JPH0228902A - Electromagnet device - Google Patents

Electromagnet device

Info

Publication number
JPH0228902A
JPH0228902A JP63180093A JP18009388A JPH0228902A JP H0228902 A JPH0228902 A JP H0228902A JP 63180093 A JP63180093 A JP 63180093A JP 18009388 A JP18009388 A JP 18009388A JP H0228902 A JPH0228902 A JP H0228902A
Authority
JP
Japan
Prior art keywords
permanent magnet
leg
central leg
spring load
magnetic flux
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.)
Pending
Application number
JP63180093A
Other languages
Japanese (ja)
Inventor
Shoichi Yamaguchi
彰一 山口
Kazutsugu Hayashi
和嗣 林
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 JP63180093A priority Critical patent/JPH0228902A/en
Publication of JPH0228902A publication Critical patent/JPH0228902A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To easily match an electromagnet device to a monostable operation spring load by composing an auxiliary permanent magnet for supplying a magnetic flux to a central leg in the same direction as that of the magnetic flux of a permanent magnet which flows through the central leg in a state that the magnet is moved by a spring load to attract an armature to the central and side legs as part of the central leg. CONSTITUTION:A permanent magnet 3 is energized in one direction of the moving direction of the magnet 3 directly by a spring load or through armatures 4, 5. The spring load may employ a single return spring, or may be replaced with a contact spring in case of a relay or the like. An auxiliary permanent magnet 6 is so composed at the part of a central leg 7 as to supply a magnetic flux to the leg 7 in the same direction as that of the magnetic flux of the magnet 3 to flow through the leg 7 in a state that a permanent magnet 1 is moved by a spring load to attract the armature 2 to the leg 7 and side legs 8, 9. More specifically, it is interposed between the leg 7 and a yoke piece 10 to be magnetically and mechanically coupled. The magnet 6 is so magnetized in the thicknesswise direction in the same direction as a coil axis direction.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、3相モータの開閉用の電磁接触器等に適用
される電磁石装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an electromagnet device applied to an electromagnetic contactor for opening/closing a three-phase motor.

〔従来の技術〕[Conventional technology]

第8図に従来例を示す。すなわち、この電磁石装置は、
中央脚50と一対の側脚51.52を有する略E字形の
ヨーク53と、中央脚50に巻装されたコイル54と、
中央脚50の先端側に配置されて一対の側脚51,52
の先端部にそれぞれ磁極N、  Sが向くとともに磁極
N、Sの方向に移動可能な永久磁石55と、この永久磁
石55の磁極N、Sの各々に設けられて先端部が中央脚
50と一対の側脚51,52との間に位置する一対のア
ーマチュア56と、永久磁石55の移動方向の一方向で
アーマチュア56が中央脚50および側脚51,52に
吸着される復帰位置に永久磁石55を付勢するばね負荷
(図示せず)とを備えている。
FIG. 8 shows a conventional example. That is, this electromagnetic device is
a substantially E-shaped yoke 53 having a central leg 50 and a pair of side legs 51 and 52; a coil 54 wound around the central leg 50;
A pair of side legs 51 and 52 are arranged on the distal end side of the central leg 50.
A permanent magnet 55 with magnetic poles N and S facing each other and movable in the direction of the magnetic poles N and S is provided at each of the magnetic poles N and S of this permanent magnet 55, and the tip end is paired with the central leg 50. A pair of armatures 56 are located between the center leg 50 and the side legs 51, 52, and the permanent magnet 55 is in a return position where the armature 56 is attracted to the center leg 50 and the side legs 51, 52 in one direction of the movement direction of the permanent magnet 55. and a spring load (not shown) for biasing the .

なお、ヨーク53の側脚51.52はU字形のヨーク片
により形成され、その中央に中央脚50を立設している
The side legs 51 and 52 of the yoke 53 are formed by U-shaped yoke pieces, and the central leg 50 is erected at the center thereof.

