JPS61129804A - Bistable rotary solenoid - Google Patents

Bistable rotary solenoid

Info

Publication number
JPS61129804A
JPS61129804A JP25247084A JP25247084A JPS61129804A JP S61129804 A JPS61129804 A JP S61129804A JP 25247084 A JP25247084 A JP 25247084A JP 25247084 A JP25247084 A JP 25247084A JP S61129804 A JPS61129804 A JP S61129804A
Authority
JP
Japan
Prior art keywords
rotor
magnetic core
plane
facing
permanent magnet
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
JP25247084A
Other languages
Japanese (ja)
Other versions
JPH0219608B2 (en
Inventor
Yasuo Ueno
康男 上野
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.)
Kokusai Gijutsu Kaihatsu Co Ltd
Original Assignee
Kokusai Gijutsu Kaihatsu 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 Kokusai Gijutsu Kaihatsu Co Ltd filed Critical Kokusai Gijutsu Kaihatsu Co Ltd
Priority to JP25247084A priority Critical patent/JPS61129804A/en
Publication of JPS61129804A publication Critical patent/JPS61129804A/en
Publication of JPH0219608B2 publication Critical patent/JPH0219608B2/ja
Granted legal-status Critical Current

Links

Classifications

    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F7/00—Magnets
    • H01F7/06—Electromagnets; Actuators including electromagnets
    • H01F7/08—Electromagnets; Actuators including electromagnets with armatures
    • H01F7/14—Pivoting armatures
    • H01F7/145—Rotary electromagnets with variable gap

Abstract

PURPOSE:To decrease the electric power required by providing a phase difference to the changes in the facing areas of the magnetic poles for the rotor and the magnetic core for the stator which occur along with the revolution of the rotor. CONSTITUTION:While the rotor 9 rotates for -30--90 deg., the outside plane 8'1 on the permanent magnet 8' is facing the whole plane of the magnetic core 4' without changing its facing area even if the rotor 9 rotates a little bit. However, the outside plane 8-1 on the permanent magnet 8 is facing the magnetic core 4 and the auxiliary, magnetic core 2. Therefore, when the power is conducted to the coil so that the circular arc plane 4-1 will be the N pole, the rotor 9 rotates counterclockwise, resulting in that the rotatory power acting on the rotor 9 is in proportion to the alteration ratio of the facing area between the outside plane 8-1 on the permanent magnet 8 and the circular arc plane 4-1. Then, when the position of the rotor 9 is almost at the neutral point, a uniform rotatory power acts in proportion to the alteration ratio of the facing area between the circular arc planes 4-1 and 4'-1 on the iron cores 4 and 4' and the outside plane 8'-1 on the magnet 8'. When the rotor is in the position of +30 deg.-+90 deg., the rotatory power acts on the rotor 9 in proportion to the alteration ratio of the facing area between the outside plane 8-1 and the circular arc plane 4'-1.

Description

【発明の詳細な説明】 （イ）産業上の利用分野 本発明は動作時のみに電力を消費し、保持状態では電力
消費のない、アクチュエーターの一棟である双安定ロー
タリーソレノイドに関するものであり、特に従来のもの
に比べて小型で消費電力が少なく、又作動力が大きく保
持力の大きさを任意に設定し得る双安定ロータリーンレ
ノイドに関するものである。[Detailed description of the invention] (a) Industrial application field The present invention relates to a bistable rotary solenoid, which is a part of an actuator, which consumes power only during operation and does not consume power when in a holding state. In particular, the present invention relates to a bistable rotary lean renoids that are smaller in size and consume less power than conventional ones, have a large operating force, and can arbitrarily set the magnitude of the holding force.

