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JPH071737B2 - Polarized electromagnet - Google Patents
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JPH071737B2 - Polarized electromagnet - Google Patents

Polarized electromagnet

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Publication number
JPH071737B2
JPH071737B2 JP62228859A JP22885987A JPH071737B2 JP H071737 B2 JPH071737 B2 JP H071737B2 JP 62228859 A JP62228859 A JP 62228859A JP 22885987 A JP22885987 A JP 22885987A JP H071737 B2 JPH071737 B2 JP H071737B2
Authority
JP
Japan
Prior art keywords
magnetic pole
yoke
piece
permanent magnet
magnetic
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.)
Expired - Lifetime
Application number
JP62228859A
Other languages
Japanese (ja)
Other versions
JPS6472510A (en
Inventor
洋一 横山
博昭 浜口
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP62228859A priority Critical patent/JPH071737B2/en
Publication of JPS6472510A publication Critical patent/JPS6472510A/en
Publication of JPH071737B2 publication Critical patent/JPH071737B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔従来分野〕 この発明は、シングル型リレー等に適用される有極電磁
石に関するものである。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a polarized electromagnet applied to a single type relay or the like.

〔背景技術〕[Background technology]

第8図および第9図に示すように、両端部を第1の磁極
部53a,53bとした第1の磁極片51と両端部を第2の磁極
部54a,54bとした第2の磁極片52とを相対向し第1の磁
極片51と第2の磁極片52との間に永久磁石50を介在した
永久磁石部55と、第1の磁極部53a,53bと第2の磁極部5
4a,54bとの間に両端部56a,56bを有するヨーク57の中間
部にコイル58を巻装したコイル部59とを備え、永久磁石
部55およびコイル部59のいずれか一方を他方に対して回
動自在に構成するとともに、一方の第1の磁極部53aの
ヨーク57の端部56aに対向する対向面積を第1の磁極部5
3aに対向する第2の磁極部54aよりも小さくした有極電
磁石がある。
As shown in FIGS. 8 and 9, a first magnetic pole piece 51 whose both ends are first magnetic pole portions 53a and 53b and a second magnetic pole piece whose both ends are second magnetic pole portions 54a and 54b. 52 facing each other, the permanent magnet portion 55 having the permanent magnet 50 interposed between the first magnetic pole piece 51 and the second magnetic pole piece 52, the first magnetic pole portions 53a and 53b, and the second magnetic pole portion 5
4a, 54b and a coil portion 59 having a coil 58 wound around the middle portion of a yoke 57 having both end portions 56a, 56b between them and one of the permanent magnet portion 55 and the coil portion 59 with respect to the other. The first magnetic pole portion 5 has a facing area facing the end portion 56a of the yoke 57 of the one first magnetic pole portion 53a while being rotatable.
There is a polarized electromagnet that is smaller than the second magnetic pole portion 54a facing 3a.

この有極電磁石は、第1の磁極部53a、53bおよび第2の
磁極部54a,54bの対向面積をすべて同じにした双安定型
から、第1の磁極部53aの対向面積をたとえば磁極部53a
の一部を切断することにより他よりも小さくしたもので
あり、たとえば接点部(図示せず)のばね荷重とのマッ
チングを図ることにより、ヨーク57の端部56aと第2の
磁極部54aが接近した状態を安定状態とするシングル型
の有極電磁石を容易に実現できるものである。
This polarized electromagnet is a bistable type in which the facing areas of the first magnetic pole portions 53a and 53b and the second magnetic pole portions 54a and 54b are all the same, and the facing area of the first magnetic pole portion 53a is, for example, the magnetic pole portion 53a.
Is cut by cutting a part thereof to make it smaller than the other. For example, by matching the spring load of a contact portion (not shown), the end portion 56a of the yoke 57 and the second magnetic pole portion 54a are It is possible to easily realize a single-type polarized electromagnet that brings the approaching state into a stable state.

