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JPS5843883B2 - electromagnet device - Google Patents
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JPS5843883B2 - electromagnet device - Google Patents

electromagnet device

Info

Publication number
JPS5843883B2
JPS5843883B2 JP51148240A JP14824076A JPS5843883B2 JP S5843883 B2 JPS5843883 B2 JP S5843883B2 JP 51148240 A JP51148240 A JP 51148240A JP 14824076 A JP14824076 A JP 14824076A JP S5843883 B2 JPS5843883 B2 JP S5843883B2
Authority
JP
Japan
Prior art keywords
armature
iron core
magnetic pole
valve
tip
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
Application number
JP51148240A
Other languages
Japanese (ja)
Other versions
JPS5372166A (en
Inventor
正次 山内
隆 棚橋
滋 白井
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 JP51148240A priority Critical patent/JPS5843883B2/en
Publication of JPS5372166A publication Critical patent/JPS5372166A/en
Publication of JPS5843883B2 publication Critical patent/JPS5843883B2/en
Expired legal-status Critical Current

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  • Electromagnets (AREA)

Description

【発明の詳細な説明】 本発明は励磁コイルの中心に鉄芯を設け、鉄芯の一端に
継鉄が固着され、前記鉄芯か又は継鉄に接極子が支点支
持され、前記接極子が揺動する電磁石装置に係り、その
目的とするところは電流に対して比例的に、かつ安定し
て動作し、耐久信頼性の高い電磁石装置を提供すること
にある。
Detailed Description of the Invention The present invention provides an iron core at the center of an excitation coil, a yoke is fixed to one end of the iron core, an armature is supported as a fulcrum on the iron core or the yoke, and the armature is The purpose of the oscillating electromagnet device is to provide an electromagnet device that operates stably in proportion to current and has high durability and reliability.

ことに弁として応用すれば応答性が速く、遠隔制御の可
能な工業的に極めて有用なものである。
In particular, when applied as a valve, it has quick response and can be controlled remotely, making it extremely useful industrially.

第1図は比例電磁石装置ではないが本発明と構成的に近
いと思われる従来例の基本構成図で、101は鉄芯、1
02は励磁コイル、103は継鉄、104は接極子、1
05はアーム、106は弁、10γは弁座、108はボ
ディ、109はハウジング: 110はガスケット、1
11はスプリングである。
Fig. 1 is a basic configuration diagram of a conventional example that is not a proportional electromagnet device but is considered to be structurally similar to the present invention, in which 101 is an iron core;
02 is an excitation coil, 103 is a yoke, 104 is an armature, 1
05 is an arm, 106 is a valve, 10γ is a valve seat, 108 is a body, 109 is a housing, 110 is a gasket, 1
11 is a spring.

動作は励磁コイル102に所定の電流を人、切すること
により、接極子104が鉄芯101に吸着され、あるい
は解放されて、揺動し、弁106を弁座107に対して
開閉するもので、比例的な動作を得ることは困難であっ
た。
In operation, by turning off a predetermined current to the excitation coil 102, the armature 104 is attracted to or released from the iron core 101, swinging, and opening/closing the valve 106 relative to the valve seat 107. , it was difficult to obtain proportional behavior.

本発明は従来の電磁石装置がいわゆる0N−OFF動作
であるのに対して、比例的な動作を安定して得ようとす
るものである。
The present invention aims to stably obtain proportional operation, whereas conventional electromagnetic devices operate in a so-called ON-OFF manner.

そのための構成として、本発明は、励磁コイルを具備す
る鉄芯と、前記鉄芯を固定する継鉄と、この継鉄の一端
に支点を介して支持され復帰ばねと鉄芯の吸引力との作
用力で動作する接極子を設け、前記鉄芯の吸引作用面に
は、動作開始位置における接極子先端部の回転動作円弧
接線に対して傾斜し、かつその傾斜方向が、前記接極子
が鉄芯吸引方向に回動するとき、前記接極子の先端部と
鉄芯磁極面との空隙がわずかずつ狭まる方向とした傾斜
面を設け、前記傾斜した鉄芯磁極面と、前記接極子の先
端部との間で主動作空隙を形成するとともに、前記鉄芯
または接極子の吸引力作用面を凸状にしたものである。
As a configuration for this purpose, the present invention includes an iron core provided with an excitation coil, a yoke that fixes the iron core, a return spring supported via a fulcrum at one end of the yoke, and an attractive force of the iron core. An armature operated by acting force is provided, and the suction surface of the iron core is inclined with respect to the circular arc tangent of the tip of the armature at the operation start position, and the direction of the inclination is such that the armature is made of iron. An inclined surface is provided in such a direction that the gap between the tip of the armature and the iron core magnetic pole surface gradually narrows when the armature rotates in the core attracting direction, and the inclined iron core magnetic pole surface and the tip of the armature A main operating gap is formed between the iron core and the armature, and the attractive force acting surface of the iron core or armature is made convex.

