JPS6089761A - Wide band current transofrmer measuring current of power transmission line - Google Patents
Wide band current transofrmer measuring current of power transmission lineInfo
- Publication number
- JPS6089761A JPS6089761A JP58198877A JP19887783A JPS6089761A JP S6089761 A JPS6089761 A JP S6089761A JP 58198877 A JP58198877 A JP 58198877A JP 19887783 A JP19887783 A JP 19887783A JP S6089761 A JPS6089761 A JP S6089761A
- Authority
- JP
- Japan
- Prior art keywords
- current
- current transformer
- secondary winding
- light emitting
- transmission line
- 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.)
- Granted
Links
- 230000005540 biological transmission Effects 0.000 title claims description 12
- 238000004804 winding Methods 0.000 claims abstract description 23
- 239000013307 optical fiber Substances 0.000 claims description 9
- 230000003287 optical effect Effects 0.000 claims description 7
- 229910000859 α-Fe Inorganic materials 0.000 abstract description 3
- 230000035699 permeability Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 3
- 230000005284 excitation Effects 0.000 description 3
- 230000009466 transformation Effects 0.000 description 3
- 229910000976 Electrical steel Inorganic materials 0.000 description 1
- 230000006378 damage Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 229910001120 nichrome Inorganic materials 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
- 230000001052 transient effect Effects 0.000 description 1
Landscapes
- Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
- Emergency Protection Circuit Devices (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は送電線の電流を測定する広帯域変流器に関す
るものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a broadband current transformer for measuring current in a power transmission line.
電力系統に流れる電流を測定する従来の変流器は、珪素
鋼板をコアとして使用し、変成比に応じて多数回の巻線
を施して構成されるため、本質的に周波数応答域が狭く
、商用周波電流は測定できるが、送電線系統における事
故発生時のサージ電流波形を測定することは困難とされ
ていた。Conventional current transformers that measure the current flowing in power systems use a silicon steel plate as a core and are constructed with multiple windings depending on the transformation ratio, so they inherently have a narrow frequency response range. Although commercial frequency current can be measured, it has been difficult to measure surge current waveforms when an accident occurs in a power transmission line system.
したがって、この発明の目的は、サージ電流等の高周波
電流を忠実に測定することができる送電線の電流を測定
する広帯域変流器を提供することである。Therefore, an object of the present invention is to provide a broadband current transformer for measuring current in a power transmission line that can faithfully measure high frequency currents such as surge currents.
この発明の送電線の電流を測定する広帯域変流器は、2
次巻線に一定巻数毎にタップを有する貫通形変流器本体
と、一定抵抗値毎にタップを有し前記貫通形変流器本体
の2次巻線に並列接続されるとともに各タップを前記2
次巻線の各タップに順次対応接続した抵抗と、この抵抗
に並列接続した可飽和リアクトルと、この可飽和リアク
トルの両端間に接続された発光素子と、この発光素子か
ら出力される光信号を伝送する光ファイバと、この光フ
ァイバによシ伝送された光信号を受信する受信機とを備
える構成にしたことを特徴とする。The broadband current transformer for measuring the current of a power transmission line according to the present invention has two
A through-type current transformer main body having a tap at every fixed number of turns in the secondary winding, and a tap at every fixed resistance value, which is connected in parallel to the secondary winding of the through-hole current transformer main body, and each tap is connected to the secondary winding of the through-hole current transformer main body. 2
A resistor connected to each tap of the next winding in a corresponding manner, a saturable reactor connected in parallel to this resistor, a light emitting element connected between both ends of this saturable reactor, and an optical signal output from this light emitting element. It is characterized by having a configuration that includes an optical fiber for transmission and a receiver for receiving the optical signal transmitted by the optical fiber.
以下、この発明の実施例を図面に基づいて詳細に説明す
る。Hereinafter, embodiments of the present invention will be described in detail based on the drawings.
