JPH02268509A - Oscillator - Google Patents

Oscillator

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Publication number
JPH02268509A
JPH02268509A JP9103989A JP9103989A JPH02268509A JP H02268509 A JPH02268509 A JP H02268509A JP 9103989 A JP9103989 A JP 9103989A JP 9103989 A JP9103989 A JP 9103989A JP H02268509 A JPH02268509 A JP H02268509A
Authority
JP
Japan
Prior art keywords
conductive
capacitor
transistors
anode
transistor
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
JP9103989A
Other languages
Japanese (ja)
Inventor
Kazumi Narita
成田 一省
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP9103989A priority Critical patent/JPH02268509A/en
Publication of JPH02268509A publication Critical patent/JPH02268509A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To prevent oscillation from being stopped by cutting off a current on a resistor connected to the anode of a programmable unijunction transistor with an oscillation output signal. CONSTITUTION:The oscillation can be obtained by energizing the programmable unijunction transistors P1 and P2 alternately. Assuming that the energized states between the anodes A and cathodes K of the programmable unijunction transistors P1 and P2 are set accidentally, transistors Q1 and Q2 are energized, and transistors Q3 and Q4 are de-energized, and no power source Vs is applied on both resistors R1 and R2. In such a way, a state where the power source of a multivibrator is applied can be set again, which restarts an oscillation process.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は商品名プログラマブル・ユニジャンクション・
トランジスタ(以後PUTと称する)あるいはダブルベ
ース・ダイオードを使った発振器(マルチバイブレータ
)に関する。
[Detailed Description of the Invention] (Industrial Application Field) The present invention is based on the product name Programmable Unijunction.
It relates to an oscillator (multivibrator) using a transistor (hereinafter referred to as PUT) or a double base diode.

(従来技術および問題点) 第2図はPUTを使ったマルチバイブレータの回路構成
を示す。図のマルチバイブレータは、PUT、P、とP
UT、Plが交互に充電用コンデンサCの電流を放電し
て発振する。即ち、まず抵抗器R1からコンデンサCに
充電されたとすると、PUT、Plのゲート電位で定ま
るしきい値でPUT、P、がコンデンサCの電荷を放電
してPUT、P□のアノード・カソード間が導通状態と
なり、次に抵抗器R2からコンデンサCが充電されて、
PUT、Plのゲート電位で定まるしきい値でPUT、
PlがコンデンサCの電荷を放電してPUT、Plのア
ノード・カソード間が導通状態となり、次に抵抗器R□
からコンデンサCが充電されてPUT、P□がコンデン
サCの電荷を放電する。この課程がPUT、P’、とP
lの間で交互に繰り返されて図の回路は発振する。
(Prior Art and Problems) FIG. 2 shows the circuit configuration of a multivibrator using PUT. The multivibrators in the figure are PUT, P, and P
UT and Pl alternately discharge the current of the charging capacitor C and oscillate. That is, if capacitor C is first charged from resistor R1, PUT, P discharges the charge of capacitor C at a threshold value determined by the gate potential of PUT, Pl, and the voltage between the anode and cathode of PUT, P□ becomes It becomes conductive, and then capacitor C is charged from resistor R2,
PUT, PUT at the threshold determined by the gate potential of Pl,
Pl discharges the charge of capacitor C, PUT becomes conductive between the anode and cathode of Pl, and then resistor R□
Capacitor C is charged from PUT and P□ discharges the charge of capacitor C. This process is PUT, P', and P
The circuit shown in the figure oscillates by alternating between 1 and 1.

しかしながら、図の回路は、PUT、PtとPlの両方
のアノード・カソード間が誤って導通状態になると、コ
ンデンサCの両方の端子がアース電位となって発振が停
止してしまう。
However, in the circuit shown in the figure, if the anode and cathode of PUT and both Pt and Pl are accidentally brought into conduction, both terminals of the capacitor C become ground potential and oscillation stops.

く本発明の解決手段) このため、本発明では、PUTのアノード・カソード間
が導通状態になったとき、そのアノードに接続される充
電抵抗器の電流を強制的に遮断する構成としている。
Therefore, in the present invention, when the anode and cathode of the PUT become conductive, the current of the charging resistor connected to the anode is forcibly cut off.

(作用) この構成とすることによって、万一2つのPUTのアノ
ード・カソード間が共に導通状態になった場合、2つの
PUTのアノード電流は共に遮断されるので、改めてマ
ルチバイブレータ電源が投入された状態と等しい状態と
なって発振過程が再開される。
(Function) With this configuration, if the anodes and cathodes of two PUTs become conductive, the anode currents of both PUTs will be cut off, so the multivibrator power can be turned on again. The oscillation process is restarted with a state equal to the state.

