JPH01168011A - Polarized electromagnet - Google Patents

Polarized electromagnet

Info

Publication number
JPH01168011A
JPH01168011A JP62326321A JP32632187A JPH01168011A JP H01168011 A JPH01168011 A JP H01168011A JP 62326321 A JP62326321 A JP 62326321A JP 32632187 A JP32632187 A JP 32632187A JP H01168011 A JPH01168011 A JP H01168011A
Authority
JP
Japan
Prior art keywords
magnetic pole
piece
magnetic
yoke
iron core
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP62326321A
Other languages
Japanese (ja)
Other versions
JP2613904B2 (en
Inventor
Yoichi Yokoyama
洋一 横山
Hiroaki Hamaguchi
浜口 博昭
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP62326321A priority Critical patent/JP2613904B2/en
Priority to DE3852624T priority patent/DE3852624T2/en
Priority to EP88116765A priority patent/EP0321664B1/en
Priority to US07/267,219 priority patent/US4855701A/en
Publication of JPH01168011A publication Critical patent/JPH01168011A/en
Application granted granted Critical
Publication of JP2613904B2 publication Critical patent/JP2613904B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01HELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
    • H01H89/00Combinations of two or more different basic types of electric switches, relays, selectors and emergency protective devices, not covered by any single one of the other main groups of this subclass
    • H01H89/06Combination of a manual reset circuit with a contactor, i.e. the same circuit controlled by both a protective and a remote control device
    • H01H89/08Combination of a manual reset circuit with a contactor, i.e. the same circuit controlled by both a protective and a remote control device with both devices using the same contact pair
    • H01H89/10Combination of a manual reset circuit with a contactor, i.e. the same circuit controlled by both a protective and a remote control device with both devices using the same contact pair with each device controlling one of the two co-operating contacts
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01HELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
    • H01H51/00Electromagnetic relays
    • H01H51/22Polarised relays
    • H01H51/2209Polarised relays with rectilinearly movable armature

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  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Electromagnets (AREA)

Abstract

PURPOSE:To improve magnetic efficiency at the time of energizing and to obtain a sufficient attraction force of a polarized electromagnet for moving a core longitudinally of a pole piece by the energization of a coil by disposing the pole faces of any pole piece and the core for forming one or two main air gaps in a nonfacing manner at the time of nonenergizing, and extending the end of the piece to the core, or the end of the core to the pole piece. CONSTITUTION:The end of a yoke 6 at the opposite side to an L-shaped piece 6a is extended to an armature piece 5, the length of the piece 5 is shortened as compared with the size between both the yokes 6 and 6 to be inserted between the two yokes 6 and 6, thereby providing an air gap of a leakage type. A magnetic flux phi1 flows in a nonenergizing state. When a coil 1 is energized, a magnetic flux phi2 tends to flow. In this case, in a main air gap (3), the distance between the pole face of the end face of the yoke 6 and the pole face of the end face of the armature piece 5 is approached, thereby reducing its magnetic resistance. Accordingly, the magnetic resistance of the whole loop of magnetic flux phi2 is reduced at the time of energizing, thereby improving its energizing efficiency.

Description

【発明の詳細な説明】 [技術分野] 本発明は、4つの主空隙を有する4空隙ブリッジ型磁気
回路楕成からなる有極電磁石に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to a polarized electromagnet consisting of a four-gap bridge type magnetic circuit ellipse having four main gaps.

[背景技術J 第11図は従来の電磁開閉装置を示し、この電磁開閉装
置は常閉型(b接、α型)単安定動作タイプであり、第
12図にその吸引力とバネ負荷特性を示している。第1
1図において、外周にコイル1を巻装したコイルボビン
2内に可動鉄心3がその軸方向移動自在に嵌入されてい
る。この可動鉄心3の両端には夫々接極子4,5が固着
しである。
[Background Art J Figure 11 shows a conventional electromagnetic switchgear. This electromagnetic switchgear is a normally closed (b-contact, α-type) monostable operation type, and Figure 12 shows its attraction force and spring load characteristics. It shows. 1st
In FIG. 1, a movable core 3 is fitted into a coil bobbin 2 having a coil 1 wound around its outer periphery so as to be movable in the axial direction. Armatures 4 and 5 are fixed to both ends of the movable core 3, respectively.

