JPH0212752Y2 - - Google Patents

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Publication number
JPH0212752Y2
JPH0212752Y2 JP1983045220U JP4522083U JPH0212752Y2 JP H0212752 Y2 JPH0212752 Y2 JP H0212752Y2 JP 1983045220 U JP1983045220 U JP 1983045220U JP 4522083 U JP4522083 U JP 4522083U JP H0212752 Y2 JPH0212752 Y2 JP H0212752Y2
Authority
JP
Japan
Prior art keywords
circuit
constant
rectangular wave
pulse
output signal
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
JP1983045220U
Other languages
Japanese (ja)
Other versions
JPS59152827U (en
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 filed Critical
Priority to JP4522083U priority Critical patent/JPS59152827U/en
Publication of JPS59152827U publication Critical patent/JPS59152827U/en
Application granted granted Critical
Publication of JPH0212752Y2 publication Critical patent/JPH0212752Y2/ja
Granted legal-status Critical Current

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  • Pulse Circuits (AREA)

Description

【考案の詳細な説明】 本考案はサンプリング回路等で使用されるパル
ス発生回路に関する。
[Detailed Description of the Invention] The present invention relates to a pulse generation circuit used in a sampling circuit or the like.

従来から、短時間幅のパルスを発生させるため
にステツプリカバリダイオード(以下SRDと称
す)を利用したパルス発生回路がある(特開昭57
−118428号参照)。前記パルス発生回路において
は、矩形波入力信号のパルス幅が変動すると出力
パルスの電圧値が変動し又、周波数特性も劣化す
る。したがつて、これを防止するために、SRD
を飽和領域で使用しており、消費電力が極めて大
きいという欠点を有していた。
Conventionally, there has been a pulse generation circuit that uses a step recovery diode (hereinafter referred to as SRD) to generate short-time pulses (Japanese Patent Laid-Open No. 57
-Refer to No. 118428). In the pulse generating circuit, when the pulse width of the rectangular wave input signal fluctuates, the voltage value of the output pulse fluctuates and the frequency characteristics also deteriorate. Therefore, to prevent this, SRD
is used in the saturation region, and has the disadvantage of extremely high power consumption.

本考案は上記欠点に鑑みなされたもので、矩形
波入力信号を所定の波形に整形することにより、
矩形波入力信号のパルス幅変動の影響をなくし、
低消費電力且つ広帯域なパルス発生回路を提供す
ることを目的とする。
The present invention was developed in view of the above drawbacks, and by shaping the rectangular wave input signal into a predetermined waveform,
Eliminates the influence of pulse width fluctuations of square wave input signals,
The purpose of the present invention is to provide a pulse generation circuit with low power consumption and wide band.

本考案のパルス発生回路は矩形波入力信号を受
け、所定パルス幅の矩形波出力信号を出力する波
形整形回路と、SRDを有し前記矩形波出力信号
に応答してパルスを発生するパルス発生部とから
構成されている。
The pulse generation circuit of the present invention includes a waveform shaping circuit that receives a rectangular wave input signal and outputs a rectangular wave output signal with a predetermined pulse width, and a pulse generator that has an SRD and generates a pulse in response to the rectangular wave output signal. It is composed of.

以下本考案の実施例を用いて詳述する。 The present invention will be described in detail below using examples.

第1図は本考案のパルス発生回路の実施例を表
わすブロツク図である。
FIG. 1 is a block diagram showing an embodiment of the pulse generating circuit of the present invention.

第1図において、波形整形回路1はパルス発生
部2に接続されている。パルス発生部2は特開昭
57−118428号で開示されているパルス発生回路と
同様の回路で、定電圧源3、定電流源4、微分回
路5、SRD6で構成されている。このように構
成された第1図のパルス発生回路の動作を以下に
説明する。
In FIG. 1, a waveform shaping circuit 1 is connected to a pulse generator 2. In FIG. Pulse generator 2 is made by JP-A-Sho.
This circuit is similar to the pulse generating circuit disclosed in No. 57-118428, and is composed of a constant voltage source 3, a constant current source 4, a differentiating circuit 5, and an SRD 6. The operation of the pulse generating circuit shown in FIG. 1 constructed in this manner will be described below.

波形整形回路1は矩形波入力信号Viを波形整形
し、そのパルス幅を所定幅に変換した後、矩形波
出力信号V1を出力する。矩形波出力信号V1は定
電圧源3、定電流源4に導入される。定電圧源3
と定電流源4は相補的に動作する。例えば矩形波
出力信号V1が高レベルの時、定電流源4が動作
し、定電圧源3は動作を停止している。この場
合、SRD6には順方向に充電電流iCが流れる。矩
形波出力信号V1のパルス幅は一定なので、SRD
6の蓄積電荷は矩形波出力信号V1のパルス幅に
対応する値で一定となる。
The waveform shaping circuit 1 shapes the waveform of a rectangular wave input signal Vi , converts its pulse width into a predetermined width, and then outputs a rectangular wave output signal V1 . The rectangular wave output signal V 1 is introduced into a constant voltage source 3 and a constant current source 4 . Constant voltage source 3
and constant current source 4 operate complementarily. For example, when the rectangular wave output signal V1 is at a high level, the constant current source 4 operates, and the constant voltage source 3 stops operating. In this case, charging current i C flows in the SRD 6 in the forward direction. Since the pulse width of the square wave output signal V 1 is constant, SRD
The accumulated charge of 6 becomes constant at a value corresponding to the pulse width of the rectangular wave output signal V1 .

