JPS601814A - Solenoid with built-in permanent magnet - Google Patents

Solenoid with built-in permanent magnet

Info

Publication number
JPS601814A
JPS601814A JP58109540A JP10954083A JPS601814A JP S601814 A JPS601814 A JP S601814A JP 58109540 A JP58109540 A JP 58109540A JP 10954083 A JP10954083 A JP 10954083A JP S601814 A JPS601814 A JP S601814A
Authority
JP
Japan
Prior art keywords
permanent magnet
electromagnetic coil
fixed
yoke
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.)
Pending
Application number
JP58109540A
Other languages
Japanese (ja)
Inventor
Shigeru Shirai
滋 白井
Yoshio Yamamoto
山本 芳雄
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 Holdings Corp
Original Assignee
Matsushita Electric Industrial Co 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 Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP58109540A priority Critical patent/JPS601814A/en
Publication of JPS601814A publication Critical patent/JPS601814A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F7/00Magnets
    • H01F7/06Electromagnets; Actuators including electromagnets
    • H01F7/08Electromagnets; Actuators including electromagnets with armatures
    • H01F7/16Rectilinearly-movable armatures
    • H01F7/1607Armatures entering the winding
    • H01F7/1615Armatures or stationary parts of magnetic circuit having permanent magnet
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F7/00Magnets
    • H01F7/06Electromagnets; Actuators including electromagnets
    • H01F7/08Electromagnets; Actuators including electromagnets with armatures
    • H01F7/121Guiding or setting position of armatures, e.g. retaining armatures in their end position
    • H01F7/122Guiding or setting position of armatures, e.g. retaining armatures in their end position by permanent magnets

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Electromagnets (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は永久磁石を付設したソレノイドに係り、特に低
電力用のソレノイドに関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a solenoid equipped with a permanent magnet, and more particularly to a solenoid for low power use.

永久磁石を付設したソレノイドには、永久磁石の吸引力
で自己保持し、電磁コイルへ通電することによって永久
磁石の吸引力を低減させて可動鉄心を離反させる、いわ
ゆる自己保持型ソレノイドと、電磁コイルへの通電によ
る吸引力と永久磁石の吸引力とで吸着状態を保持する非
自己保持型ツレ・ノイドとがあるが、本発明はいずれの
ソレノイドにも適するものである。
Solenoids equipped with permanent magnets include so-called self-holding solenoids, which hold themselves by the attractive force of the permanent magnet, and when energized to the electromagnetic coil, reduce the attractive force of the permanent magnet and separate the movable iron core. There is a non-self-holding type solenoid that maintains the attracted state by the attraction force caused by energization and the attraction force of a permanent magnet, but the present invention is suitable for any type of solenoid.