この電磁石装置は、コーク53.コイル54゜永久磁石
55.アーマチュア56の寸法をコイル軸方向の中心v
AMに対して対称にした場合、磁気吸引力は第11図に
示すようになる。図において、Qlは定格電圧を印加し
たときの磁気吸引力特性曲線、Q2は永久磁石55のみ
による磁気吸引力特性曲線、Q3はQlと逆方向に定格
電圧を印加したときの磁気吸引力特性曲線、Q4は双安
定動作用のばね負荷線である。
This electromagnetic device is made of coke 53. Coil 54° Permanent magnet 55. The dimensions of the armature 56 are the center v in the coil axial direction.
When made symmetrical with respect to AM, the magnetic attraction force becomes as shown in FIG. In the figure, Ql is a magnetic attraction force characteristic curve when the rated voltage is applied, Q2 is a magnetic attraction force characteristic curve due only to the permanent magnet 55, and Q3 is a magnetic attraction force characteristic curve when the rated voltage is applied in the opposite direction to Ql. , Q4 is the spring load line for bistable operation.

しかし、電磁接触器等の場合には双安定型ではなく、単
安定動作用の電磁石を用いるのが一般的であり、この場
合ばね負荷は第12図に示すよってQlは定格電圧を印
加したときの磁気吸引力特性曲線、Q2は永久磁石55
のみによる磁気吸引力特性曲線、Q、Lは単安定動作用
のばね負荷線である。
However, in the case of electromagnetic contactors, etc., it is common to use monostable electromagnets instead of bistable ones, and in this case, the spring load is as shown in Figure 12, and Ql is when the rated voltage is applied. Magnetic attraction characteristic curve, Q2 is permanent magnet 55
The magnetic attraction force characteristic curves, Q and L are spring loading lines for monostable operation.

従来、この種のばね負荷にマツチングできる磁気吸引力
を得るため、第9図に示すようにヨーク53の側111
1I51,52のアーマチュア56に対する対向面積を
左右非対称にしたり、第10図に示すようにアーマチュ
ア56の相互の表面積を異ならせたりして、コイル54
に対する左右ギャップの磁極面積を変える方法をとって
いた。57はレシジュアルプレートである。
Conventionally, in order to obtain a magnetic attraction force that can match this type of spring load, as shown in FIG.
By making the facing areas of the 1I51 and 52 with respect to the armature 56 asymmetrical, or by making the mutual surface areas of the armatures 56 different as shown in FIG.
The method used was to change the magnetic pole area of the left and right gaps. 57 is a casual plate.

これらの従来例は、部品の寸法を変えるだけでよく、部
品点数が増えないという利点を有する。
These conventional examples have the advantage that only the dimensions of the parts need to be changed and the number of parts does not increase.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

ところが、これらの電磁石装置は、動作側あるいは復帰
側の端部における磁気吸引力が、磁極面積を小さくした
ために非常に急峻なものとなる。
However, in these electromagnetic devices, the magnetic attraction force at the operating side or return side end becomes very steep because the magnetic pole area is made small.

そのため厚めのレシジュアルプレート57を使用する必
要があり、また厚めのレシジュアルプレート57を用い
るとトータルの磁気ギャップが大きくなり、しかもギャ
ップ対向面積が双安定動作用の第8図の電磁石はどはと
れないので、磁気ギャップの磁気抵抗が大きくなり、そ
のため磁気吸引力幅が小さくなってしまうという問題が
あった。
Therefore, it is necessary to use a thicker regular plate 57, and using a thicker regular plate 57 increases the total magnetic gap. Therefore, there is a problem in that the magnetic resistance of the magnetic gap becomes large and the width of the magnetic attraction force becomes small.

したがって、これらの電磁石装置は、単安定動作用のば
ね負荷とマツチングしにくいという欠点があった。
Therefore, these electromagnetic devices have the disadvantage that they are difficult to match with a spring load for monostable operation.

したがって、この発明の目的は、単安定動作用のばね負
荷とマツチングしやすい電磁石装置を提供することであ
る。
Therefore, it is an object of the present invention to provide an electromagnetic device that is easy to match with a spring load for monostable operation.

(課題を解決するための手段〕 この発明の電磁石装置は、ばね負荷により永久磁石が移
動してアーマチュアが中央脚および側脚に吸着された状
態で中央脚を流れる永久磁石の磁束と同方向に中央脚に
磁束を供給する補助永久磁石を中央脚の一部に構成した
ものである。
(Means for Solving the Problems) In the electromagnet device of the present invention, the permanent magnet is moved by a spring load so that the armature is attracted to the center leg and the side legs, and the armature is moved in the same direction as the magnetic flux of the permanent magnet flowing through the center leg. An auxiliary permanent magnet that supplies magnetic flux to the center leg is constructed as a part of the center leg.

