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JPS6122263B2 - - Google Patents
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JPS6122263B2 - - Google Patents

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Publication number
JPS6122263B2
JPS6122263B2 JP13635676A JP13635676A JPS6122263B2 JP S6122263 B2 JPS6122263 B2 JP S6122263B2 JP 13635676 A JP13635676 A JP 13635676A JP 13635676 A JP13635676 A JP 13635676A JP S6122263 B2 JPS6122263 B2 JP S6122263B2
Authority
JP
Japan
Prior art keywords
switch
differential amplifier
amplifier
signal
output
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
JP13635676A
Other languages
Japanese (ja)
Other versions
JPS5361377A (en
Inventor
Tsunetaka Sudo
Takashi Yagi
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.)
NTT Inc
Original Assignee
Nippon Telegraph and Telephone Corp
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 Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP13635676A priority Critical patent/JPS5361377A/en
Publication of JPS5361377A publication Critical patent/JPS5361377A/en
Publication of JPS6122263B2 publication Critical patent/JPS6122263B2/ja
Granted legal-status Critical Current

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  • Amplifiers (AREA)

Description

【発明の詳細な説明】 本発明は、スイツチング波形、増幅器のステツ
プレスポンス等の整定時間の測定の様に、周期的
に変化している波形の微細レベルを拡大して観測
する装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a device for magnifying and observing minute levels of periodically changing waveforms, such as measuring settling time of switching waveforms, amplifier step responses, etc. .

従来の波形観測用増幅器は第1図に示すよう
に、被観測信号源1の被観測波形信号2と比較電
圧発生器4の出力である比較電圧5とを入力する
差動増幅器3で、前記2つの入力の差を増幅した
出力6を、信号源1からの同期信号7で同期をと
つたオシロスコープ8で観測するようになつてい
た。信号2の振幅が小さい場合はこの様な構成で
問題はないが、信号2の振幅が大きくなつてくる
と、増幅器3の初段トランジスタがオン、オフを
するため、熱バランスがくずれて出力6には増幅
器3の熱応答も含まれ、この熱応答と信号2の波
形との識別が困難となり、このことが観測の限界
となつていた。また信号2のレベルに合わせて電
圧発生器4の比較電圧5を調整する場合、数Vの
電圧値を100μV程度の精度で合わせるには非常
な労力を必要とし、電圧発生器4としても、標準
器級の電圧発生器にノイズフイルタを組合せたも
のが必要であるとう問題があつた。
As shown in FIG. 1, a conventional waveform observation amplifier is a differential amplifier 3 that receives an observed waveform signal 2 from an observed signal source 1 and a comparison voltage 5 that is the output of a comparison voltage generator 4. The output 6, which is the amplified difference between the two inputs, was observed using an oscilloscope 8 synchronized with a synchronization signal 7 from the signal source 1. If the amplitude of signal 2 is small, there is no problem with this configuration, but when the amplitude of signal 2 becomes large, the first stage transistor of amplifier 3 turns on and off, which upsets the thermal balance and causes output 6 to includes the thermal response of amplifier 3, making it difficult to distinguish this thermal response from the waveform of signal 2, which has been a limitation of observation. In addition, when adjusting the comparison voltage 5 of the voltage generator 4 according to the level of the signal 2, it requires a great deal of effort to adjust the voltage value of several volts with an accuracy of about 100 μV, and the voltage generator 4 is also used as a standard The problem was that a noise filter was required in combination with an instrument-grade voltage generator.

本発明は上記の様な従来の波形観測用増幅器の
問題点を解決した増幅器を提供することを目的と
する。
An object of the present invention is to provide an amplifier that solves the problems of the conventional waveform observation amplifiers as described above.

