、制
御電圧VcがE−0.7(V)以上では、ダイオード9の端
子間に加わる電圧は0.7V以下となり、要するにカソー
ドの電位が高くなって電流は殆ど流れず、Vc′≒Vcと
なる。In such a circuit, when the control voltage Vc is applied to the series circuit 11 via the high-frequency blocking resistor 6, the voltage Vc 'between terminals of the series circuit 11 becomes as follows. That is, when the control voltage Vc is equal to or higher than E-0.7 (V), the voltage applied between the terminals of the diode 9 is equal to or lower than 0.7 V, that is, the potential of the cathode is increased and almost no current flows, and Vc '≒ Vc.
【0015】制御電圧VcがE−0.7(V)以下ではアノ
ードの電位が高くなってダイオード9に電流が流れ、V
c′>Vcとなる。そして、ダイオード9の端子間電圧が
0.7V以上になると、指数関数的に電流が増大する。し
たがって、制御電圧VcがE−0.7(V)以下になってダ
イオード9の端子間電圧が0.7V以上になると、指数関
数的に電流が増大して端子間電圧(補正電圧)Vc′は
指数関数的に減少する。When the control voltage Vc is equal to or lower than E-0.7 (V), the potential of the anode becomes high, and a current flows through the diode 9;
c ′> Vc. And the voltage between the terminals of the diode 9 is
When the voltage exceeds 0.7 V, the current increases exponentially. Therefore, when the control voltage Vc falls below E-0.7 (V) and the voltage between the terminals of the diode 9 becomes 0.7 V or more, the current increases exponentially and the terminal voltage (correction voltage) Vc 'becomes an exponential function. Decrease.
【0016】Vc=0では、高周波阻止抵抗6の抵抗値
をR1、直列回路11での抵抗10の抵抗値をR2とする
と、Vc′=(E−0.7)R2/(R1+R2)(V)とな
る。したがって、第2図に示したように、高周波抵抗6
及び抵抗10の抵抗値R1及びR2によって補正電圧V
c′の下限値が設定され、制御電圧VcがE−0.7(V)
以下では端子間電圧Vc′は曲線的になる。但し、E−
0.7(V)以上では従来同様に直線的になる。When Vc = 0, assuming that the resistance of the high-frequency blocking resistor 6 is R1 and the resistance of the resistor 10 in the series circuit 11 is R2, Vc '= (E−0.7) R2 / (R1 + R2) (V). Become. Therefore, as shown in FIG.
And the resistance value R1 and R2 of the resistor 10, the correction voltage V
The lower limit value of c 'is set, and the control voltage Vc becomes E-0.7 (V).
Hereinafter, the inter-terminal voltage Vc 'becomes a curve. However, E-
Above 0.7 (V), it becomes linear as in the prior art.
【0017】そして、電圧可変容量素子1には、直列回
路11の端子間電圧Vc′即ち制御電圧Vcの補正電圧V
c′が印加される。補正電圧Vc′は前述のようにE−0.
7(V)以下では曲線的になる。A voltage Vc 'between terminals of the series circuit 11, ie, a correction voltage Vc of the control voltage Vc is applied to the voltage variable capacitance element 1.
c 'is applied. The correction voltage Vc 'is equal to E-0.
Below 7 (V), it is curved.
【0018】これらのことから、第3図に示したよう
に、制御電圧Vcに対する発振周波数fは、E−0.7
(V)以下の電圧領域では直線的になる。したがって、
制御電圧Vcに対する発振周波数fの変化特性を改善で
きる。特に、小電力化による電源電圧が小さくなるほど
(例えば2V以下)、その効果は大きい。From these facts, as shown in FIG. 3, the oscillation frequency f with respect to the control voltage Vc is E-0.7
(V) It becomes linear in the voltage range below. Therefore,
The change characteristic of the oscillation frequency f with respect to the control voltage Vc can be improved. In particular, as the power supply voltage due to the reduction in power becomes smaller (for example, 2 V or less), the effect becomes larger.
【0019】[0019]
【他の事項】上記実施例では、水晶振動子2と共振回路
を形成する一方のコンデンサを可変容量ダイオード1と
したが、他方のコンデンサ3も電圧可変容量素子1とし
て補正電圧Vc′を印加してもよい。また、電圧可変容
量素子1は可変容量ダイオード1Aとしたが、電圧に対
して端子間の容量が実質的に変化する半導体素子であれ
ば適用できる。[Other Matters] In the above embodiment, one of the capacitors forming the resonance circuit with the crystal resonator 2 is the variable capacitance diode 1. However, the other capacitor 3 is applied with the correction voltage Vc 'as the voltage variable capacitance element 1. You may. Further, the voltage variable capacitance element 1 is the variable capacitance diode 1A, but any semiconductor element whose capacitance between terminals substantially changes with respect to voltage can be applied.