(実施例) 第1図は、本発明の実施例を示す回路図で、V5は電源
、R1、PzはPUT、Cはコンデンサ、Ri、Rxは
コンデンサCを充電するために、PUT、P、、Pzの
アノードに接続されたアノード抵抗、R3、R1とR5
、R6は夫々PUT、P□とPzのゲート電位を定める
ための抵抗、Ql、Q2は夫々PUT、P、、Pzのカ
ソード電流がベースに流れると導通するトランジスタ、
R7、R8は夫々トランジスタQ、、Q2のコレクタ抵
抗、Q3、Q、は夫々トランジスタQ□、Q、が導通状
態にない時に導通し、導通状態になったら非導通となる
トランジスタである。
(Embodiment) Fig. 1 is a circuit diagram showing an embodiment of the present invention, in which V5 is a power supply, R1, Pz are PUT, C is a capacitor, Ri and Rx are PUT, P, , anode resistors connected to the anodes of Pz, R3, R1 and R5
, R6 are resistors for determining the gate potentials of PUT, P□ and Pz, respectively, Ql and Q2 are transistors that become conductive when the cathode current of PUT, P, , Pz flows to their bases, respectively.
R7 and R8 are collector resistors of transistors Q, Q2, respectively, and Q3 and Q are transistors that are conductive when transistors Q□ and Q, respectively, are not conductive, and are nonconductive when they are conductive.

次に第1図の回路の発振動作を説明する。電源vsが印
加されてこれが立ち上がる時トランジスタQ1、Q4は
導通状態にあるから、抵抗R1、R2には該電源電圧v
3が印加される。今、PUT、P□のアノード・カソー
ド間が導通したとすると、トランジスタQ1にベース電
流が供給されて導通し、このためにトランジスタQ、が
非導通となる。
Next, the oscillation operation of the circuit shown in FIG. 1 will be explained. Since the transistors Q1 and Q4 are in a conductive state when the power supply voltage V is applied and rises, the power supply voltage V is applied to the resistors R1 and R2.
3 is applied. Now, if the anode and cathode of PUT and P□ become conductive, a base current is supplied to the transistor Q1 and the transistor Q1 becomes conductive, so that the transistor Q becomes non-conductive.

そして、PUT、P□のアノード・カソード間が導通し
ている間、コンデンサCにはトランジスタQ4のコレク
タ・エミッタ間と抵抗R2を介して充電電流が流れ、こ
の電流はPUT、P□のアノード・カソード間が導通状
態にある間流れ続ける。
While the anodes and cathodes of PUT and P□ are conducting, a charging current flows through the capacitor C between the collector and emitter of transistor Q4 and through resistor R2, and this current flows between the anodes and cathodes of PUT and P□. The flow continues as long as there is continuity between the cathodes.

このコンデンサCの電位(PUT、P、のアノード電位
)が抵抗R6、R6で定まるPUT、Pzのゲート電位
を越えると、PUT、P、のアノード・カソード間が導
通し、トランジスタQ、のベース・エミッタ間を介して
、コンデンサCの電荷が放電される。この放電電流はト
ランジスタQλを導通状態にして、トランジスタQ、を
非導通状態とするために、抵抗R2の電流が遮断される
。同時に、この放電電流はトランジスタQ、のベース・
エミッタ間およびPUT、P□のアノード・カソード間
に負電位を与えるので、PUT、P□のアノード・カソ
ード間が非導通状態となると共に、トランジスタQ、が
非導通状態になるので、トランジスタQ3が導通して抵
抗R1に該電源電位Vsが印加される。この電圧の印加
によって抵抗R1、コンデンサC,PUT、P2のアノ
ード・カソード間、およびトランジスタQ2のベース・
エミッタ間を経由してコンデンサCの充電電流が流れる
When the potential of this capacitor C (anode potential of PUT, P) exceeds the gate potential of PUT, Pz determined by resistors R6 and R6, conduction occurs between the anode and cathode of PUT, P, and the base of transistor Q The charge on the capacitor C is discharged across the emitters. This discharge current makes the transistor Qλ conductive and the transistor Q non-conductive, so that the current flowing through the resistor R2 is cut off. At the same time, this discharge current flows through the base of transistor Q.
Since a negative potential is applied between the emitters and between the anodes and cathodes of PUT and P□, the anodes and cathodes of PUT and P□ become non-conductive, and transistor Q becomes non-conductive, so transistor Q3 becomes non-conductive. It becomes conductive and the power supply potential Vs is applied to the resistor R1. By applying this voltage, the voltage between the anode and cathode of resistor R1, capacitor C, PUT, and P2, and the base and
The charging current of capacitor C flows through the emitter.

