JPS6229111A - Plunger type electromagnet - Google Patents

Plunger type electromagnet

Info

Publication number
JPS6229111A
JPS6229111A JP60168241A JP16824185A JPS6229111A JP S6229111 A JPS6229111 A JP S6229111A JP 60168241 A JP60168241 A JP 60168241A JP 16824185 A JP16824185 A JP 16824185A JP S6229111 A JPS6229111 A JP S6229111A
Authority
JP
Japan
Prior art keywords
iron core
core
face
pole
movable
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
JP60168241A
Other languages
Japanese (ja)
Inventor
Yuichi Ando
安藤 祐一
Nobuaki Tsugawa
津川 信明
Kenji Iio
飯尾 謙二
Shinji Toriyama
通山 真二
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.)
IWASAKI GIKEN KOGYO KK
MIYAZAKI SEISAKUSHO KK
Original Assignee
IWASAKI GIKEN KOGYO KK
MIYAZAKI SEISAKUSHO KK
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 IWASAKI GIKEN KOGYO KK, MIYAZAKI SEISAKUSHO KK filed Critical IWASAKI GIKEN KOGYO KK
Priority to JP60168241A priority Critical patent/JPS6229111A/en
Publication of JPS6229111A publication Critical patent/JPS6229111A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain a large stroke length when low power is applied as well as to enable to adjust the sucking and retaining strength when no current flows by a method wherein the pole faces of a fixed iron core or a movable iron core are formed on the inner sidewall of a cylindrical body, and the pole faces of the other iron core opposing to said pole faces are formed on the parallel side and the right-angled end of a columnar body which is inserted and arranged in a freely slidable and displaceable manner. CONSTITUTION:Either of a fixed iron core 2 or a movable iron core 8, namely, the pole face of the fixed iron core 2, for example, is formed on the inner side face 4a of a cylindrical body 4, the pole face of the other iron core 8 opposing to the inner side face 4a, having the same axis as the inner side face of a cylindrical body, is inserted and arranged in the axial direction of the pole face of the core 8 in a freely sliding and displaceable manner, and the paralleled side face 8 in axial direction of a columnar body and a right-angled end face 8b are formed. As a result, when a current is applied on an electric winding, the magnetic flux generated by the above-mentioned application of current and the magnetic flux of a permanent magnet are supported, and the movable iron core 8 is attracted to the fixed iron core 2 by composite magnetic force. In this case, one of the core pole-face is formed on the internal side face 4a of the cylindrical body, the pole face of the other iron core is formed on the side face 8 in parallel with the axial direction of the cylindrical body of the pole-like body and the right-angled end face 8b. The distance linking both pole faces 8a and 8b is shortened, and as a void magnetic path is small, the titled electromagnet can be driven with a small type of winding and minor power is spite of having a large stroke.

Description

【発明の詳細な説明】 (イ)産業上の利用分野 この発明は、永久磁石を含むプランジャ型電磁石の改良
に関する。
DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application This invention relates to improvements in plunger type electromagnets including permanent magnets.

(ロ)従来の技術 従来の永久磁石を用いたプランジャ型電磁石としては、
例えば第5図、第6図に示すものがある。
(b) Conventional technology As a plunger type electromagnet using a conventional permanent magnet,
For example, there are those shown in FIGS. 5 and 6.

第5図のプランジャ型電磁石は、ボビンaに2個の励磁
コイルbscが巻回されるとともに、この2個の励磁コ
イルb、c間に永久磁石dが介設され、さらにボビンa
内にはヨークeに固設された固定鉄心fと可動鉄心gが
設けられて構成されている。このプランジャ型電磁石で
は、励磁コイルbに通電すると、永久磁石dによる磁束
と励磁コイルbによる磁束が重畳されて、可動鉄心gを
固定鉄心f側に吸引する力が働き、可動鉄心gは固定鉄
心fに吸着される。吸着後、励磁コイルbの通電をオフ
しても、永久磁石dの磁力により、可動鉄心gは吸着状
態で保持される。可動鉄心gの解放は、励磁コイルCに
通電することにより行われる。
The plunger type electromagnet shown in Fig. 5 has two excitation coils bsc wound around a bobbin a, a permanent magnet d interposed between these two excitation coils b and c, and a bobbin a.
A fixed iron core f fixed to a yoke e and a movable iron core g are provided inside. In this plunger-type electromagnet, when the excitation coil b is energized, the magnetic flux from the permanent magnet d and the magnetic flux from the excitation coil b are superimposed, and a force that attracts the movable core g toward the fixed core f acts, and the movable core g is connected to the fixed core. It is attracted to f. After attraction, even if the excitation coil b is de-energized, the movable core g is held in the attracted state by the magnetic force of the permanent magnet d. The movable iron core g is released by energizing the excitation coil C.

