JPH07320622A - Polar electromagnet - Google Patents

Polar electromagnet

Info

Publication number
JPH07320622A
JPH07320622A JP11108494A JP11108494A JPH07320622A JP H07320622 A JPH07320622 A JP H07320622A JP 11108494 A JP11108494 A JP 11108494A JP 11108494 A JP11108494 A JP 11108494A JP H07320622 A JPH07320622 A JP H07320622A
Authority
JP
Japan
Prior art keywords
permanent magnet
electromagnet
yoke
shaped
magnetic poles
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
JP11108494A
Other languages
Japanese (ja)
Other versions
JP2598612B2 (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
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 Individual filed Critical Individual
Priority to JP11108494A priority Critical patent/JP2598612B2/en
Publication of JPH07320622A publication Critical patent/JPH07320622A/en
Application granted granted Critical
Publication of JP2598612B2 publication Critical patent/JP2598612B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Electromagnets (AREA)

Abstract

PURPOSE:To provide a polar electromagnet which has simple enough structure to be assembled and has excellent economical properties and productivity by storing a rectangular permanent magnet symmetrically changeably in T-shaped recessed part of a flat plate-like yoke formed between mutually facing poles of a coil block. CONSTITUTION:A coil 2A is wound on a U-shaped iron core 2B to compose a coil block 2. A flat plate-like yoke 4 which composes a magnetic bypass circuit is inserted and fixed between magnetic poles 3A, 3B at both ends of the electromagnet. A permanent magnet 5 having different polarity mutually in thickness directions is set in a recessed part 4A formed in the yoke 4. A contactor 6 to be brought into contact with the permanent magnet 5 at the mountain-like projected part 6C formed in the lower face is put on the permanent magnet 5. The contactor 6 is rotated on the mountain-like projected part 6C as a fulcrum due to the function of the electromagnet in order to make the magnetic poles 6A, 6B touch or be parted mutually. Regarding the polar electromagnet 1, the recessed part 4A is made to be a T-shape and moreover the permanent magnet 5 is made to be rectangular and thus the magnet is stored symmetrically on the center line of the magnetic poles or stored asymmetrically when the magnet is set in the recessed part 4A.

Description

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

【0001】[0001]

【産業上の利用分野】この発明は構成が単純な有極電磁
石に係り、特に永久磁石の配置を変えるだけで、ラッチ
ング型有極電磁石、またはシングルステイブル型有極電
磁石が構成できる有極電磁石に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a polar electromagnet having a simple structure, and more particularly to a polar electromagnet which can be used as a latching type polar electromagnet or a single stable type polar electromagnet by simply changing the arrangement of permanent magnets. .

【0002】[0002]

【従来の技術】図6は従来の有極電磁石の一実施例断面
図であり、(a)図に従来のラッチング型有極電磁石、
(b)図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 an example of a conventional polarized electromagnet, and FIG. 6 (a) shows a conventional latching type polarized electromagnet,
(B) shows a single-stable polarized electromagnet.

【0003】従来の有極電磁石11は、略コの字型の鉄
芯12Bにコイル12Aを巻いて組立てたコイルブロッ
ク12と、鉄芯12Bの磁極13Aおよび磁極13B間
にレーザ溶接等で固定した山型永久磁石14と、山型永
久磁石14の頂点に接した支点15Aを中心として回転
運動する接極子15とから構成される。
A conventional polar electromagnet 11 is fixed to the coil block 12 assembled by winding a coil 12A around an approximately U-shaped iron core 12B and the magnetic poles 13A and 13B of the iron core 12B by laser welding or the like. It is composed of a mountain-shaped permanent magnet 14 and an armature 15 which rotates about a fulcrum 15A in contact with the apex of the mountain-shaped permanent magnet 14.

【0004】山型永久磁石14を、例えば長手方向の両
端がS極、(a)図のように山型の頂点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、
(b)図のように山型の頂点Cから所定の距離xの位置
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 14 is magnetized to have S poles at both ends in the longitudinal direction and the peak C of the mountain shape is magnetized to N pole as shown in (a), a latching type polarized electromagnet is constructed.
(B) As shown in the figure, when the position of a predetermined distance x from the peak C of the mountain shape is magnetized to the N pole, a single-stable polarized electromagnet is constructed.