（ロ）従来の技術 従来、双安定ソレノイドとしては、一般的には直動式の
ものが多く、動作範囲の両端においてプランジャーを永
久磁石の磁力により保持し、動作時には２つのコイルに
通電することにより、一方のコイルによる励磁によって
前記永久磁石による保持吸引力を打消し、他方のコイル
による励磁作　　　用によりプランジャーを他方に吸引
でる形式のものが用いられていたう 又、ロータリーンレノイドで双方向に回転し得るものと
してハ、する一つの半径方向に着磁された円形の永久磁
石によって形成したローターと、それに対向して設けた
ステーターのコイルに通電することにより動作するもの
がるる。(B) Conventional technology Conventionally, most bistable solenoids are of the direct-acting type, in which the plunger is held by the magnetic force of a permanent magnet at both ends of the operating range, and two coils are energized during operation. Due to this, the holding force of the permanent magnet is canceled by the excitation of one coil, and the plunger is attracted to the other by the excitation of the other coil. There is a rotor that can rotate in both directions, and is operated by energizing a rotor formed by a circular permanent magnet magnetized in the radial direction and a stator coil placed opposite the rotor.

前者は通常のンレノイドの吸引力がストロークの２乗に
反比例する上、一方のコイルが保持吸引力を打消す為に
使用されている為、電力のわりに初期動作吸引力はかな
り小さなものとなる。−例として、外形１８Ｘ１８Ｘ５
０ｍｍ、５Ｗの電力でストロークｋ　４ｍｍとした場合
、良好な性能のものでも初期吸引力は５０ｇｒ程度であ
る。父、コイルに印加でる電力が犬きてぎると永久磁石
の吸引力を打消した上でいわゆる再吸着現像が生じ、初
期吸引力は増加しない。In the former case, the attraction force of a normal renoid is inversely proportional to the square of the stroke, and one coil is used to cancel the holding attraction force, so the initial operation attraction force is quite small compared to the electric power. -For example, external size 18X18X5
When the stroke k is 4 mm with a power of 0 mm and 5 W, the initial suction force is about 50 gr even with good performance. If the electric power applied to the coil becomes too strong, the attraction force of the permanent magnet will be canceled and so-called re-adsorption development will occur, and the initial attraction force will not increase.

又、後者は、回転範囲の中央部ではトルクが大きいが両
端部では小さく、保持力を打消す為の電力を加算すると
、有効な動作力は極めて小さい。Furthermore, in the latter case, the torque is large at the center of the rotation range, but small at both ends, and when electric power is added to cancel the holding force, the effective operating force is extremely small.

−例として、外形２６Ｘ２６Ｘ５０ｍｍ、５Ｗの電力で
回転角変１２０°とした場合の初期駆動トルクは、４０
ｇｒ・Ｃｍ程度である。- As an example, when the outer diameter is 26 x 26 x 50 mm and the rotation angle is 120 degrees with 5 W of power, the initial driving torque is 40
It is approximately gr.Cm.

（−ウ　　発明が解決しようとでる問題点本発明はロー
ターの回転にともなうローターの磁極とステーターの磁
心との対向面積の変化に位相差？設けることによジ、上
記従来のンレノイドと同程度の力を出てのに必要な電力
を数分の−にすることの出来る双安定ロータリーソレノ
イド紮提供するものである。(-C) Problems to be Solved by the Invention The present invention provides a phase difference in the change in the facing area between the rotor's magnetic poles and the stator's magnetic core as the rotor rotates, thereby achieving The present invention provides a bistable rotary solenoid which can reduce the power required for output to several minutes.

に）問題点全解決するための手段 以下図と共にその構造整説明する。) Means to solve all problems The structure will be explained below with reference to the drawings.

第１図は本発明の一実施例の構造を示す正断面図、第２
図はその正断面図である。Fig. 1 is a front cross-sectional view showing the structure of one embodiment of the present invention;
The figure is a front sectional view thereof.

第１図及び第２図において、コの字形をしたヨーク／の
内側には中央に補助磁心コと両端に鉄心３及び！を介し
て磁心ダ、ダが設けられ、鉄心３及び！には夫々コイル
！、ｊが設けられている。In Figures 1 and 2, the inside of the U-shaped yoke has an auxiliary magnetic core in the center and iron cores 3 at both ends. The magnetic cores 3 and ! are provided through the magnetic cores 3 and ! Each has a coil! , j are provided.