第6図のプランジャ型電磁石は、励磁コイルbを1個と
するとともに、固定鉄心fと可動鉄心g間に、解放用の
バネhを設けている。このプランジャ型電磁石は、励磁
コイルbに通電すると、第5図のものと同様にして、可
動鉄心gが固定鉄心fに吸着される。そして、通電をオ
フしても、やはり永久磁石dの磁性で自己保持されてお
り、励磁コイルbに逆電流が流されると、可動鉄心gが
解放される。
The plunger type electromagnet shown in FIG. 6 has one excitation coil b and a release spring h between the fixed iron core f and the movable iron core g. In this plunger type electromagnet, when the excitation coil b is energized, the movable iron core g is attracted to the fixed iron core f in the same manner as in the one shown in FIG. Even when the current is turned off, the movable iron core g is still self-held by the magnetism of the permanent magnet d, and when a reverse current is passed through the excitation coil b, the movable iron core g is released.

(ハ)発明が解決しようとする問題点 上記例にも示すように、従来のプランジャ型電磁石は、
固定鉄心と可動鉄心の磁極面が軸方向に垂直な面で対面
するものであるため、ストローク長さの大きいものを得
ようとすれば、解放時の固定鉄心と可動鉄心の磁極面間
距離を大きくせねばならず、そのため、可動鉄心を吸引
する時には大きな励磁アンペアターンを要し、駆動電力
の増大、形状の大型化を招くという問題があった。
(c) Problems to be solved by the invention As shown in the above example, the conventional plunger type electromagnet:
Since the magnetic pole faces of the fixed core and the movable core face each other in a plane perpendicular to the axial direction, if you want to obtain a long stroke length, the distance between the magnetic pole faces of the fixed core and the movable core when released should be Therefore, when attracting the movable core, a large excitation ampere turn is required, resulting in an increase in driving power and an increase in size.

また、従来のものでは、永久磁石によるラッチング動作
の無通電時の吸着保持力の調節が困難であった。
Furthermore, in the conventional device, it is difficult to adjust the adsorption and holding force of the latching operation using the permanent magnet when no current is applied.

この発明は、上記に鑑み、小型・小電力で大きなストロ
ーク長さが取れる、しかも必要によって無通電時の吸引
保持力を調節し得るプランジャ型電磁石を提供すること
を目的としている。
In view of the above, it is an object of the present invention to provide a plunger-type electromagnet that is small in size and has a large stroke length with low electric power, and that can adjust the attracting and holding force when no current is applied as necessary.

(ニ)問題点を解決するための手段 この発明のプランジャ型電磁石は、固定鉄心、可動鉄心
、電気巻線及び永久磁石を含み、前記永久磁石が発する
磁束に前記電気巻線通電による磁束を重畳させ、前記両
鉄心の磁極面間に吸引力を発生させ、この吸引力で可動
鉄心の機械的変移を行うものにおいて、前記固定鉄心又
は可動鉄心のいずれか一方の磁極面を筒体内側面に形成
するとともに、これに対面する他方の鉄心の磁極面を、
前記筒体内側面と同一軸を持ち、この軸の方向に摺動変
移自在に挿入配置した柱状体の前記軸方向の平行側面及
び直角端面に形成している。
(d) Means for Solving the Problems The plunger type electromagnet of the present invention includes a fixed iron core, a movable iron core, an electric winding, and a permanent magnet, and the magnetic flux generated by the electric winding is superimposed on the magnetic flux generated by the permanent magnet. in which an attractive force is generated between the magnetic pole surfaces of the two iron cores, and the movable iron core is mechanically displaced by this attractive force, wherein the magnetic pole surface of either the fixed iron core or the movable iron core is formed on the inner side surface of the cylinder. At the same time, the magnetic pole surface of the other iron core facing this,
It is formed on a parallel side surface and a right-angled end surface in the axial direction of a columnar body which has the same axis as the inner side surface of the cylinder and is inserted and arranged so as to be slidable in the direction of this axis.