【0005】接極子15は、支点15Aを中心にシーソ
運動し、コイルブロック12に予め決められた極性の電
源が印加された場合にのみ一方の磁極(例えば、磁極1
3A)から他方の磁極(例えば、磁極13B)へ接続が
切替えられる。
The armature 15 makes a seesaw motion about the fulcrum 15A, and only when one of the magnetic poles (for example, the magnetic pole 1) is applied to the coil block 12 when a power source having a predetermined polarity is applied.
The connection is switched from 3A) to the other magnetic pole (for example, magnetic pole 13B).

【0006】(a)図のラッチング型有極電磁石の場
合、中心線Cを対称軸にして磁極13A側および磁極1
3B側の磁気回路が対称(磁気抵抗が等しい)に形成さ
れているとともに、山型永久磁石14も中心線CがN
極、両端がS極に磁化されているため、無励磁状態の山
型永久磁石14による磁化作用は、中心線Cを対称軸に
して磁極13A側および磁極13B側に等しく作用す
る。
In the case of the latching type polarized electromagnet shown in FIG. 1A, the center line C is the axis of symmetry and the magnetic pole 13A side and the magnetic pole 1 are located.
The magnetic circuit on the 3B side is formed symmetrically (the magnetic resistance is equal), and the mountain-shaped permanent magnet 14 has a center line C of N.
Since the poles and both ends are magnetized to the S pole, the magnetizing action of the mountain-shaped permanent magnet 14 in the non-excited state acts equally on the magnetic pole 13A side and the magnetic pole 13B side with the center line C as the axis of symmetry.

【0007】無励磁状態で何等かの作用により、例えば
接極子15が磁極13A側に接触した状態から、コイル
ブロック2に所定極性の電源が印加されると電磁石が形
成され、電磁石の作用で接極子15が磁極13A側から
離れ、磁極13B側に接触した状態となる。
When a power source of a predetermined polarity is applied to the coil block 2 from a state in which the armature 15 is in contact with the magnetic pole 13A by some action in a non-excited state, an electromagnet is formed, and the action of the electromagnet causes a contact. The pole piece 15 separates from the magnetic pole 13A side and comes into contact with the magnetic pole 13B side.

【0008】この状態から電源を除いても接極子15と
磁極13Bとの接触が保たれ、所定極性と逆の電源が印
加されると接極子15が反転して磁極13Aと接触した
状態となる。このように、無励磁状態において、接極子
15と磁極13A、および接極子15と磁極15Bがそ
れぞれ接触する2つの安定状態を形成する(a)図のラ
ッチング型有極電磁石が構成される。
Even if the power source is removed from this state, the contact between the armature 15 and the magnetic pole 13B is maintained, and when a power source having a polarity opposite to the predetermined polarity is applied, the armature 15 is inverted and comes into contact with the magnetic pole 13A. . In this way, the latching-type polar electromagnet of FIG. (A) is formed which forms two stable states in which the armature 15 and the magnetic pole 13A are in contact with each other and the armature 15 and the magnetic pole 15B are in contact with each other in the non-excited state.

【0009】一方、(b)図のシングルステイブル型有
極電磁石の場合、中心線Cを対称軸にして磁極13A側
および磁極13B側の磁気回路が対称(磁気抵抗が等し
い)に形成されるが、山型永久磁石14は山型の頂点C
から所定の距離xの位置がN極に磁化されるため、無励
磁状態の山型永久磁石14による磁化作用は、中心線C
を対称軸にして磁極13A側に偏るため、磁極13A側
に磁極13B側よりも強い磁力が作用し、無励磁状態で
は常に接極子15が磁極13Aに接触するシングルステ
イブル型有極電磁石が構成される。
On the other hand, in the case of the single-stable polar electromagnet shown in FIG. 1B, the magnetic circuits on the magnetic pole 13A side and the magnetic pole 13B side are formed symmetrically (having the same magnetic resistance) with the center line C as the axis of symmetry. , The mountain-shaped permanent magnet 14 has a mountain-shaped apex C
Since a position of a predetermined distance x from the above is magnetized to the N pole, the magnetizing action by the mountain-shaped permanent magnet 14 in the non-excited state is the center line C.
Since it is biased to the magnetic pole 13A side with the symmetry axis as the axis of symmetry, a stronger magnetic force acts on the magnetic pole 13A side than on the magnetic pole 13B side, and a single-stable polarized electromagnet in which the armature 15 always contacts the magnetic pole 13A in a non-excited state is configured. It