矩形波出力信号V1が低レベルの時には定電流
源4は動作を停止し、定電圧源3が動作する。こ
の時、SRD6の蓄積電荷は放電電流iDによつて放
電される。SRD6の両端電圧は微分回路5で微
分され、出力パルスV0が得られる。
When the rectangular wave output signal V1 is at a low level, the constant current source 4 stops operating, and the constant voltage source 3 operates. At this time, the accumulated charge in the SRD 6 is discharged by the discharge current iD . The voltage across the SRD 6 is differentiated by a differentiating circuit 5 to obtain an output pulse V 0 .

第2図は第1図の波形整形回路1の詳細回路図
である。第1図と同一部分には同一符号を付す。
FIG. 2 is a detailed circuit diagram of the waveform shaping circuit 1 of FIG. 1. The same parts as in FIG. 1 are given the same reference numerals.

第2図において、D−フリツプ・フロツプ7の
Q出力端子はコンデンサ9、可変抵抗器10およ
び反転回路8の入力部に接続されている。反転回
路8の出力部はD−フリツプ・フロツプ7のセツ
ト端子Sに接続されている。コンデンサ9の一端
は正電源(+Vcc)に接続され、他端は可変抵抗
器10に接続されている。コンデンサ9および可
変抵抗器10は時定数回路を構成している。又、
D−フリツプ・フロツプの端子Dは接地されてお
り、クロツク端子Cには矩形波入力信号Viが入力
されている。
In FIG. 2, the Q output terminal of the D-flip-flop 7 is connected to a capacitor 9, a variable resistor 10, and an input of an inverting circuit 8. The output of the inverting circuit 8 is connected to the set terminal S of the D-flip-flop 7. One end of the capacitor 9 is connected to a positive power supply (+Vcc), and the other end is connected to a variable resistor 10. Capacitor 9 and variable resistor 10 constitute a time constant circuit. or,
The terminal D of the D-flip-flop is grounded, and the clock terminal C receives a square wave input signal Vi .

第3図は、第2図の波形整形回路の動作説明図
である。以下、第2図、3図を参照しつつその動
作を説明する。
FIG. 3 is an explanatory diagram of the operation of the waveform shaping circuit of FIG. 2. The operation will be explained below with reference to FIGS. 2 and 3.

初期状態として矩形波入力信号Viは低レベルに
あるものとする(時刻t0)。
Assume that the rectangular wave input signal V i is at a low level in the initial state (time t 0 ).

この状態では、端子Qの出力電圧は高レベル、
端子の出力電圧すなわち矩形波出力信号V1
低レベルにある。結節点11の結節点電位V2
Q端子の出力電圧および正電源(+Vcc)によつ
て決まる電位に止まつている。又、反転回路8の
出力電圧V3は低レベルである。時刻t1において、
矩形波入力信号Viが高レベルになると、Q端子の
出力は低レベル、端子の出力すなわち矩形波出
力信号V1は高レベルになる。同時に結節点11
の結節点電位V2はコンデンサ9と可変抵抗器1
0との時定数で決まる傾斜で低下する。時刻t2
おいて結節点電位V2が反転回路8のスレツシユ
ホールド電圧Vthと交差すると、反転回路8の出
力電圧V3は高レベルとなり、D−フリツプ・フ
ロツプ7はセツトされる。これによつて端子Qの
出力電圧は高レベル、端子の出力電圧すなわち
矩形波出力信号V1は低レベルとなる。したがつ
て矩形波出力信号V1はコンデンサ9と可変抵抗
器10との時定数およびスレツシユホールド電圧
Vthの電圧値の関係によつて決まる一定パルス幅
の信号となる。次に結節点電位V2が上昇し、再
びスレツシユホールド電圧Vthと交差した時出力
電圧V3は低レベルとなる。時刻t3において矩形波
入力信号Viは低レベルとなる。矩形波出力信号
V1は第1図のパルス発生部2に供給され、その
結果狭い出力パルスV0が得られる。以上述べた
如く本考案のパルス発生回路は矩形波入力信号を
波形整形し、一定パルス幅の矩形波出力信号を出
力する波形整形回路を具備しているので、矩形波
入力信号のパルス幅の変動と無関係に一定パルス
幅の信号によりパルス発生部を駆動でき、SRD
を飽和状態まで駆動する必要がなく消費電力が極
めて少ない。特に、本願考案のパルス発生回路
は、矩形波入力信号が比較的低周波数から広範囲
である場合、非常に有効である。又、時定数回路
の時定数若しくはスレツシユホールド電圧値を変
えることにより矩形波出力信号のパルス幅を自由
に設定できる。
In this state, the output voltage of terminal Q is at a high level.
The output voltage of the terminal, ie the square wave output signal V1 , is at a low level. The node potential V 2 of the node 11 remains at a potential determined by the output voltage of the Q terminal and the positive power supply (+Vcc). Further, the output voltage V 3 of the inverting circuit 8 is at a low level. At time t 1 ,
When the rectangular wave input signal V i becomes high level, the output of the Q terminal becomes low level and the output of the terminal, that is, the rectangular wave output signal V 1 becomes high level. At the same time, node 11
The node potential V 2 is the capacitor 9 and the variable resistor 1.
It decreases with a slope determined by the time constant with respect to 0. When the node potential V 2 crosses the threshold voltage V th of the inversion circuit 8 at time t 2 , the output voltage V 3 of the inversion circuit 8 becomes high level and the D-flip-flop 7 is set. As a result, the output voltage of the terminal Q becomes a high level, and the output voltage of the terminal, that is, the rectangular wave output signal V1 becomes a low level. Therefore, the square wave output signal V 1 is the time constant and threshold voltage of the capacitor 9 and the variable resistor 10.
This is a signal with a constant pulse width determined by the relationship between the voltage values of V th . Next, the node potential V 2 rises and when it crosses the threshold voltage V th again, the output voltage V 3 becomes low level. At time t3 , the rectangular wave input signal V i becomes low level. Square wave output signal
V 1 is fed to the pulse generator 2 of FIG. 1, resulting in a narrow output pulse V 0 . As described above, the pulse generation circuit of the present invention is equipped with a waveform shaping circuit that shapes the rectangular wave input signal and outputs a rectangular wave output signal with a constant pulse width, so that the pulse width of the rectangular wave input signal varies. The pulse generator can be driven by a signal with a constant pulse width regardless of the SRD.
There is no need to drive the device to saturation, and power consumption is extremely low. In particular, the pulse generation circuit of the present invention is very effective when the rectangular wave input signal ranges from a relatively low frequency to a wide range. Further, by changing the time constant or threshold voltage value of the time constant circuit, the pulse width of the rectangular wave output signal can be freely set.