〔作用〕[Effect]

この発明の構成によれば、中央脚の一部に補助永久磁石
を構成したため、励磁、無励磁の各磁気。
According to the configuration of the present invention, since the auxiliary permanent magnet is formed in a part of the center leg, each magnetism is energized and non-energized.

吸引力特性曲線が全体的にアーマチュアの復帰側にずれ
たものとなる。このため、単安定型のばね負荷とマツチ
ングしやすくなる。また励磁側での吸引力が従来例より
も下がるため磁気飽和による影響が少なくなる。
The attraction force characteristic curve as a whole shifts toward the return side of the armature. This makes it easier to match with a monostable spring load. Furthermore, since the attractive force on the excitation side is lower than in the conventional example, the influence of magnetic saturation is reduced.

〔実施例〕〔Example〕

この発明の一実施例を第1図ないし第6図に基づいて説
明する。すなわち、この電磁石装置は、ヨークlと、コ
イル2と、永久磁石3と、一対のアーマチュア4,5と
、補助永久磁石6とを有する。
An embodiment of the present invention will be described based on FIGS. 1 to 6. That is, this electromagnetic device includes a yoke l, a coil 2, a permanent magnet 3, a pair of armatures 4 and 5, and an auxiliary permanent magnet 6.

ヨーク1は、中央脚7と一対の側脚8,9を有する略E
字形に形成されている。中央脚7は棒状を実施例とし、
側脚8.9はU字形のヨーク片1゜により形成され、コ
イル軸方向の中心vA17に対して対称となるように中
央脚7をその中心線17上に立設している。そして、中
央脚7および側脚8.9の先端部が磁極部148〜14
eとなる。
The yoke 1 has a central leg 7 and a pair of side legs 8, 9.
It is formed into a letter shape. The central leg 7 has a rod shape as an example,
The side legs 8.9 are formed by U-shaped yoke pieces 1°, and the center leg 7 is erected on its center line 17 so as to be symmetrical with respect to the center vA17 in the coil axis direction. The tips of the central leg 7 and the side legs 8.9 are connected to the magnetic pole parts 148 to 14.
It becomes e.

コイル2は、中央脚7に巻装されている。コイル2はコ
イル枠11の外周に巻線12を巻回してなる。コイル枠
11の中空部13は角柱形をなし、中央脚7が貫通する
The coil 2 is wound around the central leg 7. The coil 2 is formed by winding a winding 12 around the outer periphery of a coil frame 11. The hollow part 13 of the coil frame 11 has a prismatic shape, and the central leg 7 passes through it.

永久磁石3は、中央脚7の先端側に配置されて一対の側
Ij8. 9の先端部にそれぞれ磁極N、 Sが向くと
ともに磁極N、 Sの方向(矢印)に移動可能である。
The permanent magnet 3 is arranged on the tip side of the central leg 7 and is connected to the pair of sides Ij8. The magnetic poles N and S face the tips of the magnetic poles N and S, respectively, and are movable in the direction of the magnetic poles N and S (arrows).

永久磁石3の移動方向はコイル軸方向と垂直方向である
The moving direction of the permanent magnet 3 is perpendicular to the coil axis direction.

アーマチュア4.5は、永久磁石3の各磁極N。The armature 4.5 has each magnetic pole N of the permanent magnet 3.

Sに設けられて先端部が中央脚7と一対の側脚8゜9と
の間に位置する。アーマチュア2は平板状を実施例とし
、同形状のものが永久磁石3の磁極N。
S is provided, and the tip portion is located between the central leg 7 and the pair of side legs 8.9. In this embodiment, the armature 2 has a flat plate shape, and the same shape is the magnetic pole N of the permanent magnet 3.

Sに接着剤により接着固定されている。アーマチュア4
.5の先端部が磁極部15a、15bとなる。そして、
ヨーク1の磁極部14a〜14Cとアーマチュア4.5
の磁極部15a、15bとは、図のように4個のギャッ
プG1〜G4をおいてコイル軸方向と垂直な方向に対向
している。
It is fixed to S with adhesive. Armature 4
.. The tip portions of 5 become magnetic pole portions 15a and 15b. and,
Magnetic pole parts 14a to 14C of yoke 1 and armature 4.5
The magnetic pole parts 15a and 15b face each other in a direction perpendicular to the coil axis direction with four gaps G1 to G4 in between as shown in the figure.

