JPS645867Y2 - - Google Patents

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Publication number
JPS645867Y2
JPS645867Y2 JP17140681U JP17140681U JPS645867Y2 JP S645867 Y2 JPS645867 Y2 JP S645867Y2 JP 17140681 U JP17140681 U JP 17140681U JP 17140681 U JP17140681 U JP 17140681U JP S645867 Y2 JPS645867 Y2 JP S645867Y2
Authority
JP
Japan
Prior art keywords
magnetic core
current
current transformer
circuit
wound
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
JP17140681U
Other languages
Japanese (ja)
Other versions
JPS5879839U (en
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
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Priority to JP17140681U priority Critical patent/JPS5879839U/en
Publication of JPS5879839U publication Critical patent/JPS5879839U/en
Application granted granted Critical
Publication of JPS645867Y2 publication Critical patent/JPS645867Y2/ja
Granted legal-status Critical Current

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  • Breakers (AREA)

Description

【考案の詳細な説明】 この考案は回路しや断器の過電流継電器用変流
器に関し、とくに漏洩磁束による影響を少くして
変流特性が劣化するのを防ぎ、かつ小形に構成さ
れる過電流継電器用変流器に関するものである。
[Detailed description of the invention] This invention relates to a current transformer for overcurrent relays in circuits and disconnectors, and is designed to reduce the influence of leakage magnetic flux, prevent current transformation characteristics from deteriorating, and be compact. This invention relates to current transformers for overcurrent relays.

一般に回路しや断器内部に設置される過電流引
はずし装置は長限時引はずし、短限時引はずし、
瞬時引はずしの夫々の特性を備えており過負荷又
は短絡に際して適切な引はずし時限後、そのしや
断器の開閉機構を引はずし開路する。その過電流
継電器に引はずし信号を与えるセンサーとして通
常変流器が使用されるが、変流器は用途上比較的
高い電流領域まで入力−出力特性が直線性を保つ
て比例していくことが理想的である。しかして回
路しや断器内部に設置する過電流継電器用変流器
はスペース上の制約を受け回路しや断器の主電流
導体に接近して配置されるため高い電流領域にな
ると主電流導体の漏洩磁束を受け変流器の磁気鉄
心が飽和して過電流継電器用変流器の変流特性が
劣化して正確な引はずし電流値の信号が導出され
ず引はずし電流値に誤差を生ずる原因となつてい
る。
Overcurrent trip devices that are generally installed inside circuit breakers are long-time trip devices, short-time trip devices,
They have the characteristics of instantaneous tripping, and in the event of an overload or short circuit, the opening/closing mechanism of the disconnector is tripped to open the circuit after an appropriate tripping period. A current transformer is normally used as a sensor that provides a trip signal to the overcurrent relay, but due to its application, the input-output characteristic of a current transformer maintains linearity and remains proportional up to a relatively high current range. ideal. However, current transformers for overcurrent relays installed inside circuit breakers are space-constrained and are placed close to the main current conductor of the circuit breaker. The magnetic core of the current transformer becomes saturated due to the leakage magnetic flux of It is the cause.

第1図、第2図はこの考案の背景となる従来の
過電流継電器用変流器を備えた3極形回路しや断
器の一例を示す構造断面図ならびに背面図を示す
ものである。
FIGS. 1 and 2 show a structural cross-sectional view and a rear view of an example of a three-pole circuit breaker equipped with a conventional overcurrent relay current transformer, which is the background of this invention.

図において、回路しや断器の主電路は断面積が
矩形状の電源側端子導体1、固定コンタクト2な
らびに固定アーキングコンタクト3、これらと対
接する可動主コンタクト4ならびに可動アーキン
グコンタクト5、一端が可動主コンタクト4なら
びに可動アーキングコンタクト5に接続される可
撓リード板6、可撓リード板6の他端が接続され
る可撓リード板取付台7を介して負荷側端子導体
8への経路が形成されている。
In the figure, the main current path of the circuit and disconnector includes a power supply side terminal conductor 1 with a rectangular cross-sectional area, a fixed contact 2, a fixed arcing contact 3, a movable main contact 4 and a movable arcing contact 5 that are in contact with these, and one end of which is movable. A path to the load-side terminal conductor 8 is formed via a flexible lead plate 6 connected to the main contact 4 and the movable arcing contact 5, and a flexible lead plate mount 7 to which the other end of the flexible lead plate 6 is connected. has been done.