第1図はこの発明の一実施例の送電線の電流を4測定す
る広帯域変流器の構成図を示している。第1図において
、1はフェライトトロイダルコアla ・を使用した貫
通形変流器本体で、変流比に応じた巻数の2次巻線lb
を巻装してあシ、この2次巻線lbには一定数毎にタッ
プを設けている。2はニクロム線からなる抵抗で、全抵
抗値がR工であって一定抵抗値(低い値)毎にタップを
設けてあ仄貫通形変流器本体1の2次巻線lbに並列接
続し、かつ各タップを上記2次巻線lbの各タップに順
次対応接続し、上記2次巻線lbに対して分布負荷とな
るようにしている。3は貫通形変流器本体1の2次巻線
lbに並列接続した過電流保護用の可飽和リアク)yで
ある。4および5は、同一特性の発光ダイオードであっ
て、逆並列接続し電流制限抵抗6(抵抗値R2)を介し
て貫通形変流器本体lの2次巻線lbの両端間に接続さ
れ、入力電流の正および負の半波成分をそれぞれ光信号
に変換している。電流制限抵抗6には、発光ダイオード
4.5の温度補償を行うだめの負特性サーミスタも組み
込まれている。FIG. 1 shows a block diagram of a broadband current transformer for measuring four currents in a power transmission line according to an embodiment of the present invention. In Fig. 1, 1 is the main body of a through-type current transformer using a ferrite toroidal core, and the secondary winding lb has a number of turns depending on the current transformation ratio.
This secondary winding lb is provided with taps at regular intervals. 2 is a resistor made of nichrome wire, which has a total resistance value of R, and is connected in parallel to the secondary winding lb of the main body 1 of the through-hole type current transformer with taps provided at each constant resistance value (low value). , and each tap is sequentially connected to each tap of the secondary winding lb so as to provide a distributed load to the secondary winding lb. 3 is a saturable reactor y for overcurrent protection connected in parallel to the secondary winding lb of the feedthrough current transformer main body 1. 4 and 5 are light emitting diodes with the same characteristics, which are connected in antiparallel and connected between both ends of the secondary winding lb of the feedthrough current transformer body 1 via a current limiting resistor 6 (resistance value R2); The positive and negative half-wave components of the input current are each converted into optical signals. The current limiting resistor 6 also incorporates a negative characteristic thermistor for temperature compensation of the light emitting diode 4.5.
7および8は発光ダイオード4.5から出力さ゛れる光
信号を伝送する光7Tイバ、9は光フ了イパ7.8を通
して伝送された光信号を受信する受信機である。7 and 8 are optical fibers that transmit the optical signal output from the light emitting diode 4.5, and 9 is a receiver that receives the optical signal transmitted through the optical fiber 7.8.
貫通形変流器本体101次電流をIP、変流比を1とす
れば、貫通形変流器本体1の2次電流I8は1−」L
S、 ・・・・・・(11
となシ、したがって、発光ダイオード4.5の順方向抵
抗を無視すると、抵抗2の端子電圧Vは次式で表わされ
る。If the primary current of the feedthrough current transformer main body 10 is IP and the current transformation ratio is 1, the secondary current I8 of the feedthrough current transformer main body 1 is 1-''LS, ......(11). Therefore, if the forward resistance of the light emitting diode 4.5 is ignored, the terminal voltage V of the resistor 2 is expressed by the following equation.
また、発光ダイオード4.5を流れる駆動電流iは次式
で表わされる。Further, the drive current i flowing through the light emitting diode 4.5 is expressed by the following equation.
飽和しない領域での貫通形変流器本体工の2入電流■8
は1入電流Ipに比例して増大するので、送電線事故時
などには定格の400倍程まで流れる。2-input current of feedthrough current transformer body work in non-saturation region■8
Since the current increases in proportion to one input current Ip, the current flows up to about 400 times the rated value in the event of a power transmission line fault.
したがって、抵抗2の端子電圧Vも上昇するが、この値
は発光ダイオード4.5の破壊と関係する重要な問題で
あるので、直線性を考慮して定格時最良となる動作電圧
を選び、サージ電圧に対しては定格時の400倍程を許
容するが、商用周波電圧に対しては4倍程度に抑制する
必要がある。Therefore, the terminal voltage V of the resistor 2 also rises, but this value is an important issue related to the destruction of the light emitting diode 4.5. Therefore, the best operating voltage at the rated time is selected in consideration of linearity, and the surge Although the voltage is allowed to be about 400 times the rated voltage, it is necessary to suppress the commercial frequency voltage to about 4 times.