上記目的を達成するために、本発明においては
被観測信号に同期した同期信号より前縁だけが任
意の時間Δtだけ遅れれた幅T3のパルスを作る
遅延回路と、差動増幅器の出力をほとんど直流だ
けが通過可能な低域通過波器(以下、LPFと記
す)を経由して帰環させる回路とを設け、前記遅
延パルス期間は被観測信号を差動増幅器に入力し
同時に前記帰環回路のLPF出力を比較電圧として
差動増幅器に入力し、遅延パルス期間以外は差動
増幅器の入力端子間を短絡するようにした。
In order to achieve the above object, the present invention uses a delay circuit that creates a pulse with a width T 3 in which only the leading edge is delayed by an arbitrary time Δt from a synchronization signal synchronized with the observed signal, and a A loop return circuit is provided via a low-pass wave filter (hereinafter referred to as LPF) through which only direct current can pass, and during the delay pulse period, the observed signal is input to the differential amplifier, and at the same time, the loop return circuit is provided. The LPF output of is input to the differential amplifier as a comparison voltage, and the input terminals of the differential amplifier are short-circuited except during the delay pulse period.

第2図は本発明の一実施例図で、第4図はその
動作を示すタイミングチヤートである。被観測信
号源10から出力される同期信号11は遅延回路
12とオシロスコープ25に供給される。第4図
に示すように同期信号11のパルス幅はT2であ
るが、遅延回路12の出力は該同期信号に比し前
縁だけがΔtだけ遅れた幅T3のパルスであつて
このパルスがスイツチドライブ回路14に送られ
る。スイツチドライブ回路14の出力により、第
4図に示すように、被観測信号源10の出力波形
信号15を差動増幅器22の非反転入力端子19
に伝える第一スイツチ16と、帰還回路のLPF2
0と増幅器24の中間にある第三スイツチ18と
は、T3のタイミングでオン、T3以外でオフとな
りまた差動増幅器22の非反転入力端子19と反
転入力端子21とを短絡する第二スイツチ17は
T3でオフT3以外の期間はオンにドライブされ
る。差動増幅器22の出力信号23は帰還回路中
の増幅器24の非反転入力端子とオシロスコープ
25の入力端子に接続されている。増幅器24の
出力は第三スイツチ18を通してLPF20の入力
に接続されLPF20の出力は差動増幅器22の反
転入力端子21に接続されている。第4図で判る
ようにT3のタイミングに注目すると、差動増幅
器22の出力信号23の平均レベルが0Vになる
様に、増幅器22,24,LPF20のループが動
作し差動増幅器22の反転入力端子21への信号
が、非反転入力端子19への信号すなわち信号1
5のT3のタイミングでの波形の平均レベルに向
つて動き、双方が一致すると平衡状態となつて落
着くT3以外のタイミングでは差動増幅器22の
2つの入力端子間は第二スイツチ17で短絡され
て非反転入力端子19も反転入力端子21もLPF
20の出力に接続され、かつ第一スイツチ16が
開いて被観測信号源10は増幅器22と切りはな
されているから、T3以外の期間に被観測信号源
10からの信号15が大振幅で振つても増幅器2
2には影響を与えない。またこの期間にはLPF2
0の入力は第三スイツチ18によつて切りはなさ
れているのでその時までの状態を保持する。増幅
器22は入力端子19と21とが第二スイツチ1
7により同じ点に接続されているので能動範囲の
状態にあり、つぎのT3のタイミングに入つてか
ら不要な熱応答が生じる事はない。入力21の電
圧を電圧計で測定することによつて信号15の
T3での平均電圧を高精度に読取るとができ、ま
た遅延回路12の遅延時間Δtを変えることによ
つて、種々の立上り波形に対応できる。
FIG. 2 is a diagram showing an embodiment of the present invention, and FIG. 4 is a timing chart showing its operation. A synchronizing signal 11 output from the observed signal source 10 is supplied to a delay circuit 12 and an oscilloscope 25. As shown in FIG. 4, the pulse width of the synchronization signal 11 is T 2 , but the output of the delay circuit 12 is a pulse with a width T 3 in which only the leading edge is delayed by Δt compared to the synchronization signal. is sent to the switch drive circuit 14. By the output of the switch drive circuit 14, as shown in FIG.
The first switch 16 that transmits to the
The third switch 18 located between the differential amplifier 22 and the amplifier 24 is turned on at timing T3 and turned off at times other than T3 , and is a second switch that short-circuits the non-inverting input terminal 19 and the inverting input terminal 21 of the differential amplifier 22. Switch 17 is
Off at T 3. Drives on for periods other than T 3 . The output signal 23 of the differential amplifier 22 is connected to the non-inverting input terminal of an amplifier 24 in the feedback circuit and to the input terminal of an oscilloscope 25. The output of the amplifier 24 is connected to the input of the LPF 20 through the third switch 18, and the output of the LPF 20 is connected to the inverting input terminal 21 of the differential amplifier 22. As can be seen in Fig. 4, if we pay attention to the timing of T3 , the loop of amplifiers 22, 24, and LPF 20 operates so that the average level of the output signal 23 of the differential amplifier 22 becomes 0V, and the inversion of the differential amplifier 22 is performed. The signal to the input terminal 21 is the signal to the non-inverting input terminal 19, that is, the signal 1
5, the waveform moves toward the average level at timing T 3 , and when both match, it becomes an equilibrium state and settles down. At timings other than T 3 , the second switch 17 is connected between the two input terminals of the differential amplifier 22. Both non-inverting input terminal 19 and inverting input terminal 21 are short-circuited and become LPF.
Since the first switch 16 is opened and the observed signal source 10 is disconnected from the amplifier 22, the signal 15 from the observed signal source 10 has a large amplitude during periods other than T3 . Amplifier 2 even when shaken
2 is not affected. Also during this period, LPF2
Since the input of 0 has been turned off by the third switch 18, the state up to that point is maintained. The amplifier 22 has input terminals 19 and 21 connected to the second switch 1.
Since they are connected to the same point by 7, they are in the active range, and no unnecessary thermal response will occur after entering the next timing of T3 . of signal 15 by measuring the voltage at input 21 with a voltmeter.
The average voltage at T 3 can be read with high precision, and by changing the delay time Δt of the delay circuit 12, various rising waveforms can be handled.