補助磁心λ及び磁心ダ及びに′は点０″ｆ：中心とでる
円弧面−一／、グー／、４ｔ′−／を有しステーターを
形成している。又、点Ｏを細心とするシャフト乙はヨー
ク／に固定された軸受部７に対して回転自在に嵌合して
おり、該シャフト乙には円弧状の２つの永久磁石？及び
ｌｔ−有するローターヂが固着されている。永久磁石？
は円弧状の外面／−／がＳ極に個面♂−２がＮ極に層磁
され、永久磁石／′はその外面／’−／がＮ極に、内面
ｒ−コがＳ極に着磁されている。同、ヨーク／、補助磁
心２、鉄心３．！’、磁心ｇ、４ｔ’及びロータタは純
鉄等の磁性材料で作られている。又、／Ｑは軸受部７に
固着されたストッパー、／／ハこれに対応してローター
に固着されたストッパーであり、ロータータの回転角度
を１８０°以下に規制している。The auxiliary magnetic core λ and the magnetic cores Da and Ni' have circular arc surfaces -1/, Goo/, and 4t'-/ that come out from the point 0''f: center, forming a stator. The shaft O is rotatably fitted into a bearing part 7 fixed to the yoke, and a rotor having two circular arc-shaped permanent magnets and a rotor is fixed to the shaft O.
is an arc-shaped outer surface /-/ is magnetized to the S pole, and the individual surface ♂-2 is magnetized to the N pole, and the permanent magnet /' is magnetized so that its outer surface /'-/ is the N pole and the inner surface r- is the S pole. It is magnetized. Same, yoke/, auxiliary magnetic core 2, iron core 3. ! ', magnetic core g, 4t' and rotator are made of magnetic material such as pure iron. Further, /Q is a stopper fixed to the bearing portion 7, and //C is a corresponding stopper fixed to the rotor, which restricts the rotation angle of the rotator to 180° or less.

（ホ）作用 第３図は、本発明の双安定ロータリールノイドの動作状
態を示す模式正面図であジ、第４図は補助磁心コ及び磁
心グ及び夕′のローター９の永久磁石？及びｒとの対向
面積の変化を示すグラフである。(e) Operation FIG. 3 is a schematic front view showing the operating state of the bistable rotary lunoid of the present invention, and FIG. It is a graph showing the change in the facing area with and r.

第３図、第４図において、ローター９の回転角αを中央
に対して対称に左右に＋−９０°とすると、第３図（Ａ
）の場合のごとくロータータが一３０°乃至−９０°回
転している状態では永久磁石どの外面ｌ−／は磁心ダ′
の全面と対向しており、ローター？が多少回転しても対
向面積の変化はない。しかし永久磁石？の外ｒｋＪ／−
／ｌｄ磁心グ及び補助Ｈ心λと対向しておジ、ローター
タが回転すると各々の対向面積は相互に増減する。従っ
てコイルタ及びダに磁心ダの円弧面クー／がＮ極になる
様通電すれば、永久磁石ｒの外面？−／のＳ極と対向面
積が増加する方向に引合い、ローター？は反時計方向に
回転でる。又、その場合補助磁心コの円筒面と外面？−
／との対向面積は減少するので、ヨーク／を流れる総磁
束は変化せず、永久磁石ｌの外面／’−／と磁心ダの円
弧面り′−／の対向面の磁束密度は変化しない。この様
な状態にあるので、σ−タータに働く回転力は外面／−
／と円弧面グー／との対向面積の変化率に比例したもの
となり、電流が一定ならばローター９の位置が一９０°
から一３０°までの間でほぼ、一定となる。In FIGS. 3 and 4, if the rotation angle α of the rotor 9 is set to +-90° left and right symmetrically with respect to the center, then FIG.
), when the rotor is rotating from 130° to -90°, which outer surface l-/ of the permanent magnet is the magnetic core da'
It is facing the entire surface of the rotor? Even if it rotates a little, the opposing area does not change. But a permanent magnet? Outside rkJ/-
When the rotator rotates while facing the /ld magnetic core G and the auxiliary H core λ, the opposing areas of each increase and decrease. Therefore, if electricity is applied to the coils R and R so that the arcuate surface of the magnetic core R becomes the N pole, the outer surface of the permanent magnet r? The rotor attracts attention in the direction in which the facing area increases with the S pole of -/? rotates counterclockwise. Also, in that case, what about the cylindrical surface and outer surface of the auxiliary magnetic core? −
Since the area facing / decreases, the total magnetic flux flowing through the yoke / does not change, and the magnetic flux density on the facing surface between the outer surface /'-/ of the permanent magnet l and the arcuate surface '-/ of the magnetic core D does not change. In this state, the rotational force acting on the σ-tar is the outer surface/-
It is proportional to the rate of change in the opposing area between / and the circular arc surface /, and if the current is constant, the position of the rotor 9 will be 190°.
It remains almost constant between 1 and 30 degrees.

