JP5918424B2 - Magnetic contactor - Google Patents

Magnetic contactor Download PDF

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JP5918424B2
JP5918424B2 JP2015119557A JP2015119557A JP5918424B2 JP 5918424 B2 JP5918424 B2 JP 5918424B2 JP 2015119557 A JP2015119557 A JP 2015119557A JP 2015119557 A JP2015119557 A JP 2015119557A JP 5918424 B2 JP5918424 B2 JP 5918424B2
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fixed contact
contact
arc extinguishing
arc
movable contact
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JP2015159131A (en
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立川 裕之
裕之 立川
磯崎 優
優 磯崎
鹿志村 修
修 鹿志村
幸悦 高谷
幸悦 高谷
中 康弘
康弘 中
雄二 柴
雄二 柴
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Fuji Electric Co Ltd
Fuji Electric FA Components and Systems Co Ltd
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Fuji Electric Co Ltd
Fuji Electric FA Components and Systems Co Ltd
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Description

本発明は、電流路に介挿された固定接触子及び可動接触子を備えた電磁接触器に関し、固定接触子及び可動接触子の開極時すなわち電流遮断時に発生するアークを容易に消弧するようにしたものである。   The present invention relates to an electromagnetic contactor including a stationary contact and a movable contact inserted in a current path, and easily extinguishes an arc generated when the stationary contact and the movable contact are opened, that is, when a current is interrupted. It is what I did.

電気自動車やハイブリッド車等の高圧の直流電源回路に用いられる電磁接触器として、従来、図24及び図25に示す構成を有するプランジャ型電磁継電器が提案されている(例えば特許文献1参照)。このプランジャ型電磁継電器は、ハウジング100に所定間隔を保って配設された一対の固定接点101,102と、これら一対の固定接点101,102に対向して接離可能に配設された一対の可動接点103,104を両端に備えた可動接点担持体105とを備えている。また、プランジャ型電磁継電器は、一対の固定接点101,102及び一対の可動接点103,104間の接点ギャップにそれぞれ生じるアークを消弧するための一対の消弧手段106、107を備えている。   Conventionally, as an electromagnetic contactor used in a high-voltage DC power supply circuit such as an electric vehicle or a hybrid vehicle, a plunger type electromagnetic relay having a configuration shown in FIGS. 24 and 25 has been proposed (for example, see Patent Document 1). This plunger-type electromagnetic relay includes a pair of fixed contacts 101 and 102 disposed at a predetermined interval in the housing 100 and a pair of contacts disposed so as to be able to contact and separate from the pair of fixed contacts 101 and 102. A movable contact carrier 105 having movable contacts 103 and 104 at both ends is provided. The plunger type electromagnetic relay includes a pair of arc extinguishing means 106 and 107 for extinguishing arcs generated in the contact gaps between the pair of fixed contacts 101 and 102 and the pair of movable contacts 103 and 104, respectively.

ここで、一対の消弧手段106,107のそれぞれは、接点ギャップを挟んで対面する磁極面の極性が反対となるようにハウジングに固定された一対の永久磁石で構成されている。
上記従来例のアーク消弧原理を図25〜図28を用いて説明する。今、図25に示すように、可動接点担持体105が、固定接点101,102に可動接点103,104を接触させて固定接点101から可動接点103,104を通じて固定接点102に向かう電流が流れる通電状態にあるものとする。この状態から、可動接点担持体105を図示しないソレノイド部で可動接点103,104が固定接点101,102から上方に離間する方向に可動させて電流遮断状態とすると、固定接点101,102と可動接点103,104との間に図26に示すようにアーク108が発生する。
Here, each of the pair of arc extinguishing means 106 and 107 is composed of a pair of permanent magnets fixed to the housing so that the polarities of the magnetic pole faces facing each other across the contact gap are opposite.
The arc extinguishing principle of the conventional example will be described with reference to FIGS. Now, as shown in FIG. 25, the movable contact carrier 105 makes the movable contacts 103 and 104 come into contact with the fixed contacts 101 and 102, and an electric current flows from the fixed contact 101 to the fixed contact 102 through the movable contacts 103 and 104. Suppose that it is in a state. From this state, when the movable contact carrier 105 is moved in a direction in which the movable contacts 103 and 104 are separated upward from the fixed contacts 101 and 102 by a solenoid portion (not shown), the fixed contacts 101 and 102 and the movable contacts are moved. An arc 108 is generated between the terminals 103 and 104 as shown in FIG.

このとき、アーク108と直交する方向に一対の消弧手段106,107が配設されてその磁束φが図27に示すように、紙面と直交する方向に発生している。このため、この磁束φと電流の方向とにからフレミングの左手の法則にしたがってアーク108を固定接点101,102の配列方向の外側に向かうローレンツ力が作用する。このローレンツ力によって、アークを図24に示す固定接点101,102の配列方向外側に配置された消弧空間109側へと引き伸ばして消弧させる。   At this time, a pair of arc extinguishing means 106 and 107 are arranged in a direction perpendicular to the arc 108, and the magnetic flux φ is generated in a direction perpendicular to the paper surface as shown in FIG. For this reason, a Lorentz force is applied to the magnetic flux φ and the direction of current from the arc 108 toward the outside of the arrangement direction of the fixed contacts 101 and 102 in accordance with Fleming's left-hand rule. By this Lorentz force, the arc is extended to the arc extinguishing space 109 disposed outside the fixed contacts 101 and 102 shown in FIG.

また、電流の通電方向が固定接点102から可動接点104,103を介して固定接点101側に流れる逆方向となる場合には、図28に示すように、固定接点101,102及び可動接点103,104間に発生するアークを固定接点101,102の配列方向内側に引き伸ばして消弧させる。
しかしながら、上記特許文献1に記載された従来例にあっては、アークを引き伸ばしてアーク電圧を電源電圧より大きくすることで遮断している。アーク電圧はアーク電界値とアーク長の積で決まるため、より大きな電源電圧を遮断したい場合、アーク電界値を大きくするか、アーク長を長くすることが必要となる。
In addition, when the current application direction is the reverse direction from the fixed contact 102 to the fixed contact 101 side through the movable contacts 104 and 103, as shown in FIG. 28, the fixed contacts 101 and 102 and the movable contacts 103, The arc generated between 104 is extended inward in the arrangement direction of the fixed contacts 101 and 102 to extinguish the arc.
However, in the conventional example described in Patent Document 1, the arc is stretched so that the arc voltage is made higher than the power supply voltage. Since the arc voltage is determined by the product of the arc electric field value and the arc length, it is necessary to increase the arc electric field value or lengthen the arc length in order to cut off a larger power supply voltage.

雰囲気中におけるアーク電界値は、内圧、気体種類で決まっており、アーク電界は一般に気体圧力を上げることや、例えば水素等のアーク電界の大きい気体を使用することで大きくすることができる。しかし、気体圧力が大きい場合には容器の気密や、構造強度の強化が必要となってしまうという未解決の課題がある。また、水素等のアーク電界の大きい気体を使用する場合、絶縁耐圧が劣化するため接点間のギャップを開ける必要があるため、可動接点担持体を進退駆動するソレノイド部のコイルが大きくなる等の未解決の課題がある。   The arc electric field value in the atmosphere is determined by the internal pressure and the gas type, and the arc electric field can generally be increased by increasing the gas pressure or using a gas having a large arc electric field such as hydrogen. However, when the gas pressure is high, there is an unsolved problem that the container needs to be airtight and structural strength must be strengthened. In addition, when using a gas with a large arc electric field such as hydrogen, since the withstand voltage deteriorates and it is necessary to open a gap between the contacts, the coil of the solenoid unit that drives the movable contact carrier to move forward and backward becomes large. There is a problem to be solved.

一方、アーク長を長くする場合は、そのアーク長を実現するだけのアークスペースを設ける必要があり、ハウジングが大きくなるという未解決の課題がある。
これらの未解決の課題を解決するために、固定接点の配列方向の外側にそれぞれ消弧用磁石体をそれらの対向面が異極となるように配置した電磁継電器が提案されている(例えば、特許文献2参照)。この電磁継電器では、固定接点の配列方向と直交し、且つ固定接点及び可動接点の開閉方向と直交する方向における消弧用磁石体の両脇に消弧用磁石体の磁束に基づくローレンツ力によってアークを引き伸ばすための消弧空間を配置している。
On the other hand, when the arc length is increased, it is necessary to provide an arc space sufficient to realize the arc length, and there is an unsolved problem that the housing becomes large.
In order to solve these unsolved problems, electromagnetic relays have been proposed in which arc-extinguishing magnets are arranged outside the fixed contacts in the arrangement direction so that their opposing surfaces have different polarities (for example, Patent Document 2). In this electromagnetic relay, an arc is generated by the Lorentz force based on the magnetic flux of the arc extinguishing magnet body on both sides of the arc extinguishing magnet body in a direction orthogonal to the arrangement direction of the fixed contacts and orthogonal to the opening and closing directions of the fixed contact and the movable contact. An arc-extinguishing space for stretching

特開平7−235248号公報JP 7-235248 A 特開2008−226547号公報JP 2008-226547 A

ところで、上記特許文献2に記載の従来例にあっては、固定接点の配列方向外側に消弧用磁石体をそれらの対向面が異極となるように配置している。このため、消弧用磁石体で発生する磁束φは、図29に示すように、可動接触子110の長手方向の両端側に配置された消弧用磁石111及び112のそれぞれで、可動接触子110の長手方向と直交する幅方向の両端で自極のN極から直接自極のS極に向かう磁束が主流となる。このため、幅方向の中心部で消弧用磁石体112のN極から消弧用磁石体111のS極に向かう磁束が生じる。   By the way, in the conventional example described in Patent Document 2, the arc extinguishing magnet bodies are arranged outside the fixed contacts in the arrangement direction so that their opposing surfaces have different polarities. For this reason, as shown in FIG. 29, the magnetic flux φ generated in the arc-extinguishing magnet body is obtained by the arc-extinguishing magnets 111 and 112 disposed on both ends in the longitudinal direction of the movable contact 110, respectively. The magnetic flux mainly going from the N pole of the own pole to the S pole of the own pole becomes the mainstream at both ends in the width direction orthogonal to the longitudinal direction of 110. For this reason, a magnetic flux is generated from the north pole of the arc extinguishing magnet body 112 toward the south pole of the arc extinguishing magnet body 111 at the center in the width direction.

ここで、可動接触子110の消弧用磁石体112側の接点部を通る線G−Gにおける磁束分布は、図30に示すようになる。すなわち、消弧用磁石体112の幅方向の両端部が最大磁束密度となり、幅方向の中心部で最小磁束密度となる。消弧用磁石体111側の接点部についても同様に幅方向中心部で最小磁束密度となる。
このため、可動接触子110の両端部における固定接触子と接触する接点部を横切る磁束が小さくなる。この結果、電流遮断時に固定接触子及び可動接触子間で発生するアークへ作用するローレンツ力を十分に確保することができず、アークが固定接触子及び可動接触子の接点間に留まってしまうおそれがあるという未解決の課題がある。
Here, the magnetic flux distribution along the line GG passing through the contact point on the arc extinguishing magnet body 112 side of the movable contact 110 is as shown in FIG. That is, both end portions in the width direction of the arc extinguishing magnet body 112 have the maximum magnetic flux density, and the minimum magnetic flux density in the center portion in the width direction. Similarly, the contact portion on the arc extinguishing magnet body 111 side has the minimum magnetic flux density at the center in the width direction.
For this reason, the magnetic flux which crosses the contact part which contacts the fixed contact in the both ends of the movable contact 110 becomes small. As a result, the Lorentz force acting on the arc generated between the stationary contact and the movable contact when the current is interrupted cannot be sufficiently secured, and the arc may remain between the contact points of the stationary contact and the movable contact. There is an unresolved issue that there is.

この未解決の課題を解決するためには、保持力の大きな磁石を使用することとなり、大きな磁石を使う必要があるため電磁接触器が大型化してしまうという未解決の課題がある。
そこで、本発明は、上記従来例の未解決の課題に着目してなされたものであり、接点部に流れる電流の向きにかかわらず十分なアーク消弧機能を確保しながら小型化することができる電磁接触器を提供することを目的としている。
In order to solve this unsolved problem, a magnet having a large holding force is used, and since it is necessary to use a large magnet, there is an unsolved problem that the electromagnetic contactor becomes large.
Therefore, the present invention has been made paying attention to the unsolved problems of the above conventional example, and can be downsized while ensuring a sufficient arc extinguishing function regardless of the direction of the current flowing through the contact portion. The purpose is to provide an electromagnetic contactor.