従来例の構成とその問題点 自己保持型ソレノイドは吸引された位置を維持する為の
電力が不要であるため、電力消費やコイル温度上昇が問
題りなる用途に適している。特に、吸引状態を解除する
には一瞬の通電で良いから電池電源を用いる場合に有利
である。しかし、通電による起磁力は永久磁石の磁束を
打消す方向に作用するので永久磁石が減磁して吸着保持
力の低下を生じる恐れがある。特に、保持力が低い永久
磁石や、低温減磁が生じやすい永久磁石を用いた場合、
及び着磁方向の板厚が薄い永久磁石を用いると減磁を生
じる可能性が高い。このため、通電減磁を少なくする構
成として第1図に示すような従来例があった。ここで、
101はコ字型をした固定継鉄で、その底面中央に永久
磁石102が位置し、その上部には断面がT字型の補助
継鉄103が設けられている。補助継鉄103の外周で
固定継鉄101との間の空間には電磁コイル104が位
置している。固定継鉄101の脚部端面と補助継鉄10
3の上端面は同一平面に加工されていて、これら端面と
接触又は離反する板状の可動鉄心106が対応している
。この可動鉄む106は軸106によってその動きが伝
えられると共に、図示していないスプリングによって常
時離反する方向に附勢されている。第1図で(A)は吸
着保持状態を示し、永久磁石102の磁束Aによって可
動鉄心106は吸引されている。次に電磁コイル104
に通電すると補助継鉄103の底部外周と固定継鉄10
1の脚部内面との空隙107が永久磁石102の厚さよ
りも小さく設定しているので、電磁コイル104の磁束
Bと永久磁石102の磁束は前記空隙107を通ること
になる。これが第1図(B)の状態である。従って、可
動鉄心105の吸着面の磁束は激減又は方向が逆転する
から通電と同時に吸着保持力が低減し、スプリングのカ
によって同図(C)のように可動鉄心105が離反する
ものである。このように空隙107i永久磁石1o2の
磁気抵抗よりも少くすることによって、通電時に永久磁
石102の中を逆方向の磁束が通ることを防止して通電
による減磁作用を低減させるものであった。
Conventional configurations and their problems Since self-holding solenoids do not require electricity to maintain the attracted position, they are suitable for applications where power consumption and coil temperature rise are problematic. In particular, it is advantageous when using a battery power source because a momentary energization is sufficient to release the suction state. However, since the magnetomotive force caused by energization acts in a direction that cancels the magnetic flux of the permanent magnet, there is a risk that the permanent magnet will be demagnetized and the attraction and holding force will be reduced. In particular, when using permanent magnets with low coercive force or permanent magnets that are prone to low-temperature demagnetization,
Also, if a permanent magnet with a thin plate thickness in the magnetization direction is used, there is a high possibility that demagnetization will occur. For this reason, there is a conventional example as shown in FIG. 1 as a structure for reducing energization demagnetization. here,
Reference numeral 101 denotes a U-shaped fixed yoke, with a permanent magnet 102 located at the center of its bottom surface, and an auxiliary yoke 103 having a T-shaped cross section provided above. An electromagnetic coil 104 is located in the space between the fixed yoke 101 and the outer periphery of the auxiliary yoke 103. The leg end face of the fixed yoke 101 and the auxiliary yoke 10
The upper end surfaces of 3 are processed to be the same plane, and correspond to a plate-shaped movable iron core 106 that comes into contact with or separates from these end surfaces. The movement of the movable iron 106 is transmitted by the shaft 106, and the movable iron 106 is always urged in the direction of separation by a spring (not shown). In FIG. 1, (A) shows the attracting and holding state, in which the movable iron core 106 is attracted by the magnetic flux A of the permanent magnet 102. Next, the electromagnetic coil 104
When energized, the bottom outer circumference of the auxiliary yoke 103 and the fixed yoke 10
Since the air gap 107 with the inner surface of the leg 1 is set smaller than the thickness of the permanent magnet 102, the magnetic flux B of the electromagnetic coil 104 and the magnetic flux of the permanent magnet 102 pass through the air gap 107. This is the state shown in FIG. 1(B). Therefore, the magnetic flux on the attracting surface of the movable core 105 is drastically reduced or its direction is reversed, so that the attracting and holding force is reduced at the same time as the current is applied, and the movable core 105 is separated by the force of the spring as shown in FIG. In this way, by making the air gap 107i smaller than the magnetic resistance of the permanent magnet 1o2, magnetic flux in the opposite direction is prevented from passing through the permanent magnet 102 during energization, thereby reducing the demagnetization effect caused by energization.

この従来例では吸着面が固定継鉄101の両脚部端面と
補助継鉄103の中央端面と3カ所あるので、この吸着
面高さが同一平面上にあることが必要で、この高さの不
揃いや表面荒さが荒いと吸着保持力が低下する。従って
これら吸着面を組立後に研磨加工して均一な面にする必
要があり高価になっていた。
In this conventional example, there are three suction surfaces: the end surfaces of both legs of the fixed yoke 101 and the center end surface of the auxiliary yoke 103, so it is necessary that the heights of these suction surfaces be on the same plane. If the surface is rough or rough, the adsorption and holding power will decrease. Therefore, it is necessary to polish these suction surfaces after assembly to make them uniform, which increases the cost.

また第1図と同じ構成で第2図(A)のように、小さい
磁力の永久磁石102の磁束Aと電磁コイル104に通
電する微少直流電流によって生じる磁束Cによって町動
鉄藷105を吸着保持し、電磁コイル104への電流供
給を停止すると、可動鉄心105の吸着面の磁束は磁束
Aだけとなって吸着保持力が減少し、図示していない可
動鉄心105を常時離反する方向に附勢しているスプリ
ングの力によって同図(B)のように、可動鉄心105
が離反する非自己保持型ソレノイドとして使用する従来
例の場合も、吸着面が固定継鉄101の両脚部端面と補
助継鉄103の中央端面と3ケ所あるので、この吸着面
高さが同一平面上にあることが必要で、この高さの不揃
いや表面荒さが荒いと吸着保持力が低下する。したがっ
てこれら吸着面を組立後に研磨加工して均一な面にする
必要があり、高価になっていた。
In addition, with the same configuration as in Fig. 1, as shown in Fig. 2 (A), the town moving iron 105 is attracted and held by the magnetic flux A of the permanent magnet 102 with a small magnetic force and the magnetic flux C generated by the minute direct current flowing through the electromagnetic coil 104. However, when the current supply to the electromagnetic coil 104 is stopped, the magnetic flux on the attracting surface of the movable core 105 becomes only the magnetic flux A, so that the attracting and holding force decreases, and the movable core 105 (not shown) is constantly urged in the direction of separation. As shown in the same figure (B), the movable iron core 105 is
In the case of the conventional example in which the solenoid is used as a non-self-holding type solenoid that separates, there are three suction surfaces: the end surfaces of both legs of the fixed yoke 101 and the center end surface of the auxiliary yoke 103, so the height of the suction surfaces is the same plane. If the height is uneven or the surface is rough, the adsorption and holding power will decrease. Therefore, it is necessary to polish these suction surfaces after assembly to make them uniform, which increases the cost.

