JPH07335106A - Polarized electromagnet - Google Patents

Polarized electromagnet

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Publication number
JPH07335106A
JPH07335106A JP12286094A JP12286094A JPH07335106A JP H07335106 A JPH07335106 A JP H07335106A JP 12286094 A JP12286094 A JP 12286094A JP 12286094 A JP12286094 A JP 12286094A JP H07335106 A JPH07335106 A JP H07335106A
Authority
JP
Japan
Prior art keywords
permanent magnet
flat plate
armature
magnetic pole
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
JP12286094A
Other languages
Japanese (ja)
Other versions
JP2888756B2 (en
Inventor
Mitsuki Nagamoto
光樹 永本
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.)
Individual
Original Assignee
Individual
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Filing date
Publication date
Application filed by Individual filed Critical Individual
Priority to JP6122860A priority Critical patent/JP2888756B2/en
Publication of JPH07335106A publication Critical patent/JPH07335106A/en
Application granted granted Critical
Publication of JP2888756B2 publication Critical patent/JP2888756B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To make use of a conical permanent magnet with a complex shape and high cost unnecessary by fixing a pair of plate-shaped yokes with a space between the tips of both erected parts of an almost U-shaped iron core, bridging a rectangular permanent magnet between them, and moving an armature thereon. CONSTITUTION:A coil 3 is wound on a horizontal part 2a of an almost U-shaped iron core 23 comprising the horizontal part 2, and erected parts 2, 2c on both sides of the horizontal part 2a. A pair of plate-shaped yokes 4, 5 are fixed to the same height between tips (magnetic poles) of the standing parts 2b, 2c with a constant space, and a rectangular permanent magnet 6 is bridged between the yokes 4, 5. An armature 7 with a projection 7a is set on the upper surface of the permanent magnet 6, and moves right and left by using the projection 7a as a fulcrum to bring into contact with the left tip (magnetic pole) 2d or the right tip (magnetic pole) 2e. Positioning or position adjusting of the permanent magnet 6 to the armature 7 is made unnecessary and a polar electromagnet 1 whose assembly is simple can be provided.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は有極電磁石の改良に関す
る。
FIELD OF THE INVENTION The present invention relates to improvements in polarized electromagnets.

【0002】[0002]

【従来の技術】図6は従来の有極電磁石の断面図であ
り、図6(a)に従来のラッチング型有極電磁石、図6
(b)にシングルステイブル型有極電磁石を示す。
2. Description of the Related Art FIG. 6 is a sectional view of a conventional polarized electromagnet, and FIG. 6 (a) shows a conventional latching type polarized electromagnet.
(B) shows a single-stable polar electromagnet.

【0003】従来の有極電磁石100は、略コの字型の
鉄芯101にコイル102を巻いて組立てたコイルブロ
ック103と、鉄芯101の磁極101aおよび磁極1
01b間にレーザ溶接等で固着した山型永久磁石104
と、山型永久磁石104の頂点位置Cに接した突条10
5aを揺動支点として左右に揺動する接極子105とか
らなる。
A conventional polar electromagnet 100 includes a coil block 103 assembled by winding a coil 102 around an approximately U-shaped iron core 101, and a magnetic pole 101a and a magnetic pole 1 of the iron core 101.
Mountain-shaped permanent magnet 104 fixed between 01b by laser welding or the like
And the protrusion 10 in contact with the vertex position C of the mountain-shaped permanent magnet 104.
The armature 105 swings to the left and right with the swinging fulcrum 5a as a fulcrum.

【0004】山型永久磁石104を、例えば長手方向の
両端がS極に磁化し、更に、図6(a)のように山型の
頂点位置CをN極に磁化した場合にはラッチング型有極
電磁石が構成され、図6(b)のように山型の頂点位置
Cから所定の距離Lに離れた位置をN極に磁化した場合
にはシングルステイブル型有極電磁石が構成される。
For example, when the mountain-shaped permanent magnet 104 is magnetized to have S poles at both ends in the longitudinal direction and the mountain-shaped apex position C is magnetized to N pole as shown in FIG. A polar electromagnet is configured, and when a position separated from the peak-shaped position C of the mountain shape by a predetermined distance L is magnetized to the N pole as shown in FIG. 6B, a single-stable polarized electromagnet is configured.

【0005】接極子105は、突条105aを揺動支点
として左右に揺動し、コイルブロック103に予め決め
られた極性の電源電圧が印加された場合にのみ一方の磁
極(例えば、磁極101a)から他方の磁極(例えば、
磁極101b)へ接続が切替えられる。
The armature 105 swings to the left and right with the ridge 105a as a swing fulcrum, and one magnetic pole (for example, the magnetic pole 101a) is applied only when a power source voltage having a predetermined polarity is applied to the coil block 103. To the other magnetic pole (for example,
The connection is switched to the magnetic pole 101b).

【0006】[0006]

【発明が解決しようとする課題】従来の有極電磁石10
0は、永久磁石に山型永久磁石104を用いて、山型永
久磁石104の頂点に接した接極子105の突条105
aを中心として揺動するよう構成されているため、山型
永久磁石104の寸法に高精度が要求されるとともに、
形状が複雑となりコストアップを招く。
A conventional polar electromagnet 10
0 is a protrusion 105 of the armature 105 that is in contact with the apex of the mountain-shaped permanent magnet 104 by using the mountain-shaped permanent magnet 104 as the permanent magnet.
Since it is configured to oscillate about a, the dimensional accuracy of the mountain-shaped permanent magnet 104 is required to be high, and
The shape is complicated and the cost is increased.