【0010】この状態からコイルブロック2に所定極性
の電源が印加されると電磁石が形成され、電磁石の作用
で接極子15が磁極13A側から離れ、磁極13B側に
接触した状態となる。また、接極子15が磁極13B側
に接触した状態から電源を除くと、山型永久磁石14の
磁化作用により、接極子15は反転して接極子15が磁
極13Aに接触する初期の状態に復旧する。
When a power source having a predetermined polarity is applied to the coil block 2 from this state, an electromagnet is formed, and the armature 15 is separated from the magnetic pole 13A side by the action of the electromagnet and comes into contact with the magnetic pole 13B side. Further, when the power source is removed from the state where the armature 15 is in contact with the magnetic pole 13B side, the armature 15 is inverted by the magnetizing action of the mountain-shaped permanent magnet 14, and the armature 15 is restored to the initial state in which the armature 15 is in contact with the magnetic pole 13A. To do.

【0011】このように、従来の有極電磁石11は、山
型永久磁石14を鉄芯12Bの磁極13Aおよび磁極1
3B間にレーザ溶接等で固定し、山型永久磁石14の長
手方向両端をS極に磁化し、中央または中心から偏らせ
た位置をN極に磁化することにより、それぞれラッチン
グ型有極電磁石、またはシングルステイブル型有極電磁
石が構成される。
As described above, in the conventional polarized electromagnet 11, the mountain-shaped permanent magnet 14 is connected to the magnetic pole 13A of the iron core 12B and the magnetic pole 1.
3B is fixed by laser welding or the like, both longitudinal ends of the mountain-shaped permanent magnet 14 are magnetized to the S pole, and a position deviated from the center or the center is magnetized to the N pole. Alternatively, a single-stable polarized electromagnet is configured.

【0012】[0012]

【発明が解決しようとする課題】従来の有極電磁石11
は、永久磁石に山型永久磁石14を用いて山型永久磁石
14の頂点に接した接極子15の支点15Aを中心とし
て回転運動するよう構成されているため、山型永久磁石
14の寸法に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課題がある。
[Problems to be Solved by the Invention] Conventional polarized electromagnet 11
Is configured to rotate about the fulcrum 15A of the armature 15 that is in contact with the apex of the mountain-shaped permanent magnet 14 by using the mountain-shaped permanent magnet 14 as the permanent magnet. There is a problem that precision is required and the shape becomes complicated, resulting in cost increase.

【0013】また、山型永久磁石14と接極子15の位
置関係を適切に保つため、山型永久磁石14を鉄芯12
Bの対向する磁極13Aおよび磁極13B間にレーザ溶
接等で固定することが要求され、組立てが煩雑になる課
題がある。
In order to keep the positional relationship between the mountain-shaped permanent magnet 14 and the armature 15 appropriate, the mountain-shaped permanent magnet 14 is attached to the iron core 12.
It is required to fix the magnetic poles 13A and 13B opposed to each other by laser welding or the like, and there is a problem that assembly becomes complicated.

【0014】さらに、山型永久磁石14のN極の磁化位
置をラッチングタイプとシングルステイブルタイプで別
にしなければならず、また磁化した山型永久磁石14は
目視チェックでラッチングタイプなのかシングルステイ
ブルタイプかの区別ができないため、磁化作業や管理が
煩わしい課題がある。
Further, the magnetizing position of the N pole of the mountain-shaped permanent magnet 14 must be separated into a latching type and a single-stable type, and whether the magnetized mountain-shaped permanent magnet 14 is a latching type by visual check or a single-stable type. Since it cannot be distinguished, there is a problem that magnetizing work and management are troublesome.

【0015】この発明はこのような課題を解決するため
なされたもので、その目的は構成が単純で組立やすく、
同じ部品を用いてラッチング型有極電磁石、およびシン
グルステイブル型有極電磁石の双方が構成できる有極電
磁石を提供することにある。
The present invention has been made to solve the above problems, and its purpose is to have a simple structure and easy assembly.
An object of the present invention is to provide a polarized electromagnet that can be used for both a latching type polarized electromagnet and a single stable type polarized electromagnet using the same parts.

