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JPH0155422B2 - - Google Patents
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JPH0155422B2 - - Google Patents

Info

Publication number
JPH0155422B2
JPH0155422B2 JP13445280A JP13445280A JPH0155422B2 JP H0155422 B2 JPH0155422 B2 JP H0155422B2 JP 13445280 A JP13445280 A JP 13445280A JP 13445280 A JP13445280 A JP 13445280A JP H0155422 B2 JPH0155422 B2 JP H0155422B2
Authority
JP
Japan
Prior art keywords
capacitor
current
operational amplifier
value
resistor
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
JP13445280A
Other languages
Japanese (ja)
Other versions
JPS5760265A (en
Inventor
Minoru Nomura
Tetsuro Maekawa
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.)
Anritsu Corp
Original Assignee
Anritsu 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 Anritsu Corp filed Critical Anritsu Corp
Priority to JP13445280A priority Critical patent/JPS5760265A/en
Publication of JPS5760265A publication Critical patent/JPS5760265A/en
Publication of JPH0155422B2 publication Critical patent/JPH0155422B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R15/00Details of measuring arrangements of the types provided for in groups G01R17/00 - G01R29/00, G01R33/00 - G01R33/26 or G01R35/00
    • G01R15/14Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks
    • G01R15/18Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using inductive devices, e.g. transformers
    • G01R15/183Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using inductive devices, e.g. transformers using transformers with a magnetic core

Landscapes

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

Description

【発明の詳細な説明】[Detailed description of the invention]

この発明は、演算増幅器を用いた交流入力用電
流電圧変換器に関するものである。 第1図は従来の電流電圧変換器をカレント・ト
ランスに接続した一例を示す。この図で、1はカ
レント・トランスで、鉄心2に一次巻線3と二次
巻線4とが施される。5はコンデンサ、6は演算
増幅器、7はその反転入力側に出力側からフイー
ドバツクを行う抵抗器である。コンデンサ5は演
算増幅器6の反転入力側が直接二次巻線4に接続
されると、その入力が二次巻線4で接地された形
となり、直流でのフイードバツクが極端に減少
し、演算増幅器6の出力の直流安定度が悪くなる
ので、それを防止するため挿入されたものであ
る。8は出力端子である。 測定に際しては、一次巻線3に被測定電流Iを
流す。そして出力端子8に得られる出力電圧Vか
ら被測定電流Iを求める。 さて、第1図の回路において、その伝達特性を
演算増幅器6の利得が充分大きいとして求めると
下記第(1)式のようになる。 V=−R1/N・I・1/(1−1/ω2LC−jr/ωL)
…(1) ここで、N:一次、二次巻線3,4の巻線比 R1:抵抗器7の抵抗値 ω:角速度 L:二次巻線4のインダクタンス C:コンデンサ5のキヤパシタンス r:二次巻線4の内部抵抗値 第(1)式からわかるように、低周波域の特性は、
The present invention relates to an AC input current-voltage converter using an operational amplifier. FIG. 1 shows an example of a conventional current-voltage converter connected to a current transformer. In this figure, 1 is a current transformer, and a primary winding 3 and a secondary winding 4 are provided on an iron core 2. 5 is a capacitor, 6 is an operational amplifier, and 7 is a resistor for providing feedback from the output side to its inverting input side. When the inverting input side of the operational amplifier 6 of the capacitor 5 is directly connected to the secondary winding 4, the input is grounded by the secondary winding 4, and the feedback in direct current is extremely reduced. This was inserted to prevent the DC stability of the output from worsening. 8 is an output terminal. During measurement, a current to be measured I is passed through the primary winding 3. Then, the current to be measured I is determined from the output voltage V obtained at the output terminal 8. Now, in the circuit shown in FIG. 1, if the transfer characteristic is determined assuming that the gain of the operational amplifier 6 is sufficiently large, the following equation (1) is obtained. V=-R 1 /N・I・1/(1-1/ω 2 LC-jr/ωL)
...(1) Here, N: Turning ratio of primary and secondary windings 3 and 4 R 1 : Resistance value of resistor 7 ω: Angular velocity L: Inductance of secondary winding 4 C: Capacitance r of capacitor 5 : Internal resistance value of secondary winding 4 As can be seen from equation (1), the characteristics in the low frequency range are:

【式】およびω1=r/Lによつて決ま り、ω0はω1に比べて小さく、少なとも1/2に選択
しないと低周波域にピークを生ずる。ここで、 ω0=1/2ω1としたとき C=4L/r2 …(2) であり、例えば、外径68φ、内径44φ、厚さ13mm
でインダクタンス係数が4300mHのコアに、
0.32φの線材を1000ターン巻いて二次巻線4とす
ると、そのインダクタンスは約4H(ヘンリー)、
その内部抵抗rは約10Ωとなり、コンデンサ5の
必要なキヤパシタンスは第(2)式から0.16Fとなる。 このように従来の電流電圧変換器は、低周波域
まで測定範囲が必要な場合には、コンデンサ5の
キヤパシタンスCは非常に大きな値のものが必要
となる欠点があつた。 この発明は上記の欠点を除去するためになされ
たものである。以下、この発明について説明す
る。 第2図はこの発明の一実施例を示すもので、第
1図の従来例と同様にカレント・トランスに接続
した場合である。この発明では、R1なる抵抗値
をもつ帰還抵抗器7を演算増幅器6の出力側とコ
ンデンサ5の入力側に接続し、高い抵抗値R2
有する抵抗器9を演算増幅器6の出力側と反転入
力側に接続したもので、その他は第1図と同じで
ある。 第2図の回路における伝達特性を演算増幅器6
の利得が充分大きいとして求めると、下記第(3)式
のようになる。 V=−I/N・R1R2/R1+R2・1/{1−R1+r/ω
2LC(R1+R2)−j(1/ωC(R1+R2)+r/ωL)}
…(3) 第(3)式において、 R2≫R1≫r、 1/ωC(R1+R2)≪r/ωL とすると、 V=−I/N・R1R2/R1+R2 ・1/{1−1/ω2LC・R1/R2−jr/ωL}…(4
) となる。 第(1)式と第(4)式を比べるとわかるように、第(4)
式でのC×R2/R1が、第(1)式のCに相当する。 第(4)式において、フラツト域での変換特性は、 V=−I/N・R1R2/R1+R2 であるが、R2≫R1に選ぶので、 V=−−I/N・R1となる。 すなわち、従来の回路にくらべ、この発明によ
ると、1/R2/R1のコンデンサ5のキヤパシタンス 値で、同一の低周波特性を得ることができること
になる。 例えば、R1=10KΩ、R2=10MΩと選べば、
Cの値は従来にくらべ、1/107/104=1/103 で同一の特性が得られることになる。したがつ
て、前述の例においては、従来例ではC=0.16F
を必要としたのが、C=160μFでよいことにな
る。 なお、上記ではこの発明の電流電圧変換器をカ
レント・トランスに接続したが、この発明はこれ
に限定されるものでなく、他の被測定電流源であ
つてもよい。 以上詳細に説明したように、この発明は被測定
電流の電流値の応じた電圧をコンデンサを介して
演算増幅器の反転入力端子に加え、この演算増幅
器の出力側から抵抗器を介して入力側にフイード
バツクを加え、被測定電流を電圧値に変換して測
定する交流入力用電流電圧変換器において、電流
―電圧の変換率を決めるフイードバツク抵抗器を
演算増幅器の出力側とコンデンサの入力端子の間
に接続し、演算増幅器の出力側と反転入力側間を
高抵抗の抵抗器で接続することにより従来回路に
おいてはその周波数特性を実現するのに必要とす
るコンデンサの値が実用的な値とならない程大き
な場合でも、前記付加した抵抗器の抵抗値を選定
することにより等価的にそのコンデンサの値を実
現することができ、したがつて、直流安定度の良
い、低い低周波数領域まで平坦な特性をもつ交流
入力用電流電圧変換器が得られる利点がある。
It is determined by [Formula] and ω 1 =r/L, and ω 0 is smaller than ω 1 , and unless it is selected to be at least 1/2, a peak will occur in the low frequency range. Here, when ω 0 = 1/2ω 1, C = 4L/r 2 ...(2) For example, outer diameter 68φ, inner diameter 44φ, thickness 13mm
In the core with an inductance coefficient of 4300mH,
If a 0.32φ wire is wound 1000 turns to form secondary winding 4, its inductance is approximately 4H (Henry).
Its internal resistance r is about 10Ω, and the required capacitance of the capacitor 5 is 0.16F from equation (2). As described above, the conventional current-voltage converter has the disadvantage that when a measurement range extending to a low frequency range is required, the capacitance C of the capacitor 5 is required to have a very large value. This invention has been made to eliminate the above-mentioned drawbacks. This invention will be explained below. FIG. 2 shows an embodiment of the present invention, in which it is connected to a current transformer in the same way as the conventional example shown in FIG. In this invention, a feedback resistor 7 having a resistance value of R 1 is connected to the output side of the operational amplifier 6 and an input side of the capacitor 5, and a resistor 9 having a high resistance value R 2 is connected to the output side of the operational amplifier 6. It is connected to the inverting input side, and the rest is the same as in FIG. The transfer characteristics in the circuit shown in Figure 2 are expressed by the operational amplifier 6
Assuming that the gain is sufficiently large, the following equation (3) is obtained. V=-I/N・R 1 R 2 /R 1 +R 2・1/{1-R 1 +r/ω
2 LC (R 1 + R 2 ) − j (1/ωC (R 1 + R 2 ) + r/ωL)}
...(3) In equation (3), R 2 ≫R 1 ≫r, 1/ωC (R 1 +R 2 ) ≪r/ωL, then V=-I/N・R 1 R 2 /R 1 +R 2・1/{1−1/ω 2 LC・R 1 /R 2 −jr/ωL}…(4
) becomes. As can be seen by comparing equations (1) and (4),
C×R 2 /R 1 in the equation corresponds to C in equation (1). In equation (4), the conversion characteristic in the flat region is V=-I/N・R 1 R 2 /R 1 +R 2 , but since R 2 ≫ R 1 is selected, V=--I/ It becomes N・R 1 . That is, compared to the conventional circuit, according to the present invention, the same low frequency characteristics can be obtained with a capacitance value of the capacitor 5 of 1/R 2 /R 1 . For example, if you choose R 1 = 10KΩ and R 2 = 10MΩ,
Compared to the conventional case, the value of C is 1/10 7 /10 4 =1/10 3 and the same characteristics can be obtained. Therefore, in the above example, C=0.16F in the conventional example.
Instead of requiring , C = 160μF will suffice. Although the current-voltage converter of the present invention is connected to a current transformer in the above example, the present invention is not limited to this, and other current sources to be measured may be used. As explained in detail above, the present invention applies a voltage corresponding to the current value of the current to be measured to the inverting input terminal of an operational amplifier via a capacitor, and from the output side of the operational amplifier to the input side via a resistor. In a current-voltage converter for AC input that adds feedback and converts the current to be measured into a voltage value, a feedback resistor that determines the current-voltage conversion rate is installed between the output side of the operational amplifier and the input terminal of the capacitor. By connecting a high-resistance resistor between the output side and the inverting input side of the operational amplifier, the value of the capacitor required to achieve the frequency characteristics in the conventional circuit is no longer practical. Even if the value of the capacitor is large, it is possible to equivalently achieve the value of the capacitor by selecting the resistance value of the added resistor. Therefore, it is possible to achieve a flat characteristic down to a low frequency range with good DC stability. This has the advantage of providing a current-voltage converter for AC input.