【0007】また、山型永久磁石104と接極子105
との位置関係を適切に保つため、山型永久磁石104を
鉄芯101の対向する磁極101a及び101b間にレ
ーザ溶接等で固定することが要求され、組立が煩雑にな
る。
The mountain-shaped permanent magnet 104 and the armature 105 are also provided.
In order to maintain an appropriate positional relationship with, the mountain-shaped permanent magnet 104 is required to be fixed between the facing magnetic poles 101a and 101b of the iron core 101 by laser welding or the like, which makes the assembly complicated.

【0008】更に、山型永久磁石104のN極の磁化位
置をラッチング型とシングルステイブル型で別にしなけ
ればならず、また磁化した山型永久磁石104は目視チ
ェックでラッチング型なのかシングルステイブル型かの
区別ができないため、磁化作業や管理が煩わしい。
Further, the magnetizing position of the N pole of the mountain-shaped permanent magnet 104 must be different for the latching type and the single-stable type, and the magnetized mountain-shaped permanent magnet 104 is a latching type or a single-stable type by visual check. Since it cannot be distinguished, magnetizing work and management are troublesome.

【0009】そこで、本発明の目的は、複雑な形状をし
た高価格の山型永久磁石を用いずに単純な構成にし、永
久磁石と接極子との位置合せや調整が不要で、且つ、組
立が簡単な有極電磁石を提供することにある。また、ラ
ッチング型とシングルステイブル型とで永久磁石を共用
可能とすることにある。
Therefore, an object of the present invention is to make a simple structure without using an expensive mountain-shaped permanent magnet having a complicated shape, and to align and adjust the permanent magnet and the armature, and to assemble them. Is to provide a simple polarized electromagnet. Another object is to allow the latching type and the single stable type to share a permanent magnet.

【0010】[0010]

【課題を解決するための手段】上記目的を達成するべく
本発明の有極電磁石は、水平部とこの水平部の左右の立
上がり部とからなる略コ字状の鉄芯と、水平部に巻かれ
たコイルと、左右の立上がり部の各先端部間に一定の間
隔をあけ同一高さに固着された一対の平板状継鉄と、こ
れらの平板状継鉄間に掛け渡され上下方向に磁極を有す
る矩形状永久磁石と、この矩形状永久磁石の上面に突条
を当接しこの突条を揺動支点として左右に揺動し左又は
右の立上がり部の先端部に接触する接極子とから構成す
る。
In order to achieve the above object, a polarized electromagnet of the present invention has a substantially U-shaped iron core consisting of a horizontal portion and right and left rising portions of the horizontal portion, and a wound around the horizontal portion. The wound coil, a pair of flat plate yokes fixed at the same height with a fixed gap between each tip of the left and right rising parts, and a magnetic pole in the up-and-down direction that is spanned between these flat plate yokes. And a rectangular permanent magnet having an armature that abuts a ridge on the upper surface of the rectangular permanent magnet and swings left and right with this ridge as a swing fulcrum and contacts the tip of the left or right rising portion. Constitute.

【0011】また、前記一対の平板状継鉄を、鉄芯の左
右の立上がり部の各先端部に圧入により固着する。
Further, the pair of flat plate yokes are fixed to the respective left and right rising portions of the iron core by press fitting.

【0012】更に、鉄芯の各先端部間の中心線に対して
互いに左右対称形の一対の平板状継鉄と、互いに左右非
対称形の一対の平板状継鉄とを選択することで、矩形状
永久磁石の配設位置を設定可能にする。
Further, by selecting a pair of flat plate yokes symmetrical to each other with respect to the center line between the tip portions of the iron core and a pair of flat plate yokes asymmetrical to each other, The position of the permanent magnet can be set.

【0013】[0013]

【作用】一対の平板状継鉄間に矩形状永久磁石を掛け渡
す構成なので、単純な構成になる。また、永久磁石が矩
形状の単純な形状であるため、永久磁石と接極子との位
置合せや調整が不要である。更に、平板状継鉄を左右一
対に分離し、それぞれ鉄芯の左右の立上がり部の各先端
部に固着することで、平板状継鉄は各先端部に変形せず
に固着される。
[Function] Since the rectangular permanent magnet is laid between the pair of flat yokes, the structure is simple. Further, since the permanent magnet has a simple rectangular shape, it is not necessary to align or adjust the permanent magnet and the armature. Further, the flat plate yoke is separated into a pair of left and right parts and fixed to the respective tip parts of the left and right rising parts of the iron core, whereby the plate yoke is fixed to the respective tip parts without being deformed.

【0014】一対の平板状継鉄を、鉄芯の左右の立上が
り部の各先端部に圧入により固着することで、平板状継
鉄と鉄芯との間の磁気効率を損なうことなく磁気回路を
構成する。
A pair of flat plate yokes are press-fitted to the respective leading end portions of the right and left rising portions of the iron core, so that a magnetic circuit can be formed without impairing the magnetic efficiency between the flat plate yoke and the iron core. Constitute.

【0015】互いに左右対称形の平板状継鉄と、互いに
左右非対称形の平板状継鉄とを選択することで、矩形状
永久磁石の配設位置を設定することにより、一対の平板
状継鉄以外の部材を共用して、ラッチング型有極電磁石
とシングルステイブル型有極電磁石とを、構成できる。
A pair of flat plate yokes can be set by setting the arrangement positions of the rectangular permanent magnets by selecting flat plate yokes that are symmetrical to each other and flat plate yokes that are asymmetric to each other. A latching type polarized electromagnet and a single-stable type polarized electromagnet can be configured by sharing members other than the above.