このため、第2図のような励磁特性を持つ可飽和リアク
トル3を抵抗2に並列接続し、抵抗2の端子電圧Vのう
ち商用周波成分の上昇を定格時の4倍程度に抑制し、端
子電圧Vのサージ成分については定格時の400倍程ま
で直線性良く上昇するようにしている。第2図は、縦軸
に可飽和リアク)/L’3の端子室[EVを、横軸に励
磁電流Iをとり、定格時の電圧および電流をそれぞf′
Lvn、Inとし、4倍の過電圧を4vn、そのときの
電流を4Inとし、実線Ylは4I、より磁芯の飽和が
始まることを示し、一点鎖線Y2は磁芯が飽和しないこ
とを示している。For this reason, a saturable reactor 3 having excitation characteristics as shown in Fig. 2 is connected in parallel to the resistor 2, and the rise in the commercial frequency component of the terminal voltage V of the resistor 2 is suppressed to about four times the rated value, and the terminal The surge component of the voltage V is designed to increase linearly to about 400 times the rated value. In Figure 2, the vertical axis represents the terminal chamber [EV of the saturable reactor)/L'3, the horizontal axis represents the excitation current I, and the voltage and current at the rated value are f', respectively.
Lvn and In, the 4 times overvoltage is 4vn, the current at that time is 4In, the solid line Yl indicates that the magnetic core begins to saturate at 4I, and the dashed line Y2 indicates that the magnetic core does not saturate. .
磁芯の透磁率をμ、空心インダクタンスをり。とすると
、可飽和リアクト/l/3のインダクタンスしは
L二μLo ・・曲(4)
で示され、μの関数として変化し、そのインピーダンス
Zは交流周波数をfHzとすると、Z = 2ifL
= 2*fμL□ ””(5)で示される。したがうて
、高周波帯(サージ電流)では、透磁率μが低くとも周
波数fが高いため、インピーダンス2が十分大きい。一
方、商用周波帯(商用周波電流)では、透磁率μが高す
ので、周波数fが低ぐてもインピーダンス2は十分大き
い。そして、正常時のインピーダンスZ ト抵m 2お
よび電流制限抵抗6との間に次の関係を成立させている
。The magnetic permeability of the magnetic core is μ, and the air core inductance is . Then, the inductance of saturable react/l/3 is expressed as L2μLo... (4) and changes as a function of μ, and its impedance Z is Z = 2ifL, assuming the AC frequency is fHz.
= 2*fμL□ ”” (5). Therefore, in a high frequency band (surge current), even if the magnetic permeability μ is low, the frequency f is high, so the impedance 2 is sufficiently large. On the other hand, in the commercial frequency band (commercial frequency current), the magnetic permeability μ is high, so even if the frequency f is low, the impedance 2 is sufficiently large. The following relationship is established between the impedance Z, the resistance m2, and the current limiting resistor 6 during normal operation.
R工<< R2<< Z ・・・・・・(6)磁気飽和
すると、磁芯の透磁率μが1となるため、周波数の低い
商用周波帯では、インピーダンス2は、R工、R2に対
し
Z < R□<< R2・−曲(71
となり、抵抗R2の端子電圧Vが抑制されて貫通形変流
器本体1の1次電流が過大となったときに発光ダイオー
ド495が保護される。一方、周波数fの高い高周波帯
では、最初から透磁率μが低いが周波数fが高いため、
第(61式の関係が維持され、抵抗2の端子電圧Vは抑
制されることがない。したがって、サージ電流に対して
は、抵抗2の端子′電圧Vは定格時の400倍程まで上
昇することができ、商用周波電流は4倍程度に抑制され
、送電線事故時のサージ電流測定が可能となる。R engineering << R2 << Z... (6) When magnetically saturated, the magnetic permeability μ of the magnetic core becomes 1, so in the low frequency commercial frequency band, the impedance 2 is reduced to R engineering and R2. On the other hand, Z <R<< R2・- (71), and when the terminal voltage V of the resistor R2 is suppressed and the primary current of the feedthrough current transformer main body 1 becomes excessive, the light emitting diode 495 is protected. On the other hand, in a high frequency band with a high frequency f, the magnetic permeability μ is low from the beginning, but the frequency f is high, so
The relationship of Equation 61 is maintained, and the terminal voltage V of resistor 2 is not suppressed. Therefore, against surge current, the terminal voltage V of resistor 2 rises to about 400 times the rated value. As a result, the commercial frequency current can be suppressed by about four times, making it possible to measure surge currents during transmission line faults.