【0016】[0016]

【課題を解決するための手段】前記課題を解決するため
この発明に係る有極電磁石は、平板状継鉄にT字型凹部
を設けるとともに、永久磁石を矩形状永久磁石で形成
し、矩形状永久磁石をT字型凹部に配置する際、永久磁
石を対向する磁極間の中心線に対称、または非対称に配
置し、収納したことを特徴とする。
In order to solve the above-mentioned problems, a polarized electromagnet according to the present invention is provided with a T-shaped recess in a flat yoke and the permanent magnet is formed of a rectangular permanent magnet. When the permanent magnets are arranged in the T-shaped recesses, the permanent magnets are arranged symmetrically or asymmetrically with respect to the center line between the opposing magnetic poles and housed.

【0017】また、この発明に係る有極電磁石は、矩形
状永久磁石を対向する磁極間の中心線に対称となるよう
T字型凹部に配置して収納し、ラッチング型有極電磁石
を構成したことを特徴とする。
In the polarized electromagnet according to the present invention, the rectangular permanent magnet is arranged and housed in the T-shaped concave portion so as to be symmetrical with respect to the center line between the opposing magnetic poles to form a latching type polarized electromagnet. It is characterized by

【0018】さらに、この発明に係る有極電磁石は、矩
形状永久磁石を前記対向する磁極間の中心線に非対称と
なるようT字型凹部に配置して収納し、シングルステイ
ブル型有極電磁石を構成したことを特徴とする。
Further, in the polarized electromagnet according to the present invention, a rectangular permanent magnet is arranged and housed in a T-shaped recess so as to be asymmetric with respect to the center line between the opposed magnetic poles, and a single-stable polarized electromagnet is provided. It is characterized by being configured.

【0019】[0019]

【作用】この発明に係る有極電磁石は、平板状継鉄にT
字型凹部を設けるとともに、永久磁石を矩形状永久磁石
で形成し、T字型凹部に配置する矩形状永久磁石の配置
を変えることにより、永久磁石を対向する磁極間の中心
線に対称、または非対称に配置して収納することができ
るので、同じ部品を用いてラッチング型有極電磁石およ
びシングルステイブル型有極電磁石を構成することがで
きる。
The polarized electromagnet according to the present invention includes a plate yoke and a T-shaped magnet.
By providing the V-shaped concave portion, forming the permanent magnet with a rectangular permanent magnet, and changing the arrangement of the rectangular permanent magnets arranged in the T-shaped concave portion, the permanent magnet is symmetrical with respect to the center line between the opposing magnetic poles, or Since they can be asymmetrically arranged and housed, the latching-type polar electromagnet and the single-stable polar electromagnet can be configured using the same parts.

【0020】[0020]

【実施例】図1〜図5にこの発明に係る有極電磁石の構
成を示す。図1にこの発明に係る有極電磁石の全体構成
図、図2にこの発明に係る有極電磁石の平板状継鉄の形
状および矩形状永久磁石の配置図、図3にこの発明に係
る有極電磁石の組立図、図4にこの発明に係る構成を適
用したラッチング型有極電磁石の断面図、図5にこの発
明に係る構成を適用したシングルステイブル型有極電磁
石の断面図を示す。
1 to 5 show the construction of a polarized electromagnet according to the present invention. FIG. 1 is an overall configuration diagram of a polarized electromagnet according to the present invention, FIG. 2 is a plan view of a flat yoke and a rectangular permanent magnet of the polarized electromagnet according to the present invention, and FIG. FIG. 4 is an assembly diagram of the electromagnet, FIG. 4 is a sectional view of a latching type polarized electromagnet to which the configuration according to the present invention is applied, and FIG. 5 is a sectional view of a single stable type polarized electromagnet to which the configuration according to the present invention is applied.

【0021】図1〜図3において、有極電磁石1は、略
コの字型の鉄芯2Bにコイル2Aを巻いたコイルブロッ
ク2と、コイルブロック2の磁極3A、3B間に挿入し
て固定し、鉄芯2Bとの間で磁気回路を形成する平板状
継鉄4と、平板状継鉄4に設けられたT字型凹部4Aに
配置した矩形状永久磁石5と、山型凸部6Cを支点とし
て回転し、端部6A、端部6Bがそれぞれ磁極3A、磁
極3Bと接触する接極子6とから構成する。
1 to 3, a polar electromagnet 1 is inserted and fixed between a coil block 2 in which a coil 2A is wound around a substantially U-shaped iron core 2B and magnetic poles 3A and 3B of the coil block 2. Then, a flat plate yoke 4 forming a magnetic circuit with the iron core 2B, a rectangular permanent magnet 5 arranged in a T-shaped concave portion 4A provided in the flat plate yoke 4, and a mountain-shaped convex portion 6C. Of the armature 6 that rotates about the fulcrum and the ends 6A and 6B contact the magnetic poles 3A and 3B, respectively.