【0016】[0016]

【実施例】本発明の実施例を添付図面に基づいて以下に
説明する。なお、図面は符号の向きに見るものとする。
先ず、図1〜図3に基づき第1実施例を説明する。図1
は本発明に係る有極電磁石の組立断面図であり、有極電
磁石1はラッチング型(双安定型)有極電磁石を構成す
る。
Embodiments of the present invention will be described below with reference to the accompanying drawings. The drawings should be viewed in the direction of the reference numerals.
First, a first embodiment will be described with reference to FIGS. Figure 1
FIG. 3 is an assembled sectional view of a polarized electromagnet according to the present invention, in which the polarized electromagnet 1 constitutes a latching type (bistable type) polarized electromagnet.

【0017】有極電磁石1は、水平部2aとこの水平部
2aの左右の立上がり部2b,2cとからなる略コ字状
の鉄芯2と、水平部2aに巻かれたコイル3と、左右の
立上がり部2b,2cの各先端部(磁極)2d,2e間
に一定の間隔をあけ同一高さに固着された左右一対の平
板状継鉄4,5と、これらの平板状継鉄4,5間に掛け
渡された矩形状永久磁石6と、この矩形状永久磁石6上
面に突条7aを当接しこの突条7aを揺動支点として左
右に揺動し左又は右の先端部(磁極)2d,2eに接触
する接極子7とからなる。
The polar electromagnet 1 has a substantially U-shaped iron core 2 composed of a horizontal portion 2a and left and right rising portions 2b and 2c of the horizontal portion 2a, a coil 3 wound around the horizontal portion 2a, and left and right sides. And a pair of left and right flat plate-like yokes 4 and 5 fixed at the same height with a fixed interval between the respective tip end portions (magnetic poles) 2d and 2e of the rising portions 2b and 2c of the flat plate-like yoke 4, 5, the rectangular permanent magnet 6 is bridged, and the ridge 7a is brought into contact with the upper surface of the rectangular permanent magnet 6 and oscillates left and right with the ridge 7a as a swing fulcrum to move the left or right tip (magnetic pole). ) 2d, 2e.

【0018】そして、樹脂製のコイル枠8,8で両側が
概ね覆われた鉄芯2と、この鉄芯2に巻かれたコイル3
とからなる構成体はコイルブロック9を構成する。コイ
ルブロック9は、電源端子(図示せず)に予め極性が決
定された電源電圧を印加することにより、コイル3に流
れる電流方向に対応(右手親指の法則)した磁極2d,
2eの極性(N極、S極)が設定され、一方、コイル3
の巻数とコイル3に流れる電流値の積(アンペアター
ン、起磁力)に比例し、磁気回路の抵抗(磁気抵抗)に
反比例した磁束を発生するものである。
Then, an iron core 2 whose both sides are substantially covered with resin coil frames 8 and a coil 3 wound around the iron core 2.
The structure consisting of and forms the coil block 9. The coil block 9 applies a power supply voltage whose polarity is determined in advance to a power supply terminal (not shown), so that the magnetic pole 2d corresponding to the direction of the current flowing through the coil 3 (law of the right hand thumb),
2e polarity (N pole, S pole) is set, while coil 3
The magnetic flux is proportional to the product of the number of turns of the current and the value of the current flowing through the coil 3 (ampere turn, magnetomotive force), and is inversely proportional to the resistance of the magnetic circuit (magnetic resistance).

【0019】一対の平板状継鉄4,5は、鉄芯2の各先
端部(磁極)2d,2e間の中心線Xに対して両側の磁
気抵抗が等しくなるように互いに左右対称形に形成され
ている。これらの平板状継鉄4,5の上面には、凹部4
a,5aが形成されている。また、これらの平板状継鉄
4,5は、嵌合孔4b,5bを立上がり部2b,2cの
各先端部2d,2eに圧入することにより、鉄芯2に固
着される。ここで、各コイル枠8,8の幅広の上端面8
a,8aは同一高さに形成されており、一対の平板状継
鉄4,5は、その下面を上端面8a,8aに当接するこ
とにより、同一高さに設定される。
The pair of flat plate yokes 4 and 5 are formed symmetrically with each other so that the magnetic resistances on both sides are equal to the center line X between the tip portions (magnetic poles) 2d and 2e of the iron core 2. Has been done. The upper surface of these flat yokes 4 and 5 has a recess 4
a and 5a are formed. The flat plate yokes 4 and 5 are fixed to the iron core 2 by press-fitting the fitting holes 4b and 5b into the tip portions 2d and 2e of the rising portions 2b and 2c. Here, the wide upper end surface 8 of each coil frame 8 is
a and 8a are formed at the same height, and the pair of flat plate yokes 4 and 5 are set to the same height by abutting their lower surfaces on the upper end surfaces 8a and 8a.

【0020】矩形状永久磁石6は、凹部4a,5a内に
配設されるように凹部4a,5aの形状並びに寸法に合
せて形成され、更に、凹部4a,5aの底面と接する下
面側がS極、上面側がN極となるように磁化されてい
る。接極子7は、中心線X位置で突条7aを揺動支点と
して左右に揺動するように配設されている。
The rectangular permanent magnet 6 is formed in conformity with the shapes and dimensions of the recesses 4a, 5a so as to be arranged in the recesses 4a, 5a, and further, the lower surface side in contact with the bottom surfaces of the recesses 4a, 5a has an S pole. , Is magnetized so that the upper surface side becomes the N pole. The armature 7 is disposed so as to swing to the left and right at the center line X position with the ridge 7a as a swing fulcrum.