尚、雨後極子4,5と可動鉄心3とで鉄心部を構成して
いる。フィル1の外側には略し型の磁極片であるヨーク
6.6が夫々配置され、このヨーク6の外側に永久磁石
7,7が夫々配置されている。
Incidentally, the rain poles 4 and 5 and the movable iron core 3 constitute an iron core portion. Yokes 6, 6, which are abbreviated magnetic pole pieces, are arranged on the outside of the fill 1, and permanent magnets 7, 7 are arranged on the outside of the yokes 6, respectively.

また、永久磁石7の外側に磁極片である略コ字型のヨー
ク8が夫々配置され、両ヨーク6.8にて永久磁石7を
はさんでいる。ここで、ヨーク6のL型片6ai−ヨー
ク8のL型片8aとの間に一方の接極子4の端部が位f
nシ、また、ヨーク8の他方のL型片8bとヨーク6の
端面との間に他方の接極子5の端部が位置している。こ
れら、#に極子4゜5とL型片(3at 8 a、 8
 bとはその磁極面が夫々対向して配置しである。シー
ク8のL型片8aの内側にはレシジュアルプレート9が
設けである。
Further, approximately U-shaped yokes 8, which are magnetic pole pieces, are arranged on the outside of the permanent magnet 7, and the permanent magnet 7 is sandwiched between the two yokes 6.8. Here, the end of one armature 4 is positioned between the L-shaped piece 6ai of the yoke 6 and the L-shaped piece 8a of the yoke 8.
Also, the end of the other armature 5 is located between the other L-shaped piece 8b of the yoke 8 and the end surface of the yoke 6. These, #, pole 4゜5 and L-shaped piece (3at 8a, 8
b means that the magnetic pole faces are arranged opposite to each other. A regular plate 9 is provided inside the L-shaped piece 8a of the seeker 8.

可動鉄心3の端部には接触子ホルダー10が取着してあ
り、この接触子ホルダー10に接点バネ12により付勢
されている可動接触子11を設けている。この可動接触
子11の両側には可動接点11mが固着してあり、可動
接点11aに相対する固定接点13aを固着した固定接
点板13が配置しである。また、可動鉄心3を復帰させ
る復帰バネ14が可動鉄心3の突出方向側に設けられて
いる。
A contact holder 10 is attached to the end of the movable iron core 3, and a movable contact 11 biased by a contact spring 12 is provided on the contact holder 10. A movable contact 11m is fixed to both sides of the movable contact 11, and a fixed contact plate 13 is arranged on which a fixed contact 13a facing the movable contact 11a is fixed. Further, a return spring 14 for returning the movable core 3 is provided on the protruding direction side of the movable core 3.

ここで、ヨーク8のL型片8aと接極子4との開を主空
隙■とし、接極子4とヨーク6のL型片(3mとの間を
主空隙■とし、ヨーク6の端部と接極子5との間を主空
隙■とし、接極子5とヨーク8のL型片8bとの間を主
空隙■とする。
Here, the opening between the L-shaped piece 8a of the yoke 8 and the armature 4 is defined as the main gap ■, the gap between the armature 4 and the L-shaped piece (3m) of the yoke 6 is defined as the main gap ■, and the end of the yoke 6 and The space between the armature 5 and the armature 5 is defined as a main gap (2), and the space between the armature 5 and the L-shaped piece 8b of the yoke 8 is defined as a main gap (2).

第11図(b)は無励磁状態を示し、この状態においで
、永久磁石7の磁束は、N極がら、ヨーク6→主空隙■
→接極子4→可動鉄心3→接極子5→主空隙■→ヨーク
8を通り永久磁石7のS極に流れるφ、を形成する。こ
の状態において、主空隙■及び主空隙■で発生する吸引
力により接極子4,5及び可動鉄心3で構成される可動
鉄心ブッロクは第11図(b)の状態に保持され、接、
σ11a。
FIG. 11(b) shows a non-excited state. In this state, the magnetic flux of the permanent magnet 7 changes from the N pole to the yoke 6 → the main air gap
-> Armature 4 -> Movable iron core 3 -> Armature 5 -> Main gap ■ -> φ flowing through the yoke 8 to the S pole of the permanent magnet 7 is formed. In this state, the movable core block composed of the armatures 4 and 5 and the movable core 3 is held in the state shown in FIG.
σ11a.