次に、第５図中）のごとくロータータの位置がほぼ中立
点にるる時は、ロータータの回転にともなう補助磁心コ
の円弧面コー／と外面／−／との対向面積の変化はない
。しかし、磁心体及びダの円弧面クー／及びクー／と、
永久磁石ｒの外面／’　−／との対向面積は相互に増減
でる。Next, when the position of the rotator is approximately at the neutral point as shown in FIG. However, the arcuate surfaces of the magnetic core and Da,
The area facing the outer surface /'-/ of the permanent magnet r increases and decreases with respect to each other.

従ッて、コイル！及び！に通電すればその通電方向によ
ジロータータには任意の方向の回転力が働き、その場合
ローター回転にともなう補助磁心２の円弧面２−／の磁
束密度の変化はない。この様な状態ではロータータには
、磁心グ及びダ′の円弧面ター／及びクー／の永久磁石
ｌの外面／’−／との対向面積の変化率に比例した一定
回転力が働く。従って、′電流が一定ならばロータータ
の位置が中立点の＋−３０°範囲ではほぼ一定の回転力
となる。Therefore, coil! as well as! When energized, a rotational force in an arbitrary direction acts on the gerotor depending on the direction of energization, and in this case, there is no change in the magnetic flux density of the arcuate surface 2-/ of the auxiliary magnetic core 2 as the rotor rotates. In this state, a constant rotational force is applied to the rotator in proportion to the rate of change in the opposing area of the arcuate surfaces of the magnetic cores G and D' and the outer surface /'-/ of the permanent magnet L. Therefore, if the current is constant, the rotational force will be approximately constant within the range of +-30 degrees from the neutral point of the rotator.

更に、嘉Ｓ図（Ｃ）においては、第５図（Ａ＞の場合と
反対に磁心グの円弧面クー／と永久磁石どの外面／’−
／との対向面積は変化せず、補助磁心λの円弧面λ−／
及び磁心ダの円弧面クー／と永久磁石♂の外面？−／と
の対向面積が相互に変化でる。Furthermore, in the KaS diagram (C), contrary to the case of FIG.
The area facing / does not change, and the arcuate surface λ−/ of the auxiliary magnetic core λ
And the arcuate surface of the magnetic core Da/and the outer surface of the permanent magnet ♂? -/The opposing area changes mutually.

この状態でコイル！及び！に通電すると、電流が一定な
らばロータータの位置が＋５０°から＋９０゜までの間
で一定の回転力を得ることが出来る。Coil in this state! as well as! If the current is constant, a constant rotational force can be obtained when the rotor position is between +50° and +90°.