【0021】このように、有極電磁石1は、中心線Xを
垂直方向に下ろした断面を中心にして左右対称の構成で
あり、ラッチング動作が可能となる。
As described above, the polar electromagnet 1 has a bilaterally symmetrical structure about the cross section obtained by vertically lowering the center line X, and enables the latching operation.

【0022】次に、有極電磁石1の組立手順を図2に基
づき説明する。図2は本発明に係る有極電磁石の組立手
順の説明図である。先ず、鉄芯2にコイル3を巻いてコ
イルブロック9を構成する。次に、嵌合孔4b,5bを
左右の立上がり部2b,2cに圧入し、各平板状継鉄
4,5の下面を上端面8a,8aに当接する。これによ
り、各平板状継鉄4,5は、各先端部(磁極)2d,2
e間に一定の間隔をあけて同一高さに固着される。
Next, the procedure for assembling the polar electromagnet 1 will be described with reference to FIG. FIG. 2 is an explanatory view of the procedure for assembling the polarized electromagnet according to the present invention. First, the coil 3 is wound around the iron core 2 to form the coil block 9. Next, the fitting holes 4b and 5b are press-fitted into the left and right rising portions 2b and 2c, and the lower surfaces of the flat plate yokes 4 and 5 are brought into contact with the upper end surfaces 8a and 8a. As a result, the flat yokes 4 and 5 are connected to the tip portions (magnetic poles) 2d and 2
It is fixed at the same height with a certain space between e.

【0023】その後、各平板状継鉄4,5の凹部4a,
5a内に矩形状永久磁石6を配設する。最後に、この矩
形状永久磁石6上に接極子7を配設して、組立を完了す
る。このように、有極電磁石1を一方向から組立ること
が可能である。
Thereafter, the recesses 4a of the flat yokes 4 and 5 are
A rectangular permanent magnet 6 is arranged in 5a. Finally, the armature 7 is arranged on the rectangular permanent magnet 6 to complete the assembly. Thus, the polar electromagnet 1 can be assembled from one direction.

【0024】次に、上記構成の有極電磁石1(ラッチン
グ型有極電磁石)の動作を図3に基づき説明する。図3
(a)〜(d)は有極電磁石の動作説明図である。図3
(a)はコイルブロック9に電源電圧が印加されていな
い無励磁の安定状態を示し、接極子7は端部7b,7c
が矩形状永久磁石6の磁化状態によって共にN極とな
り、一方、例えば磁極2dはS極、磁極2eはN極の状
態にあるため、接極子7は磁極2d側に接触した状態と
なっている。この状態では、磁極2d→左の平板状継鉄
4→矩形状永久磁石6→接極子7→磁極2dのループで
磁気回路が形成され、磁束Φ1が矢印の向きに発生す
る。
Next, the operation of the polarized electromagnet 1 (latching type polarized electromagnet) having the above-mentioned structure will be described with reference to FIG. Figure 3
(A)-(d) is operation | movement explanatory drawing of a polar electromagnet. Figure 3
(A) shows a stable state of non-excitation in which no power supply voltage is applied to the coil block 9, and the armature 7 has ends 7b and 7c.
Are both N poles depending on the magnetization state of the rectangular permanent magnet 6, while the magnetic pole 2d is an S pole and the magnetic pole 2e is an N pole, so that the armature 7 is in contact with the magnetic pole 2d side. . In this state, a magnetic circuit is formed by the loop of the magnetic pole 2d, the left plate yoke 4, the rectangular permanent magnet 6, the armature 7 and the magnetic pole 2d, and the magnetic flux Φ1 is generated in the direction of the arrow.

【0025】無励磁状態から、図3(b)のようにコイ
ルブロック9に電源電圧を印加した励磁直後、コイルブ
ロック9で構成される電磁石は、磁極2dがS極からN
極に変化し、磁極2eがN極からS極に変化するため、
接極子7と磁極2dには反発力が作用し、接極子7と磁
極2eには吸引力が作用する。この状態では、図3
(a)の磁束Φ1に加え、電源電圧の印加に伴う鉄芯2
→左の平板状継鉄4→矩形状永久磁石6→接極子7→磁
極2e→鉄芯2のループで磁気回路が形成され、磁束Φ
2が発生する。
Immediately after excitation from the non-excited state when a power supply voltage is applied to the coil block 9 as shown in FIG. 3B, the electromagnet constituted by the coil block 9 has a magnetic pole 2d from an S pole to an N pole.
The magnetic pole 2e changes from the N pole to the S pole,
Repulsive force acts on the armature 7 and the magnetic pole 2d, and attractive force acts on the armature 7 and the magnetic pole 2e. In this state,
In addition to the magnetic flux Φ1 in (a), the iron core 2 accompanying the application of the power supply voltage
→ Left plate yoke 4 → Rectangular permanent magnet 6 → Armature 7 → Magnetic pole 2e → Magnetic circuit is formed by loop of iron core 2 and magnetic flux Φ
2 occurs.