上記目的を達成するために、本発明に係る電磁接触器の第1の態様は、固定接点部及び電源に接続される固定端子部を有する第1の固定接触子と、固定接点部及び負荷に接続される固定端子部とを有する第2の固定接触子と、前記第1の固定接触子及び第2の固定接触子を、所定間隔を保ち且つ両者の前記固定端子部を外部に突出させて支持する固定接触子支持筐体と、前記第1の固定接触子の固定接点部及び前記第2の固定接触子の固定接点部に接離可能で前記固定接触子支持筐体内に配置された可動接触子と、前記可動接触子の長手方向と直交する方向で当該可動接触子を挟んで平行に配設され、互いの対向磁極面が同一極性とされた一対の消弧用磁石体と、前記可動接触子を前記第1の固定接触子及び第2の固定接触子に対して接離可能に駆動する駆動機構とを備えている。前記一対の消弧用磁石体は、前記第1の固定接触子及び前記可動接触子に対向する一対の第1の磁石体と、前記第2の固定接触子及び前記可動接触子に対向する一対の第2の磁石体とを有し、前記第1の磁石体と前記第2の磁石体との対向磁極面異なる極性に設定し、開極時に発生するアークの伸張方向を前記可動接触子を挟んで反対方向としてアーク同士の干渉を防止する。 In order to achieve the above object, a first aspect of an electromagnetic contactor according to the present invention includes a first fixed contact having a fixed contact and a fixed terminal connected to a power source, a fixed contact and a load. A second fixed contact having a fixed terminal portion to be connected, and the first fixed contact and the second fixed contact are maintained at a predetermined interval and both of the fixed terminal portions are protruded to the outside. A stationary contact support housing to be supported, and a movable contact disposed in the stationary contact support housing that can be contacted and separated from the stationary contact portion of the first stationary contact and the stationary contact portion of the second stationary contact. A pair of arc-extinguishing magnet bodies disposed in parallel across the movable contact in a direction orthogonal to the longitudinal direction of the movable contact, the opposing magnetic pole surfaces having the same polarity, and The movable contact can be moved toward and away from the first fixed contact and the second fixed contact. And a drive mechanism for driving the. The pair of arc extinguishing magnet bodies includes a pair of first magnet bodies facing the first fixed contact and the movable contact, and a pair facing the second fixed contact and the movable contact. The opposite magnetic pole surfaces of the first magnet body and the second magnet body are set to different polarities, and an extension direction of an arc generated at the time of opening is set to the movable contactor. Interference between arcs is prevented in the opposite direction across the wire.

この構成によると、第1の固定接触子の固定接点部及び第2の固定接触子の固定接点部に可動接触子が接触している投入状態から釈放状態とする際に、第1の固定接触子及び第2の固定接触子と可動接触子との間にアークが発生する。このとき、例えば一対の第1の磁石体の対向磁極面をS極とし、一対の第2の磁石体の対向磁極面をN極とすることにより、一対の第1の磁石体に対向する固定接触子及び可動接触子に対しては、可動接触子の長手方向の内側に向かって磁束が横切る。逆に一対の第2の磁石体に対向する固定接触子及び可動接触子に対しては、可動接触子の長手方向の外側に向かって磁束が横切ることになる。このため、一対の第1の磁石体と一対の第2の磁石体とでアークに対して互いに逆方向のローレンツ力を作用させることができ、アークが干渉することを確実に防止することができる。   According to this configuration, when the movable contact is in contact with the fixed contact portion of the first fixed contact and the fixed contact portion of the second fixed contact, the first fixed contact is brought into the released state. An arc is generated between the child and the second fixed contact and the movable contact. At this time, for example, the opposing magnetic pole surfaces of the pair of first magnet bodies are S poles, and the opposing magnetic pole surfaces of the pair of second magnet bodies are N poles, thereby fixing the pair of first magnet bodies facing the pair of first magnet bodies. For the contact and the movable contact, the magnetic flux crosses inward in the longitudinal direction of the movable contact. On the contrary, the magnetic flux crosses toward the outside in the longitudinal direction of the movable contact with respect to the fixed contact and the movable contact facing the pair of second magnet bodies. For this reason, the pair of first magnet bodies and the pair of second magnet bodies can cause the Lorentz forces in opposite directions to act on the arc, and reliably prevent the arc from interfering with each other. .

また、本発明に係る電磁接触器の第2の態様は、前記第1の磁石体の対向磁極面がS極とされ、前記第2の磁石体の対向磁極面がN極とされている。
この構成によると、第1の磁石体の外側面のN極から出る磁束がこれら第1の磁石体の長手方向端面側を通り、第1の固定接触子の固定接点部及び可動接触子間とを可動接触子の長手方向に内側に横切って内面側すなわち対向磁極面のS極に達することになる。このため、第1の固定接触子の固定接点部と可動接触子との間に発生するアークに対して十分なローレンツ力を作用させることができる。また、第2の磁石体の内側面すなわち対向磁極面側面のN極から出る磁束が第2の固定接触子の固定接点部及び可動接触子間を可動接触子の長手方向に外側に横切ってから第2の磁石体の長手方向端面側を通り、外面側のS極に達することになる。このため、第2の固定接触子の固定接点部と可動接触子との間に発生するアークに対して十分なローレンツ力を作用させることができる。
In the second aspect of the electromagnetic contactor according to the present invention, the opposing magnetic pole surface of the first magnet body is an S pole, and the opposing magnetic pole surface of the second magnet body is an N pole.
According to this configuration, the magnetic flux emitted from the N pole on the outer surface of the first magnet body passes through the end surface side in the longitudinal direction of the first magnet body, and between the fixed contact portion of the first fixed contact and the movable contact. Is crossed inward in the longitudinal direction of the movable contact and reaches the S pole on the inner surface side, that is, the opposing magnetic pole surface. For this reason, a sufficient Lorentz force can be applied to the arc generated between the fixed contact portion of the first fixed contact and the movable contact. Further, after the magnetic flux generated from the N pole on the inner side surface of the second magnet body, that is, the side surface of the opposing magnetic pole surface, crosses between the fixed contact portion of the second fixed contact and the movable contact outward in the longitudinal direction of the movable contact. It passes through the end surface side in the longitudinal direction of the second magnet body and reaches the south pole on the outer surface side. For this reason, a sufficient Lorentz force can be applied to the arc generated between the fixed contact portion of the second fixed contact and the movable contact.

また、本発明に係る電磁接触器の第3の態様は、前記第1の磁石体の対向磁極面がN極とされ、前記第2の磁石体の対向磁極面がS極とされている。
この構成によると、第1の磁石体の内側面すなわち対向磁極面側面のN極から出る磁束が第1の固定接触子の固定接点部及び可動接触子間を可動接触子の長手方向に外側に横切ってから第2の磁石体の長手方向端面側を通り、外面側のS極に達することになる。このため、第1の固定接触子の固定接点部と可動接触子との間に発生するアークに対して十分なローレンツ力を作用させることができる。また、第2の磁石体の外側面のN極から出る磁束がこれら第2の磁石体の長手方向端面側を通り、第2の固定接触子の固定接点部及び可動接触子間とを可動接触子の長手方向に内側に横切って内面側すなわち対向磁極面のS極に達することになる。このため、第2の固定接触子の固定接点部と可動接触子との間に発生するアークに対して十分なローレンツ力を作用させることができる。
In a third aspect of the electromagnetic contactor according to the present invention, the opposing magnetic pole surface of the first magnet body is an N pole, and the opposing magnetic pole surface of the second magnet body is an S pole.
According to this configuration, the magnetic flux generated from the N pole on the inner side surface of the first magnet body, that is, the side surface of the opposing magnetic pole surface, passes between the fixed contact portion of the first fixed contact member and the movable contact member in the longitudinal direction of the movable contact member. After crossing, it passes through the longitudinal end face side of the second magnet body and reaches the S pole on the outer face side. For this reason, a sufficient Lorentz force can be applied to the arc generated between the fixed contact portion of the first fixed contact and the movable contact. Further, the magnetic flux emitted from the N pole on the outer surface of the second magnet body passes through the end surface side in the longitudinal direction of the second magnet body, and the movable contact is made between the fixed contact portion and the movable contact of the second fixed contact. It crosses inward in the longitudinal direction of the child and reaches the south pole on the inner surface side, that is, the opposing magnetic pole surface. For this reason, a sufficient Lorentz force can be applied to the arc generated between the fixed contact portion of the second fixed contact and the movable contact.

また、本発明に係る電磁接触器の第4の態様は、前記固定接触子支持筐体が、前記第1の固定接触子及び前記可動接触子と、前記第2の固定接触子及び前記可動接触子とにそれぞれ対向する内壁面に消弧空間が形成されている。
この構成によると、第1及び第2の固定接触子及び可動接触子間に発生するアークを、一対の消弧用磁石体の磁束によるローレンツ力によって、固定接触子の側面から固定接触子及び可動接触子の側面から離れた消弧空間を通って可動接触子の背面側に至るように、又はその逆方向に引き伸ばすことができる。
According to a fourth aspect of the electromagnetic contactor of the present invention, the fixed contact support housing includes the first fixed contact and the movable contact, the second fixed contact and the movable contact. An arc extinguishing space is formed on the inner wall surface facing the child.
According to this configuration, the arc generated between the first and second stationary contacts and the movable contact is caused to move from the side surface of the stationary contact by the Lorentz force due to the magnetic flux of the pair of arc extinguishing magnet bodies. It can be stretched to reach the back side of the movable contact through the arc extinguishing space away from the side of the contact or in the opposite direction.

また、本発明に係る電磁接触器の第5の態様は、前記固定接触子支持筐体が、前記第1の固定接触子及び第2の固定接触子間に対向する外側面に前記一対の消弧用磁石体を収容する収容凹部が形成されている。
この構成によると、固定接触子支持筐体の第1の固定接触子及び第2の固定接触子間に対向する外側面に形成した収容凹部内に消弧用磁石体を収納するので、消弧用磁石体が外側に突出することがなく、可動接触子の長手方向と直交する方向の最大幅を小さくすることができ、この分電磁接触器を小型化することができる。
Further, a fifth aspect of the electromagnetic contactor according to the present invention is such that the stationary contact support housing has the pair of erasures on an outer surface facing between the first stationary contact and the second stationary contact. A housing recess for housing the arc magnet body is formed.
According to this configuration, the arc extinguishing magnet body is housed in the housing recess formed on the outer surface facing between the first stationary contact and the second stationary contact of the stationary contact support housing. The magnet body does not protrude outward, the maximum width in the direction orthogonal to the longitudinal direction of the movable contact can be reduced, and the electromagnetic contactor can be reduced in size accordingly.

本発明に係る電磁接触器の第6の態様は、前記可動接触子の長手方向の両端部に対となる消弧用補助磁石体が配設され、該消弧用補助磁石体の対向磁極面の極性が前記一対の消弧用磁石体の極性と逆極性とされている。
この構成によると、例えば第1の磁石体の対向磁極面をS極とし、消弧用補助磁石体の対向磁極面をN極としたときに、消弧用補助磁石体のN極から出た磁束の殆どが第1の固定接触子及び可動接触子の接点部を横切って第1の磁石体のS極に向かうことになり、固定接触子及び可動接触子の接点部を通る磁束が平行となる磁場を形成することができる。
According to a sixth aspect of the electromagnetic contactor of the present invention, a pair of arc extinguishing auxiliary magnet bodies are disposed at both ends in the longitudinal direction of the movable contact, and the opposing magnetic pole surface of the arc extinguishing auxiliary magnet body Is opposite to the polarity of the pair of arc extinguishing magnets.
According to this configuration, for example, when the opposing magnetic pole face of the first magnet body is the S pole and the opposing magnetic pole face of the arc extinguishing auxiliary magnet body is the N pole, the first magnet body comes out of the N pole of the arc extinguishing auxiliary magnet body. Most of the magnetic flux crosses the contact portions of the first fixed contact and the movable contact toward the S pole of the first magnet body, and the magnetic flux passing through the contact portions of the fixed contact and the movable contact is parallel. A magnetic field can be formed.