(ホ)作用 このプランジャ型電磁石では、電気巻線に通電すると、
この通電によって生じる磁束と永久磁石の磁束が重畳し
て、その合成磁力により、可動鉄心が固定鉄心に吸着さ
れる。この場合、一方の鉄心磁極面が筒体内側面に形成
され、他方の鉄心磁極面が柱状体の前記筒体の軸方向に
平行な側面及び直角端面に形成され、両磁極面を結ぶ距
離は短(なり、空隙磁路が小さいので、大きなストロー
クを取るわりには小型の電気巻線、小電力で駆動できる
(E) Effect In this plunger type electromagnet, when the electric winding is energized,
The magnetic flux generated by this energization and the magnetic flux of the permanent magnet are superimposed, and the combined magnetic force attracts the movable iron core to the fixed iron core. In this case, one core magnetic pole surface is formed on the side surface of the cylinder, and the other core magnetic pole surface is formed on the side surface parallel to the axial direction and the right-angled end surface of the columnar cylinder, and the distance connecting both magnetic pole surfaces is short. (Because the air gap magnetic path is small, it can be driven with a small electric winding and low power even though it takes a large stroke.

(へ)実施例 以下、実施例により、この発明をさらに詳細に説明する
(f) Examples The present invention will now be explained in more detail with reference to Examples.

第1図、第2図は、この発明の一実施例プランジャ型電
磁石の説明図である。
1 and 2 are explanatory diagrams of a plunger type electromagnet according to an embodiment of the present invention.

このプランジャ型電磁石1は、中央部の大径筒部3と、
その両端に連設される小径筒部4.5からなる固定鉄心
2と、前記大径筒部3内に設けられる励磁コイル(電気
巻線)6及び永久磁石7と、小径筒部4.5と励磁コイ
ル6及び永久磁石7で形成される筒内に配置される円柱
状の可動鉄心8とから構成されている。
This plunger type electromagnet 1 has a large diameter cylindrical part 3 in the center,
A fixed iron core 2 consisting of a small-diameter cylindrical portion 4.5 connected to both ends thereof, an excitation coil (electric winding) 6 and a permanent magnet 7 provided in the large-diameter cylindrical portion 3, and a small-diameter cylindrical portion 4.5. and a cylindrical movable iron core 8 disposed within a cylinder formed by an excitation coil 6 and a permanent magnet 7.

このプランジャ型電磁石1では、励磁コイル6に通電し
ない状態、つまり解放状態で、可動鉄心8は第1図に示
す状態にあり、固定鉄心2の磁極面は小径筒部4の筒内
側面4aに形成され、これに対応する可動鉄心8の磁極
面は、筒体の軸方向に平行な側面8aと、軸方向に直角
な端面8bに形成され、ここでは固定鉄心2と可動鉄心
8の磁極は軸方向に対し45°の角度で対峙している。
In this plunger type electromagnet 1, when the excitation coil 6 is not energized, that is, in the open state, the movable core 8 is in the state shown in FIG. The corresponding magnetic pole surfaces of the movable core 8 are formed on a side surface 8a parallel to the axial direction of the cylinder and an end surface 8b perpendicular to the axial direction.Here, the magnetic poles of the fixed core 2 and the movable core 8 are They face each other at an angle of 45° to the axial direction.

次に、このプランジャ型電磁石1の動作について説明す
る。
Next, the operation of this plunger type electromagnet 1 will be explained.

今、励磁コイル6に通電しない時、第1図に示す状態で
安定しているものとする。
Assume that when the excitation coil 6 is not energized, the state shown in FIG. 1 is stable.