【0026】図3(c)は図3(b)の状態から接極子
7が磁極2d側から離れて磁極2e側に接触した反転状
態を示す。この状態では、矩形状永久磁石6により、磁
極2e→右の平板状継鉄5→矩形状永久磁石6→接極子
7→磁極2eのループで磁気回路が形成されて磁束Φ3
が発生するとともに、電磁石により、鉄芯2→左の平板
状継鉄4→矩形状永久磁石6→接極子7→磁極2e→鉄
芯2のループで磁気回路が形成されて磁束Φ1が発生し
ている。
FIG. 3C shows an inverted state in which the armature 7 separates from the magnetic pole 2d side and contacts the magnetic pole 2e side from the state of FIG. 3B. In this state, the rectangular permanent magnet 6 forms a magnetic circuit in the loop of the magnetic pole 2e → the right plate yoke 5 → the rectangular permanent magnet 6 → the armature 7 → the magnetic pole 2e, and the magnetic flux Φ3.
And a magnetic circuit is formed by the loop of iron core 2 → left plate yoke 4 → rectangular permanent magnet 6 → armature 7 → magnetic pole 2e → iron core 2 by the electromagnet, and magnetic flux Φ1 is generated. ing.

【0027】この状態から、電源電圧を除くと図3
(d)の状態に移行して接極子7が磁極2eに接触した
安定状態を保つ。この状態では、矩形状永久磁石6によ
り、磁極2e→右の平板状継鉄5→矩形状永久磁石6→
接極子7→磁極2eのループで磁気回路が形成されて磁
束Φ3が発生している。
From this state, when the power supply voltage is removed, FIG.
The state moves to the state of (d), and the armature 7 contacts the magnetic pole 2e and maintains a stable state. In this state, by the rectangular permanent magnet 6, the magnetic pole 2e → the right plate yoke 5 → the rectangular permanent magnet 6 →
A magnetic circuit is formed by the loop of the armature 7 → the magnetic pole 2e, and the magnetic flux Φ3 is generated.

【0028】なお、この状態から接極子7が磁極2dに
接触する状態に移行させる場合には、電源電圧の極性を
反対にしてコイルブロック9に印加することで達成でき
る。
Incidentally, when the armature 7 is brought into contact with the magnetic pole 2d from this state, the polarity of the power supply voltage can be reversed and applied to the coil block 9.

【0029】次に、図4及び図5に基づき第2実施例を
説明する。なお、上記図1〜図3に示す第1実施例と同
構成については同一符号を付し、その説明を省略する。
図4は本発明に係る有極電磁石の組立断面図であり、有
極電磁石11は垂直方向に下ろした中心線Xに対して左
右非対称の構成にすることで、シングルステイブル型
(単安定型)有極電磁石を構成する。有極電磁石11は
鉄芯2と、コイル3と、一対の平板状継鉄14,15
と、矩形状永久磁石6と、接極子7とからなる。
Next, a second embodiment will be described with reference to FIGS. 4 and 5. The same components as those in the first embodiment shown in FIGS. 1 to 3 are designated by the same reference numerals and the description thereof will be omitted.
FIG. 4 is an assembled cross-sectional view of the polarized electromagnet according to the present invention, in which the polarized electromagnet 11 is asymmetrical with respect to the center line X vertically lowered to form a single stable type (monostable type). It constitutes a polarized electromagnet. The polarized electromagnet 11 includes an iron core 2, a coil 3, and a pair of flat plate yokes 14 and 15
And a rectangular permanent magnet 6 and an armature 7.

【0030】一対の平板状継鉄14,15は、鉄芯2の
各先端部(磁極)2d,2e間の中心線Xに対して両側
の磁気抵抗が異なるように左右非対称の形状(左の平板
状継鉄14が右の平板状継鉄15よりも長い形状)に形
成されている。これらの平板状継鉄14,15の上面に
は、凹部14a,15aが形成されている。なお、14
b,15bは立上がり部2b,2cに圧入する嵌合孔で
ある。
The pair of flat plate yokes 14 and 15 are left-right asymmetrical so that the magnetic resistance on both sides is different with respect to the center line X between the tip portions (magnetic poles) 2d and 2e of the iron core 2 (left side). The flat plate yoke 14 is formed in a shape longer than the right flat plate yoke 15). Recesses 14a and 15a are formed on the upper surfaces of these flat yokes 14 and 15, respectively. In addition, 14
Reference numerals b and 15b are fitting holes press-fitted into the rising portions 2b and 2c.

【0031】矩形状永久磁石6は、凹部14a,15a
内に配設されるように凹部14a,15aの形状並びに
寸法に合せて形成されている。そして、矩形状永久磁石
6は、磁極2d側(この図で左側)に偏った位置にあ
る。このため、コイルブロック9が無励磁状態におい
て、矩形状永久磁石6の磁力によって形成される磁気回
路は、常に磁極2d側に偏っている。接極子7は、中心
線X位置で突条7aを揺動支点として左右に揺動するよ
うに配設されている。
The rectangular permanent magnet 6 has concave portions 14a, 15a.
It is formed in accordance with the shapes and dimensions of the recesses 14a and 15a so as to be disposed inside. The rectangular permanent magnet 6 is located at a position biased to the magnetic pole 2d side (left side in this figure). Therefore, when the coil block 9 is in the non-excited state, the magnetic circuit formed by the magnetic force of the rectangular permanent magnet 6 is always biased to the magnetic pole 2d side. The armature 7 is disposed so as to swing to the left and right at the center line X position with the ridge 7a as a swing fulcrum.