本発明に係る電磁接触器の第7の形態は、前記一対の消弧用磁石体の対向磁極面とは反対側と前記対となる消弧用補助磁石体の対向磁極面とは反対側との間を接合するヨークを配置している。
この構成によると、一対の消弧用磁石体の対向磁極面とは反対側と対となる消弧用補助磁石体の対向磁極面とは反対側との間をヨークで接合しているので、このヨークで閉磁路を形成して、磁気効率が向上することで、アークを駆動する磁場を大きくできるため、アークの駆動力が増して遮断性能を向上させることができる。また、ヨークを設けない場合の磁場と同等の磁場を小さい磁石で形成することができ、全体の構成を小型化することができる。
According to a seventh aspect of the electromagnetic contactor of the present invention, the opposite side of the pair of arc extinguishing magnet bodies is opposite to the opposite magnetic pole face, and the opposite side of the pair of arc extinguishing auxiliary magnet bodies is opposite to the opposite magnetic pole face. The yoke which joins between is arranged.
According to this configuration, the yoke is joined between the opposite magnetic pole surface of the arc extinguishing auxiliary magnet body and the opposite side to the opposite magnetic pole surface of the pair of arc extinguishing magnet bodies, By forming a closed magnetic path with this yoke and improving the magnetic efficiency, the magnetic field for driving the arc can be increased, so that the driving force of the arc can be increased and the interruption performance can be improved. In addition, a magnetic field equivalent to the magnetic field when no yoke is provided can be formed with a small magnet, and the overall configuration can be reduced in size.

本発明によれば、一対の第1の磁石体と一対の第2の磁石体とでアークに対して互いに逆方向のローレンツ力を作用させることができ、アークが干渉することを確実に防止することができるとともに、第1の固定接触子及び第2の固定接触子間に流れる電流の方向にかかわらず、アークを確実に消弧することができる。   According to the present invention, the pair of first magnet bodies and the pair of second magnet bodies can cause the Lorentz forces in opposite directions to act on the arc, and reliably prevent the arc from interfering with each other. In addition, the arc can be reliably extinguished regardless of the direction of the current flowing between the first stationary contact and the second stationary contact.

本発明に係る電磁接触器の第1の実施形態を示す斜視図である。It is a perspective view which shows 1st Embodiment of the electromagnetic contactor which concerns on this invention. 図1の接点機構を示す長手方向の縦断面図である。It is a longitudinal cross-sectional view of the longitudinal direction which shows the contact mechanism of FIG. 一対の消弧用磁石体で発生する磁束を示す説明図である。It is explanatory drawing which shows the magnetic flux which generate | occur | produces with a pair of arc extinguishing magnet body. アークの引き伸ばし状態を説明する斜視図である。It is a perspective view explaining the extending state of an arc. 図3のA−A線上における電磁接触器の断面図であって、(a)は投入状態を、(b)は釈放状態をそれぞれ示す。It is sectional drawing of the magnetic contactor on the AA line | wire of FIG. 3, Comprising: (a) shows an injection | throwing-in state, (b) shows a release state, respectively. 図3のB−B線上における電磁接触器の断面図であって、(a)は投入状態を、(b)は釈放状態をそれぞれ示す。It is sectional drawing of the magnetic contactor on the BB line | wire of FIG. 3, Comprising: (a) shows an injection | throwing-in state, (b) shows a release state, respectively. 本発明に係る電磁接触器の第2の実施形態を示す斜視図である。It is a perspective view which shows 2nd Embodiment of the electromagnetic contactor which concerns on this invention. 第2の実施形態における消弧用磁石体で発生する磁束を示す説明図である。It is explanatory drawing which shows the magnetic flux which generate | occur | produces in the arc extinguishing magnet body in 2nd Embodiment. アークの引き伸ばし状態を説明する斜視図である。It is a perspective view explaining the extending state of an arc. 図8のC−C線上における電磁接触器の断面図であって、(a)は投入状態を、(b)は釈放状態をそれぞれ示す。It is sectional drawing of the magnetic contactor on the CC line of FIG. 8, Comprising: (a) shows an injection | throwing-in state, (b) shows a release state, respectively. 図8のD−D線上における電磁接触器の断面図であって、(a)は投入状態を、(b)は釈放状態をそれぞれ示す。It is sectional drawing of the electromagnetic contactor on the DD line | wire of FIG. 8, Comprising: (a) shows an injection | throwing-in state, (b) shows a release state, respectively. 本発明の第3の実施形態を示す斜視図である。It is a perspective view which shows the 3rd Embodiment of this invention. 第3の実施形態を示す平面図である。It is a top view which shows 3rd Embodiment. 第3の実施形態の長手方向の横断面図である。It is a cross-sectional view of the longitudinal direction of 3rd Embodiment. 第3の実施形態の電流方向を示す長手方向の縦断面図である。It is a longitudinal cross-sectional view of the longitudinal direction which shows the electric current direction of 3rd Embodiment. 第3の実施形態におけるアークの引き伸ばし状態を示す斜視図である。It is a perspective view which shows the extending state of the arc in 3rd Embodiment. 本発明の第4の実施形態を示す斜視図である。It is a perspective view which shows the 4th Embodiment of this invention. 第4の実施形態の長手方向の縦断面図である。It is a longitudinal cross-sectional view of the longitudinal direction of 4th Embodiment. 第4の実施形態における消弧用磁石体で発生する磁束を示す説明図である。It is explanatory drawing which shows the magnetic flux which generate | occur | produces in the arc extinguishing magnet body in 4th Embodiment. アークの引き伸ばし状態を説明する斜視図である。It is a perspective view explaining the extending state of an arc. 図19のE−E線上における電磁接触器の断面図であって、(a)は投入状態を、(b)は釈放状態をそれぞれ示す。It is sectional drawing of the electromagnetic contactor on the EE line | wire of FIG. 19, Comprising: (a) shows an injection | throwing-in state, (b) shows a release state, respectively. 図19のF−F線上における電磁接触器の断面図であって、(a)は投入状態を、(b)は釈放状態をそれぞれ示す。It is sectional drawing of the magnetic contactor on the FF line | wire of FIG. 19, Comprising: (a) shows an injection | throwing-in state, (b) shows a release state, respectively. 本発明の第5の実施形態を示す平面図である。It is a top view which shows the 5th Embodiment of this invention. 従来例を示す横断面図である。It is a cross-sectional view showing a conventional example. 従来例における通電状態における接点部と消弧手段との関係を示す模式図である。It is a schematic diagram which shows the relationship between the contact part in the electricity supply state in a prior art example, and an arc-extinguishing means. 従来例におけるアークの発生状況を示す説明図である。It is explanatory drawing which shows the generation | occurrence | production state of the arc in a prior art example. 従来例における遮断状態におけるアークと電流の向きと消弧手段による磁束の向きとの関係を示す模式図である。It is a schematic diagram which shows the relationship between the direction of the arc in the interruption | blocking state in a prior art example, and the direction of the magnetic flux by an arc extinguishing means. 従来例における電流の向きが逆となった状態の図26と同様の模式図である。It is a schematic diagram similar to FIG. 26 in a state where the direction of current in the conventional example is reversed. 他の従来例における磁界の発生状況を示す平面図である。It is a top view which shows the generation | occurrence | production state of the magnetic field in another prior art example. 図29のG−G線上の磁束分布を示す特性線図である。FIG. 30 is a characteristic diagram showing a magnetic flux distribution on the GG line of FIG. 29.

以下、本発明の実施の形態を図面(図1〜図6)に基づいて説明する。
図1は本発明の電磁接触器の第1の実施形態を示す斜視図である。この図1において、1は電磁接触器であって、この電磁接触器1は、上部の接点機構2と下部の駆動機構3とで構成されている。
接点機構2は、絶縁材料で形成された外形が略直方体状の固定接触子支持筐体4と、この固定接触子支持筐体4に所定間隔を保って支持された導電性を有する第1の固定接触子5A及び第2の固定接触子5Bと、固定接触子支持筐体4内に、第1及び第2の固定接触子5A及び5Bに接離可能に配置された導電性を有する可動接触子6とを備えている。
Embodiments of the present invention will be described below with reference to the drawings (FIGS. 1 to 6).
FIG. 1 is a perspective view showing a first embodiment of an electromagnetic contactor according to the present invention. In FIG. 1, reference numeral 1 denotes an electromagnetic contactor. The electromagnetic contactor 1 includes an upper contact mechanism 2 and a lower drive mechanism 3.
The contact mechanism 2 includes a fixed contact support case 4 having an outer shape formed of an insulating material and having a substantially rectangular parallelepiped shape, and a first conductive material supported by the fixed contact support case 4 at a predetermined interval. The fixed contact 5A and the second fixed contact 5B, and the movable contact having conductivity, which is disposed in the fixed contact support housing 4 so as to be able to contact with and separate from the first and second fixed contacts 5A and 5B. And a child 6.

第1の固定接触子5A及び第2の固定接触子5Bのそれぞれは、図2に示すように、固定接触子支持筐体4の上面板4aから上方に突出し、上面側から雌ねじ部11が形成された円柱状の固定端子部12と、この固定端子部12の下面に連接する固定端子部12の直径より小さい直径の固定接点部13とで構成されている。
そして、第1の固定接触子5Aの固定端子部12が例えば数百Vの高圧直流電源に接続された外部接続端子(図示せず)がねじ止めされて接続され、第2の固定接触子5Bの固定端子部12が負荷に接続された外部接続端子(図示せず)がねじ止めされて接続される。
As shown in FIG. 2, each of the first fixed contact 5A and the second fixed contact 5B protrudes upward from the upper surface plate 4a of the fixed contact support housing 4, and a female screw portion 11 is formed from the upper surface side. The fixed terminal portion 12 having a cylindrical shape and the fixed contact portion 13 having a diameter smaller than the diameter of the fixed terminal portion 12 connected to the lower surface of the fixed terminal portion 12 are configured.
Then, the fixed terminal portion 12 of the first fixed contact 5A is connected to an external connection terminal (not shown) connected to a high-voltage DC power supply of several hundred volts, for example, by screwing, and the second fixed contact 5B. An external connection terminal (not shown) in which the fixed terminal portion 12 is connected to a load is screwed and connected.

また、可動接触子6は、図4に示すように、第1の固定接触子5A及び第2の固定接触子5Bの固定接点部13に下方から対向する長さを有し、幅が第1の固定接触子5A及び第2の固定接触子5Bの固定接点部13の直径より広い平板状に形成されている。そして、可動接触子6が駆動機構3から突出するシャフト8の上端に固定されている。
駆動機構3は、図示しないが、励磁コイルを巻装したコイルボビンの内周側に磁性材料で構成されるコア部とプランジャとが配設され、プランジャにシャフト8が固定されている。そして、励磁コイルが非通電状態であるときには、図2に示すように、第1の固定接触子5A及び第2の固定接触子5Bの固定接点部13から可動接触子6が下方に所定距離だけ離間して接点機構2が釈放状態となる。この接点機構2の釈放状態から励磁コイルに通電すると、プランジャが上方に移動してシャフト8を介して絶縁体7と可動接触子6とが上方に移動する。これによって、可動接触子6が第1の固定接触子5Aの固定接点部13と第2の固定接触子5Bの固定接点部13との下面に接触する。このため、接点機構2が投入状態となる。
Further, as shown in FIG. 4, the movable contact 6 has a length facing the fixed contact portion 13 of the first fixed contact 5A and the second fixed contact 5B from below, and the width is the first. The fixed contact 5A and the second fixed contact 5B are formed in a flat plate shape wider than the diameter of the fixed contact portion 13 of the fixed contact 5A. The movable contact 6 is fixed to the upper end of the shaft 8 protruding from the drive mechanism 3.
Although not shown, the drive mechanism 3 is provided with a core portion made of a magnetic material and a plunger on the inner peripheral side of a coil bobbin around which an exciting coil is wound, and a shaft 8 is fixed to the plunger. When the exciting coil is in a non-energized state, as shown in FIG. 2, the movable contact 6 is moved downward by a predetermined distance from the fixed contact portion 13 of the first fixed contact 5A and the second fixed contact 5B. After separating, the contact mechanism 2 is released. When the exciting coil is energized from the released state of the contact mechanism 2, the plunger moves upward and the insulator 7 and the movable contact 6 move upward via the shaft 8. Accordingly, the movable contact 6 comes into contact with the lower surfaces of the fixed contact portion 13 of the first fixed contact 5A and the fixed contact portion 13 of the second fixed contact 5B. For this reason, the contact mechanism 2 is turned on.

一方、固定接触子支持筐体4には、第1の固定接触子5A及び第2の固定接触子5Bの配列方向すなわち、可動接触子6の長手方向と平行な両外側面4b及び4cに一対の消弧用磁石体21及び22が互いに対向されて例えば接着剤で固定されている。ここで、消弧用磁石体21及び22は、厚み方向に着磁されており、対向磁極面すなわち内側面が同一極性のS極とされ、それらの背面側即ち外側面がN極とされている。   On the other hand, the fixed contact support housing 4 has a pair of both outer surfaces 4b and 4c parallel to the arrangement direction of the first fixed contact 5A and the second fixed contact 5B, that is, the longitudinal direction of the movable contact 6. The arc extinguishing magnet bodies 21 and 22 are opposed to each other and fixed with, for example, an adhesive. Here, the arc extinguishing magnet bodies 21 and 22 are magnetized in the thickness direction, the opposite magnetic pole surface, that is, the inner side surface is the S pole with the same polarity, and the back side, that is, the outer side surface is the N pole. Yes.