しかしながら、この有極電磁石は、安定状態からコイル
58の励磁時に対向面積の小さい第1の磁極部53aにヨー
ク57の端部56aが接近する方向に回動するため、磁気抵
抗が大きく吸引力が小さくなるとともに効率が悪くなる
という欠点があった。
However, this polarized electromagnet is
When the magnet 58 is excited, the end 56a of the yoke 57 rotates in the direction in which the end 56a of the yoke 57 approaches the first magnetic pole portion 53a having a small opposing area, which has a drawback that the magnetic resistance is large, the attractive force is small, and the efficiency is low. .

すなわち、第9図において、Q1は双安定型の無励磁吸引
力曲線、Q2は同じく励磁吸引力曲線であり、Q3は第8図
のシングル型の有極電磁石の無励磁吸引曲線、Q4は励磁
吸引力曲線、Q5は接点部のばね荷重であり、励磁吸引力
曲線Q4とばね荷重Q5との差が小さくなっている。
That is, in FIG. 9, Q 1 is a bistable-type non-exciting attraction force curve, Q 2 is also an exciting attraction force curve, Q 3 is a non-excitation attraction curve of the single-type polarized electromagnet in FIG. Q 4 is the excitation attraction force curve, Q 5 is the spring load of the contact point, and the difference between the excitation attraction force curve Q 4 and the spring load Q 5 is small.

〔発明の目的〕[Object of the Invention]

この発明の目的は、励磁した場合の吸引力を大きくする
ことができ効率よくすることができる有極電磁石を提供
することである。
An object of the present invention is to provide a polarized electromagnet that can increase the attractive force when excited and can be made efficient.

〔発明の開示〕[Disclosure of Invention]

この発明の有極電磁石は、対向面積を小さくした第1の
磁極部に対向するヨークの端部および第2の磁極部の少
なくともいずれか一方に補助片を設けて、コイルの励磁
時に補助片,ヨークおよび第2の磁極片からなる閉磁路
を形成したものである。
In the polarized electromagnet of the present invention, an auxiliary piece is provided on at least one of the end portion of the yoke and the second magnetic pole portion facing the first magnetic pole portion whose facing area is small, and the auxiliary piece is provided when the coil is excited. A closed magnetic circuit including a yoke and a second magnetic pole piece is formed.

この発明の構成によれば、コイルの励磁時に前記閉磁路
を形成する補助片により、回動側となるコイル部または
永久磁石部をその動作方向と同方向に吸引するため、励
磁時の吸引力を増大することができ効率よくすることが
できる。
According to the configuration of the present invention, since the coil portion or the permanent magnet portion on the rotating side is attracted in the same direction as the operation direction by the auxiliary piece that forms the closed magnetic path when the coil is excited, the attraction force at the time of excitation Can be increased and efficiency can be improved.

実施例 この発明の第1の実施例を第1図ないし第4図に基づい
て説明する。すなわち、この有極電磁石は、永久磁石部
1と、コイル部2からなる。
Embodiments A first embodiment of the present invention will be described with reference to FIGS. 1 to 4. That is, this polar electromagnet is composed of the permanent magnet portion 1 and the coil portion 2.

永久磁石部1は、両端部を第1の磁極部6a,6bとした第
1の磁極片4と両端部を第2の磁極部7a,7bとした第2
の磁極片5とを相対向し第1の磁極片4と第2の磁極片
5との間に永久磁石3を介在している。N,Sは永久磁石
3の磁極である。
The permanent magnet portion 1 has a first magnetic pole piece 4 whose both ends are first magnetic pole portions 6a and 6b and a second magnetic pole portion 7a and 7b whose both ends are second magnetic pole portions 7a and 7b.
And the permanent magnet 3 is interposed between the first magnetic pole piece 4 and the second magnetic pole piece 5. N and S are magnetic poles of the permanent magnet 3.