9は可動コンタクトホルダーで可動コンタクト
ホルダー軸10により可動コンタクトホルダー支
持板11に回動自在に軸支され開閉機構12によ
り可動主コンタクト4ならびに可動アーキングコ
ンタクト5と固定主コンタクト2ならびに固定ア
ーキングコンタクト3と接離するよう動かして回
路しや断器は開閉操作される。
Reference numeral 9 denotes a movable contact holder, which is rotatably supported on a movable contact holder support plate 11 by a movable contact holder shaft 10, and is connected to a movable main contact 4, a movable arcing contact 5, a fixed main contact 2, and a fixed arcing contact 3 by an opening/closing mechanism 12. Circuits and disconnectors are opened and closed by moving them toward and away from each other.

絶縁物よりなる回路しや断器の基板13より背
面に突出する各相の負荷側端子導体8を囲むよう
に過電流継電器用変流器14が装着され、各相の
主電路に流れる電流が変流器14の巻線比によつ
て変換された二次電流を静止形過電流継電器15
に与え、静止形過電流継電器15の設定電流値以
上になれば磁束切換磁気引はずしアクチユエータ
(図示しない)を作動させて開閉機構の釈放装置
を釈放して回路しや断器を開路させるように構成
される。過電流継電器用変流器14は積層鉄板に
より中央に一次導体として負荷側端子導体8が通
る開口部16を有するよう矩形状に組枠された磁
気鉄心17と二次巻線18とからなり磁気鉄心1
7は一対の上下に対応する二次巻線18を巻装す
る第一の磁気鉄心部17a,17a′と、一対の左
右に対応する二次導体18を巻装しない第二の磁
気鉄心部17b,17b′とよりなり、二つに分か
れた二次巻線18a,18bは直列に接続され
る。
An overcurrent relay current transformer 14 is installed so as to surround the load-side terminal conductor 8 of each phase that protrudes from the circuit board 13 of the circuit breaker made of an insulating material, and the current flowing in the main circuit of each phase is The secondary current converted by the winding ratio of the current transformer 14 is transferred to the static overcurrent relay 15.
When the current exceeds the set value of the static overcurrent relay 15, a magnetic flux switching magnetic trip actuator (not shown) is activated to release the release device of the opening/closing mechanism and open the circuit or disconnector. configured. The current transformer 14 for an overcurrent relay is composed of a magnetic core 17 and a secondary winding 18, which are assembled into a rectangular shape with a laminated iron plate having an opening 16 in the center through which the load-side terminal conductor 8 passes as a primary conductor. Iron core 1
Reference numeral 7 designates first magnetic core portions 17a, 17a' on which a pair of upper and lower secondary windings 18 are wound, and a second magnetic core portion 17b on which a pair of left and right secondary conductors 18 are not wound. , 17b', and the two divided secondary windings 18a and 18b are connected in series.

第2図に示すように回路しや断器の小形化のた
めに各相の負荷側端子導体8は隣接する他相の負
荷側端子導体との相間距離が許容される最短に近
く設定されているため変流器14は小形に形成さ
れるが、尚変流器14の第二の磁気鉄心部17
b,17b′と開口部16を通る負荷側端子導体8
との空間が不充分であり、例えば大電流時に変流
器14の第二の磁気鉄心部17b,17b′には磁
気鉄心17を環流する磁束φに部分的にループを
形成する漏洩磁束φlが加わつて磁束密度が高ま
り、第二の磁気鉄心部17b,17b′は急速に飽
和するため、正確な二次出力を過電流継電器15
に与えずに引はずし電流値に誤差を生ずる。即
ち、第3図(横軸に一次通電々流を縦軸に二次出
力電流をとる)に示す変流器の一次電流と二次電
流の変流特性において変流器の理想的な特性を直
線19で示されているが、従来装置における変流
器の特性は曲線20で示されるように高電流領域
において誤差が大きいという欠点がある。
As shown in Figure 2, the load-side terminal conductor 8 of each phase is set as close as possible to the shortest allowable distance between the load-side terminal conductor 8 of each phase and the load-side terminal conductor of the adjacent other phase, in order to reduce the size of the circuit and disconnector. Therefore, the current transformer 14 is formed small, but the second magnetic core portion 17 of the current transformer 14
b, 17b' and the load side terminal conductor 8 passing through the opening 16
For example, at the time of a large current, leakage magnetic flux φl that partially forms a loop in the magnetic flux φ circulating through the magnetic core 17 is generated in the second magnetic core portions 17b, 17b' of the current transformer 14. As a result, the magnetic flux density increases and the second magnetic core portions 17b and 17b' rapidly saturate, so that accurate secondary output is transmitted to the overcurrent relay 15.
This will cause an error in the trip current value. In other words, the ideal characteristics of a current transformer are expressed in the current transformation characteristics of the primary current and secondary current of the current transformer shown in Figure 3 (the horizontal axis represents the primary current current and the vertical axis represents the secondary output current). Although shown by a straight line 19, the characteristics of the current transformer in the conventional device have a drawback of large errors in the high current region, as shown by a curve 20.