永久磁石3はばね負荷(図示せず)により直接またはア
ーマチュア4,5を介して永久磁石3の移動方向の一方
向(矢印A)に付勢されている。
The permanent magnet 3 is biased by a spring load (not shown) directly or via armatures 4, 5 in one direction (arrow A) in the direction of movement of the permanent magnet 3.

ばね負荷は単独の復帰ばねを用いてもよいが、リレー等
の場合接点ばねで兼用してもよい。
A single return spring may be used as the spring load, but in the case of a relay etc., a contact spring may also be used.

補助永久磁石6は、ばね負荷により永久磁石1が移動し
てアーマチュア2が中央脚7および側脚8.9に吸着さ
れた状態で中央脚7を流れる永久磁石3の磁束と同方向
に中央脚7に磁束を供給するように、中央脚7の一部に
構成されている。具体的には中央脚7とヨーク片10と
の連結部に介在され磁気的かつ機械的りこ結合されてい
る。この補助永久磁石6は薄板状を実施例とし、板厚方
向に着磁されかつコイル軸方向と同方向に磁化方向が向
けられている。
The auxiliary permanent magnet 6 moves in the same direction as the magnetic flux of the permanent magnet 3 flowing through the center leg 7 with the armature 2 being attracted to the center leg 7 and the side legs 8.9 when the permanent magnet 1 moves due to a spring load. A part of the central leg 7 is configured to supply magnetic flux to the central leg 7 . Specifically, the central leg 7 and the yoke piece 10 are interposed at a connecting portion and are magnetically and mechanically coupled. The auxiliary permanent magnet 6 has a thin plate shape, is magnetized in the thickness direction, and has its magnetization direction in the same direction as the coil axis.

なお、ヨーク1.コイル2.永久磁石3およびアーマチ
ュア4.5は、コイル軸方向の中心線17に対して対称
になっている。
In addition, yoke 1. Coil 2. The permanent magnet 3 and the armature 4.5 are symmetrical with respect to a center line 17 in the axial direction of the coil.

この電磁石の組み立ては、第2図に示すように、コイル
枠11に巻線12を巻回し、補助永久磁石6を設けたヨ
ーク1をコイル枠11に組み込む。
To assemble this electromagnet, as shown in FIG. 2, a winding 12 is wound around a coil frame 11, and a yoke 1 provided with an auxiliary permanent magnet 6 is assembled into the coil frame 11.

永久磁石3の磁極N、  Sにそれぞれアーマチュア4
.5を接着する。また永久磁石3をガイド(図示せず)
に移動可能に支持する。
Armature 4 is attached to magnetic poles N and S of permanent magnet 3, respectively.
.. Glue 5. Also guides the permanent magnet 3 (not shown)
movably supported.

つぎに動作を説明する。第3図はコイル2が励磁されて
なくばね負荷により復帰した復帰状態である。この場合
、永久磁石3の発生した磁束は主に経路φ1 (実線矢
印)を流れる。すなわち、永久磁石1の磁極N−アーマ
チュア5の磁極部15a−ギャップG1−側脚8の磁極
部14c−補助永久磁石6−中央脚7の磁極部14a−
ギャップG3−アーマチュア4の磁極部15b=永久磁
石3の磁極Sを流れる。また、補助永久磁石6より発生
した磁束は主に経路Φ3 (−点鎖線矢印)を流れる。
Next, the operation will be explained. FIG. 3 shows a return state in which the coil 2 is not energized and is returned by a spring load. In this case, the magnetic flux generated by the permanent magnet 3 mainly flows through the path φ1 (solid arrow). That is, magnetic pole N of permanent magnet 1 - magnetic pole part 15a of armature 5 - gap G1 - magnetic pole part 14c of side leg 8 - auxiliary permanent magnet 6 - magnetic pole part 14a of central leg 7 -
Flows through gap G3 - magnetic pole portion 15b of armature 4 = magnetic pole S of permanent magnet 3. Further, the magnetic flux generated by the auxiliary permanent magnet 6 mainly flows through the path Φ3 (-dotted chain arrow).