そして、コンデンサCの端子電圧(P U T 、 P
 Iのアノード電位)が、抵抗R1、R4で定まるPU
T、P、のゲート電位を越えると、PUT、Pzのアノ
ード・カソード間およびトランジスタQ□のベース・エ
ミッタ間を介してコンデンサCの放電電流が流れる。
Then, the terminal voltage of capacitor C (P UT , P
PU whose anode potential) is determined by resistors R1 and R4
When the gate potential of T and P is exceeded, the discharge current of capacitor C flows between the anode and cathode of PUT and Pz and between the base and emitter of transistor Q□.

この放電電流はトランジスタQ□を導通状態にしてトラ
ンジスタQ、を非導通状態にし、抵抗R1の電源印加を
遮断すると共に、PUT、Pzのアノード・カソード間
およびトランジスタQ2のベース・エミッタ間に負の電
位を与えて、PUT、Pzを非導通の状態にする。
This discharge current makes transistor Q□ conductive and transistor Q non-conductive, cuts off the power supply to resistor R1, and creates a negative voltage between the anode and cathode of PUT and Pz and between the base and emitter of transistor Q2. Apply a potential to make PUT and Pz non-conductive.

このようにPUT、P、とPzが交互に導通することに
よって、第1図の回路は発振する。
The circuit of FIG. 1 oscillates because PUT, P, and Pz are alternately conductive in this way.

ここで、もし、PUT、P、とP、のアノード。Here, if PUT, P, and the anode of P.

カソード間が誤って共に導通状態になったとすると、ト
ランジスタQ□、Q、共導通状態になってトランジスタ
Q1、Q4共に非導通状態になり、抵抗R,,R2共に
電源■5が印加されない。このため、PUT、PIとP
、のアノード・カソード間は導通状態を続けることがで
きず、非導通となって、改めて上の発振過程を繰り返す
ことができる。
If the cathodes are erroneously made conductive, the transistors Q□ and Q become conductive, and both the transistors Q1 and Q4 become non-conductive, and the power source 5 is not applied to both the resistors R and R2. For this reason, PUT, PI and P
The anode and cathode of , cannot continue to be electrically conductive, and become non-conductive, allowing the above oscillation process to be repeated again.

(発明の効果) 本発明の発振器によれば、万一、マルチバイブレータを
構成する2つのPUTのアノード・カソード間が共に導
通状態になって、発振できない状態になっても、アノー
ド・カソード間を流れる電流が遮断され、再び発振でき
る状態を作り出すことができ、発振は再開される。
(Effects of the Invention) According to the oscillator of the present invention, even if the anodes and cathodes of two PUTs constituting a multivibrator become conductive and become unable to oscillate, The flowing current is cut off, creating a state in which oscillation is possible again, and oscillation is restarted.

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

第1図は本発明の実施例を示す回路図、第2図は従来技
術を説明するための回路図である。 Pl、Pi・・PUT (ダブルベースダイオード)Q
l、Q4・・トランジスタ R1、R2・・抵抗 C・・・・・・コンデンサ 第1図
FIG. 1 is a circuit diagram showing an embodiment of the present invention, and FIG. 2 is a circuit diagram for explaining the prior art. Pl, Pi...PUT (double base diode) Q
l, Q4...Transistor R1, R2...Resistor C...Capacitor Fig. 1

Claims (1)

【特許請求の範囲】[Claims] 各々電源とアース間に接続されたゲート抵抗を持ち、カ
ソードをアース側電位とする2つのPUT、P_1、P
_2と、該2つのPUTのアノード間に接続されている
コンデンサCと、該コンデンサCを充電するために、該
2つのPUT、P_1、P_2の各々アノードに接続さ
れる充電用抵抗器R_1、R_2と、該2つのPUTの
アノードに接続される抵抗器R_1、R_2を流れる電
流を、発振出力信号で遮断する手段とからなるPUT発
振器。
Two PUTs, P_1 and P, each with a gate resistor connected between the power supply and ground, and with the cathode at ground side potential.
_2, a capacitor C connected between the anodes of the two PUTs, and charging resistors R_1 and R_2 connected to the anodes of the two PUTs P_1 and P_2 to charge the capacitor C, respectively. and means for interrupting current flowing through resistors R_1 and R_2 connected to the anodes of the two PUTs using an oscillation output signal.
JP9103989A 1989-04-11 1989-04-11 Oscillator Pending JPH02268509A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9103989A JPH02268509A (en) 1989-04-11 1989-04-11 Oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9103989A JPH02268509A (en) 1989-04-11 1989-04-11 Oscillator

Publications (1)

Publication Number Publication Date
JPH02268509A true JPH02268509A (en) 1990-11-02

Family

ID=14015363

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9103989A Pending JPH02268509A (en) 1989-04-11 1989-04-11 Oscillator

Country Status (1)

Country Link
JP (1) JPH02268509A (en)

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