第3図は本発明の他の実施例図である。被観測
信号源10と第一スイツチ16との間にスイツチ
26を追加し、両スイツチの接続点29との入力
との間にもスイツチ27を追加し、また増幅器2
4の反転入力端子に電圧発生器28を接続してあ
る。信号15が大振幅の場合はたは急しゆんな波
形の場合第2図に示した回路では、スイツチ16
の端子間容量を通つて信号15が入力端子19に
洩れて増幅器22を飽和させることがあるが、第
一スイツチ16と同じ動作をするスイツチ26
と、第二スイツチ17と同じ動作をするスイツチ
27とを追加することによつて上記洩れ現象を大
幅に低減することができる。また電圧発生器28
を調整することによつて、平衡時の信号23の中
心電圧を任意に設定できる。
FIG. 3 is a diagram showing another embodiment of the present invention. A switch 26 is added between the observed signal source 10 and the first switch 16, a switch 27 is also added between the input of the connection point 29 of both switches, and the amplifier 2
A voltage generator 28 is connected to the inverting input terminal of 4. If the signal 15 has a large amplitude or a steep waveform, the circuit shown in FIG.
The signal 15 may leak to the input terminal 19 through the capacitance between the terminals of the switch 26 and saturate the amplifier 22.
By adding a switch 27 that operates in the same way as the second switch 17, the leakage phenomenon described above can be significantly reduced. Also, the voltage generator 28
By adjusting , the center voltage of the signal 23 at equilibrium can be arbitrarily set.

