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JPS6333326B2 - - Google Patents
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JPS6333326B2 - - Google Patents

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Publication number
JPS6333326B2
JPS6333326B2 JP20020282A JP20020282A JPS6333326B2 JP S6333326 B2 JPS6333326 B2 JP S6333326B2 JP 20020282 A JP20020282 A JP 20020282A JP 20020282 A JP20020282 A JP 20020282A JP S6333326 B2 JPS6333326 B2 JP S6333326B2
Authority
JP
Japan
Prior art keywords
voltage
terminal
operational amplifier
diode
peak
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
JP20020282A
Other languages
Japanese (ja)
Other versions
JPS5990407A (en
Inventor
Tsunemi Gonda
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.)
Nikon Corp
Original Assignee
Nippon Kogaku KK
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 Nippon Kogaku KK filed Critical Nippon Kogaku KK
Priority to JP20020282A priority Critical patent/JPS5990407A/en
Publication of JPS5990407A publication Critical patent/JPS5990407A/en
Publication of JPS6333326B2 publication Critical patent/JPS6333326B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03DDEMODULATION OR TRANSFERENCE OF MODULATION FROM ONE CARRIER TO ANOTHER
    • H03D1/00Demodulation of amplitude-modulated oscillations
    • H03D1/08Demodulation of amplitude-modulated oscillations by means of non-linear two-pole elements
    • H03D1/10Demodulation of amplitude-modulated oscillations by means of non-linear two-pole elements of diodes

Landscapes

  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Measurement Of Current Or Voltage (AREA)
  • Manipulation Of Pulses (AREA)

Description

【発明の詳細な説明】 本発明は入力電圧のピーク位置を検出するため
のピーク検波回路に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a peak detection circuit for detecting the peak position of input voltage.

従来この種の回路は第1図、第2図のごとき構
成であり、第1図は一回限りのピーク位置を検出
する為に用いられ、第2図は連続的な交流のピー
ク位置を検出する為に用いられるものである。
Conventionally, this type of circuit has a configuration as shown in Figures 1 and 2. Figure 1 is used to detect a one-time peak position, and Figure 2 is used to detect a continuous peak position of alternating current. It is used to do.

第1図で示した従来のピーク検波回路は、演算
増幅器OP1の出力端子をダイオードDのアノー
ドに接続し、ダイオードDのカソードをコンデン
サCの一方の端子と演算増幅器OP2の非反転入
力端子に接続し、コンデンサCの他方の端子を共
通端子(アース)に接続し、コンデンサの端子間
に放電用スイツチSを設け、演算増幅器OP2の
反転入力端子と出力端子とを接続してバツフアを
構成し、この出力端子を演算増幅器OP1の反転
入力端子に接続して構成されている。そして、演
算増幅器OP1の非反転入力端子と共通端子(ア
ース)との間に入力電圧eiが印加され、演算増幅
器OP1の出力端子と共通端子(アース)との間
から出力電圧eoが取り出される。
The conventional peak detection circuit shown in Figure 1 connects the output terminal of operational amplifier OP1 to the anode of diode D, and connects the cathode of diode D to one terminal of capacitor C and the non-inverting input terminal of operational amplifier OP2. Then, the other terminal of the capacitor C is connected to the common terminal (earth), a discharge switch S is provided between the terminals of the capacitor, and the inverting input terminal and output terminal of the operational amplifier OP2 are connected to form a buffer. This output terminal is connected to the inverting input terminal of the operational amplifier OP1. Then, an input voltage ei is applied between the non-inverting input terminal of the operational amplifier OP1 and the common terminal (earth), and an output voltage eo is taken out between the output terminal of the operational amplifier OP1 and the common terminal (earth).

なお、ダイオードDのカソードとコンデンサC
の一方の端子と演算増幅器OP2の非反転入力端
子との接続点をQとする。
In addition, the cathode of diode D and capacitor C
Let Q be the connection point between one terminal of OP2 and the non-inverting input terminal of operational amplifier OP2.

