JPS62182674A - Servo circuit character measuring circuit - Google Patents
Servo circuit character measuring circuitInfo
- Publication number
- JPS62182674A JPS62182674A JP61024625A JP2462586A JPS62182674A JP S62182674 A JPS62182674 A JP S62182674A JP 61024625 A JP61024625 A JP 61024625A JP 2462586 A JP2462586 A JP 2462586A JP S62182674 A JPS62182674 A JP S62182674A
- Authority
- JP
- Japan
- Prior art keywords
- servo circuit
- circuit
- measurement
- resistor
- closed loop
- 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
- 238000005259 measurement Methods 0.000 claims abstract description 32
- 238000002347 injection Methods 0.000 claims abstract description 11
- 239000007924 injection Substances 0.000 claims abstract description 11
- 238000012546 transfer Methods 0.000 abstract description 3
- 238000010586 diagram Methods 0.000 description 9
- 238000012360 testing method Methods 0.000 description 4
- 238000006073 displacement reaction Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 230000015556 catabolic process Effects 0.000 description 1
- 238000012937 correction Methods 0.000 description 1
- 238000006731 degradation reaction Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000003780 insertion Methods 0.000 description 1
- 230000037431 insertion Effects 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000001052 transient effect Effects 0.000 description 1
Landscapes
- Moving Of The Head To Find And Align With The Track (AREA)
- Optical Recording Or Reproduction (AREA)
- Measurement Of Resistance Or Impedance (AREA)
- Testing Electric Properties And Detecting Electric Faults (AREA)
- Testing And Monitoring For Control Systems (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、サーボ回路の特性を閉ループのまま測定する
回路に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a circuit that measures the characteristics of a servo circuit in a closed loop.
CD(コンパクト・ディスク)プレーヤでは光学ピック
アップのレンズを微小移動させるためにサーボ回路を用
いるが、この種のサーボ回路の性能(安定性等)は開ル
ープ特性での利得余裕、位相余裕や過渡応答特性、閉ル
ープ周波数特性等で測定される。しかし、開ループはル
ープゲインが高い場合、飽和やS/Nの劣下等をきたし
、満足な測定結果を得にくい。そのため、測定は閉ルー
プで行う必要がある。In CD (compact disc) players, a servo circuit is used to minutely move the lens of the optical pickup, but the performance (stability, etc.) of this type of servo circuit depends on the gain margin, phase margin, and transient response of the open-loop characteristic. characteristics, closed loop frequency characteristics, etc. However, when the loop gain of the open loop is high, saturation and S/N degradation occur, making it difficult to obtain satisfactory measurement results. Therefore, measurements must be performed in a closed loop.
第3図〜第5図は従来のI11定回路の各別である。FIGS. 3 to 5 show different types of conventional I11 constant circuits.
サーボ回路は入力をX、出力をyとする閉ループで、0
人は微小な機械的変位Xを電気量に変換する回路のゲイ
ン、cBは電気量を機械的変位yに変換する回路のゲイ
ン、AI、A2は加算器である。The servo circuit is a closed loop with input as X and output as y.
Human is the gain of a circuit that converts a minute mechanical displacement X into an electrical quantity, cB is a gain of a circuit that converts an electrical quantity into a mechanical displacement y, and AI and A2 are adders.
第3図の例はcA、craの間を切断してそこに加算器
A2を接続し、ループからの信号すと周波数特性分析器
FRAからの測定用信号Cを加算して、その和信号a=
b+cをループに注入しながら測定する。例えば、信号
Cを数K Hz〜数10KHzの範囲で変化させて開ル
ープのゲインGOLを測定する。In the example shown in Fig. 3, adder A2 is connected between cA and cra, and the signal from the loop is added to the measurement signal C from the frequency characteristic analyzer FRA, resulting in the sum signal a. =
Measure b+c while injecting it into the loop. For example, the open loop gain GOL is measured by varying the signal C in the range of several kHz to several tens of kHz.
このサーボ回路本来の閉ループのゲインはy/Xである
が、CDプレーヤではx、 yがいずれも数μmオー
ダーの機械的変位であるので、直接その比を求めること
は難しい。このため、上記のようにaを入力、bを出力
とするようなループに変形して測定する。The inherent closed-loop gain of this servo circuit is y/X, but in a CD player, both x and y are mechanical displacements on the order of several μm, so it is difficult to directly determine the ratio. Therefore, as described above, the loop is transformed into a loop in which a is the input and b is the output, and the measurement is performed.