この状態で、永久磁石7の起磁力による磁束は、漏洩を
無視すれば、図示のφa1.φb、と分流し、磁束φa
、4よ可動鉄心8の磁極面8a、8bを経て、固定鉄心
2の小径筒部3の磁極面3aに入り、磁束φb、は可動
鉄心8を磁束φa、とは逆方向に通り、固定鉄心2の小
径筒部4の磁極面4aに入る。
In this state, if leakage is ignored, the magnetic flux due to the magnetomotive force of the permanent magnet 7 will be φa1. φb, and the magnetic flux φa
, 4, enters the magnetic pole surface 3a of the small diameter cylindrical portion 3 of the fixed iron core 2 through the magnetic pole surfaces 8a and 8b of the movable iron core 8, and the magnetic flux φb passes through the movable iron core 8 in the opposite direction to the magnetic flux φa, and is transferred to the fixed iron core. It enters the magnetic pole face 4a of the small diameter cylindrical portion 4 of No.2.

それぞれの磁束量は、各々その磁路の磁気抵抗値に逆比
例して所定値に設定される。また、磁束φa、φb1に
よる合成機械的作用力は零となる。
Each amount of magnetic flux is set to a predetermined value in inverse proportion to the magnetic resistance value of the respective magnetic path. Further, the combined mechanical action force due to the magnetic fluxes φa and φb1 becomes zero.

この状態で、次に励磁コイル6に通電し、こめ通電によ
り発生する磁束をφiとし、その方向を第1図の通りと
する。これにより、可動鉄心8に作用する機械的吸引力
は F+ =  K ((−φa1−φ1)2−(φb、−
φi)”)+ただし fb:バネ等によるφb 方向の力 で示される。
In this state, the excitation coil 6 is then energized, and the magnetic flux generated by the energization is defined as φi, and its direction is as shown in FIG. As a result, the mechanical attraction force acting on the movable iron core 8 is F+ = K ((-φa1-φ1)2-(φb,-
φi)”)+where fb: Indicates the force in the φb direction due to a spring, etc.

この機械的作用力F1が負の値の場合、可動鉄心8は吸
着され、第2図に示す位置まで変移する。
When this mechanical force F1 has a negative value, the movable iron core 8 is attracted and moves to the position shown in FIG.

そして、 F’z =−K ((−φat −φi)”−(+1’
bz−φi)”) +f bの負の値の保持力によって
、第2図の状態が保持される。
And F'z = -K ((-φat -φi)"-(+1'
bz-φi)") +f The state shown in FIG. 2 is maintained by the negative value of b.

次に、この状態で励磁コイル6の通電を停止すると、可
動鉄心8には Fs −−K (φ”az −φzbz) + f b
の吸着力が作用する。この場合、F、が負の値であれば
、第2図の状態が保持される。しかし、F。
Next, when the excitation coil 6 is de-energized in this state, the movable core 8 has Fs −−K (φ”az −φzbz) + f b
The adsorption force of In this case, if F is a negative value, the state shown in FIG. 2 is maintained. However, F.

が正の値の場合は、第1図の状態に復帰する。なお、小
径筒部4の端部に、ラフチングカを強めるために磁性体
vi10が設けられている。
If is a positive value, the state shown in FIG. 1 is restored. Note that a magnetic material vi10 is provided at the end of the small diameter cylindrical portion 4 in order to strengthen the rafting force.

ここで、磁束φa2、φb2の値は、空隙9a、9bの
値、磁性体板1oの有無等により、容易にrtli節・
設定が可能である。
Here, the values of the magnetic fluxes φa2 and φb2 are easily determined by the rtli node and the values of the air gaps 9a and 9b, the presence or absence of the magnetic plate 1o, etc.
Can be configured.

ところで、F3が負の値の条件では、上記のように、励
磁コイル6に通電がない場合、可動鉄心8は第2図に示
す状態に保持されているが、この状態で、第2図に示す
方向の磁束φiが生じる極性の電流を励磁コイル6に流
してやると、F、 =−K ((−φa2+φi)”−
(φb2+φi )2) +fbの吸引力が可動鉄心8
に作用し、F4が正の値となる条件で、可動鉄心8を第
1図の状態に復帰させることができる。
By the way, under the condition that F3 is a negative value, as mentioned above, when the excitation coil 6 is not energized, the movable core 8 is held in the state shown in FIG. 2; When a current with a polarity that generates magnetic flux φi in the direction shown is passed through the exciting coil 6, F, = −K ((−φa2+φi)”−
(φb2+φi)2) The attraction force of +fb is the movable iron core 8
The movable iron core 8 can be returned to the state shown in FIG. 1 under the condition that F4 becomes a positive value.