発明の目的 本発明は、低電力で機能すると共に、研磨加工を必要と
しない安価な永久磁石内蔵型ソレノイドを得ることを目
的とする。
OBJECTS OF THE INVENTION It is an object of the present invention to provide an inexpensive solenoid with a built-in permanent magnet that functions with low power and does not require polishing.

発明の構成 この目的を達成するために本発明は、電磁コイル外側の
略対称形の固定継鉄と、電磁コイルの内外に摺動自在に
設けられた可動鉄心と、固定継鉄の内面と可動鉄心との
間にあって、可動鉄心軸心に対して略対称位置に同磁極
を対向固定した永久磁石と、前記永久磁石と電磁コイル
の間にあって、かつ永久磁石よυ電磁コイルに近接して
可動鉄心を中心に略対称形の補助継鉄とを有し、補助継
鉄は可動鉄心、固定継鉄、補助継鉄、可動鉄心をめぐる
磁路の磁気的空隙が、可動鉄心、固定継鉄、永久磁石、
可動鉄心をめぐる磁路の磁気的空隙よりも小さくなる寸
法にすることによって、電磁コイルの磁束が永久磁石を
直接通ることがなく、磁気的空隙の小さい固定継鉄、補
助継鉄、可動鉄心、固定継鉄をめぐる磁路を通るので、
自己保持ソレノイドとして使用する際、永久磁石の減磁
を防止するのみならず、電磁コイルに小さい電流を流す
だけで作動する。非自己保持ソレノイドとして使用する
際も、上記同様電磁コイルの磁束は、磁気的空隙の大き
い永久磁石の部分を通らずに、磁気的空隙の小さい固定
継鉄、補助継鉄、可動鉄心、固定継鉄の経路を通るので
、低電力で吸着保持するように作用すると共に、自己保
持型、非自己保持型いずれのソレノイドとして使用する
場合も、吸着保持状態では永久磁石の磁束を補助継鉄・
可動鉄心・固定継鉄の底部に流し吸着接触面を1ケ所に
限定することによって、従来例のような組立後研磨を不
要なものにしている。
Structure of the Invention In order to achieve this object, the present invention includes a substantially symmetrical fixed yoke on the outside of the electromagnetic coil, a movable iron core that is slidably provided inside and outside the electromagnetic coil, and a movable iron core provided on the inner surface of the fixed yoke. a permanent magnet located between the iron core and having magnetic poles facing each other and fixed in substantially symmetrical positions with respect to the axis of the movable core, and a movable core located between the permanent magnet and the electromagnetic coil and close to the permanent magnet and the electromagnetic coil. The auxiliary yoke has an auxiliary yoke that is approximately symmetrical around the movable core, fixed yoke, auxiliary yoke, and a magnetic gap in the magnetic path surrounding the movable core. magnet,
By making the dimensions smaller than the magnetic gap in the magnetic path surrounding the movable iron core, the magnetic flux of the electromagnetic coil does not pass directly through the permanent magnet, making it possible to create fixed yoke, auxiliary yoke, movable iron core, etc. with small magnetic gaps. Since it passes through the magnetic path around the fixed yoke,
When used as a self-holding solenoid, it not only prevents the permanent magnet from demagnetizing, but also operates by simply passing a small current through the electromagnetic coil. When used as a non-self-holding solenoid, the magnetic flux of the electromagnetic coil does not pass through the permanent magnet part with a large magnetic gap, but instead passes through the fixed yoke, auxiliary yoke, movable iron core, and fixed joint with a small magnetic gap. Since it passes through the iron path, it acts to attract and hold with low power, and when used as a self-holding type or non-self-holding type solenoid, in the attracting and holding state, the magnetic flux of the permanent magnet is transferred to the auxiliary yoke.
By limiting the suction contact surface to one place by pouring it to the bottom of the movable core/fixed yoke, post-assembly polishing as in the conventional example is no longer necessary.

実施例の説明 以下、本発明の一実施例を第3図を用いて説明する。第
3図は自己保持型ソレノイドの実施例を示す縦断面図で
あって、同図(A)は吸着自己保持状態、(B)は通電
した瞬間の状態を示し、同図(C) fl離反状態を示
している。ここで有底円筒形Ω固定継鉄1の中央底面に
は固定鉄心2が固定されている。
DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described below with reference to FIG. FIG. 3 is a vertical cross-sectional view showing an embodiment of a self-holding solenoid, in which (A) shows the suction self-holding state, (B) shows the state at the moment of energization, and (C) shows the fl separation state. Indicates the condition. Here, a fixed iron core 2 is fixed to the center bottom surface of the bottomed cylindrical Ω fixed yoke 1.