それゆえに、この考案の主たる目的は上述の欠
点が改善された変流特性をもつ回路しや断器の過
電流継電器用変流器を提供することである。
Therefore, the main object of this invention is to provide a current transformer for overcurrent relays for circuit breakers and circuit breakers, which has current transformation characteristics that are improved from the above-mentioned drawbacks.

この考案は要約すれば過電流継電器用変流器の
積層鉄板により中心に開口を有する矩形状に組枠
された磁気鉄心本体において、二次巻線を巻装し
ない第二の磁気鉄心部に同一の積層方向に積層さ
れる補助鉄心を装着し、第二の磁気鉄心部の断面
積を増大することにより第二の磁気鉄心部におい
て磁気鉄心本体を環流せず部分的にループを形成
する漏洩磁束を受けることに起因する飽和限度を
上昇させ変流特性を改善するよう構成したもので
ある。
In summary, this idea is based on a magnetic core body that is assembled into a rectangular shape with an opening in the center using laminated iron plates of a current transformer for overcurrent relays. By installing an auxiliary core that is laminated in the stacking direction of the magnetic core and increasing the cross-sectional area of the second magnetic core, leakage magnetic flux that does not circulate through the magnetic core body but partially forms a loop in the second magnetic core is reduced. This structure is designed to increase the saturation limit caused by the current flow and improve the current characteristics.

この考案の上述の目的およびその他の目的と特
徴は以下図面を参照して行なう詳細な説明から一
層明らかとなろう。
The above-mentioned objects and other objects and features of the present invention will become clearer from the detailed description given below with reference to the drawings.

第4図は本案実施の過電流継電器用変流器の要
部斜視図であつて、第1図、第2図相当部分は同
一符号で示すと変流器14の矩形状に組枠された
磁気鉄心本体17の他相の主電路の端子導体と隣
接する二次巻線18を巻装しない第二の磁気鉄心
部17b,17b′に、積層された補助鉄心21を
第二の磁気鉄心部17b,17b′の積層鉄板の積
層方向と同方向に積層されるよう装着したもので
あつてこれは隣接する他相との限られた相間スペ
ースで磁気鉄心の断面積を増すのに有効である。
FIG. 4 is a perspective view of the main parts of the current transformer for overcurrent relay according to the present invention, and the parts corresponding to FIGS. The laminated auxiliary core 21 is attached to the second magnetic core portions 17b, 17b' which are not wound with the secondary winding 18 adjacent to the terminal conductor of the main circuit of the other phase of the magnetic core body 17. It is installed so that it is laminated in the same direction as the laminated iron plates 17b and 17b', and this is effective for increasing the cross-sectional area of the magnetic core in a limited interphase space with other adjacent phases. .

本案は上記の如く、多極形回路しや断器の比較
的近接して配置される各相の主電路の端子導体を
夫々一次導体として積層鉄板により中心に開口部
16を有する矩形状に組枠された磁気鉄心本体1
7内を貫通させ、磁気鉄心本体17は一対の対応
する二次巻線18を巻装する第一の磁気鉄心部1
7a,17a′と、他相の主電路の端子導体が、隣
接する側の一対の対応する二次巻線18を巻装し
ない第二の磁気鉄心部17b,17b′とにより構
成され、磁気鉄心本体17の第二の磁気鉄心部1
7b,17b′には同一の積層方向に積層されるよ
うに補助鉄心21を装着したものであるので従来
なら磁気鉄心本体17を環流する磁束φに部分的
にループを形成する漏洩磁束φlが加わつて最も磁
束密度の高くなるような第二の磁気鉄心部17
b,17b′における断面積が補助鉄心21を設け
ることにより増大されるため、第二磁気鉄心部の
飽和限界が高くなり磁気鉄心本体17を環流する
磁束φの阻止が少くなること、ならびに回路しや
断器の相間寸法を広げることなく、又、主電路の
端子導体の幅を狭めることなく変流器の特性改善
のために必要な第二の磁気鉄心部の断面積を増加
させることにより、第3図に示す従来装置の変流
特性曲線20を理想直線19に近づくよう改善さ
れた変流特性曲線22を得たものである。
As described above, in this case, the terminal conductors of the main circuits of each phase, which are arranged relatively close to each other in multipolar circuits and circuit breakers, are assembled into a rectangular shape with an opening 16 in the center using laminated iron plates as primary conductors. Framed magnetic core body 1
7, and the magnetic core body 17 is wound with a pair of corresponding secondary windings 18.
7a, 17a', and a second magnetic core part 17b, 17b' in which the terminal conductor of the main electric circuit of the other phase is not wound with a pair of corresponding secondary windings 18 on the adjacent side. Second magnetic core portion 1 of main body 17
Since the auxiliary core 21 is attached to 7b and 17b' so as to be laminated in the same lamination direction, the leakage magnetic flux φl that partially forms a loop is added to the magnetic flux φ circulating in the magnetic core body 17 in the conventional case. The second magnetic core portion 17 has the highest magnetic flux density.
Since the cross-sectional area at b and 17b' is increased by providing the auxiliary core 21, the saturation limit of the second magnetic core portion becomes higher, and the blockage of the magnetic flux φ circulating through the magnetic core body 17 is reduced. By increasing the cross-sectional area of the second magnetic core, which is necessary for improving the characteristics of the current transformer, without increasing the phase-to-phase dimensions of the circuit or disconnector, or reducing the width of the terminal conductor of the main circuit, A current transformation characteristic curve 22 is obtained by improving the current transformation characteristic curve 20 of the conventional device shown in FIG. 3 so that it approaches the ideal straight line 19.