以上の結果、本発明の双安定ロータリンレノイドは、−
９０°から＋９０°までの１８０°の間口−ターにほぼ
一定の回転力金量すことが出来る、尚、実際の場合磁束
の通りやすさ即ちパーミアンス値がローターが左右＋−
９０°位置が多少大きくなる為、この２点が安定点とな
り無通電の時にも一定の保持力を有し、その結果、いわ
ゆる双安定ロータリーソレノイドとしての機能を有する
ものとなる。As a result of the above, the bistable rotorinoid of the present invention has -
A nearly constant amount of rotational force can be applied to the rotor with a 180° frontage from 90° to +90°.In actuality, the ease with which magnetic flux passes, that is, the permeance value, is greater when the rotor is on the left or right side.
Since the 90° position is somewhat larger, these two points become stable points and maintain a constant holding force even when no current is applied, resulting in a so-called bistable rotary solenoid function.

第４図における線グー？、クー？、グー１１　　クーｒ
１　コーｒは夫々磁心ダと永久磁石？、りとｔ１ダと、
ｒ’Ｘ４ｔ’とｌ及び補助磁心２と永久磁石ｒとの対向
面積の変化を示すもの”であり、練Ｓはその総和を示す
ものである。線Ｓは一定値となり増減しないことが第４
図によって明らかとなる。The line in Figure 4? , Coo? , goo 11 cour
1. Is COR a magnetic core and a permanent magnet, respectively? , ri and t1 da,
r'
This becomes clear from the diagram.

（へ）実施例 第５図は、本発明の他の一実施例の構造を示す正断面図
であり、第６図はその磁心／４ｔ、　／４ｔ’及び補助
磁心コと永久磁石？及びｒとの対向面積の変化を示すグ
ラフでるる。(F) Embodiment FIG. 5 is a front sectional view showing the structure of another embodiment of the present invention, and FIG. 6 shows its magnetic cores /4t, /4t', auxiliary magnetic cores, and permanent magnets. A graph showing changes in the facing area with and r is shown.

第５図において、磁心／４を及び／４ｔ′は上方向に少
し大きく形成されている。従って、円弧面／クー／及び
／クー／と永久磁石♂及びｌとの対向面積は犬きくなり
、ロータータが左右に一９０°から＋９０°まで回転し
た場合の各対向面積の変化は第６図のごとくなり、ロー
タータの回転角の中央で最小となる。この様にすると中
央の中立点は完全な不安定点となり、動作途中この点で
停止することはない。In FIG. 5, magnetic cores /4 and /4t' are formed slightly larger in the upward direction. Therefore, the facing areas of the circular arc surfaces /Ku/ and /Ku/ and the permanent magnets ♂ and 1 become narrower, and the change in each facing area when the rotator rotates left and right from -90° to +90° is shown in Figure 6. It becomes minimum at the center of the rotation angle of the rotator. In this way, the central neutral point becomes a completely unstable point, and there is no stopping at this point during operation.

又、両端の保持力は増加し、この点での安定度は高まる
。但し、通電時の回転力は、両端でやや弱いものとなる
。しかし、総合的に見た場合、磁気回路としてのいわゆ
るギャップが小さく、効率が良い。測定結果では、外形
寸法が＋８ＸＩ８Ｘ４０のもので４３ｇｒＣｍのトルク
を出すのに必要な電力はわずか１〜１．３Ｗであり、従
来品に比べて４〜５倍の効率を示した。Also, the holding force at both ends is increased and the stability in this respect is increased. However, the rotational force when energized is somewhat weak at both ends. However, when viewed comprehensively, the so-called gap as a magnetic circuit is small and the efficiency is high. The measurement results showed that a product with external dimensions of +8XI8X40 required only 1 to 1.3 W of power to generate a torque of 43 grCm, which was 4 to 5 times more efficient than conventional products.

