[go: up one dir, main page]

JPS6350765A - Optical fiber zero phase current transformer - Google Patents

Optical fiber zero phase current transformer

Info

Publication number
JPS6350765A
JPS6350765A JP61192748A JP19274886A JPS6350765A JP S6350765 A JPS6350765 A JP S6350765A JP 61192748 A JP61192748 A JP 61192748A JP 19274886 A JP19274886 A JP 19274886A JP S6350765 A JPS6350765 A JP S6350765A
Authority
JP
Japan
Prior art keywords
optical fiber
phase current
current transformer
zero
light
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
Application number
JP61192748A
Other languages
Japanese (ja)
Other versions
JPH063475B2 (en
Inventor
Yoshiaki Tomaki
東槙 良旺
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP61192748A priority Critical patent/JPH063475B2/en
Publication of JPS6350765A publication Critical patent/JPS6350765A/en
Publication of JPH063475B2 publication Critical patent/JPH063475B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Locating Faults (AREA)
  • Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)

Abstract

PURPOSE:To obtain a small-sized light wt. safe zero phase current transformer, by winding an optical fiber around a three-phase distribution line so as to surround the same and connecting a signal converter between both ends thereof. CONSTITUTION:An optical fiber zero phase current transformer 2A is constituted of the single mode optical fiber 4 wound around a three-phase distribution line 1 and the signal converter 5 connected between both ends of the optical fiber 4. The converter 5 has a light emitting element 6, a polarizer 7, a light receiving element 9 and an electronic circuit 10 mounted therein. The light emitted from the element 6 is linearly polarized by the polarizer 7 permitting the passage only of light of a wave component in one direction to be incident to the optical fiber 4. When a magnetic field is applied to the optical fiber 4, the plane of polarization thereof rotates in proportion to the magnetic field applied by Faraday effect. Now, when an earth accident is generated, as the result of the flowing of a zero phase current to the distribution line 1, the circumference integration of the magnetic field surrounding said line 1 becomes the value proportional thereto and the plane of polarization of the linearly polarized light passing through the optical fiber 4 also receives the rotation proportional to the zero phase current and the electric signal photoelectrically converted by the element 9 through the detector 8 also changes to make it possible to detect the zero phase current.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、配電線%Tlc3相配電線の地絡事故を検
出する光ファイバ零相変流器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to an optical fiber zero-phase current transformer for detecting a ground fault in a %Tlc three-phase distribution line.

〔従来の技術〕[Conventional technology]

第3図は例えば昭和37年を月に電気書院から発行され
た池田三穂司著「計器用変成器」の第79ページに示さ
れた従来の零相変流器を示す構成図であり、図において
fハは3相配電線であって、各相電線(/&)、(/b
)A/c)から成る。Cコ)は従来の零相変流器であっ
て、J相配電@(/)が貫通される鉄心CMおよびこの
鉄心(s/)VC巻回された一次巻線(コ2)から成る
。(,71は零相変流器(,2)の一次巻線(2コ)の
両端間に接続される保hリレー等の一次負担である。
Figure 3 is a configuration diagram showing a conventional zero-phase current transformer, as shown on page 79 of ``Instrument Transformers'' by Mihoji Ikeda, published by Denkishoin in April 1960, for example. , f is a three-phase distribution line, and each phase line (/&), (/b
)A/c). C) is a conventional zero-phase current transformer, consisting of an iron core CM through which the J-phase power distribution @ (/) is passed, and a primary winding (C 2) wound with VC on this iron core (s/). (, 71 is a primary load such as an h-holding relay connected between both ends of the primary windings (2) of the zero-phase current transformer (, 2).