このような回路において、第3図aに示すごと
きパルス的な電圧eiを入力すると、第1図のQ点
の電圧及び出力電圧eoは第3図b,cに各々Q、
eoで示すごとく変化をし、入力電圧eiのピークP1
の位置が出力電圧eoにて検出される。ところが
入力電圧eiにおいて、第3図aに破線で示したご
とく、第1のピークP1に続いてピークP1より小
さい振幅の第2のピークP2が来た時には、コン
デンサーCの電荷が放電しきつていない為に、演
算増幅器OP1は動作をせず、出力電圧eoとして
は第2のピークP2が検出されない。その為に第
1のピークP1を検出した後にただちにコンデン
サCの電荷を放電させるべき、図示されていない
放電開始回路によりスイツチSをタイミング良く
閉じなければならない。従つて第1図の回路は放
電開始回路が必要であるという欠点が有る。
In such a circuit, when a pulse-like voltage ei as shown in FIG. 3a is input, the voltage at point Q in FIG.
The peak of input voltage ei changes as shown by eo, P 1
The position of is detected by the output voltage eo. However, at the input voltage ei, as shown by the broken line in Figure 3a, when a second peak P2 with a smaller amplitude than peak P1 follows the first peak P1 , the charge in the capacitor C is discharged. Since the voltage is not restricted, the operational amplifier OP1 does not operate, and the second peak P2 is not detected as the output voltage eo. For this reason, the switch S must be closed in a timely manner by a discharge starting circuit (not shown) to discharge the charge in the capacitor C immediately after the first peak P1 is detected. Therefore, the circuit of FIG. 1 has the disadvantage that a discharge starting circuit is required.

さらに第1図の回路は第3図dのei′に示すご
とく、入力のパルス的な電圧に負の直流電圧が重
畳し、そのピークPが負の電圧の時にはダイオー
ドDが逆バイアスになり、非導通になり、ピーク
Pは検出されないという欠点を有している。
Furthermore, in the circuit of Fig. 1, as shown by ei' in Fig. 3d, a negative DC voltage is superimposed on the input pulse voltage, and when the peak P is a negative voltage, the diode D becomes reverse biased. It has the disadvantage that it becomes non-conductive and the peak P is not detected.

次に第2図の回路の説明に入るが、第2図の回
路が第1図の回路と異なる点は、コンデンサCに
並列に接続した放電用のスイツチSの代わりに、
コンデンサCに並列に抵抗Rを接続したことであ
る。第2図の入力電圧eiとして第4図aにeiで示
したごとく周期Tのくり返し信号を入力すると、
コンデンサCと抵抗Rの時定数CRが周期Tに比
べて充分大きい場合、第2図のQ点の電圧は第4
図bのQのごとくになる。これは入力電圧eiの正
の傾きの時は演算増幅器OP1の出力インピーダ
ンスは低いので急速にコンデンサCを充電し、ほ
ぼ入力電圧と同一波形になるが、ピークPを通過
すると、入力電圧eiは低くなるので、コンデンサ
Cに蓄えられた電荷による電圧により、ダイオー
ドDは逆バイアスされて非導通になり、コンデン
サCと抵抗Rの時定数CRで定まる放電特性でコ
ンデンサCが放電されることによる。
Next, we will explain the circuit in Figure 2. The difference between the circuit in Figure 2 and the circuit in Figure 1 is that instead of a discharge switch S connected in parallel to the capacitor C,
This is because a resistor R is connected in parallel to the capacitor C. When a repeating signal with a period T is inputted as the input voltage ei in FIG. 2, as shown by ei in FIG. 4a,
If the time constant CR of the capacitor C and the resistor R is sufficiently large compared to the period T, the voltage at point Q in Figure 2 will be the fourth
It will look like Q in Figure b. This is because when the input voltage ei has a positive slope, the output impedance of the operational amplifier OP1 is low, so it quickly charges the capacitor C and becomes almost the same waveform as the input voltage, but when the input voltage ei passes through the peak P, the input voltage ei becomes low. Therefore, the diode D is reverse biased and becomes non-conductive due to the voltage due to the charge stored in the capacitor C, and the capacitor C is discharged according to the discharge characteristic determined by the time constant CR of the capacitor C and the resistor R.