ここで、補助永久磁石6の発生する磁束は、永久磁石3
の発生する磁束と同じ方向に流れており、復帰側の吸引
力を大きくする役割を果たしている(第5図において−
の方向)。
Here, the magnetic flux generated by the auxiliary permanent magnet 6 is
The flux flows in the same direction as the magnetic flux generated by
direction).

一方、第4図はコイル2を励磁した動作状態である。こ
の場合、永久磁石3の発生した磁束は、主に経路Φ1′
 (実線矢印)を流れる。すなわち、永久磁石1の磁極
N−アーマチュア5の磁極部15’a−ギャップG2→
中央脚7の磁極部14a−補助永久磁石6−側脚9の磁
極部14b−ギャップG、→アーマチュア4の磁極部1
5b→永久磁石3の磁極Sを流れる。また、補助永久磁
石6より発生した磁束は、主に経路Φ3′ (−点鎖線
矢印)を流れる。動作状態のとき、コイル2の発生した
磁束は経路Φ2 (破線矢印)を流れるように、コイル
2を励磁しており、そのため補助永久磁石6の磁束は永
久磁石3の磁束とコイル2の発生する磁束を打ち消す方
向に働いており、動作側の吸引力は小さくなる(第5図
において−の方向)。
On the other hand, FIG. 4 shows an operating state in which the coil 2 is excited. In this case, the magnetic flux generated by the permanent magnet 3 mainly passes through the path Φ1'
(solid arrow). That is, magnetic pole N of permanent magnet 1 - magnetic pole part 15'a of armature 5 - gap G2→
Magnetic pole part 14a of central leg 7 - auxiliary permanent magnet 6 - magnetic pole part 14b of side leg 9 - gap G, → magnetic pole part 1 of armature 4
5b → flows through the magnetic pole S of the permanent magnet 3. Further, the magnetic flux generated by the auxiliary permanent magnet 6 mainly flows through the path Φ3' (-dotted chain arrow). In the operating state, the magnetic flux generated by the coil 2 excites the coil 2 so as to flow along the path Φ2 (dashed line arrow). Therefore, the magnetic flux of the auxiliary permanent magnet 6 is equal to the magnetic flux of the permanent magnet 3 and the magnetic flux generated by the coil 2. It acts in the direction of canceling the magnetic flux, and the attractive force on the operating side becomes smaller (in the - direction in Fig. 5).

第5図はアーマチュア2の吸引力特性を示し、Plは補
助永久磁石6を設置した場合の定格電圧を印加したとき
の吸引力特性曲線、P2は補助永久磁石6を設置した場
合の怒動電圧を印加したときの吸引力特性曲線、P3は
補助永久磁石6を設置した場合の開放電圧を印加したと
きの吸引力特性曲線、P4は補助永久磁石6を設置した
場合の永久磁石3のみのときの吸引力特性曲線、P5は
単安定動作用のばね負荷であり、またP6は補助永久磁
石6がないときの定格電圧を印加したときの吸引力特性
曲線、P7は永久磁石3のみのときの吸引力特性曲線で
ある。
Figure 5 shows the attractive force characteristics of the armature 2, Pl is the attractive force characteristic curve when the rated voltage is applied when the auxiliary permanent magnet 6 is installed, and P2 is the angry voltage when the auxiliary permanent magnet 6 is installed. P3 is the attractive force characteristic curve when applying the open circuit voltage when the auxiliary permanent magnet 6 is installed, P4 is the attractive force characteristic curve when only the permanent magnet 3 is installed when the auxiliary permanent magnet 6 is installed. P5 is the spring load for monostable operation, P6 is the attractive force characteristic curve when the rated voltage is applied without the auxiliary permanent magnet 6, and P7 is the attractive force characteristic curve when only the permanent magnet 3 is used. This is a suction force characteristic curve.