従来の零相変流器(コ)は上述したように構成されてお
り、まず零相電流を検出する原理について説明する。3
相配電線(/lの各相電線(/a)、(/b’J、(I
C>を流れる電流は定常時には正相分と逆相分のみであ
る。鉄心(2/)に誘起される磁束が各相の正相分と逆
相分の電流に比例した磁界を合成した磁界によって誘起
されるので、鉄心(コ/)中の定常時の磁束は零である
。そのため、鉄心(s/)K巻回した二次巻線(ココ)
には電流が流れない。
The conventional zero-sequence current transformer (C) is configured as described above, and first, the principle of detecting zero-sequence current will be explained. 3
Each phase distribution line (/l) (/a), (/b'J, (I
In steady state, the current flowing through C> is only the positive phase component and the negative phase component. The magnetic flux induced in the iron core (2/) is induced by a magnetic field that is a combination of magnetic fields proportional to the positive and negative phase currents of each phase, so the magnetic flux in the iron core (2/) at steady state is zero. It is. Therefore, the secondary winding (here) with K windings on the iron core (s/)
No current flows through.

次に、J相配電線(ハに地絡事故が発生すると、3相分
の電流を合成しても零にならない零相分電流が流れるた
め、鉄心(コ/)中に磁束が誘起され、2次巻線(ココ
)にけ零相N流に比例した二次電流が流れる。
Next, when a ground fault occurs in the J-phase distribution line (C), a zero-phase current that does not become zero even if the three-phase currents are combined flows, so magnetic flux is induced in the iron core (C/), A secondary current proportional to the zero-phase N current flows in the next winding (here).

零相変流器【コ)は、3相配[線(1)を−括して包囲
高感度で検出して3相配電線(ハの地絡事故を検出する
ものであり、変電所の構内に設けられて地絡事故が発生
した3相配電線(ハを切離して事故の拡大を防いでいる
The zero-phase current transformer (C) is used to detect ground faults in the three-phase distribution line (C) by enclosing the three-phase distribution line (1) with high sensitivity and detecting ground faults in the three-phase distribution line (C). The 3-phase distribution line (C) where the ground fault occurred was disconnected to prevent the accident from spreading.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

近年、地絡事故が発生した場合でも、できるだけ停電区
間を限定し、しかも復旧時間を短くするため、事故点を
早期にかつ正確に発見できる手段が要望されている。こ
のため、零相変流器(−)を変電所構内だけでなく、J
相配亀線(ハの途中に多数個設置する必要がある。しか
し、従来の零相変流器(コ)は3相配電線(ハを7個の
鉄心(−/)で包囲する構造のため、屋外の配電柱の上
に設置するには鉄心(コ/)が大型化しすぎ、また導電
体の鉄心(2/)で3相配電線(ハを包囲するため、落
雷等の発生時に事故が拡大する原因となるなどの問題点
があった。
In recent years, even when a ground fault occurs, there has been a demand for means that can quickly and accurately locate the point of the fault in order to limit the power outage section as much as possible and shorten the restoration time. For this reason, zero-phase current transformers (-) are installed not only in substation premises, but also in
It is necessary to install many pieces in the middle of the phase distribution line (C). However, because the conventional zero-phase current transformer (C) has a structure in which the three-phase distribution line (C) is surrounded by seven iron cores (-/), The iron core (C/) is too large to be installed on an outdoor distribution pole, and the conductive iron core (2/) surrounds the three-phase distribution line (C), which increases the risk of accidents in the event of a lightning strike, etc. There were problems such as causes.

この発明は、このような問題点を解決するためになされ
たもので配電柱の上に設置するのに適した、軽量で、し
かも事故を拡大あるいは誘発する恐れのない光ファイバ
零相変流器を得ることを目的とする。
This invention was made to solve these problems, and provides an optical fiber zero-phase current transformer that is suitable for installation on power distribution poles, is lightweight, and has no risk of aggravating or inducing accidents. The purpose is to obtain.

〔問題点を解決するだめの手段〕[Failure to solve the problem]

この発明に係る光ファイバ零相変流器は、従来の零相変
流器の鉄心と一次巻線に代って、3相配電線を包囲する
ように光ファイバを巻回し、その両端間に発光素子およ
び受光素子を含む信号変換器を接続したものである。
The optical fiber zero-phase current transformer according to the present invention winds an optical fiber to surround a three-phase distribution line instead of the iron core and primary winding of a conventional zero-phase current transformer, and emits light between both ends of the optical fiber. A signal converter including an element and a light receiving element is connected.