第4図は加算器A2を予め閉ループ内に接続しておく方
式で、動作原理は第2図と変らない。同図(a)は全体
図で、(blは加算器A2の詳細図である。In FIG. 4, the adder A2 is connected in advance in a closed loop, and the operating principle is the same as in FIG. (a) is an overall diagram, and (bl is a detailed diagram of the adder A2).
加算器A2は信号す、cを加算する抵抗R11゜R12
とオペアンプOP、それに帰還抵抗R13からなり、非
測定時にはa −c端子をオープンにしておけば済む(
A2はゲイン1)。Adder A2 is a resistor R11゜R12 that adds signals S and c.
It consists of an operational amplifier OP, and a feedback resistor R13, and it is sufficient to leave terminals a and c open when not measuring.
A2 has a gain of 1).
第5図はループを切断することもなく、且つループ中に
加算器を接続してお(必要もない方式で、ループ中に予
め接続した抵抗R1の両端に測定用の加算器を接続する
ものである。この抵抗R1を、Gへの出力インピーダン
スよりは充分に大きく、且つGBの入力インピーダンス
よりは充分に小さい値に選定すると、測定時の接続状態
ではR1部分が切断されたと等価になり、しかも非測定
時には閉ループにχ響を与えない。Figure 5 shows a method in which the adder for measurement is connected to both ends of the resistor R1, which is connected in advance to the loop, without cutting the loop or connecting an adder in the loop. If this resistor R1 is selected to a value that is sufficiently larger than the output impedance to G and sufficiently smaller than the input impedance of GB, the connected state at the time of measurement is equivalent to the R1 part being disconnected. Moreover, when not measuring, it does not affect the closed loop.
ところが、上述した方法は全て加算器を用いるので、測
定回路1,3ではアダプタ側の回路が犬になり、また測
定回路2では被測定側が回路大になると共に高価になる
。個別には測定回路1はループの切断、接続が必要なの
で測定時間がかかり、信頼性を低下させる原因にもなる
。また、測定回路1.3は被測定回路に影響を与えて測
定精度を低下させる原因にもなる。However, since all of the above-mentioned methods use adders, the circuits on the adapter side in measurement circuits 1 and 3 become complicated, and in measurement circuit 2, the circuit to be measured becomes large and expensive. Individually, the measurement circuit 1 requires loop disconnection and connection, which takes measurement time and causes a decrease in reliability. Furthermore, the measurement circuit 1.3 affects the circuit under test and causes a reduction in measurement accuracy.
本発明は測定用信号源をフローティングにすることで加
算器をな(し、上述した欠点を除去しようとするもので
ある。The present invention attempts to eliminate the above-mentioned drawbacks by making the measurement signal source floating to form an adder.
c問題点を解決するための手段〕
本発明は、サーボ回路の閉ループの一部に測定用信号の
注入抵抗を予め挿入しておくと共に、測定時に該注入抵
抗の両端にフローティング状態の測定用信号源をアダプ
タ式に接続し、そして該抵抗の両端の電圧比から該サー
ボ回路の開ループの周波数特性を測定するようにしてな
ることを特徴とするものである。Means for Solving Problem c] The present invention provides a method in which an injection resistance for a measurement signal is inserted in advance into a part of the closed loop of a servo circuit, and a measurement signal is placed in a floating state at both ends of the injection resistance at the time of measurement. The servo circuit is characterized in that the open-loop frequency characteristic of the servo circuit is measured from the voltage ratio across the resistor by connecting the power source using an adapter.
第1図(a)に示すようにループの一部に直列に抵抗R
iを挿入しても、挿入点からループの後を見たインピー
ダンスZiが、挿入した抵抗Riよりも充分に大きけれ
ば、(Ri<Zi)被測定回路への特性の影響は無視で
きる。つまり、Ri=0としたときの電流■は
であるが、Ri+oでもRi<Ziであれば流れる電流
I′は
E/Zi
Zi十Z。As shown in Figure 1(a), a resistor R is connected in series with a part of the loop.
Even if i is inserted, if the impedance Zi seen from the insertion point to the back of the loop is sufficiently larger than the inserted resistor Ri (Ri<Zi), the influence of the characteristics on the circuit under test can be ignored. That is, when Ri=0, the current (2) is, but if Ri<Zi even with Ri+o, the flowing current I' is E/Zi Zi+Z.