【0032】このように、有極電磁石11は、中心線X
から偏った一方の位置(この図で左側位置)に矩形状永
久磁石6が配設されたことにより、コイルブロック9の
無励磁状態において、接極子7が磁極2dに接触する単
安定状態となる。
As described above, the polar electromagnet 11 has the center line X
Since the rectangular permanent magnet 6 is arranged at one position deviated from (left side position in this figure), the armature 7 is in a monostable state in which the armature 7 contacts the magnetic pole 2d in the non-excited state of the coil block 9. .

【0033】次に、上記構成の有極電磁石11(シング
ルステイブル型有極電磁石)の動作を図5に基づき説明
する。図5(a)〜(c)は有極電磁石の動作説明図で
ある。図5(a)はコイルブロック9に電源電圧が印加
されていない無励磁の安定状態を示し、接極子7は端部
7b,7cが矩形状永久磁石6の磁化状態によって共に
N極となり、一方、磁極2dは前述した構成から常にS
極、磁極2eはN極の状態にあるため、接極子7は磁極
2d側に接触した安定状態となっている。この状態で
は、磁極2d→左の平板状継鉄14→矩形状永久磁石6
→接極子7→磁極2dのループで磁気回路が形成され、
磁束Φ11が矢印の向きに発生する。
Next, the operation of the polarized electromagnet 11 (single-stable type polarized electromagnet) having the above-mentioned configuration will be described with reference to FIG. 5A to 5C are operation explanatory views of the polarized electromagnet. FIG. 5A shows a non-excited stable state in which the power source voltage is not applied to the coil block 9. The armature 7 has both ends 7b and 7c which are N poles depending on the magnetization state of the rectangular permanent magnet 6, and , The magnetic pole 2d is always S due to the above-mentioned configuration.
Since the pole and the magnetic pole 2e are in the N pole state, the armature 7 is in a stable state in contact with the magnetic pole 2d side. In this state, the magnetic pole 2d → the left plate yoke 14 → the rectangular permanent magnet 6
→ armature 7 → magnetic circuit is formed by loop of magnetic pole 2d,
A magnetic flux Φ11 is generated in the direction of the arrow.

【0034】無励磁状態から、図5(b)のようにコイ
ルブロック9に予め極性が決定された電源電圧を印加し
た励磁直後、コイルブロック9で構成される電磁石は、
磁極2dがS極からN極に変化し、磁極2eがN極から
S極に変化するため、接極子7と磁極2dには反発力が
作用し、接極子7と磁極2eには吸引力が作用する。こ
の状態では、図3(a)の磁束Φ11に加え、電源電圧
の印加に伴う鉄芯2→左の平板状継鉄14→矩形状永久
磁石6→接極子7→磁極2e→鉄芯2のループで磁気回
路が形成され、磁束Φ12が発生する。
Immediately after excitation from a non-excited state in which a power supply voltage having a predetermined polarity is applied to the coil block 9 as shown in FIG. 5B, the electromagnet constituted by the coil block 9 is
Since the magnetic pole 2d changes from the S pole to the N pole and the magnetic pole 2e changes from the N pole to the S pole, a repulsive force acts on the armature 7 and the magnetic pole 2d, and an attractive force acts on the armature 7 and the magnetic pole 2e. To work. In this state, in addition to the magnetic flux Φ11 of FIG. 3A, the iron core 2 according to the application of the power supply voltage → the left plate yoke 14 → the rectangular permanent magnet 6 → the armature 7 → the magnetic pole 2e → the iron core 2 A magnetic circuit is formed by the loop, and a magnetic flux Φ12 is generated.

【0035】図5(c)は、図5(b)の状態から接極
子7が磁極2d側から離れて磁極2e側に接触した反転
状態を示す。この状態では、矩形状永久磁石6により、
磁極2e→右の平板状継鉄15→矩形状永久磁石6→接
極子7→磁極2eのループで磁気回路が形成されて磁束
Φ13が発生するとともに、電磁石により、鉄芯2→左
の平板状継鉄14→矩形状永久磁石6→接極子7→磁極
2e→鉄芯2のループで磁気回路が形成されて磁束Φ1
4が発生する。
FIG. 5C shows an inverted state in which the armature 7 separates from the magnetic pole 2d side and contacts the magnetic pole 2e side from the state of FIG. 5B. In this state, the rectangular permanent magnet 6
The magnetic circuit is formed by the loop of the magnetic pole 2e → the right plate yoke 15 → the rectangular permanent magnet 6 → the armature 7 → the magnetic pole 2e, and the magnetic flux Φ13 is generated. The electromagnet causes the iron core 2 → the left flat plate. The magnetic circuit is formed by the loop of the yoke 14 → the rectangular permanent magnet 6 → the armature 7 → the magnetic pole 2e → the iron core 2 and the magnetic flux Φ1.
4 occurs.

【0036】この状態から電源電圧を除くと、平板状継
鉄6の磁極2e側の磁気抵抗が磁極2d側より大きく、
また、矩形状永久磁石6が磁極2d側に偏って配置され
ているため、矩形状永久磁石6の磁力による磁束が磁束
Φ13よりも大きくなり、接極子7は磁極2d側に接触
して単安定状態を保つ。
When the power supply voltage is removed from this state, the magnetic resistance of the flat yoke 6 on the magnetic pole 2e side is larger than that on the magnetic pole 2d side.
Further, since the rectangular permanent magnets 6 are arranged biased to the magnetic pole 2d side, the magnetic flux due to the magnetic force of the rectangular permanent magnets 6 becomes larger than the magnetic flux Φ13, and the armature 7 contacts the magnetic pole 2d side and is monostable. Keep the state.