〔作 用〕[For production]

光ファイバは、その中を通過する直線偏光の偏波面が光
ファイバに印加される磁界に比例して回転するファラデ
ー効果を有するため、磁界の測定に利用できる。
Optical fibers can be used to measure magnetic fields because they have a Faraday effect in which the plane of polarization of linearly polarized light passing through them rotates in proportion to the magnetic field applied to the optical fibers.

〔実施例〕〔Example〕

第1図はこの発明の一実施例を一部ブロック図で示す構
成図であり、第3図の場合と同様K(ハはJ相配を線で
、(ia)、(ib)、(/c)は3相配電線cノ)の
各相配線である。(コA)はこの発明に係る光ファイバ
零相変流器であって1,7相配電線(ハを包囲するよう
にこの3相配電線(ハに巻回されたシングルモード光フ
ァイバ〔以下、光ファイハト云う。〕(り)およびこの
光ファイバ(glの両端間に接続された信号変換器(s
)から成る。この信号変換器(jlけ発光ダイオード等
の発光素子(6)、この発光素子(6)の出力側と光フ
ァイバKlの一端との間に接続を電気に変換する受光素
子(ql、およびこの受光素子(?)で得た電気信号な
零相電流に比例する信号に変換する電子回路(10)を
内蔵している。
FIG. 1 is a block diagram partially showing the configuration of an embodiment of the present invention, and as in the case of FIG. ) is each phase wiring of the three-phase distribution line c). (A) is an optical fiber zero-phase current transformer according to the present invention, in which a single-mode optical fiber (hereinafter referred to as optical A signal converter (s) connected between both ends of this optical fiber (gl)
). This signal converter (jl) includes a light emitting element (6) such as a light emitting diode, a light receiving element (ql) that converts the connection between the output side of this light emitting element (6) and one end of the optical fiber Kl, and this light receiving element (ql), which converts the connection into electricity. It has a built-in electronic circuit (10) that converts the electric signal obtained by the element (?) into a signal proportional to the zero-sequence current.

によって直線偏光にされた後に光ファイバ(鏑へその一
端から入射てれる。光ファイバ(lIlに磁界が印加さ
れている場合には、光ファイバ(り)のファラデー効果
により、1縁偏光が光ファイバC≠)の中を進む間に、
その偏波面は印加磁界に比例して回転する。偏波面の回
転を受けかつ元ファイバ(glの他端から出射された直
線偏光は、検光子(t)を通して受光素子(9)で電気
信−号に変換される。しかしながら、検光子(ざ)が一
方向の波4)J1成分の光のみな通すため、検光子(に
)を通過する光のパ17−は偏波面の回転角! ic 
応じて変化し、従って受光素子(9)で得られた電気信
号も変化する。
After being made into linearly polarized light by While moving through C≠),
Its plane of polarization rotates in proportion to the applied magnetic field. The linearly polarized light that has undergone rotation of the plane of polarization and is emitted from the other end of the original fiber (gl) passes through the analyzer (t) and is converted into an electrical signal by the light receiving element (9). Waves in one direction 4) Only the J1 component of light passes through, so the path of the light passing through the analyzer is the rotation angle of the plane of polarization! ic
Accordingly, the electric signal obtained by the light receiving element (9) also changes.

定常時には5.7相配を線を包囲する磁界を周回積分す
れば零となるため、3相配電線(ハな包囲するように巻
回された元ファイバ(ダ1を通過する1壱偏光の受ける
偏波面の回転も光ファイバ出射端では零となっている。
In steady state, if the magnetic field surrounding the 5.7-phase wiring is integrated around the line, it becomes zero, so the polarization received by the polarized light passing through the 3-phase distribution line The rotation of the wavefront also becomes zero at the output end of the optical fiber.