【0022】コイルブロック2は電磁石を形成し、コイ
ル電極(+)2a、コイル電極(−)2b間に予め極性
が決定された電源を印加することにより、コイル2Aに
流れる電流の方向に対応(右手親指の法則)した磁極3
A、3Bの極性(N、S極)が設定され、一方、コイル
2Aの巻数とコイル2Aに流れる電流値の積(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。
The coil block 2 forms an electromagnet, and a power source having a predetermined polarity is applied between the coil electrode (+) 2a and the coil electrode (-) 2b to correspond to the direction of the current flowing through the coil 2A ( Right hand thumb rule) Magnetic pole 3
The polarities of A and 3B (N and S poles) are set, while the product of the number of turns of the coil 2A and the current value flowing in the coil 2A (magnetomotive force)
And a magnetic flux that is inversely proportional to the resistance of the magnetic circuit (magnetic resistance) is generated.

【0023】平板状継鉄4は、図2に示すように、略T
の字形状のT字型凹部4Aを備え、T字型凹部4Aは平
板状継鉄4の長手方向および幅方向に、それぞれ長さL
および長さWの辺(L>W)の組合せからなる略T字状
の溝を形成する。
As shown in FIG. 2, the flat yoke 4 has a substantially T-shaped shape.
It is provided with a T-shaped concave portion 4A having a V shape, and the T-shaped concave portion 4A has a length L in the longitudinal direction and the width direction of the flat yoke 4.
A substantially T-shaped groove composed of a combination of sides (L> W) having a length W is formed.

【0024】T字型凹部4Aは、コイルブロック2の磁
極3A、磁極3B間の中心線Xに対称となるよう平板状
継鉄4の長手方向の長さLを設定し、中心線Xに非対称
となるよう平板状継鉄4の長手方向の長さWを設定す
る。
The T-shaped recess 4A has a length L in the longitudinal direction of the plate yoke 4 which is symmetrical with respect to the center line X between the magnetic poles 3A and 3B of the coil block 2, and is asymmetrical with respect to the center line X. The length W in the longitudinal direction of the flat yoke 4 is set so that

【0025】また、T字型凹部4Aは、平板状継鉄4の
幅方向の図示しない中心線に対称となるよう長さLおよ
び長さWを設定する。
The length L and length W of the T-shaped recess 4A are set so as to be symmetrical with respect to the center line (not shown) in the width direction of the flat yoke 4.

【0026】このように形成されたT字型凹部4Aに、
それぞれ一辺の長さがほぼL、W(実際はL、Wより短
い)の長方形の面を有する矩形状永久磁石5を配置す
る。例えば、(b)図のように平板状継鉄4の長手方向
に矩形状永久磁石5の辺Lが対応するよう配置すると、
矩形状永久磁石5は中心線Xを対称軸として平板状継鉄
4の長手方向に対称に配置される。(b)図の組合せで
構成される有極電磁石1は、平板状継鉄4の長手方向に
対称に配置された矩形状永久磁石5の磁化作用により、
図4に示すラッチング型有極電磁石9を構成する。
In the T-shaped recess 4A thus formed,
The rectangular permanent magnets 5 having rectangular surfaces each having a side length of approximately L and W (actually shorter than L and W) are arranged. For example, if the side L of the rectangular permanent magnet 5 corresponds to the longitudinal direction of the flat yoke 4 as shown in FIG.
The rectangular permanent magnets 5 are symmetrically arranged in the longitudinal direction of the flat yoke 4 with the center line X as the axis of symmetry. (B) The polar electromagnet 1 configured by the combination of the figures is formed by the magnetizing action of the rectangular permanent magnets 5 symmetrically arranged in the longitudinal direction of the flat yoke 4.
The latching type polarized electromagnet 9 shown in FIG. 4 is configured.