13aは開成されている。この状態において、第11図
(b)に示すように接極子4,5に図示したN極、S極
が発生するようにコイル1を励磁すると、主空隙■では
、接極子4に発生したN極と、ヨーク6の永久磁石7に
よるN極が対抗し、磁位差は低下し磁束が著しく減少す
る。主空隙■でも同様にS極同士となって磁束は減少す
る。
13a is open. In this state, when the coil 1 is excited so that the N and S poles shown in the armatures 4 and 5 are generated as shown in FIG. The pole and the north pole formed by the permanent magnet 7 of the yoke 6 oppose each other, the magnetic potential difference decreases, and the magnetic flux decreases significantly. Similarly, in the main gap (2), the south poles become mutual, and the magnetic flux decreases.

一方、主空隙■と主空隙■では、接極子4とヨーク8、
接極子5とヨーク6とが夫々互いにN極、S極になるの
で、磁位差は増大し、磁束が増大する。従って、主空隙
■と■での吸引力が増加し、主空隙■と■での吸引力が
低下するので、可動鉄心プッロクを保持する力は低下す
る。この吸引力より接点バネ12の力が太き(なれば、
可動鉄心ブッロクは図の左方向に勤務、第11図(a)
の状態に動作する。この状態では接点11a、13aは
開成する。尚、第11図(b)の磁束φ2は励磁時にお
ける磁束の流れを示している。
On the other hand, in the main gap ■ and the main gap ■, the armature 4 and the yoke 8,
Since the armature 5 and the yoke 6 become N-pole and S-pole, respectively, the magnetic potential difference increases and the magnetic flux increases. Therefore, the suction force in the main gaps (2) and (2) increases, and the suction force in the main gaps (2) and (2) decreases, so that the force for holding the movable iron pulley decreases. The force of the contact spring 12 is greater than this suction force (if it becomes
The movable core block works toward the left in the figure, Figure 11 (a)
operate in the state of In this state, contacts 11a and 13a are open. Incidentally, the magnetic flux φ2 in FIG. 11(b) indicates the flow of magnetic flux during excitation.

この電磁石の構成は、第13図に示すように4空隙ブリ
ツジ型の磁気回路構成であり、高効率な有極磁気回路構
成として公知なものであり、電磁rl 11 !!置に
よく使われている。第11図ではレシジュアルプレート
9を挿入し、また、ヨーク6の主空隙■側での磁極面積
を小さくして、単安定動作をし易くしている。その吸引
力は第12図に示す通りである。第12図の左端が第1
1図(b)の状態で、右端が第11図(a)の状態と対
応している。
The configuration of this electromagnet is a four-gap bridge type magnetic circuit configuration as shown in FIG. 13, which is known as a highly efficient polarized magnetic circuit configuration, and the electromagnetic rl 11 ! ! It is often used for placement. In FIG. 11, a regular plate 9 is inserted, and the area of the magnetic pole on the main gap (2) side of the yoke 6 is reduced to facilitate monostable operation. The suction force is as shown in FIG. The left end of Figure 12 is the first
In the state of FIG. 1(b), the right end corresponds to the state of FIG. 11(a).

この従来例において、接点バネ荷重は、接点の位置ずれ
によるオーバートラベル(OT )@バラツキ、接、α
バネそのもののバラツキ1.接点消耗によるOTの減少
等、接点バネ荷重のバラツキ要因が多く、充分な吸引力
の余裕あることが望ましい。
In this conventional example, the contact spring load is overtravel (OT) @ variation due to positional deviation of the contact, contact, α
Variations in the spring itself 1. There are many factors that cause variations in contact spring loads, such as a decrease in OT due to contact wear, so it is desirable to have sufficient margin for suction force.

しかし、ヨーク6の端面と接極子5との磁極面とが対向
しており、その閤あ主空隙■が広く磁気抵抗が高く、充
分な吸引力が得られないという問題があった。
However, the end face of the yoke 6 and the magnetic pole face of the armature 5 face each other, and the main gap (2) between them is wide and the magnetic resistance is high, resulting in a problem that sufficient attractive force cannot be obtained.

[発明の目的] 本発明は、上述の点に鑑みて提供したものであって、励
磁時の磁気効率を向上させ、充分な吸引力を得ることを
目的とした有極電磁石を提供するものである。
[Object of the Invention] The present invention has been provided in view of the above-mentioned points, and provides a polarized electromagnet for the purpose of improving magnetic efficiency during excitation and obtaining sufficient attractive force. be.