となり、Riの影響はない。これは非測定時であるが、
測定時に外部信号源Egを接続してその出力インピーダ
ンスRsがRiと並列に接続されると、
Ri 7 Rs < Ri
となるので、更に影響が小さくなる。尚、ZiはCaの
入力インピーダンスであり、またZOはGAの出力イン
ピーダンスである。この図は、Ziに発生した電圧がC
A、C8倍されてZoに電圧Eとして現われることを示
している。Therefore, there is no influence of Ri. This is during non-measurement, but
If an external signal source Eg is connected during measurement and its output impedance Rs is connected in parallel with Ri, the influence becomes even smaller because Ri 7 Rs < Ri. Note that Zi is the input impedance of Ca, and ZO is the output impedance of GA. This figure shows that the voltage generated on Zi is C
This shows that A and C are multiplied by 8 and appear as voltage E on Zo.
次に同図(blで信号Egが注入できる理由を説明する
。信号源Egがなければ抵抗Riの両端の電圧Ei、E
oは等しいが、Egを接続するとEo−Ei=E−I
(Zo+Zi)となり、Zi)Riという条件では
となる。これを等測的に示すと同図(C1のようになリ
、Egがループ内に注入されていることになる。Next, we will explain the reason why the signal Eg can be injected in the figure (bl).If there is no signal source Eg, the voltages Ei and E across the resistor Ri
o are equal, but when Eg is connected, Eo-Ei=E-I
(Zo+Zi), and under the condition of Zi)Ri. If this is shown isometrically, as shown in the same figure (C1), Eg is injected into the loop.
但し、電流関係はE=0のとき
Ig=Ix+Iy
Ri・Ix= (Zi+Zo)Iy
であり、またEg=Oのとき(E:8:O)の電流Iは
であるから、E≠O,Eg”=:Oのときの電流IはI
=I++Iy
で表わされる。However, the current relationship is Ig=Ix+Iy Ri・Ix= (Zi+Zo)Iy when E=0, and the current I when Eg=O (E:8:O) is, so E≠O, Eg ”=: The current I when O is I
=I++Iy.
注入抵抗Riは測定用信号源Egの出力インピーダンス
Rsの終端用としても機能する。この場合、Ri(Zi
を満たすためにRiをRsより小さく設定したときは、
信号源の出力インピーダンスのマツチングをとる必要が
ある場合不足分Rs’をアダプタ側または被測定回路側
に入れればよい。The injection resistor Ri also functions as a terminal for the output impedance Rs of the measurement signal source Eg. In this case, Ri(Zi
When Ri is set smaller than Rs to satisfy
If it is necessary to match the output impedance of the signal source, the insufficient amount Rs' may be inserted into the adapter side or the circuit under test.
このときRiとRs’の分圧によって生ずる減衰は信号
源Egの出力を増大させることによって解決できる。At this time, the attenuation caused by the voltage division between Ri and Rs' can be solved by increasing the output of the signal source Eg.
一般に周波数分析器FRAの各入力は高入力インピーダ
ンス、低キャパシタンスであるが、発振器Eg出力端子
は第1図(d)に示すように大地との間に比佼的大きい
キャパシタンスCを持つため、被測定回路にKWを与え
る場合がある。この場合、等価回路が(e)のようであ
るとCの影響を受けるが、(f)のようにRs’が被測
定回路と発振器との間に入ると影響が軽減できる。Generally, each input of the frequency analyzer FRA has high input impedance and low capacitance, but the oscillator Eg output terminal has a relatively large capacitance C between it and the ground as shown in Figure 1(d), so it is KW may be applied to the measurement circuit. In this case, if the equivalent circuit is as shown in (e), it will be affected by C, but if Rs' is placed between the circuit under test and the oscillator as shown in (f), the effect can be reduced.
第2図は本発明の一実施例を示すブロック図で、第1図
と対比するとRo =Z o r RL =Z t
r R2=Rt、 R] =RS’の関係にある。従っ
て、R2<RL
Rs−R2+Rz
である。このうち、R2はループに挿入された抵抗であ
るが、R3はアダプタ側であるので、ループ側の構成は
簡単であり、またアダプタ側の構成も簡単(いずれも加
算器を要しない)である。FIG. 2 is a block diagram showing an embodiment of the present invention, and when compared with FIG. 1, Ro = Z o r RL = Z t
The relationship is r R2=Rt, R]=RS'. Therefore, R2<RL Rs-R2+Rz. Of these, R2 is a resistor inserted into the loop, but R3 is on the adapter side, so the configuration on the loop side is simple, and the configuration on the adapter side is also simple (no adder is required in either case). .
第7図は本発明による測定結果(上段は周波数特性、下
段は位相特性)であり、これは第6図(第4図による測
定結果)と変りない。FIG. 7 shows the measurement results according to the present invention (the upper row shows the frequency characteristics, and the lower row shows the phase characteristics), which is the same as FIG. 6 (the measurement results according to FIG. 4).