この実施例によれば、第6図に示すように、従来の磁極
面積を変えて単安定動作向きとする第9図および第10
図の電磁石により得られた動作側の端部の急峻な吸引力
特性曲線R2に比べて、この実施例により得られる動作
側端部の吸引力特性曲線P3の方が傾きおよび伸びがゆ
るやかで動作側端部の単安定動作用ばね負荷曲線P、よ
り吸引力が上回りにクク、従来例のようにレシジュアル
プレート57を用いて、動作側端部の磁気吸引力をカッ
トする必要がない。また磁極面積を変えなくてよいため
、左右対称部品が使える。
According to this embodiment, as shown in FIG. 6, the conventional magnetic pole area is changed to make it oriented for monostable operation, as shown in FIGS. 9 and 10.
Compared to the attractive force characteristic curve R2 at the operating end obtained by the electromagnet shown in the figure, which has a steep attraction force characteristic curve R2, the attractive force characteristic curve P3 at the operating end obtained by this example has a gentler slope and elongation. The monostable operation spring load curve P at the side end has a higher attractive force, and there is no need to use the regular plate 57 to cut off the magnetic attraction force at the operating side end, as in the conventional example. Also, since there is no need to change the magnetic pole area, symmetrical parts can be used.

また、レシジュアルプレート57が不要なために、トー
タルの磁気ギャップの対向面積を第9図および第1θ図
のように小さくする必要もないので磁気ギャップの磁気
抵抗を小さくすることができ、電磁接触器特有のばね負
荷力が急増する部分の第5図の位置T付近の磁気吸引力
の変化幅F1が大きくとれ、このため電磁接触器のよう
な片寄ったばね負荷ともマツチングしやすくなる。
Furthermore, since the regular plate 57 is not required, there is no need to reduce the total facing area of the magnetic gap as shown in FIG. 9 and FIG. The range of change F1 in the magnetic attraction force near the position T in FIG. 5 where the spring load force peculiar to the device rapidly increases can be increased, and therefore it becomes easier to match even a biased spring load such as an electromagnetic contactor.

また、補助永久磁石5をコイル枠11の中空部13に嵌
め込む構造であるので、補助永久磁石6を固定しやすい
Moreover, since the structure is such that the auxiliary permanent magnet 5 is fitted into the hollow part 13 of the coil frame 11, it is easy to fix the auxiliary permanent magnet 6.

第7図は中央脚7とヨーク片10と補助永久磁石6とを
固着する他の実施例であり、補助永久磁石6の磁極方向
の両面に接着剤18を塗布し、補助永久磁石6の吸着力
+接着剤18の接着力でヨーク片10と補助永久磁石6
とを結合している。
FIG. 7 shows another embodiment in which the central leg 7, the yoke piece 10, and the auxiliary permanent magnet 6 are fixed together. An adhesive 18 is applied to both sides of the auxiliary permanent magnet 6 in the magnetic pole direction, and the auxiliary permanent magnet 6 is attracted to the auxiliary permanent magnet 6. The yoke piece 10 and the auxiliary permanent magnet 6 are attached by the adhesive force of force + adhesive 18.
and are combined.

(発明の効果〕 この発明の電磁石装置によれば、中央脚の一部に補助永
久磁石を構成したため、励磁、無励磁の各磁気吸引力特
性曲線が全体的にアーマチュアの復帰側にずれたものと
なる。このため、単安定型のばね負荷とマツチングしや
すくなる。したがって、従来例のようにギャップの磁極
面積を小さくしたり、レシジュアルプレートを設けたり
あるいはこれを厚くしたりする必要がなく、単安定動作
用電磁石として高効率なものを得ることができる。
(Effects of the Invention) According to the electromagnetic device of the present invention, since the auxiliary permanent magnet is formed in a part of the central leg, the magnetic attraction force characteristic curves of energized and non-energized states are entirely shifted toward the return side of the armature. Therefore, it is easier to match with a monostable spring load.Therefore, there is no need to reduce the magnetic pole area of the gap, provide a regular plate, or make it thicker as in the conventional example. , a highly efficient monostable electromagnet can be obtained.

また励磁側での吸引力が従来例よりも下がるため磁気飽
和による影響が少なくなるという効果かある。
Also, since the attractive force on the excitation side is lower than in the conventional example, there is an effect that the influence of magnetic saturation is reduced.