その結果、出力電圧eoは第4図cのeoのごと
き波形となりピークPの位置が検出される。
As a result, the output voltage eo has a waveform such as eo in FIG. 4c, and the position of the peak P is detected.

ここで入力電圧eiの周期Tを大きくし時定数
CRに近ずけていくと、第2図のQ点の波形は第
4図dのQ′で示すごとく、ピーク付近では入力
電圧ei(第4図a参照)に近ずいてしまう為に、
その出力電圧eoは第4図eの信号eo′に示すごと
く、検出されるピークPの位置には時間tの遅れ
誤差を生じてしまう。この事は、時定数CRに対
して入力電圧eiの周期Tはある範囲内でなければ
ならないという欠点を有している事を示してい
る。
Here, increase the period T of input voltage ei and set the time constant
As we approach CR, the waveform at point Q in Figure 2 approaches the input voltage ei (see Figure 4a) near the peak, as shown by Q' in Figure 4d.
The output voltage eo causes a delay error of time t in the position of the detected peak P, as shown by the signal eo' in FIG. 4e. This shows that there is a drawback that the period T of the input voltage ei must be within a certain range with respect to the time constant CR.

さらに第4図fのei′に示すごとく入力電圧eiが
負の電圧範囲で生じている場合、第1図の場合と
同様にダイオードDは常に逆バイアスされるため
に非導通となり、ピークPの位置は検出されない
と云う欠点がある。
Furthermore, when the input voltage ei occurs in the negative voltage range as shown by ei' in Figure 4f, the diode D becomes non-conducting because it is always reverse biased, as in the case of Figure 1, and the peak P The disadvantage is that the position is not detected.

本発明はこれらの欠点を解決し、周波数依存性
が小さく、パルス的入力及びくり返し入力電圧に
も対応が出来ると共に、入力電圧が零ボルト以下
の負の電圧においてもそのピーク位置が検出出来
るピーク検波回路を得る事を目的とする。
The present invention solves these shortcomings and provides a peak detection system that has low frequency dependence, can handle pulsed input and repeated input voltage, and can detect the peak position even when the input voltage is a negative voltage below zero volts. The purpose is to obtain a circuit.

以下、図面に示した実施例に基づいて本発明を
説明する。
The present invention will be described below based on embodiments shown in the drawings.

第5図は本発明の第1実施例であり、演算増幅
器OP1の出力端子をダイオードD1のアノード
に接続し、ダイオードD1のカソードをコンデン
サCの一方の端子とダイオードD2のアノードと
演算増幅器OP1の反転入力端子に接続し、コン
デンサCの他方の端子を共通端子(アース)に接
続し、ダイオードD2のカソードを演算増幅器
OP2の出力端子に接続し、演算増幅器OP2の非
反転入力端子を演算増幅器OP1の非反転入力端
子に接続し、演算増幅器OP2の反転入力端子を
その出力端子に接続して成る。第5図の回路にお
いて、演算増幅器OP1の非反転入力端子と共通
端子との間に入力電圧eiを印加し、演算増幅器
OP1の出力端子と共通端子との間から出力電圧
eoを取り出す。なお、ダイオードD1のカソー
ドとコンデンサCの一方の端子とダイオードD2
のアノードと演算増幅器OP1の反転入力端子と
の接続点をQとする。
FIG. 5 shows a first embodiment of the present invention, in which the output terminal of the operational amplifier OP1 is connected to the anode of the diode D1, and the cathode of the diode D1 is connected to one terminal of the capacitor C, the anode of the diode D2, and the anode of the operational amplifier OP1. Connect to the inverting input terminal, connect the other terminal of capacitor C to the common terminal (ground), and connect the cathode of diode D2 to the operational amplifier.
The non-inverting input terminal of the operational amplifier OP2 is connected to the non-inverting input terminal of the operational amplifier OP1, and the inverting input terminal of the operational amplifier OP2 is connected to its output terminal. In the circuit shown in Fig. 5, input voltage ei is applied between the non-inverting input terminal of operational amplifier OP1 and the common terminal, and the operational amplifier
Output voltage from between the output terminal of OP1 and the common terminal
Take out eo. Note that the cathode of diode D1, one terminal of capacitor C, and diode D2
Let Q be the connection point between the anode of and the inverting input terminal of the operational amplifier OP1.