このプランジャ型電磁石1では、解放時に通電すると、
上記のように磁極面4aと磁極面8a、8bに磁束が集
中し、空隙9aが小さいので、初期駆動力が大となる。
In this plunger type electromagnet 1, when energized when released,
As described above, the magnetic flux is concentrated on the magnetic pole surface 4a and the magnetic pole surfaces 8a and 8b, and the air gap 9a is small, so the initial driving force is large.

第3図、第4図は、この発明の他の実施例を示すプラン
ジャ型電磁石の説明図である。
FIGS. 3 and 4 are explanatory views of plunger type electromagnets showing other embodiments of the present invention.

この実施例プランジャ型電磁石11は、ポビン12に2
個の励磁コイル(電気巻線)13.14が巻回されると
ともに、この2個の励磁コイル13.14間に永久磁石
15が介設されている。なお16は、補助磁性片である
The plunger type electromagnet 11 of this embodiment has two
Excitation coils (electrical windings) 13, 14 are wound, and a permanent magnet 15 is interposed between these two excitation coils 13, 14. Note that 16 is an auxiliary magnetic piece.

また、励磁コイル13.14及び永久磁石15を囲撓し
て、磁路形成用のヨーク17が設けられ、このヨーク1
7に固設される固定鉄心18と、可動鉄心19がボビン
12内に挿設されている。
Further, a yoke 17 for forming a magnetic path is provided surrounding the excitation coils 13 and 14 and the permanent magnet 15, and this yoke 1
A fixed iron core 18 fixed to the bobbin 7 and a movable iron core 19 are inserted into the bobbin 12.

固定鉄心18は、凹状の磁極部20を備え、この磁極部
20の凹状底部に、さらに凹部21を設けている。また
、可動鉄心19は、前記固定鉄心18の凹状の磁極部2
0に対面して、凸状の磁極部22を備え、この磁極部2
2の凸状頂部に、さらに凹部23を設けている。凹部2
1と凹部23間にバネ24が介設され、このバネ24に
抗し、あるいはバネ24力により、可動鉄心19の凸状
磁極部22が固定鉄心18の凹状磁極部20に挿脱変移
自在に構成されている。
The fixed core 18 includes a concave magnetic pole part 20, and a concave bottom part of the magnetic pole part 20 is further provided with a concave part 21. Furthermore, the movable iron core 19 has a concave magnetic pole portion 2 of the fixed iron core 18.
0, a convex magnetic pole part 22 is provided, and this magnetic pole part 2
A concave portion 23 is further provided on the convex top portion of No. 2. Recess 2
A spring 24 is interposed between 1 and the recess 23, and the convex magnetic pole part 22 of the movable core 19 can be freely inserted into and removed from the concave magnetic pole part 20 of the fixed core 18 by resisting this spring 24 or by the force of the spring 24. It is configured.

このプランジャ型電磁石11では、励磁コイル13.1
4に通電しない状態、つまり解放状態で、可動鉄心19
は第3図に示す位置にある。この状態では、固定鉄心1
8の凹状磁極部20の底部と可動鉄心19の凸状磁極部
22の頂部間は距離りで、比較的大であるが、凹状磁極
部20の周縁壁部20aと凸状磁極部22の頂部22a
との距離及びヨーク17の先端17aと可動鉄心19と
の距離は微小である。そのため、ここで励磁コイル13
を通電すると、この通電により磁束と永久磁石15によ
る磁束が重畳して、可鉄心19は固定鉄心18に吸引さ
れ、第4図に示す状態に吸着保持される この状態では、ヨーク17の先端17aと可動鉄心19
との距離が大となるので、永久磁石15よりの磁束は、
大部分が可動鉄心19の凸状磁極部22の頂部22aと
固定鉄心18の凹状磁極部20の周壁部の接面に集中す
ることになる。つまり、強力な保持力が得られる。ここ
で、励磁コイル13の通電をオフしても、保持力が高い
と可動鉄心19は第4図の状態に保持されたままである
In this plunger type electromagnet 11, the exciting coil 13.1
4 is not energized, that is, in an open state, the movable iron core 19
is in the position shown in FIG. In this state, fixed core 1
The distance between the bottom of the concave magnetic pole part 20 of No. 8 and the top of the convex magnetic pole part 22 of the movable iron core 19 is relatively large; 22a
and the distance between the tip 17a of the yoke 17 and the movable iron core 19 are minute. Therefore, here, the excitation coil 13
When electricity is applied, the magnetic flux and the magnetic flux from the permanent magnet 15 are superimposed, and the ironable core 19 is attracted to the fixed iron core 18, and in this state where it is attracted and held in the state shown in FIG. 4, the tip 17a of the yoke 17 and movable iron core 19
Since the distance from the permanent magnet 15 is large, the magnetic flux from the permanent magnet 15 is
Most of it is concentrated on the contact surface between the top 22a of the convex magnetic pole part 22 of the movable core 19 and the peripheral wall of the concave magnetic pole part 20 of the fixed core 18. In other words, a strong holding force can be obtained. Here, even if the excitation coil 13 is de-energized, if the holding force is high, the movable core 19 remains held in the state shown in FIG. 4.