その固定鉄心2の外周面にはOリング3を挿入して、さ
らに外側の非磁性円筒4にOリング3は密着している。
An O-ring 3 is inserted into the outer peripheral surface of the fixed iron core 2, and the O-ring 3 is in close contact with an outer non-magnetic cylinder 4.

さらに固定鉄心2と同心状で非磁性円筒4の外側にコイ
ルボビン5に巻回した電磁コイル6が納められ、電磁コ
イル6のすぐ上部でかつ固定鉄心2と同心状に、円環状
の補助継鉄7の外周面を固定継鉄1の内周面に内接させ
て積み重ね、さらに補助継鉄7の上部に非磁注弾注体8
を積み重ね、非磁注弾注体8の上に円環状で内周面がN
極、外周面がS極になるように着磁した永久磁石9が固
定しである。可動鉄心ICIj、非磁性円筒4の内部で
摺動自在に挿入しである。ここで補助継鉄7の内周面と
可動鉄心10の間の磁気的空隙は、補助継鉄7の内径と
可動鉄心10の外径とによって定められるが、この部分
の磁気的空隙よりも永久磁石9を介した固定継鉄1の内
周面とi1動鉄心10との間の磁気的空隙の方が大きく
なるように径方向の寸法が定められている。したがって
第3図(A)の吸着保持状態では永久磁石9の磁束A[
可動鉄心1oから、固定鉄心2・固定鉄心10を経て永
久磁石9へ戻る経路を流れているが、同図(B)のよう
に電磁コイル6に通電すると、その磁束Bは固定鉄心2
・可動鉄心10・補助継鉄γ固定継鉄1・固定鉄心2と
いう経路を通り、可動鉄心10の吸着面11には永久磁
石9の磁束人とは逆方向に流れている。この結果、吸着
保持力は激減するので図示していない別設のスプリング
の力によって、可動鉄心ICIj固定鉄心2から離反し
て第3図(c)のようになるよう作用する。
Further, an electromagnetic coil 6 wound around a coil bobbin 5 is housed concentrically with the fixed iron core 2 and outside the non-magnetic cylinder 4, and an annular auxiliary yoke is placed immediately above the electromagnetic coil 6 and concentrically with the fixed iron core 2. 7 are inscribed in the inner peripheral surface of the fixed yoke 1, and the non-magnetic injection body 8 is stacked on top of the auxiliary yoke 7.
are stacked on top of the non-magnetic injection body 8 in an annular shape with an inner circumferential surface of N.
A permanent magnet 9 is fixed and magnetized so that the outer peripheral surface becomes the S pole. The movable iron core ICIj is slidably inserted inside the non-magnetic cylinder 4. Here, the magnetic gap between the inner peripheral surface of the auxiliary yoke 7 and the movable iron core 10 is determined by the inner diameter of the auxiliary yoke 7 and the outer diameter of the movable iron core 10, but is more permanent than the magnetic gap in this part. The radial dimension is determined so that the magnetic gap between the inner circumferential surface of the fixed yoke 1 and the i1 moving iron core 10 via the magnet 9 is larger. Therefore, in the adsorption/holding state shown in FIG. 3(A), the magnetic flux A[
The magnetic flux B flows from the movable core 1o, passes through the fixed core 2 and the fixed core 10, and returns to the permanent magnet 9. When the electromagnetic coil 6 is energized as shown in FIG.
- The magnetic flux of the permanent magnet 9 flows through the path of the movable iron core 10, the auxiliary yoke γ, the fixed yoke 1, and the fixed iron core 2 to the attraction surface 11 of the movable iron core 10 in the opposite direction to that of the magnetic flux of the permanent magnet 9. As a result, the suction holding force is drastically reduced, and the force of a separate spring (not shown) acts to cause the movable core ICIj to separate from the fixed core 2 as shown in FIG. 3(c).

電磁コイル6に通電した時に生じる永久磁石9の磁束A
を打消す方向の磁束Bは、第3図(B)に示したように
永久磁石9自体を流れることがなく、永久磁石9と共通
の磁気回路の中で打消す方向に流れているのみであるか
ら、永久磁石9には減磁方向の磁界がほとんど加わらす
減磁を防止することが可能になっている。もちろん、吸
着する部分は可動鉄心10の端面11と固定鉄心2の上
端面12のみなので組立後に平面度を出すだめの研磨加
工の必要も無くなった。
Magnetic flux A of the permanent magnet 9 generated when the electromagnetic coil 6 is energized
The magnetic flux B in the direction of canceling does not flow through the permanent magnet 9 itself as shown in FIG. Because of this, it is possible to prevent demagnetization, which is caused by almost all magnetic fields in the demagnetizing direction being applied to the permanent magnet 9. Of course, since the only parts to be attracted are the end face 11 of the movable core 10 and the upper end face 12 of the fixed core 2, there is no need for polishing to achieve flatness after assembly.