【0020】[0020]
【発明の効果】本発明は、電圧可変容量素子の端子間に
定電圧源(電圧E)、ダイオード及び抵抗の直列回路を
接続して、制御電圧Vcを電圧可変容量素子と直列回路
の接続点に印加したので、制御電圧Vcに対する周波数
変化特性の非直線性を改善した電圧制御発振器を提供で
きる。According to the present invention, a series circuit of a constant voltage source (voltage E), a diode and a resistor is connected between terminals of a voltage variable capacitance element, and a control voltage Vc is applied to a connection point between the voltage variable capacitance element and the series circuit. Applied to the control voltage Vc, it is possible to provide a voltage controlled oscillator with improved non-linearity of the frequency change characteristic with respect to the control voltage Vc.
【図1】本発明の一実施例を説明する電圧制御発振器の
回路図である。FIG. 1 is a circuit diagram of a voltage-controlled oscillator illustrating one embodiment of the present invention.
【図2】本発明の一実施例を説明する制御電圧Vcに対
する補正電圧Vc′の特性図である。FIG. 2 is a characteristic diagram of a correction voltage Vc 'with respect to a control voltage Vc for explaining an embodiment of the present invention.
【図3】本発明の一実施例を説明する制御電圧に対する
発振周波数の変化特性図である。FIG. 3 is a graph showing a change characteristic of an oscillation frequency with respect to a control voltage for explaining an embodiment of the present invention;
【図4】従来例を説明する電圧制御発振器の回路図であ
る。FIG. 4 is a circuit diagram of a voltage controlled oscillator illustrating a conventional example.
【図5】従来例を説明する制御電圧に対する電圧可変容
量素子の容量特性図である。FIG. 5 is a diagram illustrating capacitance characteristics of a voltage variable capacitance element with respect to a control voltage for explaining a conventional example.
【図6】従来例を説明する制御電圧に対する発振周波数
の変化特性図である。FIG. 6 is a diagram illustrating a change characteristic of an oscillation frequency with respect to a control voltage for explaining a conventional example.
1 電圧可変容量素子、2 水晶振動子、3(ab)
分割コンデンサ、4帰還抵抗、5 インバータ増幅素
子、6 高周波阻止抵抗、7 直流阻止コンデンサ、8
定電圧源、9 ダイオード、10 抵抗、11 直列
回路.1 voltage variable capacitance element, 2 crystal oscillator, 3 (ab)
Divided capacitor, 4 feedback resistor, 5 inverter amplifying element, 6 high frequency blocking resistor, 7 DC blocking capacitor, 8
Constant voltage source, 9 diode, 10 resistor, 11 series circuit.
Claims (1)
を接続し、前記電圧可変容量素子に高周波阻止抵抗を経
て制御電圧を印加し、前記発振回路の発振周波数を制御
してなる電圧制御発振器において、前記電圧可変容量素
子の端子間に定電圧源、ダイオード及び抵抗の直列回路
を接続し、前記電圧可変容量素子と前記直列回路の接続
点に前記制御電圧を印加したことを特徴とする電圧制御
発振器。A voltage controlled oscillator comprising a voltage variable capacitance element connected in a closed loop of an oscillation circuit, a control voltage applied to the voltage variable capacitance element via a high-frequency blocking resistor, and an oscillation frequency of the oscillation circuit controlled. Wherein a series circuit of a constant voltage source, a diode, and a resistor is connected between terminals of the voltage variable capacitance element, and the control voltage is applied to a connection point between the voltage variable capacitance element and the series circuit. Controlled oscillator.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2001093747A JP2002290152A (en) | 2001-03-28 | 2001-03-28 | Voltage-controlled oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2001093747A JP2002290152A (en) | 2001-03-28 | 2001-03-28 | Voltage-controlled oscillator |
Publications (1)
Publication Number | Publication Date |
---|---|
JP2002290152A true JP2002290152A (en) | 2002-10-04 |
Family
ID=18948045
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2001093747A Pending JP2002290152A (en) | 2001-03-28 | 2001-03-28 | Voltage-controlled oscillator |
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Country | Link |
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JP (1) | JP2002290152A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7301412B2 (en) | 2005-03-29 | 2007-11-27 | Fujitsu Limited | Variable capacity circuit and control method of variable capacity circuit |
CN103973228A (en) * | 2014-04-18 | 2014-08-06 | 南京信息工程大学 | C wave band voltage-controlled oscillator |
-
2001
- 2001-03-28 JP JP2001093747A patent/JP2002290152A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7301412B2 (en) | 2005-03-29 | 2007-11-27 | Fujitsu Limited | Variable capacity circuit and control method of variable capacity circuit |
CN103973228A (en) * | 2014-04-18 | 2014-08-06 | 南京信息工程大学 | C wave band voltage-controlled oscillator |
CN103973228B (en) * | 2014-04-18 | 2016-08-17 | 南京信息工程大学 | A kind of C-band voltage controlled oscillator |
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