上述の回路において入力電圧eiとして第6図a
のごときくり返し信号eiを入力すると演算増幅器
OP2の出力端子には入力電圧eiと同一電圧が生
じている事は言うまでもない。他方演算増幅器
OP1はコンデンサCの電荷が零から始まるので、
ダイオードD1は導通し、Q点は第6図bに示す
ごとく、入力電圧eiと同一振幅で増加する。入力
電圧eiがピークPになる位置までの演算増幅器
OP1の出力電圧eoは入力電圧eiに対して第6図
cに示した如く、ダイオードD1の順方向電圧
Vf1分だけ高い電圧で変化する。また、ダイオー
ドD2の両端の電圧は各々入力電圧eiと同じ値で
あるので、ダイオードD2は何ら動作に寄与しな
い。そして入力電圧eiがピークPの位置を通過す
るとコンデンサCはピーク電圧に充電されている
ので演算増幅器OP1の反転入力端子もピーク電
圧になる。続いて入力電圧eiは減少しだすので、
演算増幅器OP1の非反転入力端子の電圧は反転
入力端子の電圧より低くなり、その出力電圧eo
は第6図cに示したように演算増幅器OP1のマ
イナス飽和電圧Vsまで低下する。その結果、ダ
イオードD1は逆バイアスされて非導通になる。
そして入力電圧eiがさらに減少し、演算増幅器
OP2の出力端子の電圧がQ点の電圧よりダイオ
ードD2の順方向電圧Vf2以下に低下するとダイ
オードD2は導通しだし、コンデンサCの電荷は
ダイオードD2を通して演算増幅器OP2の出力
端子に放電し、その後、Q点の電圧は入力電圧ei
よりもVf2分だけ高い電圧で変化する。この様子
を第6図bに示す。同図における二点鎖線は、従
来のCR放電特性を示す(第4図b参照)。
In the circuit described above, as the input voltage ei, Fig. 6a
When a repeated signal ei such as is input, the operational amplifier
Needless to say, the same voltage as the input voltage ei is generated at the output terminal of OP2. Operational amplifier on the other hand
In OP1, the charge on capacitor C starts from zero, so
The diode D1 becomes conductive and the Q point increases with the same amplitude as the input voltage ei, as shown in FIG. 6b. Operational amplifier up to the point where the input voltage ei reaches the peak P
The output voltage eo of OP1 is the forward voltage of diode D1 with respect to the input voltage ei, as shown in Figure 6c.
Vf changes at a higher voltage by 1 minute. Furthermore, since the voltages across the diode D2 are each the same value as the input voltage ei, the diode D2 does not contribute to the operation at all. When the input voltage ei passes the peak P, the capacitor C is charged to the peak voltage, so the inverting input terminal of the operational amplifier OP1 also becomes the peak voltage. Subsequently, the input voltage ei begins to decrease, so
The voltage at the non-inverting input terminal of operational amplifier OP1 is lower than the voltage at the inverting input terminal, and its output voltage eo
decreases to the negative saturation voltage Vs of the operational amplifier OP1, as shown in FIG. 6c. As a result, diode D1 becomes reverse biased and non-conducting.
Then the input voltage ei is further reduced and the operational amplifier
When the voltage at the output terminal of OP2 drops below the voltage at point Q to the forward voltage Vf 2 of diode D2, diode D2 begins to conduct, and the charge in capacitor C is discharged to the output terminal of operational amplifier OP2 through diode D2, and then , the voltage at point Q is the input voltage ei
The voltage changes by 2 minutes higher than Vf. This situation is shown in FIG. 6b. The two-dot chain line in the same figure shows the conventional CR discharge characteristics (see FIG. 4b).