【0027】また、(c)図のように平板状継鉄4の幅
方向に矩形状永久磁石5の辺Lが対応するよう配置する
と、矩形状永久磁石5は中心線Xを対称軸として平板状
継鉄4の長手方向に非対称に配置される。(c)図の組
合せで構成される有極電磁石1は、平板状継鉄4の長手
方向に非対称に配置された矩形状永久磁石5の磁化作用
により、図5に示すシングルステイブル型有極電磁石1
0を構成する。
Further, when the rectangular permanent magnets 5 are arranged such that the sides L of the rectangular permanent magnets 5 correspond to the width direction of the flat yoke 4 as shown in FIG. The yoke 4 is arranged asymmetrically in the longitudinal direction. (C) The polar electromagnet 1 configured by the combination shown in the figure is a single-stable polar electromagnet shown in FIG. 5 due to the magnetizing action of the rectangular permanent magnets 5 asymmetrically arranged in the longitudinal direction of the flat yoke 4. 1
Configure 0.

【0028】このように、平板状継鉄4に矩形状永久磁
石5を収納するT字型凹部4Aを設け、矩形状永久磁石
5の配置を変更するだけで、同じ部品点数の同じ部品を
用いてラッチング型有極電磁石9およびシングルステイ
ブル型有極電磁石10を構成する。
In this way, the flat yoke 4 is provided with the T-shaped recess 4A for accommodating the rectangular permanent magnet 5, and the arrangement of the rectangular permanent magnet 5 is simply changed to use the same parts having the same number of parts. To constitute a latching type polarized electromagnet 9 and a single-stable type polarized electromagnet 10.

【0029】矩形状永久磁石5は、平板状継鉄4に設け
られたT字型凹部4A内に収容可能なよう、T字型凹部
4Aの形状に合せて形成(L*Wの長方形)し、T字型
凹部4Aの底面と接する面側をS極、反対面側がN極と
なるよう磁化する。
The rectangular permanent magnet 5 is formed according to the shape of the T-shaped recess 4A (L * W rectangle) so that it can be housed in the T-shaped recess 4A provided in the flat yoke 4. , The surface contacting the bottom surface of the T-shaped recess 4A is magnetized so as to have an S pole and the opposite surface has an N pole.

【0030】また、T字型凹部4Aを設けた平板状継鉄
4と矩形状永久磁石5を用いることにより、平板状継鉄
4の固定はコイルブロック2の磁極3A、磁極3B間に
圧入で固定でき、矩形状永久磁石5の精度も緩やかにで
きるので、部品形状および有極電磁石1の構成が単純と
なる。
Further, by using the flat plate yoke 4 provided with the T-shaped recess 4A and the rectangular permanent magnet 5, the flat plate yoke 4 can be fixed between the magnetic poles 3A and 3B of the coil block 2 by press fitting. Since it can be fixed and the precision of the rectangular permanent magnet 5 can be loosened, the component shape and the configuration of the polar electromagnet 1 are simplified.

【0031】接極子6は、図4〜図5に示すように中心
線X上で矩形状永久磁石5と接触する部分に、傾斜部を
有する山型凸部6Cを設け、この山型凸部6Cを支点と
して前記接極子が回転運動して端部6A、端部6Bがそ
れぞれ磁極3A、磁極3Bに接触するよう構成するの
で、安定した回転運動が得られる。
As shown in FIGS. 4 to 5, the armature 6 is provided with a mountain-shaped convex portion 6C having an inclined portion at a portion in contact with the rectangular permanent magnet 5 on the center line X, and the mountain-shaped convex portion is formed. Since the armature rotates about 6C as a fulcrum and the ends 6A and 6B come into contact with the magnetic poles 3A and 3B, respectively, a stable rotary motion can be obtained.

【0032】有極電磁石1の組立ては、図3に示すよう
に、コイルブロック2に平板状継鉄4を圧入し、平板状
継鉄4のT字型凹部4A内に矩形状永久磁石5を挿入し
た後、矩形状永久磁石5上に接極子6を配置することに
より、一方向の組立てが可能となる。
To assemble the polar electromagnet 1, as shown in FIG. 3, the plate yoke 4 is press-fitted into the coil block 2 and the rectangular permanent magnet 5 is inserted into the T-shaped recess 4A of the plate yoke 4. After the insertion, by disposing the armature 6 on the rectangular permanent magnet 5, it is possible to assemble in one direction.