しかしながら、3相配電線(ハに地絡事故が発生すると
、3相配電線(ハVc5厚相電流が流れる結果、これを
包囲する磁界の周回積分は零相電流に比例する値となり
、光ファイバ(≠)を通過する直線偏光の偏波面も零相
電流て比例した回転を受け、検光子ffflを通して受
光素子(テ)で光電変換された電気信号も変化するため
、零相電流の検出が可能となる。
However, when a ground fault occurs in the 3-phase distribution line (C), as a result of the flow of the Vc5 thick phase current, the circuit integral of the magnetic field surrounding it becomes a value proportional to the zero-sequence current, and the optical fiber (≠) The polarization plane of the linearly polarized light passing through is also rotated in proportion to the zero-sequence current, and the electrical signal photoelectrically converted by the light receiving element (te) through the analyzer fffl also changes, making it possible to detect the zero-sequence current.

次に、この発明の他の実施例(コB)を一部フe+ツク
図で示す構成図である第一図について説明する。(t*
)は3相配電線を包囲するように巻回されかつ表面に磁
歪材料が塗布されたシングルモード光ファイバ、(’t
B”)はこの磁歪材料塗布陽光ファイバ(4(A’lと
同じ処理をしかつ同一長さにした光ファイバ、(//)
は発光素子(6)と磁歪材料塗布陽光ファイバ(ψA)
の一端との間に接続された光分配器、(/コ)はp磁歪
材料塗布陽光承ファイバζψA)の他端と受光素子(?
)との間に接続された光合波器である。発光素子(6)
から出た光は光分配器(//)で分けられ、一方は磁歪
材料塗布陽光ファイバ(taA)を通り、他方は光分配
器(l/)と光合成器(/−)との間て接続された磁歪
材料上布済光ファイバ(uB”)を通って光合波器(/
コ)において磁歪材料塗布陽光ファイバ(u人)からの
光と合成されて受光素子(り1で光電変換される。
Next, FIG. 1, which is a block diagram partially showing another embodiment (B) of the present invention, will be described. (t*
) is a single-mode optical fiber that is wound around a three-phase distribution line and whose surface is coated with magnetostrictive material.
B") is this optical fiber coated with magnetostrictive material (4
is a light emitting element (6) and a solar fiber coated with magnetostrictive material (ψA)
The optical distributor (/) is connected between one end of the optical fiber ζψA) coated with a p-magnetostrictive material and the other end of the photodetector (?A).
) is an optical multiplexer connected between the Light emitting element (6)
The light emitted from the is split by a light splitter (//), one passes through a magnetostrictive material-coated optical fiber (taA), and the other is connected between the light splitter (l/) and the photosynthesizer (/-). An optical multiplexer (/
It is combined with the light from the magnetostrictive material-coated solar fiber (U) in the photodetector element (R1) and photoelectrically converted.

通常、磁歪材料塗布陽光ファイバ(rH,’+、(qs
)を通過する光は光ファイバ長が同じであるため同時に
光合波器(/コ)VC達するが、3相配電線(ハの事故
時ては、磁歪材料塗布陽光ファイバ(uA’)のこれに
よって光ファイバ長が変化するため、磁歪材料塗布陽光
ファイバ(u*)を通過する光と磁歪材料塗布陽光ファ
イバ(uB)を通過する光が光合波器(/コ)VC達す
る時間に差を生じるため、2つの光の間に光の位相差を
生じる。この位相差は零相電流の大きさに比例するため
、この位相差を検出することにより、J相 出することが可能てなる。この方法はマツハツエンダ−
干渉系と称されるが、光の位相差を電気出力として取り
出す方法としてヘテロゲイン検波法あるいはホモダイン
検波法が用いられ、また、発光素子および受光素子とし
てレーザーおよびアバランシェホトダイオードが使用さ
れる。
Usually, a solar fiber coated with magnetostrictive material (rH,'+, (qs
) Since the optical fiber lengths are the same, the light that passes through the optical multiplexer (/co) VC reaches the optical multiplexer (/co) at the same time. Because the fiber length changes, there is a difference in the time between the light passing through the magnetostrictive material-coated optical fiber (u*) and the light passing through the magnetostrictive material-coated optical fiber (uB), reaching the optical multiplexer (/co) VC. A phase difference occurs between the two lights. This phase difference is proportional to the magnitude of the zero-sequence current, so by detecting this phase difference, it is possible to output the J phase. This method Matsuha Tsuender
Although called an interference system, a heterogain detection method or a homodyne detection method is used as a method for extracting the phase difference of light as an electrical output, and a laser and an avalanche photodiode are used as a light emitting element and a light receiving element.