永久磁石部1はコイル部2に対して回動自在に構成され
る。たとえば第1図および第2図のように永久磁石3の
中央位置に軸10を立設し、軸10を軸受(図示せず)で軸
支する。また一方の第1の磁極部6aの対向面積をこれに
対向する第2の磁極部7aの対向面積よりも小さくしてい
る。
The permanent magnet part 1 is configured to be rotatable with respect to the coil part 2. For example, as shown in FIGS. 1 and 2, the shaft 10 is erected at the center of the permanent magnet 3, and the shaft 10 is supported by bearings (not shown). Further, the facing area of one of the first magnetic pole portions 6a is made smaller than the facing area of the second magnetic pole portion 7a which faces the first magnetic pole portion 6a.

コイル部2は、表1の磁極部6a,6bと第2の磁極部7a,7b
との間に両端部11a,11bを有するヨーク8の中間部にコ
イル9を巻装している。
The coil portion 2 is composed of the magnetic pole portions 6a and 6b and the second magnetic pole portions 7a and 7b shown in Table 1.
A coil 9 is wound around an intermediate portion of a yoke 8 having both end portions 11a and 11b between and.

そして補助片12が、対向面積を小さくした第1の磁極部
6aに対向するヨーク8の端部11aに設けられ、補助片12
と,ヨーク8と,第2の磁極片5とによりコイル9の励
磁時の閉磁路を形成するように、補助片12の先端部12a
を第2の磁極部7aの第1の磁極部6aの対向側と反対側に
延出している。
And the auxiliary piece 12 is the first magnetic pole part having a small facing area.
The auxiliary piece 12 is provided at the end 11a of the yoke 8 facing the 6a.
, The yoke 8 and the second magnetic pole piece 5 form a closed magnetic path when the coil 9 is excited, so that the tip portion 12a of the auxiliary piece 12 is formed.
Of the second magnetic pole portion 7a extends to the opposite side of the first magnetic pole portion 6a from the opposite side.

第3図はこの有極電磁石の等価回路を示し、 Rg1,Rg2は第2図に示すように、ヨーク8の両端部11a,
11bと第2の磁極部7a,7bとの間の空隙の磁気抵抗、R
g3,Rg4はヨーク8の両端部11a,11bと第1の磁極部6a,6
bとの間の空隙の磁気抵抗、Rg5は第2の磁極部7aと補助
片12の先端部12aとの間の空隙の磁気抵抗である。
FIG. 3 shows an equivalent circuit of this polarized electromagnet, and Rg 1 and Rg 2 are, as shown in FIG.
Magnetic resistance of the air gap between 11b and the second magnetic pole portions 7a, 7b, R
g 3 and Rg 4 are both end portions 11a and 11b of the yoke 8 and the first magnetic pole portions 6a and 6
Rg 5 is the magnetic resistance of the air gap between the second magnetic pole portion 7a and the tip 12a of the auxiliary piece 12, and Rg 5 is the magnetic resistance of the air gap between the second magnetic pole portion 7a and the tip 12a of the auxiliary piece 12.

無励磁状態では、第2の磁極部7a,7bに磁極Nが現れ、
第1の磁極部6a,6bに磁極Sが現れる。そして、安定状
態では永久磁石3の磁束が第3図の破線矢印の経路Φ1
を流れる。すなわち、第1図において第2の磁極部7aが
ヨーク8の端部11aに接近し第1の磁極部6bが端部11bに
接近して、磁極N→第2の磁極片5→第2の磁極部7a→
磁気抵抗Rg1の空隙→ヨーク8の端部11a→ヨーク8→ヨ
ーク8の端部11b→磁気抵抗Rg3の空隙→第1の磁極片4
の第1の磁極部6b→第1の磁極片4→磁極Sを流れる。
In the non-excitation state, the magnetic pole N appears on the second magnetic pole portions 7a and 7b,
The magnetic pole S appears on the first magnetic pole portions 6a and 6b. Further, in the stable state, the magnetic flux of the permanent magnet 3 is the path Φ 1 indicated by the broken line arrow in FIG.
Flowing through. That is, in FIG. 1, the second magnetic pole portion 7a approaches the end portion 11a of the yoke 8 and the first magnetic pole portion 6b approaches the end portion 11b, so that the magnetic pole N → the second magnetic pole piece 5 → the second magnetic pole piece 5 Magnetic pole part 7a →
Gap of magnetic resistance Rg 1 → End 11a of yoke 8 → Yoke 8 → End 11b of yoke 8 → Gap of magnetic resistance Rg 3 → First pole piece 4
Flowing from the first magnetic pole portion 6b to the first magnetic pole piece 4 to the magnetic pole S.