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

第1図は従来の電流電圧変換器の一例を示す回
路図、第2図はこの発明の一実施例を示す回路図
である。 図中、1はカレント・トランス、2は鉄心、3
は一次巻線、4は二次巻線、5はコンデンサ、6
は演算増幅器、7は抵抗器、8は出力端子、9は
抵抗器である。
FIG. 1 is a circuit diagram showing an example of a conventional current-voltage converter, and FIG. 2 is a circuit diagram showing an embodiment of the present invention. In the figure, 1 is the current transformer, 2 is the iron core, 3
is the primary winding, 4 is the secondary winding, 5 is the capacitor, 6
is an operational amplifier, 7 is a resistor, 8 is an output terminal, and 9 is a resistor.

Claims (1)

【特許請求の範囲】[Claims] 1 被測定電流の電流値に応じた値の電圧が一方
の電極に印加されるコンデンサと、このコンデン
サの他方の電極に反転入力側が接続された演算増
幅器と、この演算増幅器の出力側と前記反転入力
側との間に接続された抵抗器と、前記演算増幅器
の出力側と前記コンデンサの一方の電極との間に
接続された抵抗器からなり、前記反転入力側に接
続された抵抗器の抵抗値が前記コンデンサの一方
の入力側に接続された抵抗器の抵抗値に比して充
分大きな値に選定されたことを特徴とする交流入
力用電流電圧変換器。
1 A capacitor to which a voltage corresponding to the current value of the current to be measured is applied to one electrode, an operational amplifier whose inverting input side is connected to the other electrode of this capacitor, and an output side of this operational amplifier and the inverting input side connected to the other electrode of the capacitor. and a resistor connected between the output side of the operational amplifier and one electrode of the capacitor, and the resistance of the resistor connected to the inverting input side. 1. A current-voltage converter for AC input, characterized in that the value is selected to be sufficiently larger than the resistance value of a resistor connected to one input side of the capacitor.
JP13445280A 1980-09-29 1980-09-29 Current voltage converter for ac input Granted JPS5760265A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13445280A JPS5760265A (en) 1980-09-29 1980-09-29 Current voltage converter for ac input

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13445280A JPS5760265A (en) 1980-09-29 1980-09-29 Current voltage converter for ac input

Publications (2)

Publication Number Publication Date
JPS5760265A JPS5760265A (en) 1982-04-12
JPH0155422B2 true JPH0155422B2 (en) 1989-11-24

Family

ID=15128667

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13445280A Granted JPS5760265A (en) 1980-09-29 1980-09-29 Current voltage converter for ac input

Country Status (1)

Country Link
JP (1) JPS5760265A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101846702A (en) * 2010-05-10 2010-09-29 伊博电源(杭州)有限公司 Inductive current detection circuit

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2388914B (en) * 2002-05-10 2005-09-28 Pri Ltd Clamp-on ct
CN109541513B (en) * 2018-12-25 2022-02-08 北京东方计量测试研究所 Alternating current micro-current tracing device and method

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101846702A (en) * 2010-05-10 2010-09-29 伊博电源(杭州)有限公司 Inductive current detection circuit
CN101846702B (en) 2010-05-10 2012-05-30 伊博电源(杭州)有限公司 Inductive current detection circuit

Also Published As

Publication number Publication date
JPS5760265A (en) 1982-04-12

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