そして、消弧用磁石体21及び22は、左右方向の中心部が第1の固定接触子5A及び第2の固定接触子5Bの中心軸間の中心と一致し、且つ左右両端部が少なくとも第1の固定接触子5A及び第2の固定接触子5Bの固定接点部13の中心軸と略対向する位置となるように配置されている。このため、消弧用磁石体21及び22の外側のN極から出る磁束φが、平面から見て図3に示すように、消弧用磁石体21及び22のそれぞれで、左右方向の中央部で左右に分かれ、左右方向の端部を回って第1の固定接触子5Aの固定接点部13及び可動接触子6間と、第2の固定接触子5Bの固定接点部13及び可動接触子6間とを可動接触子6の長手方向に内側に横切ってから各消弧用磁石体21及び22の内側のS極に達する磁界が形成される。   The arc extinguishing magnet bodies 21 and 22 have a center portion in the left-right direction that coincides with the center between the center axes of the first fixed contact 5A and the second fixed contact 5B, and at least the left and right ends are at least first. The first fixed contact 5A and the second fixed contact 5B are arranged so as to be substantially opposite to the central axis of the fixed contact portion 13 of the second fixed contact 5B. For this reason, the magnetic flux φ from the N pole outside the arc extinguishing magnet bodies 21 and 22 is shown in FIG. Are divided into right and left, and turn around the end in the left-right direction, between the fixed contact 13 and the movable contact 6 of the first fixed contact 5A, and between the fixed contact 13 and the movable contact 6 of the second fixed contact 5B. A magnetic field reaching the south pole inside each arc-extinguishing magnet body 21 and 22 is formed after crossing the gap inward in the longitudinal direction of the movable contact 6.

さらに、図5及び図6に示すように、固定接触子支持筐体4の第1の固定接触子5Aの固定接点部13及び可動接触子6間と、第2の固定接触子5Bの固定接点部13及び可動接触子6間に対向する内側面に消弧空間23及び24が形成されている。
次に、上記第1の実施形態の動作を説明する。
先ず、第1の固定接触子5Aの固定端子部12に高電圧直流電源に接続された外部接続端子をねじ止めによって接続し、第2の固定接触子5Bの固定端子部12に負荷に接続された外部接続端子を同様にねじ止めによって接続する。
Further, as shown in FIGS. 5 and 6, between the fixed contact portion 13 and the movable contact 6 of the first fixed contact 5A of the fixed contact support housing 4, and the fixed contact of the second fixed contact 5B. Arc extinguishing spaces 23 and 24 are formed on the inner surface facing the portion 13 and the movable contact 6.
Next, the operation of the first embodiment will be described.
First, the external connection terminal connected to the high voltage DC power source is connected to the fixed terminal portion 12 of the first fixed contact 5A by screwing, and is connected to the load to the fixed terminal portion 12 of the second fixed contact 5B. Connect the external connection terminals in the same way with screws.

この状態で、駆動機構3の図示しない励磁コイルが非通電状態であるときには、駆動機構3内に配設された図示しない復帰スプリングによって可動接触子6のシャフト8が下方に移動され、図2に示すように、第1の固定接触子5A及び第2の固定接触子5Bの固定接点部13に対して可動接触子6が下方に所定距離離間した釈放状態となっている。このため、第1の固定接触子5A及び第2の固定接触子5B間が非導通状態となって、高圧直流電源からの電流が負荷に供給されない電流遮断状態となっている。   In this state, when an excitation coil (not shown) of the drive mechanism 3 is in a non-energized state, the shaft 8 of the movable contact 6 is moved downward by a return spring (not shown) disposed in the drive mechanism 3, and FIG. As shown, the movable contact 6 is in a released state with a predetermined distance from the fixed contact portion 13 of the first fixed contact 5A and the second fixed contact 5B. For this reason, the first stationary contact 5A and the second stationary contact 5B are in a non-conducting state, and the current from the high-voltage DC power supply is not supplied to the load.

この釈放状態から駆動機構3の図示しない励磁コイルに通電すると、駆動機構3内に配設された図示しないプランジャが復帰スプリングに抗して上方に移動し、これによって可動接触子6のシャフト8が上方に移動される。このため、図5及び図6に示すように、第1の固定接触子5A及び第2の固定接触子5Bの固定接点部13の下面に可動接触子6の上面が接触して投入状態となる。   When an excitation coil (not shown) of the drive mechanism 3 is energized from this released state, a plunger (not shown) disposed in the drive mechanism 3 moves upward against the return spring, whereby the shaft 8 of the movable contact 6 is moved. Moved upwards. Therefore, as shown in FIGS. 5 and 6, the upper surface of the movable contact 6 comes into contact with the lower surfaces of the fixed contact portions 13 of the first fixed contact 5 </ b> A and the second fixed contact 5 </ b> B. .

この投入状態では、第1の固定接触子5Aの固定端子部12に入力される電流が第1の固定接触子5Aの固定接点部13から可動接触子6を通って第2の固定接触子5Bの固定接点部13に入り、この第2の固定接触子5Bの固定端子部12から負荷に電流が供給される電流供給状態となる。
その後、電流供給状態を解除するために、駆動機構3の励磁コイルへの通電を遮断すると、図示しないプランジャが復帰スプリングによって下降を開始するので、接点機構2では、図2に示すように、可動接触子6が第1の固定接触子5A及び第2の固定接触子5Bの固定接点部13から下方に離間することになる。このとき、第1の固定接触子5A及び第2の固定接触子5Bの固定接点部13と可動接触子6との間でアーク30が発生し、このアーク30によって電流の通電状態が継続される。
In this input state, the current input to the fixed terminal portion 12 of the first fixed contact 5A passes from the fixed contact portion 13 of the first fixed contact 5A through the movable contact 6 to the second fixed contact 5B. The fixed contact portion 13 enters the current supply state in which current is supplied to the load from the fixed terminal portion 12 of the second fixed contact 5B.
Thereafter, when the energization to the exciting coil of the drive mechanism 3 is interrupted in order to release the current supply state, the plunger (not shown) starts to descend by the return spring, so that the contact mechanism 2 is movable as shown in FIG. The contact 6 is separated downward from the fixed contact portions 13 of the first fixed contact 5A and the second fixed contact 5B. At this time, an arc 30 is generated between the fixed contact portion 13 of the first fixed contact 5A and the second fixed contact 5B and the movable contact 6, and the current conduction state is continued by the arc 30. .

このとき、消弧用磁石体21及び22の対向磁極面がS極であり、その外側がN極であるので、このN極が出た磁束が、平面から見て図3に示すように、各消弧用磁石体21及び22の左右端部を回って第1の固定接触子5Aの固定接点部13と可動接触子6との対向部のアーク発生部を可動接触子6の長手方向に内側に横切ってS極に達するとともに、第2の固定接触子5Bの固定接点部13と可動接触子6との対向部のアーク発生部を可動接触子6の長手方向に内側に横切ってS極に達する磁界が形成される。   At this time, since the opposing magnetic pole surfaces of the arc extinguishing magnet bodies 21 and 22 are the S poles and the outside thereof is the N poles, the magnetic flux emitted from the N poles is as shown in FIG. Around the left and right ends of each arc-extinguishing magnet body 21 and 22, the arc generating portion of the opposing portion of the fixed contact portion 13 of the first fixed contact 5 </ b> A and the movable contact 6 extends in the longitudinal direction of the movable contact 6. The S pole is traversed inward and reaches the S pole, and the arc generating portion of the opposing portion of the fixed contact portion 13 of the second fixed contact 5B and the movable contact 6 is traversed inward in the longitudinal direction of the movable contact 6. A magnetic field reaching is established.

したがって、消弧用磁石体21及び22の磁束がともに第1の固定接触子5Aの固定接点部13及び可動接触子6間と第2の固定接触子5Bの固定接点部13及び可動接触子6間を可動接触子6の長手方向で互いに逆方向に横切ることになる。このため、第1の固定接触子5Aの固定接点部13と可動接触子6との間では、図5(b)に示すように、電流Iが固定接触子5A側から可動接触子6側に流れるとともに、磁束φの向きが紙面に向かう方向となるので、フレミングの左手の法則によって、可動接触子6の長手方向と直交し且つ第1の固定接触子5Aの固定接点部13と可動接触子6との開閉方向と直交して消弧用磁石体21側に向かう大きなローレンツ力が作用する。このローレンツ力によって、第1の固定接触子5Aの固定接点部13と可動接触子6との間に発生したアーク30が図5(b)に示すように、固定接点部13の側面から消弧用磁石体21の内側に形成された消弧空間23内を通って可動接触子6の底面側に達するように大きく引き伸ばされて消弧される。また、消弧空間23では、その上方側及び下方側で、第1の固定接触子5Aの固定接点部13及び可動接触子6間の磁束の向きに対して上方側に及び下方側に磁束が傾くことになる。このため、傾いた磁束によって消弧空間23に引き伸ばされたアーク30が消弧空間23の隅の方向へさらに引き伸ばされ、アーク長を長くすることができ、良好な遮断性能を得ることができる。   Therefore, the magnetic fluxes of the arc extinguishing magnet bodies 21 and 22 are both between the fixed contact portion 13 and the movable contact 6 of the first fixed contact 5A and between the fixed contact 13 and the movable contact 6 of the second fixed contact 5B. The gaps cross in the opposite directions in the longitudinal direction of the movable contact 6. For this reason, between the fixed contact portion 13 of the first fixed contact 5A and the movable contact 6, the current I flows from the fixed contact 5A to the movable contact 6 as shown in FIG. 5B. Since the direction of the magnetic flux φ is the direction toward the paper surface as it flows, the fixed contact portion 13 of the first fixed contact 5A and the movable contact are orthogonal to the longitudinal direction of the movable contact 6 according to Fleming's left-hand rule. A large Lorentz force acting on the arc extinguishing magnet body 21 side acts perpendicularly to the opening / closing direction with respect to 6. The arc 30 generated between the fixed contact portion 13 of the first fixed contact 5A and the movable contact 6 by this Lorentz force is extinguished from the side surface of the fixed contact portion 13 as shown in FIG. The arc is extended and extinguished so as to reach the bottom surface side of the movable contact 6 through the arc extinguishing space 23 formed inside the magnet body 21. Further, in the arc extinguishing space 23, the magnetic flux is on the upper side and the lower side with respect to the direction of the magnetic flux between the fixed contact portion 13 of the first fixed contact 5 </ b> A and the movable contact 6 and on the lower side. Will tilt. For this reason, the arc 30 extended to the arc extinguishing space 23 by the inclined magnetic flux is further extended in the direction of the corner of the arc extinguishing space 23, the arc length can be lengthened, and good interruption performance can be obtained.

一方、第2の固定接触子5Bの固定接点部13と可動接触子6との間では、図6(b)に示すように、電流Iが可動接触子6側から第2の固定接触子5B側に流れるとともに、磁束φの向きが紙面から手前に向かう方向となるので、フレミングの左手の法則によって、可動接触子6の長手方向と直交し且つ第2の固定接触子5Bの固定接点部13と可動接触子6との開閉方向と直交して消弧用磁石体21側に向かう大きなローレンツ力が作用する。このローレンツ力によって、第2の固定接触子5Bの固定接点部13と可動接触子6との間に発生したアーク30が図6(b)に示すように、可動接触子6の底面側から消弧用磁石体21の内側に形成された消弧空間23内を通って第2の固定接触子5Bの側面側に達するように大きく引き伸ばされて消弧される。また、消弧空間23では、上述したように、その上方側及び下方側で、第1の固定接触子5Aの固定接点部13及び可動接触子6間の磁束の向きに対して上方側に及び下方側に磁束が傾くことになる。このため、傾いた磁束によって消弧空間23に引き伸ばされたアーク30が消弧空間23の隅の方向へさらに引き伸ばされ、アーク長を長くすることができ、良好な遮断性能を得ることかできる。   On the other hand, between the fixed contact portion 13 of the second fixed contact 5B and the movable contact 6, as shown in FIG. 6B, the current I flows from the movable contact 6 side to the second fixed contact 5B. Since the direction of the magnetic flux φ is the direction toward the front from the paper surface, the fixed contact portion 13 of the second fixed contact 5B is orthogonal to the longitudinal direction of the movable contact 6 according to Fleming's left-hand rule. A large Lorentz force acting on the arc extinguishing magnet body 21 side acts perpendicularly to the opening / closing direction of the movable contact 6. The arc 30 generated between the fixed contact portion 13 of the second fixed contact 5B and the movable contact 6 by this Lorentz force is extinguished from the bottom surface side of the movable contact 6 as shown in FIG. The arc is extinguished by being greatly stretched so as to reach the side surface side of the second stationary contact 5B through the arc extinguishing space 23 formed inside the arc magnet body 21. Moreover, in the arc extinguishing space 23, as described above, the upper side and the lower side are above the upper side with respect to the direction of the magnetic flux between the fixed contact portion 13 of the first fixed contact 5A and the movable contact 6. The magnetic flux is inclined downward. For this reason, the arc 30 extended to the arc extinguishing space 23 by the tilted magnetic flux is further extended in the direction of the corner of the arc extinguishing space 23, the arc length can be increased, and good interruption performance can be obtained.