一方、第2の磁極部7bが端部11bに接近し第1の磁極部6
aが端部11aに接近している場合の磁束の経路Φ2は第3
図の矢印のようになる。しかし、第1の磁極部6aの対向
面積が小さく磁気抵抗Rg4が大きいため、磁束は小さく
吸引力が小さい。このときの吸引力を接点部(図示せ
ず)のばね荷重よりも小さく設定すると、永久磁石部1
は安定せず前記安定状態に復帰するので、シングル動作
となる。なおこの場合、補助片12と第2の磁極部7aとが
接近するが、ヨーク8の端部11bは第2の磁極部7bに接
近するため永久磁石3による吸引力は発生しない。
On the other hand, the second magnetic pole portion 7b approaches the end portion 11b, and the first magnetic pole portion 6b
The path Φ 2 of the magnetic flux when a is close to the end 11a is the third
It becomes like the arrow in the figure. However, since the facing area of the first magnetic pole portion 6a is small and the magnetic resistance Rg 4 is large, the magnetic flux is small and the attractive force is small. If the attraction force at this time is set to be smaller than the spring load of the contact portion (not shown), the permanent magnet portion 1
Is not stable and returns to the stable state, so that single operation is performed. In this case, the auxiliary piece 12 and the second magnetic pole portion 7a approach each other, but the end portion 11b of the yoke 8 approaches the second magnetic pole portion 7b, so that the attraction force by the permanent magnet 3 is not generated.

また第4図は吸引力特性曲線を示し、P1は無励磁吸引力
曲線、P2はばね荷重である。第2の磁極部7aが端部11a
に接近する位置では反対向きに吸引力よりも大きいばね
荷重P2が加わるため、永久磁石部位置が安定位置へ復帰
することがわかる。
Further, FIG. 4 shows an attractive force characteristic curve, P 1 is a non-excitation attractive force curve, and P 2 is a spring load. The second magnetic pole portion 7a is the end portion 11a
It can be seen that the spring load P 2 larger than the attractive force is applied in the opposite direction at the position approaching, and the permanent magnet portion position returns to the stable position.