第７図はソレノイドの動作特性を示すグラフである。第
７図（Ａ）は従来の直動型双安定ソレノイド、第７図（
Ｂ）は従来の双安定ロータリーソレノイド、第７図（Ｃ
）　ｕ本願の双安定ロータリーソレノイドの動作特性を
示すものでめ９、横軸は、第７図（Ａ）の場合はストロ
ークＢ、、第７図（Ｂ）、　（Ｃ）の場合は回転角αを
表わし、縦軸は第７図（Ａ）の場合は動作力Ｆ１第７図
（１９，（Ｃ）の場合は動作トルクＴｉ示すものである
。又、一点鎖線は無通電の場合、実線は通電時の特性を
示す。又、点Ａは起動点、矢印は動作方向を示す。尚、
磁心ダ、Ｚ′及び／４ｔ１層の円弧面クー／、グ′−／
、厚−７、／クー／の大きさは必要な特性に応じて任意
に設定し得るものでアリ、各各の対向面積の変化がロー
タータの回転角度に対して一定位相ずれた状態となって
おり、少なくともその内の２つが相互に変化しているこ
とが本発明のロータリールノイドの特性を向上させる上
で大きな効果を上げている。FIG. 7 is a graph showing the operating characteristics of the solenoid. Figure 7 (A) shows a conventional direct-acting bistable solenoid;
B) is a conventional bistable rotary solenoid, Fig. 7 (C
) This shows the operating characteristics of the bistable rotary solenoid of the present application.The horizontal axis is the stroke B in the case of Fig. 7 (A), and the rotation angle in the case of Fig. 7 (B) and (C). The vertical axis represents the operating force F1 in the case of Fig. 7 (A), and the operating torque Ti in the case of (C).Also, the one-dot chain line indicates the operating torque Ti in the case of no energization, and the solid line indicates the characteristics when energized. Also, point A is the starting point, and the arrow indicates the direction of operation.
The circular arc surface of the magnetic core Da, Z' and /4t1 layer Ku/, Gu'-/
, thickness -7, and /ku/ can be set arbitrarily depending on the required characteristics, and the change in each opposing area is in a state with a certain phase shift with respect to the rotation angle of the rotator. The mutual variation of at least two of them is highly effective in improving the characteristics of the rotary lunoid of the present invention.

（ト）発明の効果 △ 積の変化により回転力を得るという新しい考え方のもの
でろり、いわゆるギャップの変化はなく、構造も簡単で
効率も従来のものと比較して４〜５倍と大巾に高いもの
でロシ、その用途は広く、本発明の効果は極めて著しい
。(g) Effects of the invention △ It is based on a new concept of obtaining rotational force by changing the product, so there is no change in the so-called gap, the structure is simple, and the efficiency is 4 to 5 times greater than that of the conventional one. It has a wide range of uses, and the effects of the present invention are extremely remarkable.

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

第１図は本発明の一実施例の構造を示す正断面図であり
、第２図はその正断面図、第５図はその動作を示す模式
正面図、第４図は磁心と永久磁石の対向面の変化金示で
グラフであり、第５図は本発明の他の実施例の構造を示
で正断面図、第６図はその磁心と永久磁石の対向面の変
化を示すグラフ、第７図は動作特性を示すグラフである
。 ／・・・・・・ヨーク、λ・・・・・・補助磁心、３・
・・・・・鉄心、グ・・・・・・磁心、！・・・・・・
コイル、ｇ・・・・・・／ヤフト、？・・・・・・永久
磁石、９・・・・・・ローター、厚・・・・・・磁心。 特許出願人　　国際技術開発株式会社 ／・・・ヨーク、コ・・・補助磁心、３・　鉄心グ・・
・磁心、！・・・コイル、ｔ・・・・・永久磁石り・・
−・・ローター ！！４１／／７１０　　　グ′Fig. 1 is a front sectional view showing the structure of an embodiment of the present invention, Fig. 2 is a front sectional view thereof, Fig. 5 is a schematic front view showing its operation, and Fig. 4 is a diagram of the magnetic core and permanent magnet. FIG. 5 is a front sectional view showing the structure of another embodiment of the present invention, and FIG. 6 is a graph showing changes in the opposing surface of the magnetic core and permanent magnet. FIG. 7 is a graph showing the operating characteristics. /... Yoke, λ... Auxiliary magnetic core, 3.
...Iron core, G...Magnetic core!・・・・・・
Coil, g.../Yaft,? ...Permanent magnet, 9 ...Rotor, thickness ...Magnetic core. Patent applicant: Kokusai Technological Development Co., Ltd./...Yoke, Co...Auxiliary magnetic core, 3. Iron core...
·core,! ...Coil, T...Permanent magnet...
-Rotor! ! 41//710 g'