発光ダイオード4.5の光出力は駆動電流iに比例し、
駆動電流iは第(3)式よシ明らかなように抵抗2の端
子電圧Vに比例するので、発光ダイオード4.5は、端
子’jlL圧Vに比例する光出力を光ファイバ7.8へ
送り出し、光ファイバ7.8によυ伝送されてきた振幅
変調光信号を受端に設けた受信機Rが電気信号に復元し
、適当な方法で発光ダイオード4.5のしきい値歪を補
正し、貫通形変流器本体1の1次電流IPに比例した電
圧または電流の形で出力する。The light output of the light emitting diode 4.5 is proportional to the drive current i,
As is clear from equation (3), the drive current i is proportional to the terminal voltage V of the resistor 2, so the light emitting diode 4.5 sends a light output proportional to the terminal voltage V to the optical fiber 7.8. The receiver R installed at the receiving end restores the amplitude modulated optical signal sent out and υ transmitted through the optical fiber 7.8 into an electrical signal, and corrects the threshold distortion of the light emitting diode 4.5 using an appropriate method. It outputs a voltage or current proportional to the primary current IP of the feedthrough current transformer main body 1.
このように、この実施例は、フェライトコアを用いた周
波数特性の良好な貫通形変流器本体102′/に巻線l
bに抵抗2を分布接続して周波数特性をさらに良好にし
、この貫通形変流器本体1の2次巻線1bに可能′和す
アク)7し3を並列接続して発光ダイオード4.5の保
護を行った上で、貫通形変流器本体1の2次電流を発光
ダイオード4゜5で直線性よく光変換し、光ファイバ7
.8により測定値を伝送するようにしたため、送電線事
故の過渡電流波形を忠実に測定することができる。In this way, this embodiment uses a winding l in the feedthrough current transformer main body 102'/ which uses a ferrite core and has good frequency characteristics.
A resistor 2 is connected in parallel to the secondary winding 1b of the through-type current transformer body 1 to further improve the frequency characteristics by distributingly connecting a resistor 2 to the current transformer body 1. The secondary current of the feedthrough current transformer main body 1 is converted into light with good linearity by a light emitting diode 4.5, and the optical fiber 7 is
.. 8 to transmit the measured values, it is possible to faithfully measure the transient current waveform of a power transmission line fault.
以上のように、この発明の送電線の電流を測定する広帯
域変流器によれば、サージ電流等の高周波電流を忠実に
測定できるという効果がある。As described above, the broadband current transformer for measuring current in a power transmission line according to the present invention has the effect of being able to faithfully measure high frequency currents such as surge currents.
第1図1仕この発明の一実施例の構成図、第2図は可飽
和リアク)/しの励磁特性を示す特性図である。FIG. 1 is a block diagram of an embodiment of the present invention, and FIG. 2 is a characteristic diagram showing the excitation characteristics of a saturable reactor.