[発明の開示] (構成) 本発明は、永久磁石と、該永久磁石をはさむ2つの磁極
片と、コイルが巻装されて上記磁極片と磁気回路を形成
する鉄心部とを1Jc(filL、、上記2つの磁極片
の両端部の間に鉄心部の端部が夫々位置して2つの磁極
片と鉄心部とにより4つの主空隙を形成する4空隙ブリ
ッジ型磁気回路h1成であって、コイルの励磁により鉄
心部が磁極片の長子方向に移動す2る有極電磁石におい
て、無励磁時に1つ若しくは2つの主空隙を構成するい
ずれかの磁極片の磁極面と鉄心部側の磁極面とを非対向
に配置し、磁極片の端部を鉄心部側に、あるいは鉄心部
の端部を磁極片側に延出形成することにより、無励磁時
に1つ若しくは2つの主空隙を心!成する磁極片と鉄心
部との両磁極面を対向させずに配置し、磁極片のra部
を鉄心部側に、あるいは鉄心部の端部を磁極片側に延出
形成して、当該主空隙を狭くして両磁極面間の磁気抵抗
を小さくし、もって励磁時に充分な吸引力を得るように
したことをvf徴とするものである。
[Disclosure of the Invention] (Structure) The present invention provides a permanent magnet, two magnetic pole pieces sandwiching the permanent magnet, and an iron core portion around which a coil is wound to form a magnetic circuit with the magnetic pole pieces. , a four-gap bridge type magnetic circuit h1 configuration in which the ends of the iron core are located between the ends of the two magnetic pole pieces, and four main gaps are formed by the two magnetic pole pieces and the iron core, In a two-poled electromagnet in which the core moves in the longitudinal direction of the pole pieces when the coil is energized, the pole face of one of the pole pieces that constitutes one or two main gaps when not energized and the pole face on the core side By arranging the pole pieces not facing each other, and by forming the end of the magnetic pole piece on the iron core side, or the end of the iron core part extending to one side of the magnetic pole, one or two main gaps are formed in the center when not energized. The main gap is formed by arranging the magnetic pole surfaces of the magnetic pole piece and the iron core part so that they do not face each other, and by forming the RA part of the magnetic pole piece on the iron core side or the end of the iron core part extending to one side of the magnetic pole. The vf characteristic is that the magnetic resistance between the two magnetic pole faces is reduced by narrowing the magnetic field, thereby obtaining sufficient attractive force during excitation.

(実施例1) 以下、本発明の実施例を図面を参照して説明する。第1
図は本発明を示し、同図(a)は励磁状態を、同図(b
)は無励磁状態を夫々示している。
(Example 1) Hereinafter, an example of the present invention will be described with reference to the drawings. 1st
The figures show the present invention, with (a) showing the excitation state and (b) showing the excitation state.
) indicate the non-excited state.

本発明は第1図に示すように、L型片6aとは反対側の
ヨーク6の端部を接極子5側に延出形成し、接極子5の
長さを両ヨーク6.6開の寸法より短くし、2つのヨー
ク6.6間にもぐり込むようにして、リーケージ型の空
隙にしたものである。すなわち、ヨーク6の接極子5g
Aの磁極面と、接極子5の磁極面とを対向させずに磁極
面同士が直交する形とし、ヨーク6の端部の磁極面と接
極子5の磁極面との開を主空隙■とし、この主空隙■の
寸法を短くして磁気抵抗を小さくしたものである。
As shown in FIG. 1, in the present invention, the end of the yoke 6 on the opposite side to the L-shaped piece 6a is formed to extend toward the armature 5 side, and the length of the armature 5 is set so that both yokes 6 and 6 are open. It is made shorter than the dimensions and fits between the two yokes 6.6 to form a leakage-type gap. That is, the armature 5g of the yoke 6
The magnetic pole surface of A and the magnetic pole surface of the armature 5 are not opposed, but are perpendicular to each other, and the opening between the magnetic pole surface of the end of the yoke 6 and the magnetic pole surface of the armature 5 is defined as the main gap ■. , the size of this main gap (2) is shortened to reduce magnetic resistance.

他の構成は第11図の従来例と同じである。f52図は
本電磁石装装置の斜視図を示している。
The other configurations are the same as the conventional example shown in FIG. Figure f52 shows a perspective view of the present electromagnetic device.