Claims (2)

【特許請求の範囲】[Claims] （１）円周上に一対の円弧状磁極面を有するローターと
、該円周に対向する２個の磁心と、１個の補助磁心とか
らなるステータを有し、該２個の磁心の各々に励磁コイ
ルを設けると共に補助磁心とヨークで結合し、前記ロー
ターの磁極面と２個の磁心及び補助磁心の３面との対向
面積の内少なくとも２面が、ローターの１８０°以内の
回転にともなつて、相補的に変化するごとく構成したこ
とを特徴とする双安定ロータリーソレノイド。(1) It has a stator consisting of a rotor having a pair of arc-shaped magnetic pole faces on the circumference, two magnetic cores facing the circumference, and one auxiliary magnetic core, and each of the two magnetic cores is provided with an excitation coil and coupled to the auxiliary magnetic core by a yoke, so that at least two of the opposing areas between the magnetic pole surface of the rotor and the three surfaces of the two magnetic cores and the auxiliary magnetic core are arranged such that when the rotor rotates within 180 degrees, A bistable rotary solenoid characterized by being configured to change in a complementary manner. （２）ローターの磁極面とステーターの２個の磁心及び
補助磁心の３面との対向面積の総和が、ローター回転範
囲内の両端において大きくなるごとく構成したことを特
徴とする特許請求の範囲第１項記載の双安定ロータリー
ソレノイド。(2) Claim 1 characterized in that the sum of the opposing areas of the magnetic pole surface of the rotor and the three surfaces of the two magnetic cores and the auxiliary magnetic core of the stator increases at both ends within the rotor rotation range. The bistable rotary solenoid according to item 1.
JP25247084A 1984-11-29 1984-11-29 Bistable rotary solenoid Granted JPS61129804A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25247084A JPS61129804A (en) 1984-11-29 1984-11-29 Bistable rotary solenoid

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25247084A JPS61129804A (en) 1984-11-29 1984-11-29 Bistable rotary solenoid

Publications (2)

Publication Number Publication Date
JPS61129804A true JPS61129804A (en) 1986-06-17
JPH0219608B2 JPH0219608B2 (en) 1990-05-02

Family

ID=17237826

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25247084A Granted JPS61129804A (en) 1984-11-29 1984-11-29 Bistable rotary solenoid

Country Status (1)

Country Link
JP (1) JPS61129804A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05182682A (en) * 1991-12-27 1993-07-23 Honda Motor Co Ltd Humidifying gas preheater and preheating method thereof for fuel cell system
JP2008047648A (en) * 2006-08-11 2008-02-28 Hamanako Denso Co Ltd Rotary solenoid
WO2020004514A1 (en) * 2018-06-26 2020-01-02 ミツミ電機株式会社 Rotary reciprocating drive actuator

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05182682A (en) * 1991-12-27 1993-07-23 Honda Motor Co Ltd Humidifying gas preheater and preheating method thereof for fuel cell system
JP2008047648A (en) * 2006-08-11 2008-02-28 Hamanako Denso Co Ltd Rotary solenoid
WO2020004514A1 (en) * 2018-06-26 2020-01-02 ミツミ電機株式会社 Rotary reciprocating drive actuator
JPWO2020004514A1 (en) * 2018-06-26 2021-06-10 ミツミ電機株式会社 Rotary reciprocating drive actuator
EP3817204A4 (en) * 2018-06-26 2022-03-09 Mitsumi Electric Co., Ltd. Rotary reciprocating drive actuator
US11909291B2 (en) 2018-06-26 2024-02-20 Mitsumi Electric Co., Ltd. Rotary reciprocating drive actuator with movable element and magnets and rotating mirror

Also Published As

Publication number Publication date
JPH0219608B2 (en) 1990-05-02

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