【0033】また、有極電磁石1を組立てた状態で、矩
形状永久磁石5の配置を目視チェックすることにより、
ラッチング型有極電磁石9か、シングルステイブル型有
極電磁石10かの確認ができる。
Further, by visually checking the arrangement of the rectangular permanent magnets 5 with the polarized electromagnet 1 assembled,
It can be confirmed whether it is the latching type polarized electromagnet 9 or the single-stable type polarized electromagnet 10.

【0034】[0034]

【発明の効果】以上説明したように、この発明に係る有
極電磁石は、平板状継鉄にT字型凹部を設けるととも
に、永久磁石を矩形状永久磁石で形成し、T字型凹部に
配置する矩形状永久磁石の配置を変更し、永久磁石を対
向する磁極間の中心線に対称、または非対称に配置して
収納することにより、同じ部品を用いてラッチング型有
極電磁石およびシングルステイブル型有極電磁石を容易
に構成することができる。
As described above, in the polar electromagnet according to the present invention, the flat yoke is provided with the T-shaped concave portion, and the permanent magnet is formed by the rectangular permanent magnet and is arranged in the T-shaped concave portion. By changing the arrangement of the rectangular permanent magnets and arranging the permanent magnets symmetrically or asymmetrically with respect to the center line between the opposing magnetic poles and storing them, the same parts are used for latching type polar electromagnet and single stable type magnet. The polar electromagnet can be easily constructed.

【0035】よって、構成が単純で組立やすく、経済性
および生産性に優れた有極電磁石を提供することができ
る。
Therefore, it is possible to provide a polarized electromagnet having a simple structure, easy assembly, and excellent economical efficiency and productivity.

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

【図1】この発明に係る有極電磁石の全体構成図FIG. 1 is an overall configuration diagram of a polarized electromagnet according to the present invention.

【図2】この発明に係る有極電磁石の平板状継鉄の形状
および矩形状永久磁石の配置図
FIG. 2 is a layout view of a flat yoke and a rectangular permanent magnet of a polarized electromagnet according to the present invention.

【図3】この発明に係る有極電磁石の組立図FIG. 3 is an assembly diagram of a polarized electromagnet according to the present invention.

【図4】この発明に係る構成を適用したラッチング型有
極電磁石の断面図
FIG. 4 is a sectional view of a latching-type polarized electromagnet to which the configuration according to the present invention is applied.

【図5】この発明に係る構成を適用したシングルステイ
ブル型有極電磁石の断面図
FIG. 5 is a sectional view of a single-stable polar electromagnet to which the configuration according to the present invention is applied.

【図6】従来の有極電磁石の一実施例断面図FIG. 6 is a sectional view of an example of a conventional polarized electromagnet.

【符号の説明】[Explanation of symbols]