一方、電磁接触器1の投入状態で、負荷側から直流電源側に回生電流が流れている状態で、釈放状態とする場合には、前述した図5及び図6における電流の方向が逆となることから、ローレンツ力が消弧用磁石体22側に作用し、アーク30が消弧空間24側に引き伸ばされることを除いては同様の消弧機能が発揮される。
このように、上記第1の実施形態によると、可動接触子6の長手方向と直交する方向で、第1の固定接触子5A及び第2の固定接触子5Bと可動接触子6とを挟んで対向するように消弧用磁石体21及び22を配置し、両消弧用磁石体21及び22の対向磁極面を同一極性としている。
On the other hand, when the electromagnetic contactor 1 is turned on and the regenerative current is flowing from the load side to the DC power supply side and the release state is set, the direction of the current in FIGS. 5 and 6 is reversed. Therefore, the same arc extinguishing function is exhibited except that the Lorentz force acts on the arc extinguishing magnet body 22 side and the arc 30 is extended to the arc extinguishing space 24 side.
Thus, according to the first embodiment, the first fixed contact 5A, the second fixed contact 5B, and the movable contact 6 are sandwiched in a direction orthogonal to the longitudinal direction of the movable contact 6. The arc extinguishing magnet bodies 21 and 22 are arranged so as to face each other, and the opposing magnetic pole surfaces of the arc extinguishing magnet bodies 21 and 22 have the same polarity.

このため、各消弧用磁石体21及び22で発生する磁束がともに第1の固定接触子5A及び第2の固定接触子5Bと可動接触子6との間を可動接触子6の長手方向に横切ることになる。
したがって、第1の固定接触子5A及び第2の固定接触子5Bと可動接触子6との間を横切る磁束量を前述した従来例に比較して格段に高めることができる。この磁束と、第1の固定接触子5A及び第2の固定接触子5Bと可動接触子6との間を流れる電流とにより、フレミングの左手の法則によって、消弧用磁石体21及び22の何れかに向かう大きなローレンツ力を発生させることができる。
For this reason, the magnetic flux generated in each of the arc extinguishing magnet bodies 21 and 22 is between the first fixed contact 5A and the second fixed contact 5B and the movable contact 6 in the longitudinal direction of the movable contact 6. Will cross.
Therefore, the amount of magnetic flux crossing between the first fixed contact 5A and the second fixed contact 5B and the movable contact 6 can be significantly increased as compared with the conventional example described above. Any of the arc extinguishing magnet bodies 21 and 22 is determined by Fleming's left-hand rule by the magnetic flux and the current flowing between the first fixed contact 5A and the second fixed contact 5B and the movable contact 6. It can generate a large Lorentz force toward

このローレンツ力によって、消弧用磁石体21及び22に対向して固定接触子支持筐体4の内側面に形成した消弧空間23及び24の何れかにアーク30を大きく引き伸ばして消弧させることができる。したがって、消弧用磁石体21及び22の保持力を大きくすることなく、直流高電圧を遮断することができ、電磁接触器を小型化することができる。
しかも、第1の固定接触子5Aの固定接点部13及び可動接触子6から引き伸ばしたアーク30と、第2の固定接触子5Bの固定接点部13及び可動接触子6から引き伸ばしたアーク30とは電流の方向が逆となっても互いに近接することはなく、両者が干渉することを確実に防止することができる。
By this Lorentz force, the arc 30 is greatly stretched and extinguished in any one of the arc extinguishing spaces 23 and 24 formed on the inner surface of the stationary contact support housing 4 so as to face the arc extinguishing magnet bodies 21 and 22. Can do. Therefore, the DC high voltage can be cut off without increasing the holding force of the arc extinguishing magnet bodies 21 and 22, and the electromagnetic contactor can be downsized.
Moreover, the arc 30 extended from the fixed contact portion 13 and the movable contact 6 of the first fixed contact 5A and the arc 30 extended from the fixed contact portion 13 and the movable contact 6 of the second fixed contact 5B are as follows. Even if the directions of the currents are reversed, they are not close to each other, and the two can be reliably prevented from interfering with each other.

また、第1の固定接触子5A及び第2の固定接触子5Bの固定接点部13と可動接触子6との間に流れる電流の向きが逆になれば、ローレンツ力の向きも逆向きに作用する。すなわち、可動接触子6の長手方向の両脇すなわち消弧用磁石体21及び22の何れかの固定側にアーク30が引き伸ばされるかは、第1の固定接触子5A及び第2の固定接触子5Bの固定接点部13と可動接触子6との間に流れる電流の向きによって決まる。   In addition, if the direction of the current flowing between the fixed contact portion 13 of the first fixed contact 5A and the second fixed contact 5B and the movable contact 6 is reversed, the direction of the Lorentz force is also reversed. To do. That is, whether the arc 30 is extended on both sides of the movable contact 6 in the longitudinal direction, that is, on the fixed side of the arc extinguishing magnet bodies 21 and 22, is determined by the first fixed contact 5A and the second fixed contact. It is determined by the direction of the current flowing between the 5B fixed contact portion 13 and the movable contact 6.

したがって、可動接触子6の長手方向の両脇すなわち消弧用磁石体21及び22側にそれぞれ消弧空間23及び24を設けることにより、アーク電流の向きすなわち固定接点部及び可動接触子間に流れる電流の向きにかかわらず、確実なアークの消弧機能を発揮することができる。
以上のように第1の実施形態によると、接点部に流れる電流の向きにかかわらず、高電圧の電源に対して十分なアーク消弧機能を有する小型の電磁接触器を提供することができる。
Therefore, by providing the arc extinguishing spaces 23 and 24 on both sides in the longitudinal direction of the movable contact 6, that is, on the side of the arc extinguishing magnet bodies 21 and 22, respectively, the direction of the arc current, that is, the flow between the fixed contact and the movable contact A reliable arc extinguishing function can be exhibited regardless of the current direction.
As described above, according to the first embodiment, it is possible to provide a small-sized electromagnetic contactor having a sufficient arc extinguishing function for a high-voltage power source regardless of the direction of the current flowing through the contact portion.

なお、上記第1の実施形態においては、消弧用磁石体21及び22の対向磁極面をS極とした場合について説明したが、これに限定されるものではなく、消弧用磁石体21及び22の対向磁極面をN極とすることもできる。
この場合には、消弧用磁石体21及び22の内面側のN極から出た磁束が、第1の固定接触子5Aの固定接点部13及び可動接触子6間を通るとともに、第2の固定接触子5Bの固定接点部13及び可動接触子6間を通って消弧用磁石体21及び22の外側面のS極に入ることになる。
In addition, in the said 1st Embodiment, although the case where the opposing magnetic pole surface of the arc extinguishing magnet bodies 21 and 22 was made into the S pole was demonstrated, it is not limited to this, The arc extinguishing magnet body 21 and The 22 opposing magnetic pole surfaces may be N poles.
In this case, the magnetic flux emitted from the N pole on the inner surface side of the arc extinguishing magnet bodies 21 and 22 passes between the fixed contact portion 13 and the movable contact 6 of the first fixed contact 5A, and the second The S pole on the outer surface of the arc extinguishing magnet bodies 21 and 22 passes between the fixed contact portion 13 and the movable contact 6 of the fixed contact 5B.

このため、上記した第1の実施形態におけるローレンツ力の作用方向が逆方向となることを除いては上記第1の実施形態と同様の作用効果を得ることができる。
次に、本発明の第2の実施形態を図7〜図11について説明する。
この第2の実施形態では、上述した第1の実施形態において、一対の消弧用磁石体21及び22のそれぞれを左右方向に2つの磁石体に分割するようにしたものである。
For this reason, the same effect as the said 1st Embodiment can be obtained except the action direction of Lorentz force in the above-mentioned 1st Embodiment becoming a reverse direction.
Next, a second embodiment of the present invention will be described with reference to FIGS.
In the second embodiment, in the first embodiment described above, each of the pair of arc extinguishing magnet bodies 21 and 22 is divided into two magnet bodies in the left-right direction.

すなわち、第2の実施形態では、図7及び図8に示すように、前述した第1の実施形態における一対の消弧用磁石体21及び22のそれぞれを左右方向で2つに分割した2つの分割磁石体21a及び21b、22a及び22bで構成し、分割磁石体21a及び21b間と分割磁石体22a及び22b間とにそれぞれ所定長の隙間を設けていることを除いては前述した図1及び図3と同様の構成を有し、図1及び図3との対応部分には同一符号を付し、その詳細説明はこれを省略する。   That is, in the second embodiment, as shown in FIGS. 7 and 8, each of the pair of arc extinguishing magnet bodies 21 and 22 in the first embodiment described above is divided into two in the left-right direction. FIG. 1 and FIG. 1 described above except that they are composed of divided magnet bodies 21a and 21b, 22a and 22b, and a predetermined length gap is provided between the divided magnet bodies 21a and 21b and between the divided magnet bodies 22a and 22b. 3 has the same configuration as that of FIG. 3, and the same reference numerals are given to corresponding parts to those in FIGS. 1 and 3, and the detailed description thereof will be omitted.

ここで、分割磁石体21a〜22bの内、互いに対向する一方の分割磁石体21a及び22aの対向磁極面が同一極性の例えばS極とされている。また、互いに対向する他方の分割磁石体21b及び22bの対向磁極面が同一極性で、分割磁石体21a及び22aとは異なる極性となるN極とされている。
この第2の実施形態によると、第1の固定接触子5Aの固定接点部13及びこれに対向する可動接触子6を挟んで対向する分割磁石体21a及び22aの対向磁極面がS極とされている。また、これら分割磁石体21a及び22aに対して左右方向に所定の間隙を開けて配設された分割磁石体21b及び22bが、第2の固定接触子5Bの固定接点部13及びこれに対向する可動接触子6を挟んで対向配置され、両分割磁石体21b及び22bの対向磁極面がN極とされている。
Here, of the divided magnet bodies 21a to 22b, the opposed magnetic pole surfaces of one of the divided magnet bodies 21a and 22a facing each other are set to, for example, S poles having the same polarity. Further, the opposing magnetic pole surfaces of the other divided magnet bodies 21b and 22b facing each other have the same polarity and are N poles having different polarities from the divided magnet bodies 21a and 22a.
According to the second embodiment, the opposed magnetic pole surfaces of the divided magnet bodies 21a and 22a facing each other with the fixed contact portion 13 of the first fixed contact 5A and the movable contact 6 facing the fixed contact portion 13 being the S pole are set as the S poles. ing. Further, the divided magnet bodies 21b and 22b arranged with a predetermined gap in the left-right direction with respect to the divided magnet bodies 21a and 22a are opposed to the fixed contact portion 13 of the second fixed contact 5B. Oppositely arranged with the movable contact 6 in between, the opposing magnetic pole surfaces of both divided magnet bodies 21b and 22b are N poles.

このため、各分割磁石体21a,22a及び21b,22bで発生する磁束は、平面から見て図8に示すようになる。すなわち、分割磁石体21aの外側のN極から出る磁束の半部は固定接触子支持筐体4の外側を通って第1の固定接触子5Aの固定接点部13及び可動接触子6間を通って自身のS極に達し、この半部が隣接する分割磁石体21bの外側のS極に達する。   For this reason, the magnetic flux generated in each of the divided magnet bodies 21a, 22a and 21b, 22b is as shown in FIG. That is, half of the magnetic flux emitted from the N pole outside the split magnet body 21 a passes between the fixed contact portion 13 of the first fixed contact 5 </ b> A and the movable contact 6 through the outside of the fixed contact support housing 4. Reaches its own S pole, and this half reaches the S pole outside the adjacent divided magnet body 21b.