〔発明の効果〕〔Effect of the invention〕

この発明は、以上説明したようIc、  J相を包囲す
る光ファイバ並びに発光素子および受光素子を含む信号
変換器を設けたことにより、従来のように鉄心を使用し
なくても3相配電線の零相電流を検出できるので、小形
、軽量で、かつ光ファイバが絶縁物であるため安全な光
ファイバ零相変流器が得られ、従来困難であった配電柱
上への設置も可能となる効果がある。
As explained above, by providing an optical fiber surrounding the Ic and J phases, and a signal converter including a light emitting element and a light receiving element, the present invention can reduce the zero of a three-phase distribution line without using an iron core as in the conventional case. Since the phase current can be detected, an optical fiber zero-phase current transformer that is small, lightweight, and safe because the optical fiber is an insulator can be obtained, and it can also be installed on distribution poles, which was previously difficult. There is.

【図面の簡単な説明】 第1図はこの発明の一実施例を一部ブロック図で示す構
成図、第1図は他の実施例を一部ブロック図で示す構成
図、第3図は従来の零相変流器を示す構成図である。 図において、(ハはJ相配配置紐線(コA)と(sB”
)は光ファイバ零相変流器、(q)は光ファイバ、(t
tA)と(’IB’)Y′i磁歪材料塗布済光ファイバ
、(5)と(5A)は信号変換器、(6)は発光素子、
(7)は偏光子、(g)は検光子、(?1は受光素子、
(10)は電子回路、(//)は光分配器、(/コ’)
f′i光合成器である。 なお、図中、同一符号は同−又は相当部分を示す。 1 ;3袷rl−を線 2A   た7フイlで1L相1虻烹呑4   穴7フ
イハ0 2B   :  fファイバ”零l唱1ヒ言ミ4A、4
B     裁量をオ↑十璧iイIilトηA7フイハ
゛11  ° 光うt励こ器 12   光ケ成券
[BRIEF DESCRIPTION OF THE DRAWINGS] Fig. 1 is a block diagram partially showing one embodiment of the present invention; Fig. 1 is a block diagram partially showing another embodiment; Fig. 3 is a conventional block diagram; FIG. 2 is a configuration diagram showing a zero-phase current transformer of FIG. In the figure, (C is the J phase arrangement string line (CoA) and (sB”
) is an optical fiber zero-phase current transformer, (q) is an optical fiber, (t
tA) and ('IB') Y'i magnetostrictive material coated optical fibers, (5) and (5A) are signal converters, (6) is a light emitting element,
(7) is a polarizer, (g) is an analyzer, (?1 is a light receiving element,
(10) is an electronic circuit, (//) is an optical distributor, (/ko')
f'i is a photosynthesizer. In addition, in the figures, the same reference numerals indicate the same or corresponding parts. 1 ;3 line RL- with line 2A 7 fill with 1L phase 1 hole 7 fill 0 2B: f fiber” zero chant 1 whisper 4A, 4
B Discretion ↑ 10 perfect i Iil to ηA7

Claims (3)