【0037】以上の説明から明らかなように、鉄芯2の
各先端部2d,2e間の中心線Xに対して互いに左右対
称形である平板状継鉄4,5と、左右非対称形である平
板状継鉄14,15とを選択することで、矩形状永久磁
石6の配設位置を設定することにより、一対の平板状継
鉄4,5,14,15以外の部材(矩形状永久磁石6を
含む)を共用して、第1実施例の有極電磁石1(ラッチ
ング型有極電磁石)と、第2実施例の有極電磁石11
(シングルステイブル型有極電磁石)とを、極めて簡単
に構成できる。
As is apparent from the above description, the flat plate yokes 4 and 5 are symmetrical to each other with respect to the center line X between the tip portions 2d and 2e of the iron core 2 and the asymmetrical type. By selecting the flat plate yokes 14 and 15 to set the arrangement position of the rectangular permanent magnets 6, members other than the pair of flat plate yokes 4, 5, 14 and 15 (rectangular permanent magnets). 6) in common, and the polar electromagnet 1 (latching type polar electromagnet) of the first embodiment and the polar electromagnet 11 of the second embodiment.
(Single-stable polar electromagnet) can be configured very easily.

【0038】[0038]

【発明の効果】本発明は上述のとおり構成されているの
で、次に記載する効果を奏する。請求項1の有極電磁石
は、鉄芯の左右の立上がり部の各先端部間に、一定の間
隔をあけて同一高さに固着された一対の平板状継鉄と、
これらの平板状継鉄間に掛け渡され上下方向に磁極を有
する矩形状永久磁石と、この矩形状永久磁石の上面に突
条を当接し、この突条を揺動支点として左右に揺動し、
立上がり部の先端部に接触する接極子とからなることに
より、一対の平板状継鉄間に単純な形状の矩形状永久磁
石を掛け渡すことができるので、従来のように複雑な形
状で高価格の山型永久磁石を用いる必要がなく、コスト
低減になる。
Since the present invention is configured as described above, it has the following effects. The polarized electromagnet according to claim 1 has a pair of flat plate yokes fixed at the same height with a constant interval between the respective tip portions of the left and right rising portions of the iron core,
A rectangular permanent magnet, which has a magnetic pole in the up-down direction, is hung between these flat yokes, and a ridge is brought into contact with the upper surface of the rectangular permanent magnet. ,
Since it consists of an armature that contacts the tip of the rising part, a rectangular permanent magnet with a simple shape can be hung between a pair of flat plate yokes. Since it is not necessary to use the mountain-shaped permanent magnet, the cost can be reduced.

【0039】また、永久磁石を矩形状にしたので単純な
構成にすることができ、この永久磁石と接極子との位置
合せや調整が不要である。更に、平板状継鉄を左右一対
に分離し、それぞれ鉄芯の左右の立上がり部の各先端部
に固着したので、単一の平板状継鉄を左右の立上がり部
の各先端部間に圧入した場合に比べて、無理なく固着で
きるので、平板状継鉄の変形を防止できる。
Further, since the permanent magnet has a rectangular shape, the permanent magnet can have a simple structure, and it is not necessary to align or adjust the permanent magnet and the armature. Furthermore, since the flat plate yokes are separated into a pair of left and right parts and fixed to the respective leading end parts of the left and right rising parts of the iron core, a single flat plate yoke is press-fitted between the respective leading end parts of the left and right rising parts. As compared with the case, the plate-like yoke can be prevented from being deformed because it can be firmly fixed.

【0040】請求項2の有極電磁石は、一対の平板状継
鉄を、鉄芯の左右の立上がり部の各先端部に圧入により
固着したので、平板状継鉄と鉄芯との間の磁気効率を損
なうことがなく、また、レーザ溶接等で固定する必要が
ないので組立が簡単である。
In the polarized electromagnet according to the second aspect of the present invention, the pair of flat plate yokes are press-fitted to the respective leading end portions of the right and left rising portions of the iron core, so that the magnetism between the flat plate yoke and the iron core is increased. Assembling is easy because there is no loss in efficiency and there is no need to fix it by laser welding or the like.

【0041】請求項3の有極電磁石は、鉄芯の各先端部
間の中心線に対して互いに左右対称形の一対の平板状継
鉄と、互いに左右非対称形の一対の平板状継鉄とを選択
することで、矩形状永久磁石の配設位置を設定すること
により、一対の平板状継鉄以外の部材(矩形状永久磁石
を含む)を共用して、ラッチング型有極電磁石とシング
ルステイブル型有極電磁石とを、極めて簡単に構成でき
る。
According to a third aspect of the polarized electromagnet, a pair of plate-like yokes symmetrical to each other with respect to the center line between the tip portions of the iron core and a pair of plate-like yokes symmetrical to each other are provided. By selecting the arrangement position of the rectangular permanent magnets by selecting, the members (including the rectangular permanent magnets) other than the pair of flat plate yokes are shared, and the latching type polarized electromagnet and the single stable Type electromagnet can be constructed very easily.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明に係る有極電磁石(第1実施例)の組立
断面図
FIG. 1 is an assembled sectional view of a polarized electromagnet (first embodiment) according to the present invention.

【図2】本発明に係る有極電磁石(第1実施例)の組立
手順の説明図
FIG. 2 is an explanatory view of an assembling procedure of the polarized electromagnet (first embodiment) according to the present invention.

【図3】本発明に係る有極電磁石(第1実施例)の動作
説明図
FIG. 3 is an operation explanatory diagram of a polarized electromagnet (first embodiment) according to the present invention.