動作原理は第11図の従来例と全く同じであり、第1図
の無励磁状態においては従来と同様に磁束φ1が流れる
。そして、コイル1を励磁すると、従来と同様に磁束φ
2が流れようとする。この時、主空隙■において、ヨー
ク6の端面の磁極面と接極子5の端面の磁極面との距離
が第11図の(11)の場合よりも近く、磁気抵抗は小
さくなりでいる。従って、励磁時、磁束φ2のループ全
体の磁気抵抗は、第11図(1,)の場合より小さくな
り、励磁効率が良くなる。t53図はこの場合の吸引力
特性を示している。第3図の動作開始吸引力特性におい
て、実線は本発明の実施例の場合を示し、破線は一従来
例の場合を示している。従って、動作開始時においては
Fの吸引力の差が生じ、同じ励磁7ンベアターンで吸引
力は大きくなるものである。
The operating principle is exactly the same as the conventional example shown in FIG. 11, and in the non-excited state shown in FIG. 1, the magnetic flux φ1 flows as in the conventional example. Then, when coil 1 is excited, the magnetic flux φ
2 is about to flow. At this time, in the main gap (2), the distance between the magnetic pole surface of the end surface of the yoke 6 and the magnetic pole surface of the end surface of the armature 5 is closer than in the case (11) of FIG. 11, and the magnetic resistance is small. Therefore, during excitation, the magnetic resistance of the entire loop of magnetic flux φ2 is smaller than in the case of FIG. 11 (1,), and the excitation efficiency is improved. The t53 diagram shows the attraction force characteristics in this case. In the operation start suction force characteristics shown in FIG. 3, the solid line shows the case of the embodiment of the present invention, and the broken line shows the case of a conventional example. Therefore, at the start of operation, there is a difference in the attraction force of F, and the attraction force increases with the same excitation seven bearing turns.

このように構成することにより、励磁時の吸引力が大き
くなり、接点OTのバラツキ、接点消耗等によりバネ荷
重が変動しても、電磁開閉装置の動作電圧は所定値で動
作することができるものである。また、電磁開閉装置の
高感度化も可能であ・る。
With this configuration, the attractive force during excitation becomes large, and even if the spring load fluctuates due to variations in contact OT, contact wear, etc., the operating voltage of the electromagnetic switchgear can operate at a predetermined value. It is. It is also possible to increase the sensitivity of electromagnetic switching devices.

ところで、第1図は、可動鉄心3を中心としてヨーク6
.8、永久磁石7が対象に配置された構成であるが、1
4図に示すように、可動鉄心3の片側のみにヨーク6.
8、永久磁石7を配置した構成でも上記と同じ効果が得
られる。尚、この場合、可動鉄心3の両端上り接極子4
,5を一体的に形成している。
By the way, FIG. 1 shows the yoke 6 centered around the movable core 3.
.. 8. The permanent magnet 7 is arranged on the target, but 1
As shown in Figure 4, a yoke 6. is attached only to one side of the movable core 3.
8. The same effect as above can be obtained even with a configuration in which permanent magnets 7 are arranged. In this case, the upward armature 4 at both ends of the movable iron core 3
, 5 are integrally formed.

(実施例2) 第5図は2ツチングタイプの有極電峨石を示し、ヨーク
6はコ字型に形成してあり、端部のL型片6 a、 6
 bと外側のヨーク8,8のL型片8a、8bとの間に
可動鉄心3に固着した接極子4.5を夫々配置したもの
である。この第5図に示すも!戊から、第6図に示すよ
うに、ヨーク6のL型片6a。
(Example 2) Fig. 5 shows a two-touching type polarized electromagnetic stone, in which the yoke 6 is formed in a U-shape, and the L-shaped pieces 6a, 6 at the ends are formed in a U-shape.
Armatures 4.5 fixed to the movable core 3 are arranged between the L-shaped pieces 8a and 8b of the outer yokes 8 and 8, respectively. This is also shown in Figure 5! From the bottom, as shown in FIG. 6, the L-shaped piece 6a of the yoke 6.

G I)の部分を削除し、第1図の場合と同様に接極子
4,5を両ヨ7り6,6間の寸法より短くしたものであ
る。ここで、ヨーク8のL型片8aと接極子4との間を
主空隙■とし、接極子4の端部とヨーク6の端部との間
を主空隙■とし、ヨーク6の他方の端部と接極子5の端
部との開を主空隙■とし、接極子5とヨーク8のL型片
8bとの開を主空隙■としている。
GI) is deleted, and the armatures 4 and 5 are made shorter than the length between the two sides 6 and 6, as in the case of FIG. Here, the main gap (■) is between the L-shaped piece 8a of the yoke 8 and the armature 4, the main gap (■) is between the end of the armature 4 and the end of the yoke 6, and the other end of the yoke 6 is The opening between the armature 5 and the end of the armature 5 is defined as a main gap (2), and the opening between the armature 5 and the L-shaped piece 8b of the yoke 8 is defined as a main gap (2).