この様にピークPの位置を通過後は従来と異な
り、コンデンサCの電圧はダイオードD2の順方
向電圧Vf2分のみの差で入力電圧eiに追従してい
るので、余分な電荷の蓄積がなく、その後の入力
変化に対して追従しやすい状態になつている。す
なわち周波数依存性が少ない。
In this way, after passing the peak P position, unlike the conventional case, the voltage of the capacitor C follows the input voltage ei with a difference of only 2 minutes of the forward voltage Vf of the diode D2, so there is no accumulation of excess charge. , it is now in a state where it can easily follow subsequent input changes. In other words, there is little frequency dependence.

続いて入力電圧eiが増加しだすと、演算増幅器
OP1の反転入力端子と非反転入力端子間の電圧
は電圧Vf2の値よりもしだい小さくなりついには
同一となり(第6図bのl点)、その値を越すと
演算増幅器OP1の出力電圧eoは正の方向に立ち
上ると共に、ダイオードD1は導通しダイオード
D2は非導通になり、初めの時と同様な状態にな
る。この様にしてピーク位置Pは検出される。
Subsequently, when the input voltage ei begins to increase, the operational amplifier
The voltage between the inverting input terminal and the non-inverting input terminal of OP1 gradually becomes smaller than the value of the voltage Vf 2 and finally becomes the same (point l in Fig. 6b), and when that value is exceeded, the output voltage eo of the operational amplifier OP1 rises in the positive direction, and the diode D1 becomes conductive and the diode D2 becomes non-conductive, resulting in the same state as at the beginning. In this way, the peak position P is detected.

さらに入力電圧eiとして第6図dに示すごと
く、全体として負の電圧で変化している場合にお
いても、相対的に各素子間の電圧は前記と同様で
あるので同様にピークPの位置は検出される。た
だしその時の出力電圧eoは第6図eのようにな
る。
Furthermore, even when the input voltage ei is changing as a negative voltage as a whole as shown in Figure 6d, the relative voltage between each element is the same as above, so the position of the peak P can be detected in the same way. be done. However, the output voltage eo at that time is as shown in FIG. 6e.

このように第5図の回路によれば、入力電圧の
周波数に依存することが少なく、かつ従来のもの
では検出出来なかつた負の電圧範囲においてもピ
ーク位置の検出が可能であるという利点がある。
As described above, the circuit shown in Fig. 5 has the advantage that it is less dependent on the frequency of the input voltage, and that it is possible to detect the peak position even in the negative voltage range, which could not be detected with conventional circuits. .

なお、上述の実施例では演算増幅器OP2によ
るバツフアを用いていたが、出力インピーダンス
の低い信号源から電圧を入力する場合には、バツ
フアを用いない第7図のような構成でも良い事は
云うまでもない。本発明の第2実施例を示した第
7図の動作は第5図と全く同じであるので、同一
部材には同一図番を付し説明を省略する。
In the above embodiment, a buffer provided by the operational amplifier OP2 was used, but it goes without saying that if a voltage is input from a signal source with low output impedance, a configuration as shown in FIG. 7 without using a buffer may be used. Nor. The operation of FIG. 7 showing the second embodiment of the present invention is completely the same as that of FIG. 5, so the same parts are given the same numbers and the explanation will be omitted.

また、第5図、第7図において、ダイオードD
1,D2の接続方向を逆にすれば入力電圧の最小
位置が検出出来るのは当然である。
In addition, in FIGS. 5 and 7, the diode D
It goes without saying that the minimum position of the input voltage can be detected by reversing the connection direction of 1 and D2.

さらに第8図に示すごとく、第7図の回路に演
算増幅器OP2′を加えることにより、第9図aの
信号ei,e′,ei″いずれの場合も、同第9図bに示
すようにピークPの位置が演算増幅器OP2の出
力端子に矩形波として検出される。なお、第9図
cに演算増幅器OP1の出力端子の電圧eoを示す。
Furthermore, as shown in Fig. 8, by adding an operational amplifier OP2' to the circuit shown in Fig. 7, the signals ei, e', ei'' in Fig. 9a can be changed as shown in Fig. 9b. The position of the peak P is detected as a rectangular wave at the output terminal of the operational amplifier OP2. FIG. 9c shows the voltage eo at the output terminal of the operational amplifier OP1.