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

第1図はこの発明の一実施例の断面図、第2図はその分
解斜視図、第3図はその無励磁状態の断面図、第4図は
その励磁状態の断面図、第5図はそのアーマチュアの磁
気吸引力およびばね負荷特性図、第6図はその動作側に
おけるアーマチュアの磁気吸引力およびばね負荷特性図
、第7図は他の実施例の補助永久磁石の取付状態の側面
図、第8図は従来例の断面図、第9図および第10図は
それぞれ別の従来例の分解斜視図、第11図は双安定型
の磁気吸引力およびばね負荷特性図、第12図は単安定
型の磁気吸引力およびばね負荷特性図である。 l・・・ヨーク、2・・・コイル、3・・・永久磁石、
4゜5・・・アーマチュア、6・・・補助永久磁石、7
・・・中央脚、8.9・・・側脚 第2図 第 図 第 因 第 図 第 図 第 手続補正書 (自発 1゜ 2゜ 3゜ 1肩牛の耘 昭和63年特 発明の名称 電磁石装置 補正をする者 事件との関係
FIG. 1 is a cross-sectional view of an embodiment of the present invention, FIG. 2 is an exploded perspective view thereof, FIG. 3 is a cross-sectional view of the non-excited state, FIG. 4 is a cross-sectional view of the excited state, and FIG. A magnetic attraction force and spring load characteristic diagram of the armature, FIG. 6 is a magnetic attraction force and spring load characteristic diagram of the armature on the operating side, and FIG. 7 is a side view of another embodiment with the auxiliary permanent magnet installed. Fig. 8 is a sectional view of a conventional example, Figs. 9 and 10 are exploded perspective views of different conventional examples, Fig. 11 is a bistable magnetic attraction force and spring load characteristic diagram, and Fig. 12 is a bistable type magnetic attraction force and spring load characteristic diagram. FIG. 3 is a diagram of stable magnetic attraction force and spring load characteristics. l...Yoke, 2...Coil, 3...Permanent magnet,
4゜5... Armature, 6... Auxiliary permanent magnet, 7
...Central leg, 8.9...Side leg Fig. 2 Fig. Cause Fig. Fig. Procedure amendment (Spontaneous 1゜2゜3゜1 Shoulder cow 1988 Name of special invention Electromagnet Relationship with the device correction case

Claims (1)

【特許請求の範囲】[Claims]  中央脚と一対の側脚を有する略E字形のヨークと、前
記中央脚に巻装されたコイルと、前記中央脚の先端側に
配置されて前記一対の側脚の先端部にそれぞれ磁極が向
くとともに前記磁極の方向に移動可能な永久磁石と、こ
の永久磁石の前記磁極の各々に設けられて先端部が前記
中央脚と前記一対の側脚との間に位置する一対のアーマ
チュアと、前記永久磁石の移動方向の一方向で前記アー
マチュアが前記中央脚および前記側脚に吸着される復帰
位置に前記永久磁石を付勢するばね負荷とを備えた電磁
石装置において、前記永久磁石の前記復帰位置で前記中
央脚を流れる前記永久磁石の磁束と同方向に前記中央脚
に磁束を供給する補助永久磁石を前記中央脚の一部に構
成したことを特徴とする電磁石装置。
a substantially E-shaped yoke having a central leg and a pair of side legs; a coil wound around the central leg; and a coil disposed on the distal end side of the central leg, with magnetic poles facing the distal ends of the pair of side legs. a permanent magnet that is movable in the direction of the magnetic poles; a pair of armatures that are provided on each of the magnetic poles of the permanent magnets and whose tips are located between the central leg and the pair of side legs; and a spring load that biases the permanent magnet to a return position in which the armature is attracted to the central leg and the side legs in one direction of the magnet movement, wherein the permanent magnet is in the return position. An electromagnetic device characterized in that an auxiliary permanent magnet that supplies magnetic flux to the central leg in the same direction as the magnetic flux of the permanent magnet flowing through the central leg is configured as a part of the central leg.
JP63180093A 1988-07-19 1988-07-19 Electromagnet device Pending JPH0228902A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63180093A JPH0228902A (en) 1988-07-19 1988-07-19 Electromagnet device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63180093A JPH0228902A (en) 1988-07-19 1988-07-19 Electromagnet device

Publications (1)

Publication Number Publication Date
JPH0228902A true JPH0228902A (en) 1990-01-31

Family

ID=16077316

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63180093A Pending JPH0228902A (en) 1988-07-19 1988-07-19 Electromagnet device

Country Status (1)

Country Link
JP (1) JPH0228902A (en)

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