励磁コイル14に通電すると、バネ24力とこの励磁コ
イル14による磁力が前記保持力を越え、可動鉄心19
は吸着保持を解かれ、第3図に示す状態に復帰する。
When the excitation coil 14 is energized, the force of the spring 24 and the magnetic force of the excitation coil 14 exceed the holding force, and the movable iron core 19
is released from the suction hold and returns to the state shown in FIG.

(ト)発明の効果 この発明によれば、可動鉄心のストローク距離に対し、
解放時の固定鉄心と可動鉄心の磁極面間距離が小さいの
で、所定のストロークを得るのに、小型・小電力でよい
し、逆に所定の電ノコで大きなストロークのプランジャ
型電磁石を得ることができる。
(g) Effect of the invention According to this invention, the stroke distance of the movable iron core is
Since the distance between the magnetic pole faces of the fixed core and the movable core when released is small, a small size and low power are required to obtain a specified stroke, and conversely, it is possible to obtain a plunger type electromagnet with a large stroke using a specified electric saw. can.

その上、可動鉄心の長さを適宜選定し、吸着時における
非吸着部の固定鉄心と可動鉄心の距離を設定・変更すれ
ば、無通電時の保持力を調整することができる。
Furthermore, by appropriately selecting the length of the movable core and setting or changing the distance between the fixed core and the movable core of the non-capturing portion during suction, the holding force during non-energization can be adjusted.

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

第1図、第2図は、この発明の一実施例プランジャ型電
磁石の説明図であり、第1図は、可動鉄心解放時を示す
説明図、第2図は、可動鉄心吸着時を示す説明図、第3
図、第4図は、この発明の他の実施例プランジャ型電磁
石の説明図であり、第3図は、可動鉄心解放時を示す説
明図、第4図は、可動鉄心吸着時を示す説明図、第5図
、第6図は、従来のプランジャ型電磁石を示す図である
。 1・11;プランジャ型電磁石、 2・18:固定鉄心、 6・13・14:励磁コイル、 7・15:永久磁石、 8・19:可動鉄心。 特許出願人        岩崎技研工業株式会社(ほ
か1名) 代理人     弁理士  中 村 茂 信第1図 2:圓定註・(− 第3図 18:圓定欽l(・ 第5図 jl!6図
1 and 2 are explanatory diagrams of a plunger type electromagnet according to an embodiment of the present invention. FIG. 1 is an explanatory diagram showing when the movable core is released, and FIG. 2 is an explanatory diagram showing when the movable core is attracted. Figure, 3rd
4 are explanatory diagrams of a plunger type electromagnet according to another embodiment of the present invention, FIG. 3 is an explanatory diagram showing when the movable core is released, and FIG. 4 is an explanatory diagram showing when the movable core is attracted. , FIG. 5, and FIG. 6 are diagrams showing conventional plunger type electromagnets. 1.11: Plunger type electromagnet, 2.18: Fixed iron core, 6.13.14: Exciting coil, 7.15: Permanent magnet, 8.19: Movable iron core. Patent applicant: Iwasaki Giken Kogyo Co., Ltd. (and 1 other person) Agent: Patent attorney Shigeru Nakamura

Claims (4)