【特許請求の範囲】[Claims] (1)3相配電線を包囲するように巻回された光ファイ
バと、この光ファイバの両端間に接続され発光素子およ
び受光素子を含む信号変換器とを備えたことを特徴とす
る光ファイバ零相変流器。
(1) An optical fiber zero characterized by comprising an optical fiber wound so as to surround a three-phase distribution line, and a signal converter connected between both ends of the optical fiber and including a light emitting element and a light receiving element. Phase current transformer.
(2)信号変換器は、発光素子の出力側と光ファイバの
一端との間に接続された偏光子、および前記光ファイバ
の他端と受光素子の入力側との間に接続された検光子を
含むことを特徴とする特許請求の範囲第1項記載の光フ
ァイバ零相変流器。
(2) The signal converter includes a polarizer connected between the output side of the light emitting element and one end of the optical fiber, and an analyzer connected between the other end of the optical fiber and the input side of the light receiving element. An optical fiber zero-phase current transformer according to claim 1, characterized in that the optical fiber zero-phase current transformer includes:
(3)光ファイバはシングルモード光ファイバ表面に磁
歪材料を塗布したものであり、信号変換器はマツハツエ
ンダー干渉を利用したものであることを特徴とする特許
請求の範囲第1項記載の光ファイバ零相変流器。
(3) The optical fiber according to claim 1, wherein the optical fiber is a single mode optical fiber whose surface is coated with a magnetostrictive material, and the signal converter utilizes Matsuhatsu-Ender interference. Fiber zero-phase current transformer.
JP61192748A 1986-08-20 1986-08-20 Optical fiber zero-phase current transformer Expired - Lifetime JPH063475B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61192748A JPH063475B2 (en) 1986-08-20 1986-08-20 Optical fiber zero-phase current transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61192748A JPH063475B2 (en) 1986-08-20 1986-08-20 Optical fiber zero-phase current transformer

Publications (2)

Publication Number Publication Date
JPS6350765A true JPS6350765A (en) 1988-03-03
JPH063475B2 JPH063475B2 (en) 1994-01-12

Family

ID=16296395

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61192748A Expired - Lifetime JPH063475B2 (en) 1986-08-20 1986-08-20 Optical fiber zero-phase current transformer

Country Status (1)

Country Link
JP (1) JPH063475B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59190247U (en) * 1983-06-03 1984-12-17 長友 正明 Warm utensil

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62150673U (en) * 1986-03-14 1987-09-24

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62150673U (en) * 1986-03-14 1987-09-24

Also Published As

Publication number Publication date
JPH063475B2 (en) 1994-01-12

Similar Documents

Publication Publication Date Title
CN102753986B (en) For the MS master-slave fibre optic current sensor of differential protection scheme
JPH023370B2 (en)
JPS6350765A (en) Optical fiber zero phase current transformer
Aikawa et al. Development of new concept optical zero-sequence current/voltage transducers for distribution network
CN109581024B (en) Optical fiber current transformer
JPS6350761A (en) Optical fiber zero phase current transformer
RU2321000C2 (en) Fiber-optic current transformer
Yoshida et al. New fault locating system for air-insulated substations using optical current detector
Ferdous et al. Cable fault detection: optical fiber current sensor cable link noise reduction
Minkner et al. A new flexible fiber optic current-measuring-system for AC-and DC-current in high voltage systems
Zapella et al. Solving old problems with new technology: How to monitor and measure GIC and OPD currents
KR100659564B1 (en) Optical current sensor
JPH0619396B2 (en) Zero-phase current transformer
JPS63313074A (en) Zero-phase current transformer
JPH0519818Y2 (en)
Nakamura et al. Development of fault section detecting system for gas insulated transmission lines
JPS63274322A (en) Zero-phase current transformer
JPS62110162A (en) Zero-sequence current detection device
JPH0668509B2 (en) Zero-phase voltage detector for three-phase power line
JPH01304363A (en) Optical zero-phase current transformer
JPH08262065A (en) Optical current transformer
JP2673573B2 (en) Zero-phase current detector
JPH02108976A (en) Double rated type light applied current sensor
Kesri et al. Latest Trends in Non-Conventional Instrument Transformers
JPH0641963B2 (en) Optical zero-phase current transformer