また永久磁石9を円環状とし、固定継鉄1の内面を永久
磁石9の外周面に内接させることにより、同図(A)の
ように永久磁石9の磁束Aの磁路の磁気抵抗を小さくす
ることができ、その結果、必要な自己保持吸着力を得る
ための永久磁石を、小型化することが可能である。
Furthermore, by making the permanent magnet 9 circular and inscribing the inner surface of the fixed yoke 1 into the outer peripheral surface of the permanent magnet 9, the magnetic resistance of the magnetic path of the magnetic flux A of the permanent magnet 9 can be reduced as shown in FIG. As a result, it is possible to downsize the permanent magnet for obtaining the necessary self-holding attraction force.

また補助継鉄7・を円環状とし、固定継鉄1の内面に補
助継鉄7の外周面を内接させることにより同図(B)の
ように永久磁石9の磁束Aを打消すための電磁コイル6
による磁束Bの磁路の磁気抵抗を小さくすることができ
、その結果、電磁コイル6の寸法を小型化することが可
能となる。
In addition, by making the auxiliary yoke 7 into an annular shape and inscribing the outer peripheral surface of the auxiliary yoke 7 into the inner surface of the fixed yoke 1, it is possible to cancel the magnetic flux A of the permanent magnet 9 as shown in the same figure (B). Electromagnetic coil 6
The magnetic resistance of the magnetic path of the magnetic flux B can be reduced, and as a result, the size of the electromagnetic coil 6 can be reduced.

また固定鉄心2にOリングを挿入し、その外周に密着し
て非磁性円筒4を挿入して、さらに同心状に電磁コイル
6を挿入、補助継鉄・非磁注弾注体8・永久磁石9を積
み重ね、その外側に固定継鉄1を同心状に配置した構成
のため、結果、各部品の相対位置がバラツキなく定まる
ため、組立てがし易く、かつ特注が安定してバラツキを
押さえられ、量産をよりし易くできる。
In addition, an O-ring is inserted into the fixed iron core 2, a non-magnetic cylinder 4 is inserted in close contact with the outer periphery of the O-ring, and an electromagnetic coil 6 is further inserted concentrically, and an auxiliary yoke, a non-magnetic injection body 8, and a permanent magnet are inserted. 9 are stacked, and the fixed yoke 1 is placed concentrically on the outside.As a result, the relative position of each part is determined without any variation, making it easy to assemble, and making custom orders stable and suppressing variations. Mass production can be made easier.

第3図の実施例では固定継鉄1は有底円筒形であったが
コ字型でも良いし、永久磁石9は円環状でなく複数個に
分割されて、同極を対向配置する構成でもよい。また固
定鉄心2は省略が可能で、固定継鉄1の底面が吸着面と
なってもよりし、底面を加工によって一部だけ突き出し
た構成でもよい。
In the embodiment shown in FIG. 3, the fixed yoke 1 has a cylindrical shape with a bottom, but it may also be U-shaped, and the permanent magnet 9 may be divided into a plurality of pieces instead of annular, with the same poles facing each other. good. Further, the fixed iron core 2 may be omitted, and the bottom surface of the fixed yoke 1 may serve as a suction surface, or the bottom surface may be partially protruded by processing.

第4図は非自己保持型ソレノイドの実施例を示すもので
、同図(A)は電磁コイル6に通電し、電磁コイル6の
磁束Bと永久磁石9の磁束Aとで図示していないスプリ
ングのカに打勝って、可動鉄心10を吸着保持している
状態、(B)は電磁コイル6への通電を停止し、スプリ
ングのカで可動鉄心1゜が離反した状態を示している。
FIG. 4 shows an embodiment of a non-self-holding solenoid, and FIG. 4 (A) shows an electromagnetic coil 6 energized, and the magnetic flux B of the electromagnetic coil 6 and the magnetic flux A of the permanent magnet 9 generate a spring (not shown). (B) shows a state in which the movable core 10 is attracted and held by the force of the spring, and (B) shows a state in which the electromagnetic coil 6 is de-energized and the movable core 1° is separated by the force of the spring.