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

第1図、第2図はこの考案の背景となる従来装
置の変流器を備えた回路しや断器の一例を示す構
造断面図ならびに背面図である。第3図は変流器
の一次電流と二次電流との相関を示す変流特性
図、第4図は本案装置の要部を示す斜視図であ
る。 図で8は端子導体、14は過電流継電器用変流
器、16は開口部、17は磁気鉄心本体、17
a,17a′は第一の磁気鉄心部、17b,17
b′は第二の磁気鉄心部、18a,18bは二次巻
線、21は補助鉄心。
FIGS. 1 and 2 are a structural cross-sectional view and a rear view showing an example of a circuit or breaker equipped with a current transformer, which is a conventional device that forms the background of this invention. FIG. 3 is a current transformation characteristic diagram showing the correlation between the primary current and secondary current of the current transformer, and FIG. 4 is a perspective view showing the main parts of the device of the present invention. In the figure, 8 is a terminal conductor, 14 is a current transformer for overcurrent relay, 16 is an opening, 17 is a magnetic core body, 17
a, 17a' are the first magnetic core parts, 17b, 17
b' is a second magnetic core, 18a and 18b are secondary windings, and 21 is an auxiliary core.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 多極形回路しや断器の比較的近接して配置され
る各相の主電路の端子導体を夫々一次導体として
積層鉄板により中心に開口部を有し矩形状に組枠
された磁気鉄心本体内を貫通させ、前記磁気鉄心
本体は一対の対応する二次巻線を巻装する第一の
磁気鉄心部と、一対の対応する二次巻線を巻装し
ない隣接の第二の磁気鉄心部とより構成され、前
記磁気鉄心本体の第二の磁気鉄心部に同一の積層
方向をもつて積層されるように補助鉄心を装着し
てなる回路しや断器の過電流継電器用変流器。
A magnetic core body assembled into a rectangular shape with an opening in the center using laminated iron plates with the terminal conductors of the main circuits of each phase placed relatively close to each other as primary conductors of multipolar circuits and disconnectors. a first magnetic core part on which a pair of corresponding secondary windings are wound, and an adjacent second magnetic core part on which a pair of corresponding secondary windings are not wound. A current transformer for an overcurrent relay for a circuit breaker, comprising: an auxiliary core attached to the second magnetic core portion of the magnetic core body so as to be laminated in the same lamination direction.
JP17140681U 1981-11-19 1981-11-19 Current transformer for overcurrent relay for circuit breakers Granted JPS5879839U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17140681U JPS5879839U (en) 1981-11-19 1981-11-19 Current transformer for overcurrent relay for circuit breakers

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17140681U JPS5879839U (en) 1981-11-19 1981-11-19 Current transformer for overcurrent relay for circuit breakers

Publications (2)

Publication Number Publication Date
JPS5879839U JPS5879839U (en) 1983-05-30
JPS645867Y2 true JPS645867Y2 (en) 1989-02-14

Family

ID=29963331

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17140681U Granted JPS5879839U (en) 1981-11-19 1981-11-19 Current transformer for overcurrent relay for circuit breakers

Country Status (1)

Country Link
JP (1) JPS5879839U (en)

Also Published As

Publication number Publication date
JPS5879839U (en) 1983-05-30

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