以上述べたように本発明によれば、簡単な構成(基本的
には注入抵抗だけ)でサーボ回路の伝達特性を閉ループ
のまま測定することができ、しかも被測定側に与える影
響が少な(、またアダプタ構成としてその着脱が容易と
なる利点がある。As described above, according to the present invention, the transfer characteristics of a servo circuit can be measured in a closed loop with a simple configuration (basically only an injection resistor), and there is little influence on the side to be measured ( Further, the adapter structure has the advantage that it can be easily attached and detached.
第1図は本発明の原理説明図、第2図は本発明の一実施
例を示すブロック図、第3図〜第5図は従来の測定回路
の異なる例を示すブロック図、第6図は従来の測定回路
2による測定結果の特性図、第7図は本発明回路による
測定結果の特性図である。
図中、CA、CBはサーボ回路のゲイン、FRAは周波
数特性分析器、Egは測定用信号源、Rsはその出力イ
ンピーダンス、Ri、R2は信号注入抵抗、R3’、R
3は補正抵抗である。
本塾卯壇九倒
箪2図
機末の測定11各1
第3図
、Δ箇
Δ(、。 、部具 侶Fig. 1 is a diagram explaining the principle of the present invention, Fig. 2 is a block diagram showing an embodiment of the invention, Figs. 3 to 5 are block diagrams showing different examples of conventional measurement circuits, and Fig. 6 is a block diagram showing an embodiment of the present invention. FIG. 7 is a characteristic diagram of the measurement results obtained by the conventional measuring circuit 2, and FIG. 7 is a characteristic diagram of the measurement results obtained by the circuit of the present invention. In the figure, CA and CB are gains of the servo circuit, FRA is a frequency characteristic analyzer, Eg is a measurement signal source, Rs is its output impedance, Ri, R2 are signal injection resistors, R3', R
3 is a correction resistance. Measurement of the end of the Honjuku Udan Kutaken 2 drawings 11 each 1 Fig. 3, ΔKΔ(,., Parts
Claims (2)
抵抗を予め挿入しておくと共に、測定時に該注入抵抗の
両端にフローティング状態の測定用信号源をアダプタ式
に接続し、そして該抵抗の両端の電圧比から該サーボ回
路の開ループの周波数特性を測定するようにしてなるこ
とを特徴とするサーボ回路の特性測定回路。(1) Insert a measurement signal injection resistor into a part of the closed loop of the servo circuit in advance, and at the time of measurement, connect a floating measurement signal source to both ends of the injection resistor in an adapter type, and 1. A characteristic measuring circuit for a servo circuit, characterized in that the open loop frequency characteristic of the servo circuit is measured from the voltage ratio between both ends of the servo circuit.
れることを特徴とする特許請求の範囲第1項記載のサー
ボ回路の特性測定回路。(2) A characteristic measuring circuit for a servo circuit according to claim 1, wherein the injection resistor is also used for terminating a measurement signal source.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61024625A JPS62182674A (en) | 1986-02-06 | 1986-02-06 | Servo circuit character measuring circuit |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61024625A JPS62182674A (en) | 1986-02-06 | 1986-02-06 | Servo circuit character measuring circuit |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62182674A true JPS62182674A (en) | 1987-08-11 |
Family
ID=12143324
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61024625A Pending JPS62182674A (en) | 1986-02-06 | 1986-02-06 | Servo circuit character measuring circuit |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62182674A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006010596A (en) * | 2004-06-29 | 2006-01-12 | Fuji Electric Systems Co Ltd | Electronic transformer with oscillation determination function |
US8410791B2 (en) | 2007-03-06 | 2013-04-02 | Nec Corporation | Impulse immunity test apparatus |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6027370B2 (en) * | 1979-09-03 | 1985-06-28 | 日立電線株式会社 | Airtightness inspection method for plastic pipe terminal connections |
-
1986
- 1986-02-06 JP JP61024625A patent/JPS62182674A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6027370B2 (en) * | 1979-09-03 | 1985-06-28 | 日立電線株式会社 | Airtightness inspection method for plastic pipe terminal connections |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006010596A (en) * | 2004-06-29 | 2006-01-12 | Fuji Electric Systems Co Ltd | Electronic transformer with oscillation determination function |
JP4557139B2 (en) * | 2004-06-29 | 2010-10-06 | 富士電機システムズ株式会社 | Electronic transformer with oscillation judgment function |
US8410791B2 (en) | 2007-03-06 | 2013-04-02 | Nec Corporation | Impulse immunity test apparatus |
JP5177902B2 (en) * | 2007-03-06 | 2013-04-10 | 日本電気株式会社 | Impulse immunity evaluation device |
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