構成は第3図と同じであり、永久磁石9の磁力および電
磁コイル6の巻線仕様が異なるだけであり、同じ部品に
同番号を附し、構成の説明は省略する。この場合も第3
図の自己保持型ソレノイドと同様、吸着する部分は可動
鉄心10の端面11と固定鉄心2の上端面12のみなの
で組立後に平面度を出すための研磨加工の必要も無くな
った。
The configuration is the same as in FIG. 3, and the only difference is the magnetic force of the permanent magnet 9 and the winding specifications of the electromagnetic coil 6. The same numbers are given to the same parts, and a description of the configuration will be omitted. In this case as well, the third
Similar to the self-holding solenoid shown in the figure, the only parts that are attracted are the end face 11 of the movable core 10 and the upper end face 12 of the fixed core 2, so there is no need for polishing to achieve flatness after assembly.

また永久磁石9を円環状とし、固定鉄心1の内面に永久
磁石9の外周面が接する構成とし、第4図(A)のよう
に永久磁石9の磁束Aの磁路の磁気抵抗を小さくし、結
果、永久磁石を小型にし、ソレノイド全体の小型化がで
きる。
In addition, the permanent magnet 9 is annular, and the outer circumferential surface of the permanent magnet 9 is in contact with the inner surface of the fixed iron core 1, so that the magnetic resistance of the magnetic path of the magnetic flux A of the permanent magnet 9 is reduced as shown in FIG. 4(A). As a result, the permanent magnet can be made smaller and the entire solenoid can be made smaller.

また補助継鉄7を円環状とし、固定継鉄1の内面に補助
継鉄7の外周面が接する構成とし、同図(B)のように
電磁コイル6による磁束Bの磁路の磁気抵抗を小さくし
、結果、可動鉄心10を吸着保持するための電磁コイル
6による起磁力は小さくて良いことになり、したがって
電磁コイル6を小型化できたり、低電力通電で吸着保持
が可能となる。組立やすさについては第3図の自己保持
型ソレノイドと同様である。
In addition, the auxiliary yoke 7 is annular, and the outer peripheral surface of the auxiliary yoke 7 is in contact with the inner surface of the fixed yoke 1, so that the magnetic resistance of the magnetic path of the magnetic flux B caused by the electromagnetic coil 6 is reduced as shown in FIG. As a result, the magnetomotive force of the electromagnetic coil 6 for attracting and holding the movable iron core 10 can be small, so that the electromagnetic coil 6 can be made smaller and it is possible to attract and hold the movable iron core 10 with low power supply. The ease of assembly is similar to that of the self-holding solenoid shown in FIG.

なお第3図、第4図の実施例のソレノイドを、たとえば
家庭用ガス機器のガス通路の安全遮断を行なうソレノイ
ドパルプに応用する場合、可動鉄心1oの吸着面11と
は反対側の端面に弁ゴムを装着し、ガス流路閉止用の弁
座を有したボディに取付ければ、簡単に安全遮断弁を構
成することができる。まだこの場合、ガス通路外にガス
が洩出しないようにするために、非磁性円筒4の内側は
固定鉄心2との間をOリング3で気密にシールしている
ため、遮断弁として構成する際、ボディと非磁性円筒と
の間を、○リングのような固定パツキンでシールするだ
けで、簡単確実で信頼性の高いシール構造が可能である
In addition, when the solenoid of the embodiment shown in FIGS. 3 and 4 is applied to a solenoid pulp that safely shuts off the gas passage of household gas appliances, a valve is installed on the end surface of the movable core 1o opposite to the suction surface 11. By attaching rubber to a body having a valve seat for closing the gas flow path, a safety shutoff valve can be easily constructed. In this case, in order to prevent gas from leaking out of the gas passage, the inside of the non-magnetic cylinder 4 is airtightly sealed between the fixed iron core 2 and the O-ring 3, so it is configured as a shutoff valve. In this case, simply sealing between the body and the non-magnetic cylinder with a fixed gasket such as a ring allows for a simple, secure and highly reliable sealing structure.

発明の効果 以上のように本発明の永久磁石内蔵型ソレノイドによれ
ば次の効果が得られる。
Effects of the Invention As described above, the permanent magnet built-in solenoid of the present invention provides the following effects.