以上説明した様に、従来は振幅が数Vの波形の
整定状態を1μs以下の速度で観測できるのは
1mV程度止りであつたが、本発明ではスイツチ
回路を設けて不要な電圧が増幅器22に加わらな
いようにしたので、波形の速度は増幅器22その
ものの速度(実験の結果によれば100ns程度であ
つて、スイツチ16,17のスイツチングノイズ
に対する回復時間である)が得られ、波形の分解
能も増幅器22のノイズ領域(50〜100μVpp
までに改善される。また帰還回路により比較電圧
の調整が自動化されているため高価な電圧発生器
およびその調整が不要になるなど、本発明の効果
は顕著である。
As explained above, conventionally it is possible to observe the settling state of a waveform with an amplitude of several volts at a speed of 1 μs or less.
However, in the present invention, a switch circuit is provided to prevent unnecessary voltage from being applied to the amplifier 22, so the speed of the waveform is reduced to the speed of the amplifier 22 itself (according to experimental results, it is approximately 100 ns). The recovery time for the switching noise of the switches 16 and 17 is obtained, and the waveform resolution is also within the noise range of the amplifier 22 (50 to 100 μV pp ).
will be improved by. Further, since the adjustment of the comparison voltage is automated by the feedback circuit, an expensive voltage generator and its adjustment are not required, and the effects of the present invention are remarkable.

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

第1図は従来の波形観測用増幅器を示す図、第
2図は本発明の一実施例図、第3図は本発明の他
の実施例図、第4図は第2図に示した実施例のタ
イミングチヤートである。 10…被観測信号源、12…遅延回路、14…
スイツチドライブ回路、16…第一スイツチ、1
7…第二スイツチ、18…第三スイツチ、20…
LPF、22…差動増幅器、25…オシロスコー
プ。
FIG. 1 is a diagram showing a conventional waveform observation amplifier, FIG. 2 is a diagram of one embodiment of the present invention, FIG. 3 is a diagram of another embodiment of the present invention, and FIG. 4 is a diagram of the implementation shown in FIG. 2. This is an example timing chart. 10... Observed signal source, 12... Delay circuit, 14...
Switch drive circuit, 16...first switch, 1
7...Second switch, 18...Third switch, 20...
LPF, 22...differential amplifier, 25...oscilloscope.

Claims (1)

【特許請求の範囲】 1 A 被観測信号が第一スイツチを介して一方
の入力端子に入力される差動増幅器と、 B 上記差動増幅器の出力が低減通過濾波器を介
して上記差動増幅器の他方の入力端子に帰還す
る帰還回路と、 C 上記差動増幅器の2つの入力端子を短絡する
第二スイツチと、 D 上記被観測信号に同期した同期信号より任意
時間前縁の遅れたパルスを発生する遅延回路
と、 E 上記遅延回路により発生したパルス期間のみ
上記第一スイツチを閉じて上記差動増幅器の一
方の端子に上記被観測信号を入力し、上記遅延
回路により発生したパルス期間以外のみ上記第
二スイツチを閉じて上記差動増幅器の入力端子
間を短絡するスイツチ駆動手段と、から成るこ
とを特徴とする波形観測用増幅器。
[Claims] 1 A: a differential amplifier into which the observed signal is input to one input terminal via a first switch; B: an output from the differential amplifier is connected to the differential amplifier via a low-pass filter; C a second switch that shorts the two input terminals of the differential amplifier; D a pulse whose leading edge is delayed by an arbitrary period of time from a synchronization signal synchronized with the observed signal. The first switch is closed only during the pulse period generated by the delay circuit, and the observed signal is inputted to one terminal of the differential amplifier, and only during the pulse period other than the pulse period generated by the delay circuit. A waveform observation amplifier comprising switch driving means for closing the second switch to short-circuit the input terminals of the differential amplifier.
JP13635676A 1976-11-15 1976-11-15 Amplifier for waveform observation Granted JPS5361377A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13635676A JPS5361377A (en) 1976-11-15 1976-11-15 Amplifier for waveform observation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13635676A JPS5361377A (en) 1976-11-15 1976-11-15 Amplifier for waveform observation

Publications (2)

Publication Number Publication Date
JPS5361377A JPS5361377A (en) 1978-06-01
JPS6122263B2 true JPS6122263B2 (en) 1986-05-30

Family

ID=15173259

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13635676A Granted JPS5361377A (en) 1976-11-15 1976-11-15 Amplifier for waveform observation

Country Status (1)

Country Link
JP (1) JPS5361377A (en)

Also Published As

Publication number Publication date
JPS5361377A (en) 1978-06-01

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