つぎに、無励磁の安定状態で、コイル9にヨーク8を通
過する無励磁の経路Φ1の磁束の方向と反対向きにコイ
ル9を励磁するように電流を流すと、第1の磁極部6bお
よび第2の磁極部7aに現れている磁極N,Sと同極の磁極
がヨーク8の両端部11a,11bにそれぞれ現れるので反発
力を生じ、永久磁石部1は軸10を中心に回転して、ヨー
ク8の両端部11a,11bが第1の磁極部6aおよび第2の磁
極部7bに吸引され、磁束は第3図の経路Φ2のように流
れる。またヨーク8→端部11a→補助片12→補助片12の
先端部12a→磁気抵抗Rg5の空隙→第2の磁極部7a→第2
の磁極片5→第2の磁極部7b→磁気抵抗Rg2の空隙→端
部11b→ヨーク8の経路Φ3を閉磁路として磁束が流れる
ので、永久磁石部1の前記回転方向と同方向に補助片12
による吸引力が永久磁石部1に発生する。
Next, in the stable state of non-excitation, when a current is applied to the coil 9 so as to excite the coil 9 in the direction opposite to the direction of the magnetic flux of the non-excitation path Φ 1 passing through the yoke 8, the first magnetic pole portion 6b And magnetic poles having the same polarity as the magnetic poles N and S appearing on the second magnetic pole portion 7a appear on both end portions 11a and 11b of the yoke 8, respectively, so that a repulsive force is generated and the permanent magnet portion 1 rotates about the shaft 10. Both ends 11a and 11b of the yoke 8 are attracted to the first magnetic pole portion 6a and the second magnetic pole portion 7b, and the magnetic flux flows as the path Φ 2 in FIG. Further, the yoke 8 → the end 11a → the auxiliary piece 12 → the tip 12a of the auxiliary piece 12 → the gap of the magnetic resistance Rg 5 → the second magnetic pole portion 7a → the second
Magnetic pole piece 5 → second magnetic pole portion 7b → gap of magnetic resistance Rg 2 → end portion 11b → the magnetic flux flows through the path Φ 3 of the yoke 8 as a closed magnetic path, so that it is in the same direction as the rotation direction of the permanent magnet portion 1. Auxiliary piece 12
Is generated in the permanent magnet section 1.

第4図のP3はこのときの励磁吸引力曲線である。P4は補
助片12がない場合の前記励磁吸引力曲線Q4と同じ励磁吸
引力曲線であり、励磁吸引力曲線P4が大きくなっている
ことがわかる。
P 3 in FIG. 4 is an exciting force curve at this time. P 4 is the same excitation attraction force curve as the excitation attraction force curve Q 4 when the auxiliary piece 12 is not provided, and it can be seen that the excitation attraction force curve P 4 is large.

なお、コイル9の励磁を解くと前記吸引力が発生しなく
なるので、接点部のばね荷重P2により永久磁石部1は無
励磁の安定状態に復帰する。
Since the attraction force is not generated when the coil 9 is de-excited, the permanent magnet portion 1 returns to the non-excited stable state by the spring load P 2 of the contact portion.

この実施例によれば、コイル9を励磁した場合に補助片
12と,ヨーク8と,第2の磁極片5からなる閉磁路が形
成され、補助片12と第2の磁極部7穿設との間および第
2の磁極部7bと端部11bとの間に発生する吸引力が、端
部11aと第1の磁極部6aとを接近させる吸引力に加わる
ため、励磁時の吸引力が増大するとともに効率がよくな
る。
According to this embodiment, when the coil 9 is excited, the auxiliary piece
12, a yoke 8 and a second magnetic pole piece 5 form a closed magnetic path, and between the auxiliary piece 12 and the second magnetic pole portion 7 and between the second magnetic pole portion 7b and the end portion 11b. The attraction force generated at the time is added to the attraction force that causes the end portion 11a and the first magnetic pole portion 6a to approach each other, so that the attraction force at the time of excitation is increased and the efficiency is improved.

この発明の第2の実施例を第5図に示す。すなわち、こ
の有極電磁石は、第1の実施例において、補助片12を第
2の磁極部7aに設け、その先端部12aを第1の磁極部6a
側に位置したものである。第1の実施例と同様に励磁時
にはヨーク8,補助片12および磁極片5の経路Φ3で磁束
が発生し、ヨーク8の端部11aと補助片12の先端部12aと
の間、および第2の磁極部7bと端部11bとの間に吸引力
が発生する。このため、第4図の励磁吸引力曲線P3と同
じ吸引力を得ることができる。その他は第1の実施例と
同様である。
A second embodiment of the present invention is shown in FIG. That is, in this polarized electromagnet, in the first embodiment, the auxiliary piece 12 is provided on the second magnetic pole portion 7a, and the tip portion 12a of the auxiliary piece 12 is provided on the first magnetic pole portion 6a.
It is located on the side. Similar to the first embodiment, during excitation, magnetic flux is generated in the path Φ 3 of the yoke 8, the auxiliary piece 12 and the magnetic pole piece 5, between the end portion 11a of the yoke 8 and the tip portion 12a of the auxiliary piece 12, and An attractive force is generated between the second magnetic pole portion 7b and the end portion 11b. Therefore, the same attractive force as the exciting attractive force curve P 3 in FIG. 4 can be obtained. Others are the same as those in the first embodiment.