(1)電磁コイル外側の略対称形の固定継鉄内側に永久
磁石の同磁極を対向固定し、永久磁石より電磁コイルに
近接して可動鉄心の軸心を中心に、略対称形の補助継鉄
を配し、可動鉄心が吸着状態時永久磁石を介した固定継
鉄、可動鉄心間の磁気的空隙より、補助継鉄を介した固
定継鉄・可動鉄心間の磁気的空隙が小さい構成としてい
るので、電磁コイルの磁束は、磁気抵抗の大きい永久磁
石を通らず、磁気抵抗の小さい補助継鉄を通って、−ケ
所の可動鉄心吸着面を通るように作用し、従来例のよう
に平面度を確保するだめの組立後の研磨加工を必要とせ
ず安価な永久磁石内蔵型ソレノイドの提供が可能になっ
たものである。
(1) The same magnetic poles of a permanent magnet are fixed facing each other inside a substantially symmetrical fixed yoke outside the electromagnetic coil, and a substantially symmetrical auxiliary yoke is placed closer to the electromagnetic coil than the permanent magnet and centered around the axis of the movable iron core. When the movable iron core is in an attracted state, the magnetic gap between the fixed yoke and the movable iron core via the auxiliary yoke is smaller than the magnetic gap between the fixed yoke and the movable iron core via the auxiliary yoke. Therefore, the magnetic flux of the electromagnetic coil does not pass through the permanent magnet, which has a high magnetic resistance, but through the auxiliary yoke, which has a low magnetic resistance, and passes through the movable core attracting surface at two locations, so that it does not pass through the flat surface as in the conventional example. This makes it possible to provide an inexpensive solenoid with a built-in permanent magnet that does not require post-assembly polishing of the reservoir to ensure accuracy.

(2)電磁コイルの磁束が直接永久磁石を通らないので
、自己保持型ソレノイドとして使用する場合にも、永久
磁石減磁の恐れがない。
(2) Since the magnetic flux of the electromagnetic coil does not directly pass through the permanent magnet, there is no risk of permanent magnet demagnetization even when used as a self-holding solenoid.

(3ン 電磁コイルの磁束が電磁コイルに近くて磁気的
空隙が小さい補助継鉄を通り、可動鉄心吸着面に作用す
るので、電磁コイルに加える電力は低電力でよい。
(3) The magnetic flux of the electromagnetic coil passes through the auxiliary yoke, which is close to the electromagnetic coil and has a small magnetic gap, and acts on the adsorption surface of the movable core, so the power applied to the electromagnetic coil can be low.

(4)補助継鉄を永久磁石から離した構成としているの
で、可動鉄心吸着保持状態で、可動鉄心の吸着面以外に
漏洩する磁束を少なくかつ、吸着面に有効に作用し、永
久磁石の小型化ができる。
(4) Since the auxiliary yoke is configured to be separated from the permanent magnet, when the movable iron core is attracted and held, there is less magnetic flux leaking to areas other than the attraction surface of the movable iron core, and it acts effectively on the attraction surface, making it possible to reduce the size of the permanent magnet. can be converted into

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

第1図(A) 、 (B) 、 (C)は従来の永久磁
石内蔵型ソレノイドの自己保持型ソレノイドの吸着保持
状態。 通電状態、離反状態を示す縦断面図、第2図(A)。 (B)は同非自己保持型ソレノイドの吸着保持状態。 離反状態を示す縦断面図、第3図(A) 、 (B) 
、 CG)は本発明の一実施例における永久磁石内蔵型
ソレノイドの自己保持型ソレノイドの吸着保持状態1通
電状態、離反状態を示す縦断面図、第4図(A) 、 
(B)は同非自己保持ソレノイドの吸着保持状態、離反
状態を示す縦断面図である。 1・・・・・・固定継鉄、6・・・・・・電磁コイル、
7・・・・・・補助継鉄、9・・・・・・永久磁石、1
o゛°゛°°可動鉄心〇代理人の氏名 弁理士 中 尾
 敏 男 ほか1名第1図 第2図 01 第3図 第4図
Figures 1 (A), (B), and (C) show the adsorption and holding state of a conventional self-holding solenoid with a built-in permanent magnet. FIG. 2(A) is a vertical cross-sectional view showing the energized state and the separated state. (B) shows the adsorption and holding state of the same non-self-holding solenoid. Longitudinal cross-sectional view showing separation state, Fig. 3 (A), (B)
, CG) is a vertical cross-sectional view showing the self-holding solenoid of the permanent magnet built-in solenoid in the adsorption/holding state 1 energized state and separated state in an embodiment of the present invention, FIG. 4(A),
(B) is a longitudinal cross-sectional view showing the non-self-holding solenoid in an adsorption/holding state and a separated state. 1... fixed yoke, 6... electromagnetic coil,
7... Auxiliary yoke, 9... Permanent magnet, 1
o゛°゛°°Movable iron core〇 Name of agent Patent attorney Toshio Nakao and one other person Figure 1 Figure 2 Figure 01 Figure 3 Figure 4

Claims (4)