第7図は吸引力特性を示し、実線は第6図の場合を示し
、破線はf55図の場合を示している。
FIG. 7 shows the attraction force characteristics, the solid line shows the case of FIG. 6, and the broken line shows the case of f55.

第7図のΔは第6図の場合の吸引力幅を示し、Bは第5
図の場合の吸引力幅を示している。そして、A>Bとな
っている。第6図に示すような構成とすることにより、
先の実施例と同様に主空隙をリーケージ型として磁気効
率を向上させて吸引力を向上させることができる。尚、
第7図に示すように、ストロークの最終端付近は、永久
磁石7による吸引力は低下するが、動磁した時の吸引力
幅は増え、励磁効率が改善されるものである。
Δ in Fig. 7 indicates the suction force width in the case of Fig. 6, and B indicates the width of the suction force in the case of Fig. 6.
The width of the suction force in the case shown in the figure is shown. Then, A>B. By having the configuration as shown in Figure 6,
As in the previous embodiment, the main gap can be of a leakage type to improve magnetic efficiency and improve attractive force. still,
As shown in FIG. 7, near the final end of the stroke, the attractive force by the permanent magnet 7 decreases, but the width of the attractive force when magnetized increases, and the excitation efficiency is improved.

@6図は、可動鉄心3を中心としてヨーク6會8、永久
磁石7が対象に配置されたラッチングタイプの構成であ
るが、第8図に示すように、可動鉄心3の片側のみにヨ
ーク6.8、永久磁石7を配置した構成でも上記と同じ
効果が得られる。尚、この場合、可動鉄心3の両端より
接極子4,5を一体的に形成している。
Figure @6 shows a latching type configuration in which a yoke 6 and a permanent magnet 7 are arranged symmetrically around a movable core 3, but as shown in FIG. 8. The same effect as above can be obtained even with a configuration in which permanent magnets 7 are arranged. In this case, the armatures 4 and 5 are integrally formed from both ends of the movable iron core 3.

(実施例3) 第9図は第3実施例を示し、先の実施例のヨーク8の両
側のL型片8 m、 8 bを削除して、ヨーク8の両
端と接極子4,5の端部との間を主空隙としたものであ
る。第9図の場合もラッチングタイプの有極電磁石構成
である。第10図は第9図の場合の片側構成とした実施
例である。この場合、可動鉄心3の両端より接極子4,
5を一体的に形成してヨーク8側まで延出している。
(Embodiment 3) FIG. 9 shows a third embodiment, in which the L-shaped pieces 8m and 8b on both sides of the yoke 8 of the previous embodiment are deleted, and both ends of the yoke 8 and the armatures 4 and 5 are replaced. The main gap is between the ends. The case shown in FIG. 9 also has a latching type polar electromagnet configuration. FIG. 10 shows an embodiment of the one-sided structure in the case of FIG. 9. In this case, the armature 4,
5 is integrally formed and extends to the yoke 8 side.