この発明の第3の実施例を第6図に示す。すなわち、こ
の有極電磁石は、第1の実施例において、永久磁石部1
を固定し、コイル部2の中央部に軸部14を設けて、コイ
ル部2を永久磁石部1に対して回動可能としたものであ
る。この実施例の無励磁および励磁動作ではコイル部2
が永久磁石部1に対して回動するほかは第1の実施例と
同様である。
A third embodiment of the present invention is shown in FIG. That is, this polarized electromagnet is the same as that of the permanent magnet portion 1 in the first embodiment.
Is fixed and a shaft portion 14 is provided at the center of the coil portion 2 so that the coil portion 2 can be rotated with respect to the permanent magnet portion 1. In the non-excitation and excitation operations of this embodiment, the coil unit 2
Is the same as that of the first embodiment except that it rotates with respect to the permanent magnet section 1.

この発明の第4の実施例を第7図に示す。すなわち、こ
の有極電磁石は、第2の実施例において、永久磁石部1
を固定し、コイル部2の中央部に軸部14を設けて、コイ
ル部2を永久磁石部1に対して回動可能としたものであ
る。この実施例の無励磁および励磁動作ではコイル部2
が永久磁石部1に対して回動するほかは第2の実施例と
同様である。
A fourth embodiment of the present invention is shown in FIG. That is, this polarized electromagnet is the same as that of the permanent magnet portion 1 in the second embodiment.
Is fixed and a shaft portion 14 is provided at the center of the coil portion 2 so that the coil portion 2 can be rotated with respect to the permanent magnet portion 1. In the non-excitation and excitation operations of this embodiment, the coil unit 2
Is the same as the second embodiment except that it rotates with respect to the permanent magnet section 1.

なお、補助片12はたとえば第1の実施例ではヨーク8に
設け、第2の実施例では第2の磁極部7aに設けたが、両
方に設けてもよい。
The auxiliary piece 12 is provided on the yoke 8 in the first embodiment and on the second magnetic pole portion 7a in the second embodiment, but may be provided on both.

〔発明の効果〕〔The invention's effect〕

この発明の有極電磁石によれば、対向面積を小さくした
第1の磁極部に対向するヨークの端部および第2の磁極
部の少なくともいずれか一方に補助片を設けて、コイル
の励磁時に補助片,ヨークおよび第2の磁極片からなる
閉磁路を形成したため、コイルの励磁時に回動側となる
コイル部または永久磁石部の動作方向と同方向に補助片
による吸引力が発生する。したがって、励磁時の吸引力
を増大することができ効率よくすることができるという
効果がある。
According to the polarized electromagnet of the present invention, an auxiliary piece is provided on at least one of the end portion of the yoke and the second magnetic pole portion facing the first magnetic pole portion having a small facing area to assist the excitation of the coil. Since the closed magnetic circuit formed by the one piece, the yoke, and the second magnetic pole piece is formed, when the coil is excited, an attractive force is generated by the auxiliary piece in the same direction as the operating direction of the coil portion or the permanent magnet portion on the rotating side. Therefore, there is an effect that the attractive force at the time of excitation can be increased and the efficiency can be improved.