逆に、分割磁石体21bの内側のN極から出る磁束は、その半部が隣接する分割磁石体21aのS極に達し、他の半部が第2の固定接触子5Bの固定接点部13及び可動接触子6間を通り、固定接触子支持筐体4の外側を通って自身のS極に達する。
同様に、分割磁石体22aの外側のN極から出る磁束の半部が固定接触子支持筐体4の外側を通って第1の固定接触子5Aの固定接点部13及び可動接触子6間を通って自身のS極に達し、残りの半部が隣接する分割磁石体22bの外側のS極に達する。
On the contrary, the magnetic flux emitted from the N pole inside the split magnet body 21b reaches the S pole of the adjacent split magnet body 21a, and the other half is the fixed contact portion 13 of the second fixed contact 5B. And passes between the movable contacts 6 and passes through the outside of the stationary contact support housing 4 to reach its S pole.
Similarly, a half portion of the magnetic flux emitted from the N pole outside the divided magnet body 22a passes through the outside of the fixed contact support housing 4 and between the fixed contact portion 13 and the movable contact 6 of the first fixed contact 5A. It reaches its own S pole, and the remaining half reaches the S pole outside the adjacent divided magnet body 22b.

逆に、分割磁石体22bの内側のN極から出る磁束は、その半部が隣接する分割磁石体22aの内側のS極に達し、残りの半部が第2の固定接触子5Bの固定接点部13及び可動接触子6間を通り、固定接触子支持筐体4の外側を通って自身の外側のS極に達する。 このため、第1の固定接触子5Aの固定接点部13及び可動接触子6間には、分割磁石体21a及び22aからの磁束が可動接触子6の長手方向で内側向きに横切る。逆に、第2の固定接触子5Bの固定接点部13及び可動接触子6間には、分割磁石体21b及び22bからの磁束が可動接触子6の長手方向で外側向きに横切る。   On the contrary, the magnetic flux emitted from the N pole inside the split magnet body 22b reaches the S pole inside the adjacent split magnet body 22a, and the remaining half is the fixed contact of the second fixed contact 5B. It passes between the part 13 and the movable contact 6, passes through the outside of the stationary contact support housing 4, and reaches the S pole outside itself. For this reason, the magnetic flux from the divided magnet bodies 21 a and 22 a crosses inward in the longitudinal direction of the movable contact 6 between the fixed contact portion 13 of the first fixed contact 5 </ b> A and the movable contact 6. On the contrary, the magnetic flux from the divided magnet bodies 21 b and 22 b crosses outward in the longitudinal direction of the movable contact 6 between the fixed contact portion 13 and the movable contact 6 of the second fixed contact 5 </ b> B.

そして、駆動機構3の励磁コイルに通電してシャフト8を介して可動接触子6を上昇させて第1及び第2の固定接触子5A及び5Bの固定接点部13の下面に接触させた投入状態とする。この投入状態となると、第1の固定接触子5A及び可動接触子6間では、図10(a)に示すように、第1の固定接触子5Aの固定接点部13から可動接触子6側に電流が流れるとともに、磁束が紙面に向かう方向に横切る。   Then, an energized state in which the exciting coil of the drive mechanism 3 is energized and the movable contact 6 is raised through the shaft 8 to be brought into contact with the lower surfaces of the fixed contact portions 13 of the first and second fixed contacts 5A and 5B. And In this charged state, between the first fixed contact 5A and the movable contact 6, as shown in FIG. 10A, the fixed contact portion 13 of the first fixed contact 5A is moved to the movable contact 6 side. As current flows, the magnetic flux crosses in the direction toward the page.

同様に、第2の固定接触子5B及び可動接触子6間では、図11(a)に示すように、可動接触子6から第2の固定接触子5Bの固定接点部13へ電流が流れるとともに、磁束が紙面に向かう方向に横切る。
このため、投入状態から釈放状態に移行する際に、第1及び第2の固定接触子5A及び5Bの固定接点部13と可動接触子6とが離間して、これら間にアーク30が発生したときに、第1の固定接触子5A及び可動接触子6間では、図10(b)に示すように、分割磁石体21aに向かう大きなローレンツ力Fが発生する。
Similarly, between the second fixed contact 5B and the movable contact 6, current flows from the movable contact 6 to the fixed contact portion 13 of the second fixed contact 5B as shown in FIG. 11A. The magnetic flux crosses in the direction toward the paper.
For this reason, when shifting from the charged state to the released state, the fixed contact portion 13 of the first and second fixed contacts 5A and 5B and the movable contact 6 are separated, and an arc 30 is generated between them. Sometimes, a large Lorentz force F toward the split magnet body 21a is generated between the first fixed contact 5A and the movable contact 6 as shown in FIG. 10 (b).

このローレンツ力Fによって、発生したアーク30が図10(b)に示すように第1の固定接触子5Aの固定接点部13の側面から分割磁石体21a側の消弧空間23を上から下に通って可動接触子6の底面側に達するように長く引き伸ばされて消弧される。
また、消弧空間23では、その上方側及び下方側で、第1の固定接触子5Aの固定接点部13及び可動接触子6間の磁束の向きに対して上方側に及び下方側に磁束が傾くことになる。このため、傾いた磁束によって消弧空間23に引き伸ばされたアーク30が消弧空間23の隅の方向へさらに引き伸ばされ、アーク長を長くすることができ、良好な遮断性能を得ることかできる。
Due to the Lorentz force F, the generated arc 30 moves the arc-extinguishing space 23 on the divided magnet body 21a side from the top to the bottom from the side surface of the fixed contact portion 13 of the first fixed contact 5A as shown in FIG. It is stretched long so as to reach the bottom surface side of the movable contact 6 and is extinguished.
Further, in the arc extinguishing space 23, the magnetic flux is on the upper side and the lower side with respect to the direction of the magnetic flux between the fixed contact portion 13 of the first fixed contact 5 </ b> A and the movable contact 6 and on the lower side. Will tilt. For this reason, the arc 30 extended to the arc extinguishing space 23 by the tilted magnetic flux is further extended in the direction of the corner of the arc extinguishing space 23, the arc length can be increased, and good interruption performance can be obtained.

また、第2の固定接触子5B及び可動接触子6間では、図11(a)に示すように、分割磁石体22bに向かう大きなローレンツ力Fが発生する。このローレンツ力Fによって、発生したアーク30が図11(b)に示すように可動接触子6の底面から分割磁石体22b側の消弧空間24を下から上に通って第2の固定接触子5Bの固定接点部13の側面に達するように長く引き伸ばされて消弧される。   Further, between the second fixed contact 5B and the movable contact 6, a large Lorentz force F toward the split magnet body 22b is generated as shown in FIG. Due to the Lorentz force F, the generated arc 30 passes through the arc extinguishing space 24 on the divided magnet body 22b side from the bottom surface of the movable contact 6 as shown in FIG. It is elongated and extinguished so as to reach the side surface of the fixed contact portion 13 of 5B.

また、消弧空間24では、その上方側及び下方側で、第2の固定接触子5Bの固定接点部13及び可動接触子6間の磁束の向きに対して上方側に及び下方側に磁束が傾くことになる。このため、傾いた磁束によって消弧空間23に引き伸ばされたアーク30が消弧空間24の隅の方向へさらに引き伸ばされ、アーク長を長くすることができ、良好な遮断性能を得ることができる。   Further, in the arc extinguishing space 24, the magnetic flux is on the upper side and the lower side with respect to the direction of the magnetic flux between the fixed contact portion 13 of the second fixed contact 5 </ b> B and the movable contact 6 and on the lower side. Will tilt. For this reason, the arc 30 extended to the arc extinguishing space 23 by the inclined magnetic flux is further extended in the direction of the corner of the arc extinguishing space 24, the arc length can be lengthened, and good interruption performance can be obtained.

このように、第2の実施形態によると、投入状態から釈放状態に移行する際に、アーク30が発生したときに、図9に示すように、第1の固定接触子5A側では消弧空間23側に引き伸ばされ、第2の固定接触子5B側では逆側の消弧空間24側に引き伸ばされる。
このため、引き伸ばされたアーク30が逆側の消弧空間23及び24を通るので、引き伸ばされたアーク同士が干渉することを確実に防止することができる。このため、第1の固定接触子5A及び第2の固定接触子5B間の間隔を狭くすることができる。したがって、電磁接触器を小型化することができる。
Thus, according to the second embodiment, when the arc 30 is generated when shifting from the charged state to the released state, the arc-extinguishing space is formed on the first fixed contact 5A side as shown in FIG. It is stretched to the 23 side, and is stretched to the arc extinguishing space 24 side on the opposite side on the second stationary contact 5B side.
For this reason, since the stretched arc 30 passes through the arc extinguishing spaces 23 and 24 on the opposite side, it is possible to reliably prevent the stretched arcs from interfering with each other. For this reason, the space | interval between 5 A of 1st stationary contacts and the 2nd stationary contacts 5B can be narrowed. Therefore, the electromagnetic contactor can be reduced in size.

また、第1及び第2の固定接触子5A及び5Bの固定接点部13及び可動接触子6間に流れる電流の向きが逆になると、ローレンツ力の向きも逆向きに作用する。すなわち、第1及び第2の固定接触子5A,5Bの固定接点部13と、可動接触子6との間の接点部の開閉方向及び消弧用磁石体が形成する磁束の向きに直交する方向のどちらにアーク30が引き伸ばされるかは、接点部に流れる電流の向きによって決まる。そのため、上記接点部の開閉方向及び消弧用磁石体が形成する磁束の向きに直交する方向で可動接触子6の両脇すなわち分割磁石体21a,21b及び22a,22bの双方に消弧空間を設けることにより、アーク電流の向きすなわち、接点部を流れる電流の向きにかかわらず、アークの消弧を十分に行うことができる。   Further, when the direction of the current flowing between the fixed contact portion 13 and the movable contact 6 of the first and second fixed contacts 5A and 5B is reversed, the direction of the Lorentz force is also reversed. That is, the direction orthogonal to the opening / closing direction of the contact portion between the fixed contact portion 13 of the first and second fixed contacts 5A and 5B and the movable contact 6 and the direction of the magnetic flux formed by the arc extinguishing magnet body. The direction in which the arc 30 is stretched depends on the direction of the current flowing through the contact portion. Therefore, an arc extinguishing space is provided on both sides of the movable contact 6 in the direction perpendicular to the opening / closing direction of the contact portion and the direction of the magnetic flux formed by the arc extinguishing magnet body, that is, both of the divided magnet bodies 21a, 21b and 22a, 22b. By providing, the arc can be sufficiently extinguished regardless of the direction of the arc current, that is, the direction of the current flowing through the contact portion.

このように一対の消弧空間23,24でアークを十分に消弧することができるため、電磁接触器のコンパクト化を図ることができる。すなわち、釈放時における接点部のギャップを大きく設けなくても、上記一対の消弧空間によりアークを十分に消弧させることができる。また、例えば接点部が二つ形成されている場合などにおいても、アークを消弧させるための空間を設けるために接点部同士を比較的離隔して配置しなくても、アークを消弧空間へと引き伸ばすことができる。   Thus, since the arc can be sufficiently extinguished by the pair of arc extinguishing spaces 23 and 24, the electromagnetic contactor can be made compact. That is, the arc can be sufficiently extinguished by the pair of arc extinguishing spaces without providing a large gap between the contact points when released. For example, even when two contact portions are formed, the arc can be transferred to the arc extinguishing space even if the contact portions are not relatively separated to provide a space for extinguishing the arc. And can be stretched.

以上のことから接点部に流れる電流の向きにかかわらず十分なアーク消弧機能を発揮することができる小型の電磁接触器を得ることができる。
この第2の実施形態においては、分割磁石体21a及び22aの対向磁極面をS極とし、分割磁石体21b及び22bの対向磁極面をN極とした場合について説明したが、これに限定されるものではなく、分割磁石体21a及び22aの対向磁極面をN極とし、分割磁石体21b及び22bの対向磁極面をS極としても、上記第2の実施形態と同様の作用効果を得ることができる。
From the above, it is possible to obtain a small electromagnetic contactor that can exhibit a sufficient arc extinguishing function regardless of the direction of the current flowing through the contact portion.
In the second embodiment, the case has been described in which the opposing magnetic pole surfaces of the divided magnet bodies 21a and 22a are S poles and the opposing magnetic pole surfaces of the divided magnet bodies 21b and 22b are N poles. The same effect as the second embodiment can be obtained even if the opposing magnetic pole surfaces of the divided magnet bodies 21a and 22a are N poles and the opposing magnetic pole surfaces of the divided magnet bodies 21b and 22b are S poles. it can.