【特許請求の範囲】[Claims] (1)固定鉄心、可動鉄心、電気巻線及び永久磁石を含
み、前記永久磁石が発する磁束に前記電気巻線通電によ
る磁束を重畳させ、前記両鉄心の磁極面間に吸引力を発
生させ、この吸引力で可動鉄心の機械的変移を行うプラ
ンジャ型電磁石において、 前記固定鉄心又は可動鉄心のいずれか一方の磁極面を筒
体内側面に形成するとともに、これに対面する他方の鉄
心の磁極面を、前記筒体内側面と同一軸を持ち、この軸
方向に摺動変移自在に挿入配置して柱状体の前記軸方向
の平行側面及び直角端面に形成してなることを特徴とす
るプランジャ型電磁石。
(1) A fixed core, a movable core, an electric winding, and a permanent magnet are included, and the magnetic flux generated by the permanent magnet is superimposed on the magnetic flux generated by energizing the electric winding to generate an attractive force between the magnetic pole surfaces of the two iron cores; In a plunger type electromagnet that mechanically shifts a movable core using this attractive force, the magnetic pole surface of either the fixed core or the movable core is formed on the inner side surface of the cylinder, and the magnetic pole surface of the other core facing this is formed on the inner side surface of the cylinder. , a plunger type electromagnet having the same axis as the inner side surface of the cylinder, and being inserted and arranged so as to be slidable in the axial direction, and formed on the parallel side surface and the right-angled end surface of the columnar body in the axial direction.
(2)前記筒体内側面の一方の端部に磁性体板が設けら
れた特許請求の範囲第1項記載のプランジャ型電磁石。
(2) The plunger type electromagnet according to claim 1, wherein a magnetic plate is provided at one end of the inner side surface of the cylinder.
(3)前記固定鉄心及び可動鉄心は、相対する磁極部の
一方を軸方向断面が凹状に、磁極部の他方を軸方向断面
が凸状となるように形成し、凹状部と凸状部を挿脱変移
自在に配置した特許請求の範囲第1項記載のプランジャ
型電磁石。
(3) The fixed iron core and the movable iron core are formed such that one of the opposing magnetic pole parts has a concave axial cross section and the other magnetic pole part has a convex axial cross section, and the concave part and the convex part are formed. A plunger-type electromagnet according to claim 1, which is arranged so as to be freely inserted and removed.
(4)前記固定鉄心と可動鉄心は、解放時に両鉄心の離
隔距離を比較的小さくし、吸着時に非吸着端側の離隔距
離が前記解放時の離隔距離よりも大となるように、前記
可動鉄心の軸方向長さを選定してなる特許請求の範囲第
1項記載のプランジャ型電磁石。
(4) The fixed core and the movable core are arranged such that the distance between the two cores is relatively small when they are released, and the distance between the two cores when they are attracted is larger than the distance when they are released. A plunger type electromagnet according to claim 1, wherein the axial length of the iron core is selected.
JP60168241A 1985-07-29 1985-07-29 Plunger type electromagnet Pending JPS6229111A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60168241A JPS6229111A (en) 1985-07-29 1985-07-29 Plunger type electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60168241A JPS6229111A (en) 1985-07-29 1985-07-29 Plunger type electromagnet

Publications (1)

Publication Number Publication Date
JPS6229111A true JPS6229111A (en) 1987-02-07

Family

ID=15864376

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60168241A Pending JPS6229111A (en) 1985-07-29 1985-07-29 Plunger type electromagnet

Country Status (1)

Country Link
JP (1) JPS6229111A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007227766A (en) * 2006-02-24 2007-09-06 Toshiba Corp Electromagnetic actuator

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58158904A (en) * 1982-03-16 1983-09-21 Matsushita Electric Ind Co Ltd Self-holding type solenoid
JPS5913307A (en) * 1982-07-14 1984-01-24 Matsushita Electric Works Ltd Thin polarized solenoid

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58158904A (en) * 1982-03-16 1983-09-21 Matsushita Electric Ind Co Ltd Self-holding type solenoid
JPS5913307A (en) * 1982-07-14 1984-01-24 Matsushita Electric Works Ltd Thin polarized solenoid

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007227766A (en) * 2006-02-24 2007-09-06 Toshiba Corp Electromagnetic actuator

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