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

第1図は本考案のパルス発生回路のブロツク
図。第2図は第1図のパルス発生回路に使用する
波形整形回路の詳細回路図。第3図は第2図の波
形整形回路の動作説明図。 1:波形整形回路、2:パルス発生部、6:
SRD、7:D−フリツプ・フロツプ、8:反転
回路。
FIG. 1 is a block diagram of the pulse generation circuit of the present invention. FIG. 2 is a detailed circuit diagram of a waveform shaping circuit used in the pulse generation circuit of FIG. 1. FIG. 3 is an explanatory diagram of the operation of the waveform shaping circuit of FIG. 2. 1: Waveform shaping circuit, 2: Pulse generator, 6:
SRD, 7: D-flip-flop, 8: Inverting circuit.

Claims (1)

【実用新案登録請求の範囲】 互いに相補的に交互に動作する定電流源及び定
電圧源と前記定電流源と前記定電圧源に接続され
たステツプリカバリダイオードと前記ステツプリ
カバリダイオードの出力信号を微分する微分回路
より成るパルス発生回路において、 前記ステツプリカバリダイオードを飽和させな
いように前記定電流源及び定電圧源への入力信号
のパルス幅を調整する波形整形手段を含むことを
特徴とするパルス発生回路。
[Claims for Utility Model Registration] A constant current source and a constant voltage source that operate complementary to each other and a constant voltage source, a step recovery diode connected to the constant current source and the constant voltage source, and differentiating the output signal of the step recovery diode. A pulse generating circuit comprising a differentiating circuit comprising: a waveform shaping means for adjusting the pulse width of the input signal to the constant current source and the constant voltage source so as not to saturate the step recovery diode. .
JP4522083U 1983-03-29 1983-03-29 Pulse generation circuit Granted JPS59152827U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4522083U JPS59152827U (en) 1983-03-29 1983-03-29 Pulse generation circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4522083U JPS59152827U (en) 1983-03-29 1983-03-29 Pulse generation circuit

Publications (2)

Publication Number Publication Date
JPS59152827U JPS59152827U (en) 1984-10-13
JPH0212752Y2 true JPH0212752Y2 (en) 1990-04-10

Family

ID=30175735

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4522083U Granted JPS59152827U (en) 1983-03-29 1983-03-29 Pulse generation circuit

Country Status (1)

Country Link
JP (1) JPS59152827U (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4873054A (en) * 1971-12-24 1973-10-02
JPS5136977A (en) * 1974-09-24 1976-03-29 Omron Tateisi Electronics Co SEKISANJIKANKEI
JPS57118428A (en) * 1981-01-14 1982-07-23 Yokogawa Hewlett Packard Ltd Pulse generating circuit

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4735842U (en) * 1971-05-11 1972-12-21

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4873054A (en) * 1971-12-24 1973-10-02
JPS5136977A (en) * 1974-09-24 1976-03-29 Omron Tateisi Electronics Co SEKISANJIKANKEI
JPS57118428A (en) * 1981-01-14 1982-07-23 Yokogawa Hewlett Packard Ltd Pulse generating circuit

Also Published As

Publication number Publication date
JPS59152827U (en) 1984-10-13

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