[発明の効果] 本発明は上述のように、永久磁石と、該永久磁石をはさ
む2つの磁極片と、コイルが巻装されて上記磁極片と磁
気回路を形成する鉄心部とを具備し、上記2つの磁極片
の両端部の間に鉄心部の端部が夫々位置して2つの磁極
片と鉄心部とにより4つの主空隙を形成する4空隙ブリ
ッジ型磁気回路構成であって、フィルの励磁により鉄心
部が磁極片の長手方向に移動する有極電磁石において、
無励磁時に1つ若しくは2つの主空隙を構成するいずれ
かの磁極片の磁極面と鉄心部側の磁極面とを非対向に配
置し、磁極片の端部を鉄心部側に、あるいは鉄心部の?
@部を磁極片側に延出形成したものであるから、無励磁
時に1つ若しくは2つの主空隙を構成する磁極片と鉄心
部との両磁極面を対向させずに配置し、磁極片の端部を
鉄心部側に、あるいは鉄心部の端部を磁極片側に延出形
成して、当該主空隙を狭くして両磁極面間の磁気抵抗を
小さくし、もって励磁時に充分な吸引力を得ることがで
きる効果を奏するものである。
[Effects of the Invention] As described above, the present invention includes a permanent magnet, two magnetic pole pieces sandwiching the permanent magnet, and an iron core portion around which a coil is wound to form a magnetic circuit with the magnetic pole piece. A four-gap bridge type magnetic circuit configuration in which the ends of the iron core are located between the ends of the two magnetic pole pieces, and four main gaps are formed by the two magnetic pole pieces and the iron core. In a polarized electromagnet in which the iron core moves in the longitudinal direction of the magnetic pole piece due to excitation,
When not energized, the magnetic pole surface of one of the magnetic pole pieces constituting one or two main gaps and the magnetic pole surface on the iron core side are arranged non-opposingly, and the end of the magnetic pole piece is placed on the iron core side or of?
Since the @ part is formed to extend to one side of the magnetic pole, the pole surfaces of the magnetic pole piece and the iron core part, which constitute one or two main gaps when not energized, are arranged so as not to face each other, and the end of the magnetic pole piece is The main gap is narrowed by forming a part on the iron core side or an end of the iron core part extending to one side of the magnetic pole to reduce the magnetic resistance between the two magnetic pole faces, thereby obtaining sufficient attractive force during excitation. It has the effect that it can.

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

第1図(aHb)は本発明の実施例の励磁状態を示す断
面図、及び無励磁状態を示す断面図、第2図は同上の斜
視図、fpJ3図は同上の吸引力特性を示す特性図、t
jS4図は同上の片側構成とした実施例を示す断面図、
第5図は同上の他の実施例の従来例となるラッチングタ
イプの有極電磁石の断面図、第6図は同上の他の実施例
の断面図、rJS7図は同上の吸引力特性を示す特性図
、第8図は同上の片側構成とした実施例を示す断面図、
第9図は同上の実施例3の断面図、第10図は同上の片
側構成とした実施例を示す断面図、r511図(a)(
1,)は従来例の励磁状態を示す断面図、及び無rIJ
h、磁状態を示す断面図、第12図は従来例の吸引力特
性を示す特性図、第13図は同上の等価回路図である。 1はコイル、3は可動鉄心、4,5は接極子、6はヨー
ク、7は永久磁石、8はヨーク、■〜■は主空隙である
。 代理人 弁理士 石 1)長 七 1・・・コイル 6・・・ヨーク 7・・・永久磁石 (b) 第3図 第4図 第5図 第9図 :1 5 第11図 (b) 第12図 第13図
Fig. 1 (aHb) is a sectional view showing an excitation state and a sectional view showing an unexcited state of the embodiment of the present invention, Fig. 2 is a perspective view of the same as above, and Fig. fpJ3 is a characteristic diagram showing the attraction force characteristics of the same as above. ,t
Figure jS4 is a sectional view showing an embodiment with the same one-sided configuration as above,
Fig. 5 is a sectional view of a latching type polar electromagnet which is a conventional example of another embodiment of the same as above, Fig. 6 is a sectional view of another embodiment of the same as above, and rJS7 is a characteristic showing the attraction force characteristics of the same as above. FIG. 8 is a sectional view showing an embodiment with the same one-sided configuration as above,
FIG. 9 is a cross-sectional view of the third embodiment same as above, FIG. 10 is a cross-sectional view showing an embodiment with one side configuration same as above,
1,) is a sectional view showing the excitation state of the conventional example and the non-rIJ
h is a sectional view showing the magnetic state, FIG. 12 is a characteristic diagram showing the attraction force characteristics of the conventional example, and FIG. 13 is an equivalent circuit diagram of the same. 1 is a coil, 3 is a movable iron core, 4 and 5 are armatures, 6 is a yoke, 7 is a permanent magnet, 8 is a yoke, and ■ to ■ are main gaps. Agent Patent Attorney Stone 1) Long 71... Coil 6... Yoke 7... Permanent magnet (b) Figure 3 Figure 4 Figure 5 Figure 9: 1 5 Figure 11 (b) Figure 12 Figure 13

Claims (1)