以下、本発明の一実施例につき、図面に沿って詳細に説
明する。
Hereinafter, one embodiment of the present invention will be described in detail with reference to the drawings.

第2図、第3図において、1は一端に切欠きAを有する
鉄芯、2は励磁コイル、3は一端を鉄芯1に固着し、他
端を月形にしたL字状継鉄で、ケース12に収納しであ
る。
In Figures 2 and 3, 1 is an iron core with a notch A at one end, 2 is an excitation coil, and 3 is an L-shaped yoke with one end fixed to the iron core 1 and the other end shaped like a moon. , and is housed in a case 12.

4は接極子で、一部に凹部Bを設け、前記継鉄3の月形
部にかみ合って支点を形威し、鉄芯1に近い部分に弁取
付具6を介して弁5が傾斜自在に遊着され、他端にはば
ね掛具7.復帰ばね8.ばね力調節ねじ9.ナツト10
を設け、接極子4に作用するばね力を調節出来る構造に
なっており、調節後シール材11を充填する。
Reference numeral 4 denotes an armature, which has a recess B in a part thereof and forms a fulcrum by engaging with the moon-shaped part of the yoke 3, and a valve 5 can be freely tilted through a valve fitting 6 in a part close to the iron core 1. and a spring hook 7 on the other end. Return spring 8. Spring force adjustment screw9. Natsu 10
It has a structure in which the spring force acting on the armature 4 can be adjusted, and the sealing material 11 is filled after adjustment.

13.14は非磁性材よりなるストッパである。13 and 14 are stoppers made of non-magnetic material.

鉄芯1の切欠きAは、接極子4が鉄芯1の吸引する方向
へ回動するとき、接極子の磁極面Cと鉄芯磁極面りとの
空隙が徐々に狭まるように傾斜していることが重要であ
る。
The notch A of the iron core 1 is inclined so that when the armature 4 rotates in the direction in which the iron core 1 is attracted, the gap between the magnetic pole face C of the armature and the iron core magnetic pole face gradually narrows. It is important to be present.

また、接極子の磁極面Cは鉄芯1の軸線方向から見て平
面図である第2図に示すように、円弧的凸状に形成され
ている。
Further, the magnetic pole surface C of the armature is formed in an arcuate convex shape as shown in FIG. 2, which is a plan view when viewed from the axial direction of the iron core 1.

次に動作を説明する。Next, the operation will be explained.

第3図の状態は励磁コイル2に通電していない時で、復
帰ばね8の初荷重により弁5は仮想線で示した弁座に押
圧されている。
The state shown in FIG. 3 is when the excitation coil 2 is not energized, and the valve 5 is pressed against the valve seat indicated by the phantom line by the initial load of the return spring 8.

励磁コイル2の電流をしだいに増加してゆくと磁気的吸
引力もしだいに増加しやがて弁5は弁座より浮上する。
As the current of the excitation coil 2 is gradually increased, the magnetic attraction force is also gradually increased, and the valve 5 eventually rises above the valve seat.

そして接極子4の先端がストップ14に当接するまで励
磁コイル2の電流による磁気的吸引力と復帰ばね8の力
が吻合ながらいわば比例的、連続的に動作し、従って弁
5は比例的、連続的に弁座の開度を変える。
Then, until the tip of the armature 4 comes into contact with the stop 14, the magnetic attraction force due to the current of the excitation coil 2 and the force of the return spring 8 are anastomosed and operate proportionally and continuously, so to speak, the valve 5 operates proportionally and continuously. change the opening degree of the valve seat.