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

第1図はこの発明の第1の実施例の斜視図、第2図はそ
の平面略図、第3図は等価磁気回路図、第4図は吸引力
特性図、第5図は第2の実施例の斜視図、第6図は第3
の実施例の斜視図、第7図は第4の実施例の斜視図、第
8図は従来例の斜視図、第9図はその吸引力特性図であ
る。 1……永久磁石部、2……コイル部、3……永久磁石、
4……第1の磁極片、5……第2の磁極片、6a,6b……
第1の磁極部、7a,7b……第2の磁極部、8……ヨー
ク、9……コイル、11a,11b……両端部、12……補助片
FIG. 1 is a perspective view of a first embodiment of the present invention, FIG. 2 is a schematic plan view thereof, FIG. 3 is an equivalent magnetic circuit diagram, FIG. 4 is an attraction force characteristic diagram, and FIG. 5 is a second embodiment. FIG. 6 is a perspective view of an example, and FIG.
FIG. 7 is a perspective view of the fourth embodiment, FIG. 8 is a perspective view of a conventional example, and FIG. 9 is a suction force characteristic diagram thereof. 1 ... permanent magnet part, 2 ... coil part, 3 ... permanent magnet,
4 ... 1st pole piece, 5 ... 2nd pole piece, 6a, 6b ...
1st magnetic pole part, 7a, 7b ... 2nd magnetic pole part, 8 ... Yoke, 9 ... Coil, 11a, 11b ... Both ends, 12 ... Auxiliary piece

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】両端部を第1の磁極部とした第1の磁極片
と両端部を第2の磁極部とした第2の磁極片とを相対向
し前記第1の磁極片と第2の磁極片との間に永久磁石を
介在した永久磁石部と、前記第1の磁極部と第2の磁極
部との間に両端部を有するヨークの中間部にコイルを巻
装したコイル部とを備え、前記永久磁石部およびコイル
部のいずれか一方を他方に対して回動自在に構成すると
ともに、一方の前記第1の磁極部の前記ヨークの端部に
対向する対向面積を前記第1の磁極部に対向する第2の
磁極部よりも小さくした有極電磁石において、前記対向
面積を小さくした前記第1の磁極部に対向する前記ヨー
クの端部および前記第2の磁極部の少なくともいずれか
一方に補助片を設けることにより、前記コイルの励磁時
に前記補助片,前記ヨークおよび前記第2の磁極片から
なる閉磁路を形成したことを特徴とする有極電磁石。
1. A first magnetic pole piece whose both ends are first magnetic pole portions and a second magnetic pole piece whose both end portions are second magnetic pole portions are opposed to each other, and the first magnetic pole piece and the second magnetic pole piece are opposed to each other. A permanent magnet portion having a permanent magnet interposed between the magnetic pole piece and a coil portion in which a coil is wound around an intermediate portion of a yoke having both ends between the first magnetic pole portion and the second magnetic pole portion. One of the permanent magnet portion and the coil portion is configured to be rotatable with respect to the other, and the facing area facing the end portion of the yoke of the one first magnetic pole portion is set to the first area. In a polarized electromagnet smaller than the second magnetic pole portion facing the magnetic pole portion, at least one of the end of the yoke and the second magnetic pole portion facing the first magnetic pole portion having the smaller facing area. By providing an auxiliary piece on either side, the auxiliary piece and front Polarized electromagnet, characterized in that the formation of the yoke and the closed magnetic circuit consisting of the second pole piece.
JP62228859A 1987-09-11 1987-09-11 Polarized electromagnet Expired - Lifetime JPH071737B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62228859A JPH071737B2 (en) 1987-09-11 1987-09-11 Polarized electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62228859A JPH071737B2 (en) 1987-09-11 1987-09-11 Polarized electromagnet

Publications (2)

Publication Number Publication Date
JPS6472510A JPS6472510A (en) 1989-03-17
JPH071737B2 true JPH071737B2 (en) 1995-01-11

Family

ID=16883001

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62228859A Expired - Lifetime JPH071737B2 (en) 1987-09-11 1987-09-11 Polarized electromagnet

Country Status (1)

Country Link
JP (1) JPH071737B2 (en)

Also Published As

Publication number Publication date
JPS6472510A (en) 1989-03-17

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