Claims (1)
体と、一定抵抗値毎にタップを有し前記貫通形変流器本
体の2次巻線に並列接続されるとともに各タップを前記
2次巻線の各タップに順次対応接続した抵抗と、この抵
抗に並列接続した可飽和リアクトルと、この可飽和リア
クトルの両端間に接続された発光素子と、この発光素子
から出力される光信号を伝送する光ファイバと、この光
ファイバにより伝送された光信号を受信する受信機とを
備えた送電線の電流を測定する広帯域変流器。A through-type current transformer main body having a tap for each fixed number of turns in the secondary winding, and a through-type current transformer main body having a tap for each fixed resistance value and connected in parallel to the secondary winding of the above-mentioned through-type current transformer main body, and each tap A resistor connected in a corresponding manner to each tap of the secondary winding, a saturable reactor connected in parallel to the resistor, a light emitting element connected between both ends of the saturable reactor, and light output from the light emitting element. A broadband current transformer for measuring current in a power transmission line, comprising an optical fiber for transmitting a signal and a receiver for receiving the optical signal transmitted by the optical fiber.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58198877A JPS6089761A (en) | 1983-10-24 | 1983-10-24 | Wide band current transofrmer measuring current of power transmission line |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58198877A JPS6089761A (en) | 1983-10-24 | 1983-10-24 | Wide band current transofrmer measuring current of power transmission line |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6089761A true JPS6089761A (en) | 1985-05-20 |
| JPH0345794B2 JPH0345794B2 (en) | 1991-07-12 |
Family
ID=16398404
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58198877A Granted JPS6089761A (en) | 1983-10-24 | 1983-10-24 | Wide band current transofrmer measuring current of power transmission line |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6089761A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN113241245A (en) * | 2021-05-10 | 2021-08-10 | 大连北方互感器集团有限公司 | Current transformer with constant-value resistor and preparation method thereof |
| WO2024135415A1 (en) * | 2022-12-19 | 2024-06-27 | 日置電機株式会社 | Zero flux type current sensor, and measuring device |
-
1983
- 1983-10-24 JP JP58198877A patent/JPS6089761A/en active Granted
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN113241245A (en) * | 2021-05-10 | 2021-08-10 | 大连北方互感器集团有限公司 | Current transformer with constant-value resistor and preparation method thereof |
| CN113241245B (en) * | 2021-05-10 | 2022-03-11 | 大连北方互感器集团有限公司 | Current transformer with constant-value resistor and preparation method thereof |
| WO2024135415A1 (en) * | 2022-12-19 | 2024-06-27 | 日置電機株式会社 | Zero flux type current sensor, and measuring device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0345794B2 (en) | 1991-07-12 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US6414578B1 (en) | Method and apparatus for transmitting a signal through a power magnetic structure | |
| RU2114439C1 (en) | Current measuring instrument | |
| JP2005524248A (en) | Power line high current inductive coupler and current transformer | |
| JPH10319053A (en) | Voltage insulating circuit for measuring instrument | |
| US4346340A (en) | Method and means for controlling the flux density in the core of an inductor | |
| US6437554B1 (en) | High current measurement system incorporating an air-core transducer | |
| JP3087155B2 (en) | Leakage current detection sensor | |
| GB2118000A (en) | Telecommunication system loop-back unit | |
| JPS6089761A (en) | Wide band current transofrmer measuring current of power transmission line | |
| CA1109172A (en) | Supply circuit for a subscriber's line circuit | |
| US10591514B2 (en) | Current measuring device protected against electrical surges when opening the circuit | |
| GB445977A (en) | Improvements in or relating to attenuation controlling electrical networks | |
| JP2520915Y2 (en) | Broadband current transformer for power line current measurement | |
| JP3221128B2 (en) | Current detector | |
| KR102439656B1 (en) | Electrical isolation device between input and output signals | |
| US4721863A (en) | Circuit for providing DC isolation between a pulse generator and a load | |
| US1866345A (en) | Current transformer with primary parallel resistance and flux leakage path | |
| JP3306599B2 (en) | Protection relay device | |
| US4392174A (en) | Electric protection device | |
| JPH01144359A (en) | Switching power circuit | |
| JP2708003B2 (en) | DC constant current power supply | |
| US5329414A (en) | Protective relay interface | |
| HU190346B (en) | Electric current measuring circuit arrangement | |
| SU1661652A1 (en) | Metering current-to-voltage converter | |
| SU1721524A1 (en) | Zero sequence current-to-voltage converter |