次に、本発明の第3の実施形態を図12〜図16について説明する。
この第3の実施形態では、電磁接触器1の消弧用磁石体を配置した側面間距離を縮小させるようにしたものである。
すなわち、第3の実施形態においては、図12及び図13に示すように、固定接触子支持筐体4の第1の固定接触子5A及び第2の固定接触子5B間を内側すなわち可動接触子6側に括れさせて幅狭形状として収容凹部31及び32が形成されている。
Next, a third embodiment of the present invention will be described with reference to FIGS.
In the third embodiment, the distance between the side surfaces on which the arc extinguishing magnet body of the electromagnetic contactor 1 is arranged is reduced.
That is, in the third embodiment, as shown in FIGS. 12 and 13, the first fixed contact 5 </ b> A and the second fixed contact 5 </ b> B of the fixed contact support housing 4 are arranged inside, that is, movable contacts. The housing recesses 31 and 32 are formed in a narrow shape by being narrowed to the 6 side.

そして、この収容凹部31及び32間に上下に細長い消弧用磁石体21及び22を配置している。このように、固定接触子支持筐体4は、第1の固定接触子5A及び第2の固定接触子5B間のみを幅狭としている。このため、固定接触子支持筐体4は、第1固定接触子5A及び第2の固定接触子5Bに対向する内面側には必要な大きさの消弧空間23及び24を確保することができる。   And, the arc extinguishing magnet bodies 21 and 22 that are elongated vertically are disposed between the housing recesses 31 and 32. Thus, the fixed contact support housing 4 has a narrow width only between the first fixed contact 5A and the second fixed contact 5B. For this reason, the fixed contact support housing 4 can secure arc extinguishing spaces 23 and 24 of a necessary size on the inner surface side facing the first fixed contact 5A and the second fixed contact 5B. .

この第3の実施形態によると、図14に示すように、消弧用磁石体21及び22から出る磁束が第1の固定接触子5Aの固定接点部13及び可動接触子6間と、第2の固定接触子5Bの固定接点部13及び可動接触子6間とを可動接触子6の長手方向に外側に横切ることになる。
このため、図15に示すように、例えば第2の固定接触子5B側から第1の固定接触子5A側に回生電流が流れている状態では、釈放状態に移行場合に、第1の固定接触子5Aの固定接点部13及び可動接触子6間と第2の固定接触子5Bの固定接点部13及び可動接触子6間にアーク30が発生する。
According to the third embodiment, as shown in FIG. 14, the magnetic flux emitted from the arc extinguishing magnet bodies 21 and 22 is between the fixed contact portion 13 and the movable contact 6 of the first fixed contact 5A, and the second Between the fixed contact portion 13 of the fixed contact 5B and the movable contact 6 is crossed outward in the longitudinal direction of the movable contact 6.
For this reason, as shown in FIG. 15, for example, when the regenerative current is flowing from the second fixed contact 5B side to the first fixed contact 5A side, the first fixed contact is moved to the release state. An arc 30 is generated between the fixed contact portion 13 and the movable contact 6 of the child 5A and between the fixed contact portion 13 and the movable contact 6 of the second fixed contact 5B.

このとき、消弧用磁石体21及び22の磁束と電流の向きとによって、フレミングの左手の法則により、ローレンツ力が作用し、図16に示すように、図14に示す消弧空間23側にアーク30を引き伸ばして消弧することができる。電流の向きが第1の固定接触子5A側から第2の固定接触子5B側に流れる場合には、図14に示す消弧空間24側にアーク30を引き伸ばして消弧することができる。したがって第3の実施形態でも、上述した第1の実施形態と同様の作用効果を得ることができる。   At this time, the Lorentz force acts according to Fleming's left-hand rule depending on the magnetic flux and current direction of the arc extinguishing magnet bodies 21 and 22, and as shown in FIG. 16, the arc extinguishing space 23 shown in FIG. The arc 30 can be extended and extinguished. When the direction of current flows from the first fixed contact 5A side to the second fixed contact 5B side, the arc 30 can be extended to the arc extinguishing space 24 side shown in FIG. Therefore, also in the third embodiment, it is possible to obtain the same effects as those in the first embodiment described above.

さらに、上記第3の実施形態では、固定接触子支持筐体4における消弧空間23及び24として必要のない第1の固定接触子5A及び第2の固定接触子5B間を幅狭として収容凹部31及び32を形成したので、固定接触子支持筐体4の外側面に配置する消弧用磁石体を含めた外形寸法を前述した第1の実施形態に比較して狭くすることができ、電磁接触器をより小型化することができる。   Furthermore, in the third embodiment, the space between the first fixed contact 5A and the second fixed contact 5B, which is not necessary as the arc extinguishing spaces 23 and 24 in the fixed contact support housing 4, is made narrow so as to accommodate the receiving recess. Since 31 and 32 are formed, the outer dimensions including the arc extinguishing magnet body arranged on the outer surface of the stationary contact support housing 4 can be made narrower than that of the first embodiment described above. The contactor can be further downsized.

なお、この第3の実施形態においても、消弧用磁石体21及び22の対向磁極面の極性をN極からS極に変更することもできる。
次に、本発明の第4の実施形態を図17〜図22について説明する。
この第4の実施形態は、消弧用磁石体の磁束を効率よく第1及び第2の固定接触子の固定接点部と可動接触子との間に作用させるようにしたものである。
In the third embodiment, the polarity of the opposing magnetic pole surfaces of the arc extinguishing magnet bodies 21 and 22 can be changed from the N pole to the S pole.
Next, a fourth embodiment of the present invention will be described with reference to FIGS.
In the fourth embodiment, the magnetic flux of the arc extinguishing magnet body is efficiently caused to act between the fixed contact portion and the movable contact of the first and second fixed contacts.

すなわち、第4の実施形態では、前述した第3の実施形態における細長い消弧用磁石体21及び22を固定接触子支持筐体4における第1の固定接触子5A及び第2の固定接触子5B間に対向する外側面に配置している。また、固定接触子支持筐体4は、可動接触子6の長手方向の両外側面に消弧用補助磁石体41及び42を配置している。
そして、消弧用磁石体21及び22は対向磁極面がS極とされ、外側面がN極とされている。一方、消弧用補助磁石体41及び42は対向磁極面がN極とされ、外側面がS極とされている。
That is, in the fourth embodiment, the elongated arc extinguishing magnet bodies 21 and 22 in the third embodiment described above are replaced with the first fixed contact 5A and the second fixed contact 5B in the fixed contact support housing 4. It arrange | positions on the outer surface which opposes in between. Further, the stationary contact support housing 4 has arc extinguishing auxiliary magnet bodies 41 and 42 arranged on both outer side surfaces in the longitudinal direction of the movable contact 6.
The arc extinguishing magnet bodies 21 and 22 have an opposite magnetic pole surface as an S pole and an outer surface as an N pole. On the other hand, the arc extinguishing auxiliary magnet bodies 41 and 42 have an opposite magnetic pole surface as an N pole and an outer surface as an S pole.

このため、消弧用磁石体21及び22と消弧用補助磁石体41及び42とで図19に示す磁界が形成される。すなわち、消弧用補助磁石体41の内面側のN極から出る磁束の前側半部が第1の固定接触子5Aの固定接点部13及び可動接触子6間を可動接触子6の長手方向に内側に横切ってから消弧用磁石体21の内面側のS極に達する。
また、消弧用補助磁石体41の内面側のN極から出る磁束の後側半部が第1の固定接触子5Aの固定接点部13及び可動接触子6間を可動接触子6の長手方向に内側に横切ってから消弧用磁石体22の内面側のS極に達する。
For this reason, the magnetic field shown in FIG. 19 is formed by the arc extinguishing magnet bodies 21 and 22 and the arc extinguishing auxiliary magnet bodies 41 and 42. That is, the front half of the magnetic flux emitted from the N pole on the inner surface side of the arc extinguishing auxiliary magnet body 41 is between the fixed contact portion 13 and the movable contact 6 of the first fixed contact 5A in the longitudinal direction of the movable contact 6. After crossing inward, it reaches the south pole on the inner surface side of the arc extinguishing magnet body 21.
Further, the rear half of the magnetic flux emitted from the N pole on the inner surface side of the arc extinguishing auxiliary magnet body 41 is between the fixed contact portion 13 of the first fixed contact 5A and the movable contact 6 in the longitudinal direction of the movable contact 6. And then reaches the south pole on the inner surface side of the arc extinguishing magnet body 22.

同様に、消弧用補助磁石体42の内面側のN極から出る磁束の前側半部が第2の固定接触子5Bの固定接点部13及び可動接触子6間を可動接触子6の長手方向に内側に横切ってから消弧用磁石体21の内面側のS極に達する。
また、消弧用補助磁石体41の内面側のN極から出る磁束の後側半部が第1の固定接触子5Aの固定接点部13及び可動接触子6間を可動接触子6の長手方向に内側に横切ってから消弧用磁石体22の内面側のS極に達する。
Similarly, the front half of the magnetic flux emitted from the N pole on the inner surface side of the arc extinguishing auxiliary magnet body 42 is between the fixed contact portion 13 of the second fixed contact 5B and the movable contact 6 in the longitudinal direction of the movable contact 6. And then reaches the south pole on the inner surface side of the arc extinguishing magnet body 21.
Further, the rear half of the magnetic flux emitted from the N pole on the inner surface side of the arc extinguishing auxiliary magnet body 41 is between the fixed contact portion 13 of the first fixed contact 5A and the movable contact 6 in the longitudinal direction of the movable contact 6. And then reaches the south pole on the inner surface side of the arc extinguishing magnet body 22.

この第4の実施形態によると、第1の固定接触子5Aの固定接点部13及び可動接触子6間を横切る磁束と、第2の固定接触子5Bの固定接点部13及び可動接触子6間を横切る磁束とが前述した第1の実施形態と一致している。
このため、図18に示すように、第1の固定接触子5A側から可動接触子6を経て第2の固定接触子5B側に電流が流れる場合に、投入状態から釈放状態に移行したときに、上述したようにアーク30が発生する。発生したアーク30には、電流及び磁束の方向によりフレミングの左手の法則によって、消弧用磁石体21側に向かうローレンツ力が作用する。
According to the fourth embodiment, the magnetic flux crossing between the fixed contact portion 13 and the movable contact 6 of the first fixed contact 5A, and between the fixed contact portion 13 and the movable contact 6 of the second fixed contact 5B. Is the same as that in the first embodiment described above.
For this reason, as shown in FIG. 18, when a current flows from the first fixed contact 5A side to the second fixed contact 5B side through the movable contact 6, the transition is made from the input state to the release state. As described above, the arc 30 is generated. The generated arc 30 is subjected to Lorentz force toward the arc extinguishing magnet body 21 according to Fleming's left-hand rule according to the direction of current and magnetic flux.

このローレンツ力によって、発生したアーク30が、図20、図21(b)及び図22(b)に示すように、消弧空間23側に大きく引き伸ばされて消弧される。したがって、前述した第1の実施形態と同様の作用効果を得ることができる。
しかも、第4の実施形態では、前述した第2の実施形態のように、消弧用補助磁石体41及び42によって、アーク30が発生する第1の固定接触子5Aの固定接点部13及び可動接触子6間と第2の固定接触子5Bの固定接点部13及び可動接触子6間とで略平行な磁束による磁場を形成することができる。このため、固定接点部13の任意の部位でアーク30が発生しても狙った方向すなわち消弧空間23又は24側にアーク30を引き伸ばすことができる。
Due to this Lorentz force, the generated arc 30 is largely stretched to the arc extinguishing space 23 side and extinguished as shown in FIGS. 20, 21 (b) and 22 (b). Accordingly, it is possible to obtain the same operational effects as those of the first embodiment described above.
Moreover, in the fourth embodiment, as in the second embodiment described above, the fixed contact portion 13 and the movable portion of the first fixed contact 5 </ b> A in which the arc 30 is generated by the arc extinguishing auxiliary magnet bodies 41 and 42. A magnetic field can be formed between the contacts 6 and between the fixed contact portion 13 of the second fixed contact 5B and the movable contact 6 by a substantially parallel magnetic flux. For this reason, even if the arc 30 is generated at an arbitrary portion of the fixed contact portion 13, the arc 30 can be extended in the aimed direction, that is, the arc extinguishing space 23 or 24 side.