【特許請求の範囲】[Claims] (1)永久磁石と、該永久磁石をはさむ2つの磁極片と
、コイルが巻装されて上記磁極片と磁気回路を形成する
鉄心部とを具備し、上記2つの磁極片の両端部の間に鉄
心部の端部が夫々位置して2つの磁極片と鉄心部とによ
り4つの主空隙を形成する4空隙ブリッジ型磁気回路構
成であって、コイルの励磁により鉄心部が磁極片の長手
方向に移動する有極電磁石において、無励磁時に1つ若
しくは2つの主空隙を構成するいずれかの磁極片の磁極
面と鉄心部側の磁極面とを非対向に配置し、磁極片の端
部を鉄心部側に、あるいは鉄心部の端部を磁極片側に延
出形成して成ることを特徴とする有極電磁石。
(1) A permanent magnet, two magnetic pole pieces sandwiching the permanent magnet, and an iron core portion around which a coil is wound to form a magnetic circuit with the magnetic pole piece, and between both ends of the two magnetic pole pieces. This is a four-gap bridge type magnetic circuit configuration in which the ends of the iron core are located at the two magnetic pole pieces and the iron core to form four main gaps. In a polarized electromagnet that moves, the magnetic pole face of one of the magnetic pole pieces constituting one or two main gaps when not energized and the magnetic pole face on the iron core side are arranged non-opposingly, and the end of the magnetic pole piece is A polarized electromagnet characterized in that it is formed by forming an iron core part side or an end part of the iron core part extending to one side of the magnetic pole.
JP62326321A 1987-12-23 1987-12-23 Polarized electromagnet Expired - Fee Related JP2613904B2 (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP62326321A JP2613904B2 (en) 1987-12-23 1987-12-23 Polarized electromagnet
DE3852624T DE3852624T2 (en) 1987-12-23 1988-10-10 Polarized electromagnet.
EP88116765A EP0321664B1 (en) 1987-12-23 1988-10-10 A polarized electromagnet
US07/267,219 US4855701A (en) 1987-12-23 1988-11-03 Polarized electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62326321A JP2613904B2 (en) 1987-12-23 1987-12-23 Polarized electromagnet

Publications (2)

Publication Number Publication Date
JPH01168011A true JPH01168011A (en) 1989-07-03
JP2613904B2 JP2613904B2 (en) 1997-05-28

Family

ID=18186462

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62326321A Expired - Fee Related JP2613904B2 (en) 1987-12-23 1987-12-23 Polarized electromagnet

Country Status (1)

Country Link
JP (1) JP2613904B2 (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1137032A2 (en) * 2000-03-15 2001-09-26 Tyco Electronics AMP GmbH Magnetic switch
EP1746615A2 (en) * 2005-07-20 2007-01-24 Eja Limited Safety switch
JP2007059460A (en) * 2005-08-22 2007-03-08 Fuji Electric Fa Components & Systems Co Ltd Polarized electromagnet
JP2007207777A (en) * 2006-01-30 2007-08-16 Mitsubishi Electric Corp Polarized electromagnet
WO2011125142A1 (en) * 2010-04-01 2011-10-13 富士電機機器制御株式会社 Polar electromagnet and electromagnetic contact

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58212106A (en) * 1982-01-29 1983-12-09 Matsushita Electric Works Ltd Polarized electromagnet device
JPS6010706A (en) * 1983-06-30 1985-01-19 Matsushita Electric Works Ltd Electromagnet device having three stable positions
JPS6159313U (en) * 1984-09-25 1986-04-21

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58212106A (en) * 1982-01-29 1983-12-09 Matsushita Electric Works Ltd Polarized electromagnet device
JPS6010706A (en) * 1983-06-30 1985-01-19 Matsushita Electric Works Ltd Electromagnet device having three stable positions
JPS6159313U (en) * 1984-09-25 1986-04-21

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1137032A2 (en) * 2000-03-15 2001-09-26 Tyco Electronics AMP GmbH Magnetic switch
EP1137032A3 (en) * 2000-03-15 2003-07-16 Tyco Electronics AMP GmbH Magnetic switch
EP1746615A2 (en) * 2005-07-20 2007-01-24 Eja Limited Safety switch
EP1746615A3 (en) * 2005-07-20 2008-03-26 Eja Limited Safety switch
JP2007059460A (en) * 2005-08-22 2007-03-08 Fuji Electric Fa Components & Systems Co Ltd Polarized electromagnet
JP2007207777A (en) * 2006-01-30 2007-08-16 Mitsubishi Electric Corp Polarized electromagnet
WO2011125142A1 (en) * 2010-04-01 2011-10-13 富士電機機器制御株式会社 Polar electromagnet and electromagnetic contact

Also Published As

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