【特許請求の範囲】[Claims] (1)電磁コイルと、この電磁コイル外側の略対称形の
固定継鉄と、前記電磁コイルの内側に摺動自在に設けら
れた可動鉄心と、前記固定継鉄の内面と前記可動鉄心の
間にあって略対称位置に同磁極を対向固定した永久磁石
と、前記永久磁石と電磁コイルの間にあって、かつ永久
磁石より電磁コイルに近接して前記可動鉄心を中心に略
対称形の補助継鉄とを有し、この補助継鉄は前記可動鉄
心が吸着状態で電磁コイル通電時、前記可動鉄心、固定
継鉄、補助継鉄、可動鉄心をめぐる磁路の磁気的空隙が
、前記可動鉄心、固定継鉄、永久磁石、可動鉄心をめぐ
る磁路の磁気的空隙よりも小さくなる寸法にした永久磁
石内蔵型ソレノイド。
(1) An electromagnetic coil, a substantially symmetrical fixed yoke on the outside of the electromagnetic coil, a movable core slidably provided inside the electromagnetic coil, and a space between the inner surface of the fixed yoke and the movable core. a permanent magnet with the same magnetic poles fixed facing each other in substantially symmetrical positions, and an auxiliary yoke that is substantially symmetrical about the movable iron core and located between the permanent magnet and the electromagnetic coil and closer to the electromagnetic coil than the permanent magnet. In this auxiliary yoke, when the movable iron core is in an attracted state and the electromagnetic coil is energized, the magnetic gap of the magnetic path surrounding the movable iron core, fixed yoke, auxiliary yoke, and movable iron core is A solenoid with a built-in permanent magnet whose dimensions are smaller than the magnetic gap in the magnetic path surrounding the iron, permanent magnet, and movable iron core.
(2)永久磁石を円環状とし、固定継鉄の内面を永久磁
石外周面に内接させた特許請求の範囲第1項記載の永久
磁石内蔵型ソレノイド。
(2) The solenoid with a built-in permanent magnet according to claim 1, wherein the permanent magnet is annular, and the inner surface of the fixed yoke is inscribed in the outer peripheral surface of the permanent magnet.
(3)補助継鉄を円環状とし、固定継鉄の内面に補助継
鉄外周面を内接させた特許請求の範囲第2項記載の永久
磁石内蔵型ソレノイド。
(3) The solenoid with a built-in permanent magnet according to claim 2, wherein the auxiliary yoke is annular, and the outer peripheral surface of the auxiliary yoke is inscribed in the inner surface of the fixed yoke.
(4)電磁コイル内面に非磁性円筒を挿入し、非磁性円
筒の同軸内部に固定鉄心と可動鉄心とを有し、固定鉄心
外周の○リング溝に○リングを挿入し、非磁性円筒外側
に電磁コイル、補助継鉄、永久磁石、固定継鉄を同心軸
上に設けた特許請求の範囲第1項記載の永久磁石内蔵型
ソレノイド。
(4) Insert a non-magnetic cylinder inside the electromagnetic coil, have a fixed core and a movable core inside the coaxial part of the non-magnetic cylinder, insert the ○ ring into the ○ ring groove on the outer periphery of the fixed core, and insert the ○ ring into the ○ ring groove on the outer periphery of the fixed core, and A solenoid with a built-in permanent magnet according to claim 1, wherein an electromagnetic coil, an auxiliary yoke, a permanent magnet, and a fixed yoke are provided on a concentric axis.
JP58109540A 1983-06-17 1983-06-17 Solenoid with built-in permanent magnet Pending JPS601814A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58109540A JPS601814A (en) 1983-06-17 1983-06-17 Solenoid with built-in permanent magnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58109540A JPS601814A (en) 1983-06-17 1983-06-17 Solenoid with built-in permanent magnet

Publications (1)

Publication Number Publication Date
JPS601814A true JPS601814A (en) 1985-01-08

Family

ID=14512832

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58109540A Pending JPS601814A (en) 1983-06-17 1983-06-17 Solenoid with built-in permanent magnet

Country Status (1)

Country Link
JP (1) JPS601814A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6816048B2 (en) * 2001-01-18 2004-11-09 Hitachi, Ltd. Electromagnet and actuating mechanism for switch device, using thereof
CN104051123A (en) * 2014-06-09 2014-09-17 常熟开关制造有限公司(原常熟开关厂) Electromagnet structure
JP2016126020A (en) * 2014-12-26 2016-07-11 日本電産コパル株式会社 Shutter for camera, and camera

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6816048B2 (en) * 2001-01-18 2004-11-09 Hitachi, Ltd. Electromagnet and actuating mechanism for switch device, using thereof
US6940376B2 (en) 2001-01-18 2005-09-06 Hitachi, Ltd. Electromagnet and actuating mechanism for switch device, using thereof
US7075398B2 (en) 2001-01-18 2006-07-11 Hitachi, Ltd. Electromagnet and actuating mechanism for switch device, using thereof
CN104051123A (en) * 2014-06-09 2014-09-17 常熟开关制造有限公司(原常熟开关厂) Electromagnet structure
JP2016126020A (en) * 2014-12-26 2016-07-11 日本電産コパル株式会社 Shutter for camera, and camera

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