もちろん第9図の回路は第3図aのごときパル
ス的入力に対しても使用できる。
Of course, the circuit of FIG. 9 can also be used for pulsed inputs as shown in FIG. 3a.

以上の様に本発明によれば、パルス的入力及び
くり返し入力に対しても各々のピーク位置を検出
できるのみならず周波数依存度も小さく、かつ直
流分が多く含まれている信号においてもピーク位
置が検出出来るという利点がある。
As described above, according to the present invention, not only can each peak position be detected even for pulsed input and repeated input, but also the frequency dependence is small, and the peak position can be detected even for signals containing a large amount of DC component. It has the advantage that it can be detected.

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

第1図及び第2図は従来のピーク検波回路の回
路図、第3図は第1図の各部の波形図、第4図は
第2図の各部の波形図、第5図は本発明の一実施
例の回路図、第6図は第5図の各部の波形図、第
7図及び第8図は本発明の他の実施例の回路図、
第9図は第8図の各部の波形図である。 〔主要部分の符号の説明〕、OP1……演算増幅
器、C……コンデンサ、D1,D2……ダイオー
ド。
Figures 1 and 2 are circuit diagrams of conventional peak detection circuits, Figure 3 is a waveform diagram of each part in Figure 1, Figure 4 is a waveform diagram of each part in Figure 2, and Figure 5 is a diagram of the waveform of each part in Figure 2. A circuit diagram of one embodiment, FIG. 6 is a waveform diagram of each part of FIG. 5, FIGS. 7 and 8 are circuit diagrams of other embodiments of the present invention,
FIG. 9 is a waveform diagram of each part of FIG. 8. [Explanation of symbols of main parts] OP1... operational amplifier, C... capacitor, D1, D2... diode.

Claims (1)

【特許請求の範囲】[Claims] 1 演算増幅器の反転入力端子と共通端子との間
にコンデンサを接続し、前記反転入力端子と前記
演算増幅器の出力端子との間に第1のダイオード
を設けると共に、前記反転入力端子と前記演算増
幅器の非反転入力端子との間に第2のダイオード
を設け、前記出力端子と前記非反転入力端子間で
前記第1のダイオードと前記第2のダイオードと
が同方向になる如く互いの向きを定め、前記非反
転入力端子と共通端子との間に入力電圧を印加
し、前記出力端子と共通端子との間から出力電圧
を取り出す如く成したことを特徴とするピーク検
波回路。
1. A capacitor is connected between the inverting input terminal and the common terminal of the operational amplifier, a first diode is provided between the inverting input terminal and the output terminal of the operational amplifier, and a capacitor is connected between the inverting input terminal and the common terminal of the operational amplifier. A second diode is provided between the output terminal and the non-inverting input terminal, and the first diode and the second diode are oriented in the same direction between the output terminal and the non-inverting input terminal. A peak detection circuit characterized in that an input voltage is applied between the non-inverting input terminal and a common terminal, and an output voltage is extracted from between the output terminal and the common terminal.
JP20020282A 1982-11-15 1982-11-15 Peak detecting circuit Granted JPS5990407A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20020282A JPS5990407A (en) 1982-11-15 1982-11-15 Peak detecting circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20020282A JPS5990407A (en) 1982-11-15 1982-11-15 Peak detecting circuit

Publications (2)

Publication Number Publication Date
JPS5990407A JPS5990407A (en) 1984-05-24
JPS6333326B2 true JPS6333326B2 (en) 1988-07-05

Family

ID=16420493

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20020282A Granted JPS5990407A (en) 1982-11-15 1982-11-15 Peak detecting circuit

Country Status (1)

Country Link
JP (1) JPS5990407A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59118511U (en) * 1983-01-28 1984-08-10 株式会社新潟鐵工所 Sewage storage device for concrete mixer truck
CN111721999A (en) * 2020-06-30 2020-09-29 上海创功通讯技术有限公司 Peak voltage detection circuit

Also Published As

Publication number Publication date
JPS5990407A (en) 1984-05-24

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