1…有極電磁石、2…コイルイルブロック、2A…コイ
ル、2B…鉄芯、2a,2b…コイル電極、3A,3B
…磁極、4…平板状継鉄、4A…T字型凹部、5…矩形
状永久磁石、6…接極子、6A,6B…端部、6C…山
型凸部、9…ラッチング型有極電磁石、10…シングル
ステイブル型有極電磁石。
1 ... Polarized electromagnet, 2 ... Coil il block, 2A ... Coil, 2B ... Iron core, 2a, 2b ... Coil electrode, 3A, 3B
... magnetic poles, 4 ... plate-like yokes, 4A ... T-shaped concave portions, 5 ... rectangular permanent magnets, 6 ... armatures, 6A, 6B ... end portions, 6C ... mountain-shaped convex portions, 9 ... latching type polarized electromagnets 10 ... Single-stable polarized electromagnet.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 コの字型の鉄芯にコイルが巻かれ、対向
する両端が磁極を形成するコイルブロックと、前記対向
する磁極間に挿入して固定し、磁気バイパス回路を形成
する平板状継鉄と、この平板状継鉄に設けられた凹部に
装着し、厚み方向に互いに異なる極性に磁化した永久磁
石と、この永久磁石に接触し、電磁石の作用により回転
運動して前記磁極に接触する接極子とを備えた有極電磁
石において、 前記平板状継鉄にT字型凹部を設けるとともに、前記永
久磁石を矩形状永久磁石で形成し、この矩形状永久磁石
を前記T字型凹部に配置する際、前記永久磁石を前記対
向する磁極間の中心線に対称、または非対称に配置し、
収納したことを特徴とする有極電磁石。
1. A coil block, in which a coil is wound around a U-shaped iron core and opposite ends of which form a magnetic pole, and a flat plate shape which is inserted and fixed between the opposite magnetic poles to form a magnetic bypass circuit. A yoke and a permanent magnet magnetized to have different polarities in the thickness direction and attached to the recess provided in the flat yoke, and contact this permanent magnet, and rotate by the action of an electromagnet to contact the magnetic pole. And a T-shaped recess in the flat yoke, the permanent magnet is formed of a rectangular permanent magnet, and the rectangular permanent magnet is formed in the T-shaped recess. When arranging, the permanent magnets are arranged symmetrically or asymmetrically with respect to the center line between the opposed magnetic poles,
A polarized electromagnet characterized by being stored.
【請求項2】 前記矩形状永久磁石を前記対向する磁極
間の中心線に対称となるよう前記T字型凹部に配置して
収納し、ラッチング型有極電磁石を構成したことを特徴
とする請求項1記載の有極電磁石。
2. The latching type polarized electromagnet is configured by arranging and storing the rectangular permanent magnet in the T-shaped recess so as to be symmetrical with respect to the center line between the opposed magnetic poles. The polarized electromagnet according to item 1.
【請求項3】 前記矩形状永久磁石を前記対向する磁極
間の中心線に非対称となるよう前記T字型凹部に配置し
て収納し、シングルステイブル型有極電磁石を構成した
ことを特徴とする請求項1記載の有極電磁石。
3. A single-stable polarized electromagnet is configured by arranging and storing the rectangular permanent magnet in the T-shaped recess so as to be asymmetric with respect to the center line between the opposed magnetic poles. The polarized electromagnet according to claim 1.
JP11108494A 1994-05-25 1994-05-25 Polarized electromagnet Expired - Lifetime JP2598612B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11108494A JP2598612B2 (en) 1994-05-25 1994-05-25 Polarized electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11108494A JP2598612B2 (en) 1994-05-25 1994-05-25 Polarized electromagnet

Publications (2)

Publication Number Publication Date
JPH07320622A true JPH07320622A (en) 1995-12-08
JP2598612B2 JP2598612B2 (en) 1997-04-09

Family

ID=14551984

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11108494A Expired - Lifetime JP2598612B2 (en) 1994-05-25 1994-05-25 Polarized electromagnet

Country Status (1)

Country Link
JP (1) JP2598612B2 (en)

Also Published As

Publication number Publication date
JP2598612B2 (en) 1997-04-09

Similar Documents

Publication Publication Date Title
JPH0442770B2 (en)
EP0778602B1 (en) Electromagnetic actuator
JP2602412B2 (en) Polarized electromagnet
JP2598613B2 (en) Polarized electromagnet
JP2598612B2 (en) Polarized electromagnet
JP2598611B2 (en) Single-stable type polarized electromagnet
JP2601997B2 (en) Single-stable type polarized electromagnet
JP2897860B2 (en) Single-stable type polarized electromagnet
JP2755363B2 (en) Rotating fulcrum type polarized electromagnet
JP2755364B2 (en) Rotating fulcrum type polarized electromagnet and rotating fulcrum type polarized relay incorporating this
JP3009708U (en) Single-stable polarized electromagnet
JP3004893U (en) Rotating fulcrum type polarized relay
JP2634768B2 (en) Single-stable type polarized electromagnet
JP2888756B2 (en) Polarized electromagnet
JP2601998B2 (en) Rotating fulcrum type polarized relay
JP3005085U (en) Rotating fulcrum type polarized relay
JP3005221U (en) Rotating fulcrum type polarized relay
JP3003916U (en) Rotating fulcrum type polarized relay
JPH07282707A (en) Polarized latching electromagnet
JPS61127105A (en) Electromagnet device
JPH0343683Y2 (en)
JP2538884B2 (en) Electromagnet device
JP2601994B2 (en) Rotating fulcrum type polarized relay
JP2861413B2 (en) Polarized electromagnet
JP2601995B2 (en) Rotating fulcrum type polarized relay

Legal Events

Date Code Title Description
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 19961127