【図4】本発明に係る有極電磁石(第2実施例)の組立
断面図
FIG. 4 is an assembled cross-sectional view of a polarized electromagnet (second embodiment) according to the present invention.

【図5】本発明に係る有極電磁石(第2実施例)の動作
説明図
FIG. 5 is an operation explanatory view of a polarized electromagnet (second embodiment) according to the present invention.

【図6】従来の有極電磁石の断面図FIG. 6 is a sectional view of a conventional polarized electromagnet.

【符号の説明】[Explanation of symbols]

1,11…有極電磁石、2…鉄芯、2a…水平部、2b
…左の立上り部、2c…右の立上り部、2d,2e…先
端部(磁極)、3…コイル、4,14…左の平板状継
鉄、4a,14a…凹部、4b,14b…嵌合孔、5,
15…右の平板状継鉄、5a,15a…凹部、5b,1
5b…嵌合孔、6…矩形状永久磁石、7…接極子、7a
…突条、7b,7c…端部、8…コイル枠、8a…上端
面、9…コイルイルブロック。
1, 11 ... Polarized electromagnet, 2 ... Iron core, 2a ... Horizontal part, 2b
... Left rising part, 2c ... Right rising part, 2d, 2e ... Tip part (magnetic pole), 3 ... Coil, 4, 14 ... Left flat plate yoke 4a, 14a ... Recessed part, 4b, 14b ... Fitting Holes, 5,
15 ... Right flat plate yoke 5a, 15a ... Recessed portion, 5b, 1
5b ... Fitting hole, 6 ... Rectangular permanent magnet, 7 ... Armature, 7a
... ridges, 7b, 7c ... end portions, 8 ... coil frame, 8a ... upper end surface, 9 ... coil il block.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 水平部とこの水平部の左右の立上がり部
とからなる略コ字状の鉄芯と、前記水平部に巻かれたコ
イルと、前記左右の立上がり部の各先端部間に一定の間
隔をあけ同一高さに固着された一対の平板状継鉄と、こ
れらの平板状継鉄間に掛け渡され上下方向に磁極を有す
る矩形状永久磁石と、この矩形状永久磁石の上面に突条
を当接しこの突条を揺動支点として左右に揺動し左又は
右の立上がり部の先端部に接触する接極子とからなる有
極電磁石。
1. A substantially U-shaped iron core composed of a horizontal portion and left and right rising portions of the horizontal portion, a coil wound around the horizontal portion, and a constant distance between the respective tip portions of the left and right rising portions. A pair of flat plate yokes fixed at the same height with a space between them, a rectangular permanent magnet having magnetic poles in the up-and-down direction that are hung between these flat plate yokes, and on the upper surface of this rectangular permanent magnet. A polarized electromagnet consisting of an armature that abuts a ridge and swings left and right with the ridge as a swing fulcrum and contacts the tip of the left or right rising portion.
【請求項2】 前記一対の平板状継鉄は、前記左右の立
上がり部の各先端部に圧入により固着されたことを特徴
とする請求項1記載の有極電磁石。
2. The polarized electromagnet according to claim 1, wherein the pair of flat plate yokes are fixed to each tip of the left and right rising portions by press fitting.
【請求項3】 前記一対の平板状継鉄は、前記鉄芯の各
先端部間の中心線に対して互いに左右対称形の平板状継
鉄と、互いに左右非対称形の平板状継鉄とを選択するこ
とで、前記矩形状永久磁石の配設位置を設定可能である
ことを特徴とした請求項1又は請求項2記載の有極電磁
石。
3. The pair of flat plate yokes include a flat plate yoke which is bilaterally symmetrical to each other with respect to a center line between the respective tip portions of the iron core, and a flat plate yoke which is bilaterally asymmetrical to each other. The polar electromagnet according to claim 1 or 2, wherein the arrangement position of the rectangular permanent magnet can be set by selecting the position.
JP6122860A 1994-06-03 1994-06-03 Polarized electromagnet Expired - Fee Related JP2888756B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6122860A JP2888756B2 (en) 1994-06-03 1994-06-03 Polarized electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6122860A JP2888756B2 (en) 1994-06-03 1994-06-03 Polarized electromagnet

Publications (2)

Publication Number Publication Date
JPH07335106A true JPH07335106A (en) 1995-12-22
JP2888756B2 JP2888756B2 (en) 1999-05-10

Family

ID=14846431

Family Applications (1)

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Country Link
JP (1) JP2888756B2 (en)

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5557255U (en) * 1978-10-13 1980-04-18
JPS6212233U (en) * 1985-07-08 1987-01-24
JPS63236235A (en) * 1987-03-24 1988-10-03 オムロン株式会社 Electromagnetic relay
JPH02104547U (en) * 1989-02-06 1990-08-20
JPH04363830A (en) * 1991-03-30 1992-12-16 Anritsu Corp Electromagnetic relay
JPH05174691A (en) * 1991-12-26 1993-07-13 Fujitsu Ltd Seesaw balance type polarized relay

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5557255U (en) * 1978-10-13 1980-04-18
JPS6212233U (en) * 1985-07-08 1987-01-24
JPS63236235A (en) * 1987-03-24 1988-10-03 オムロン株式会社 Electromagnetic relay
JPH02104547U (en) * 1989-02-06 1990-08-20
JPH04363830A (en) * 1991-03-30 1992-12-16 Anritsu Corp Electromagnetic relay
JPH05174691A (en) * 1991-12-26 1993-07-13 Fujitsu Ltd Seesaw balance type polarized relay

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