なお、上記第4の実施形態においても、消弧用磁石体21及び22の対向磁極面の極性をN極とし、消弧用補助磁石体41及び42の対向磁極面の極性をS極とするようにしても、上記第4の実施形態と同様の作用効果を得ることができる。
次に、本発明の第5の実施形態を図23について説明する。
この第5の実施形態は、消弧用磁石体21及び22の対向磁極面と消弧用補助磁石体41及び42の対向磁極面との間の磁場を大きくするようにしたものである。
Also in the fourth embodiment, the polarity of the opposing magnetic pole surfaces of the arc extinguishing magnet bodies 21 and 22 is N pole, and the polarity of the opposing magnetic pole surface of the arc extinguishing auxiliary magnet bodies 41 and 42 is S pole. Even if it does, the effect similar to the said 4th Embodiment can be acquired.
Next, a fifth embodiment of the present invention will be described with reference to FIG.
In the fifth embodiment, the magnetic field between the opposing magnetic pole surfaces of the arc extinguishing magnet bodies 21 and 22 and the opposing magnetic pole surfaces of the arc extinguishing auxiliary magnet bodies 41 and 42 is increased.

すなわち、第5の実施形態では、図23に示すように、前述した第4の実施形態における図19の構成において、一対の磁性体で形成されるヨーク部51,52で構成されるヨーク50を設けたことを除いては図19と同様の構成を有する。したがって、図19の対応部分には同一符号を付し、その詳細説明はこれを省略する。
ここで、ヨーク部51は、消弧用補助磁石体41の対向磁極面とは反対側の面に接合して左右方向に固定接触支持筐体4に沿って延長する中央板部51aと、この中央板部51aの両端部から後方に延長して消弧用磁石体21及び22の対向磁極面とは反対側の中央部よりやや前端側に接合する端板部51b,51cとでC字状形状に形成されている。
That is, in the fifth embodiment, as shown in FIG. 23, in the configuration of FIG. 19 in the above-described fourth embodiment, the yoke 50 including yoke portions 51 and 52 formed of a pair of magnetic bodies is provided. Except for the provision, the configuration is the same as that of FIG. Accordingly, the corresponding parts in FIG. 19 are denoted by the same reference numerals, and detailed description thereof will be omitted.
Here, the yoke portion 51 is joined to a surface opposite to the opposing magnetic pole surface of the arc extinguishing auxiliary magnet body 41 and extends along the fixed contact support housing 4 in the left-right direction, C-shaped end plate portions 51b and 51c that extend rearward from both end portions of the center plate portion 51a and are joined to the front end side slightly from the center portion opposite to the opposing magnetic pole surfaces of the arc extinguishing magnet bodies 21 and 22. It is formed into a shape.

同様に、ヨーク部52は、消弧用補助磁石体42の対向磁極面とは反対側の面に接合して左右方向に固定接触支持筐体4に沿って延長する中央板部52aと、この中央板部52aの両端部から前方に延長して消弧用磁石体21及び22の対向磁極面とは反対側の中央部よりやや後端側に接合する端板部52b,52cとでC字形状に形成されている。
この第5の実施形態によると、消弧用磁石体21,22の対向磁極面とは反対側と消弧用補助磁石体41,42の対向磁極面とは反対側との間にヨーク部51,52が接合されているので、消弧用磁石体21,22と消弧用補助磁石体41,42との間にヨーク部51,52による閉磁路が形成される。
Similarly, the yoke portion 52 is joined to a surface opposite to the opposing magnetic pole surface of the arc extinguishing auxiliary magnet body 42 and extends along the fixed contact support housing 4 in the left-right direction, C-shaped end plate portions 52b and 52c that extend forward from both ends of the center plate portion 52a and are joined to the rear end side slightly from the center portion on the opposite side to the opposing magnetic pole surfaces of the arc extinguishing magnet bodies 21 and 22. It is formed into a shape.
According to the fifth embodiment, the yoke portion 51 is provided between the side opposite to the opposing magnetic pole surface of the arc extinguishing magnet bodies 21 and 22 and the side opposite to the opposing magnetic pole surface of the arc extinguishing auxiliary magnet bodies 41 and 42. , 52 are joined, a closed magnetic path is formed by the yoke portions 51, 52 between the arc extinguishing magnet bodies 21, 22 and the arc extinguishing auxiliary magnet bodies 41, 42.

このため、ヨーク部51,52によって、消弧用磁石体21,22と消弧用補助磁石体41,42間の磁気効率が向上することで、アークを駆動する磁場を大きくすることができる。したがって、アークの駆動力が増して遮断性能を向上させることができる。しかも、ヨーク部51,52を設けない場合の磁場と同等の磁場を小さい磁石で形成することが可能となり、電磁接触器全体の構成を小型化することができる。   Therefore, the magnetic efficiency between the arc extinguishing magnet bodies 21 and 22 and the arc extinguishing auxiliary magnet bodies 41 and 42 is improved by the yoke portions 51 and 52, so that the magnetic field for driving the arc can be increased. Therefore, the driving force of the arc is increased and the interruption performance can be improved. In addition, a magnetic field equivalent to the magnetic field in the case where the yoke portions 51 and 52 are not provided can be formed with a small magnet, and the configuration of the entire electromagnetic contactor can be reduced in size.

さらに、C字形状の一対のヨーク部51,52を形成して、消弧用磁石体及び消弧用補助磁石体間に装着することにより、容易に閉磁路を形成することができる。
なお、上記第5の実施形態においては、ヨーク部51,52をC字形状に形成したが、これに限らず、消弧用磁石体21,22と消弧用補助磁石体41,42とを磁気的に接続して閉磁路を形成できれば、任意の形状とすることができる。
Furthermore, a closed magnetic circuit can be easily formed by forming a pair of C-shaped yoke portions 51 and 52 and mounting them between the arc extinguishing magnet body and the arc extinguishing auxiliary magnet body.
In addition, in the said 5th Embodiment, although the yoke parts 51 and 52 were formed in C-shape, not only this but the arc-extinguishing magnet bodies 21 and 22 and the arc-extinguishing auxiliary magnet bodies 41 and 42 are included. Any shape can be used as long as it can be magnetically connected to form a closed magnetic circuit.

1…電磁接触器、2…接点機構、3…駆動機構、4…固定接触子支持筐体、4a…上面板、4b,4c…側面部、5A…第1の固定接触子、5B…第2の固定接触子、6…可動接触子、7…絶縁碍子、8…シャフト、11…雌ねじ部、12…固定端子部、13…固定接点部、21,22…消弧用磁石体、21a,21b,22a,22b…分割磁石体、23,24…消弧空間、30…アーク、31,32…収容凹部、41,42…消弧用補助磁石体、50…ヨーク、51,52…ヨーク部   DESCRIPTION OF SYMBOLS 1 ... Electromagnetic contactor, 2 ... Contact mechanism, 3 ... Drive mechanism, 4 ... Fixed contact support housing | casing, 4a ... Top plate, 4b, 4c ... Side part, 5A ... 1st fixed contact, 5B ... 2nd 6 ... movable contact, 7 ... insulator, 8 ... shaft, 11 ... female screw, 12 ... fixed terminal, 13 ... fixed contact, 21, 22 ... arc extinguishing magnet, 21a, 21b 22a, 22b ... split magnet body, 23, 24 ... arc extinguishing space, 30 ... arc, 31, 32 ... receiving recess, 41, 42 ... auxiliary magnet body for arc extinguishing, 50 ... yoke, 51, 52 ... yoke part

Claims (7)

固定接点部及び電源に接続される固定端子部を有する第1の固定接触子と、固定接点部及び負荷に接続される固定端子部とを有する第2の固定接触子と、
前記第1の固定接触子及び第2の固定接触子を、所定間隔を保ち且つ両者の前記固定端子部を外部に突出させて支持する固定接触子支持筐体と、
前記第1の固定接触子の固定接点部及び前記第2の固定接触子の固定接点部に接離可能で前記固定接触子支持筐体内に配置された可動接触子と、
前記可動接触子の長手方向と直交する方向で当該可動接触子を挟んで平行に配設され、互いの対向磁極面が同一極性とされた一対の消弧用磁石体と、
前記可動接触子を前記第1の固定接触子及び第2の固定接触子に対して接離可能に駆動する駆動機構とを備え、
前記一対の消弧用磁石体は、前記第1の固定接触子及び前記可動接触子に対向する一対の第1の磁石体と、前記第2の固定接触子及び前記可動接触子に対向する一対の第2の磁石体とを有し、
前記第1の磁石体と前記第2の磁石体との対向磁極面を異なる極性に設定し、開極時に発生するアークの伸張方向を、前記可動接触子を挟んで反対方向としてアーク同士の干渉を防止する
ことを特徴とする電磁接触器。
A first fixed contact having a fixed contact and a fixed terminal connected to a power source; a second fixed contact having a fixed contact and a fixed terminal connected to a load;
A fixed contact support housing for supporting the first fixed contact and the second fixed contact by keeping a predetermined distance and projecting the fixed terminal portions of both to the outside;
A movable contact disposed in the stationary contact support housing and capable of contacting and separating from the stationary contact portion of the first stationary contact and the stationary contact portion of the second stationary contact;
A pair of arc extinguishing magnet bodies disposed in parallel across the movable contact in a direction orthogonal to the longitudinal direction of the movable contact, the opposing magnetic pole surfaces having the same polarity;
A drive mechanism for driving the movable contact so as to be able to contact and separate with respect to the first fixed contact and the second fixed contact;
The pair of arc extinguishing magnet bodies includes a pair of first magnet bodies facing the first fixed contact and the movable contact, and a pair facing the second fixed contact and the movable contact. A second magnet body,
The opposing magnetic pole surfaces of the first magnet body and the second magnet body are set to different polarities, and the arc extension direction generated at the time of opening is set as the opposite direction across the movable contact so that the arcs interfere with each other. An electromagnetic contactor characterized by preventing
前記第1の磁石体の対向磁極面がS極とされ、前記第2の磁石体の対向磁極面がN極とされていることを特徴とする請求項1に記載の電磁接触器。   The electromagnetic contactor according to claim 1, wherein the opposing magnetic pole surface of the first magnet body is an S pole and the opposing magnetic pole surface of the second magnet body is an N pole. 前記第1の磁石体の対向磁極面がN極とされ、前記第2の磁石体の対向磁極面がS極とされていることを特徴とする請求項1に記載の電磁接触器。   The electromagnetic contactor according to claim 1, wherein the opposing magnetic pole surface of the first magnet body is an N pole, and the opposing magnetic pole surface of the second magnet body is an S pole. 前記固定接触子支持筐体は、前記第1の固定接触子及び前記可動接触子と、前記第2の固定接触子及び前記可動接触子とにそれぞれ対向する内壁面に消弧空間が形成されていることを特徴とする請求項1から3の何れか1項に記載の電磁接触器。   The fixed contact support housing has an arc extinguishing space formed on an inner wall surface facing the first fixed contact and the movable contact, and the second fixed contact and the movable contact, respectively. The electromagnetic contactor according to any one of claims 1 to 3, wherein the electromagnetic contactor is provided. 前記固定接触子支持筐体は、前記第1の固定接触子及び第2の固定接触子間に対向する外側面に前記一対の消弧用磁石体を収容する収容凹部が形成されていることを特徴とする請求項1から4の何れか1項に記載の電磁接触器。   The stationary contact support housing has an accommodation recess for accommodating the pair of arc extinguishing magnet bodies on an outer surface facing between the first stationary contact and the second stationary contact. The electromagnetic contactor according to claim 1, wherein the electromagnetic contactor is characterized in that: 前記可動接触子の延長方向の両端部に対となる消弧用補助磁石体が配設され、該消弧用補助磁石体の対向磁極面の極性が前記一対の消弧用磁石体の極性と逆極性とされていることを特徴とする請求項1から5の何れか1項に記載の電磁接触器。   A pair of arc extinguishing auxiliary magnet bodies are disposed at both ends of the movable contact in the extending direction, and the polarity of the opposing magnetic pole surface of the arc extinguishing auxiliary magnet body is the same as the polarity of the pair of arc extinguishing magnet bodies. The electromagnetic contactor according to claim 1, wherein the magnetic contactor has reverse polarity. 前記一対の消弧用磁石体の対向磁極面とは反対側と前記対となる消弧用補助磁石体の対向磁極面とは反対側との間を接合するヨークを配置したことを特徴とする請求項6に記載の電磁接触器。   A yoke is provided for joining between the opposite side of the pair of arc extinguishing magnet bodies and the opposite side of the pair of arc extinguishing auxiliary magnet bodies. The electromagnetic contactor according to claim 6.
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