電流を減少させる場合も同様であり、勿論弁の開度を任
意の位置で保持することもできる。
The same applies when reducing the current, and of course the opening degree of the valve can also be maintained at an arbitrary position.

この比例的動作を可能にした最も重要な点は、鉄芯1の
磁極部に接極子4に対してやや傾いた切欠き部Aを作り
、接極子4の先端が大体においてその切欠き部Aの内側
で動作するようにしたことにある。
The most important point that made this proportional operation possible is that a notch A is formed in the magnetic pole part of the iron core 1, which is slightly inclined with respect to the armature 4, and the tip of the armature 4 is approximately located in the notch A. The reason is that it works inside the .

つまり接極子4が鉄芯1が吸引する方向へ回動するとき
、接極子磁極面Cとの空隙が徐々に狭まるように傾斜さ
せた鉄芯磁極面りを設け、この鉄芯1の傾斜磁極面りと
接極子の磁極面との間で主動作空隙を形成しているので
、励磁コイル2の電流をある値一定のまま、接極子4の
回動位置、すなわち弁ストロークを変位させても、吸引
力が接極子4に回転トルクとして作用する分力は、はぼ
一定の回転トルクを保つことができるからである。
In other words, when the armature 4 rotates in the direction that the iron core 1 attracts, the iron core magnetic pole face is inclined so that the air gap with the armature magnetic pole face C gradually narrows, and this inclined magnetic pole of the iron core 1 is provided. Since the main operating gap is formed between the face and the magnetic pole surface of the armature, even if the rotational position of the armature 4, that is, the valve stroke, is changed while the current of the exciting coil 2 remains constant, This is because the component force of the attractive force acting on the armature 4 as rotational torque can maintain an approximately constant rotational torque.

なぜならば接極子4が鉄芯1に吸引される方向に回動す
ると鉄芯1と接極子4の両磁極間空隙はわずかずつ小さ
くなり、磁気抵抗が減少して両磁極間吸引力は、空隙の
略2乗に比例して増大するが、鉄芯1つの磁極面りが傾
斜しているため、磁極面に垂直方向の力は増大しても、
接極子4を回動しようとするトルクに寄与する比率は次
第に減少し、結果的に弁ストロークの変位に対して、接
極子4を回動しようとする回転力を、あまり変化させな
い構成が可能となるものである。
This is because when the armature 4 rotates in the direction in which it is attracted to the iron core 1, the air gap between the two magnetic poles of the iron core 1 and the armature 4 becomes smaller little by little, the magnetic resistance decreases, and the attractive force between the two magnetic poles is reduced by the air gap. However, since the magnetic pole face of one iron core is inclined, even if the force perpendicular to the magnetic pole face increases,
The ratio contributing to the torque that attempts to rotate the armature 4 gradually decreases, and as a result, it is possible to create a configuration in which the rotational force that attempts to rotate the armature 4 does not change much with respect to the displacement of the valve stroke. It is what it is.

また接極子磁極部Cを鉄芯1の軸線方向から見て、つま
り平面図である第2図で見て円弧的凸状に形成している
ので、接極子4が左右に横ぶれしようとしても、接極子
4の凸状先端と鉄芯1との空隙が最も小さくなる位置す
なわち、中心に安定しようとするように作用しようし、
継鉄3の月形エツジと接極子4の■溝の摩耗も変則的に
なったすせず耐久信頼性が向上するとともに安定した特
性が得られる。
Furthermore, since the armature magnetic pole portion C is formed in an arcuate convex shape when viewed from the axial direction of the iron core 1, that is, when viewed from the top view of FIG. , it acts to stabilize at the position where the gap between the convex tip of the armature 4 and the iron core 1 is the smallest, that is, at the center,
The wear of the moon-shaped edge of the yoke 3 and the ■groove of the armature 4 also becomes irregular, and durability and reliability are improved and stable characteristics are obtained.

第6図は接極子4と鉄芯1のいずれの磁極面も仮に平面
で構成した場合の不都合を説明するための図で、第2図
と同じ方向から見た鉄芯1と接極子4を示したものであ
る。
FIG. 6 is a diagram for explaining the disadvantages if both the magnetic pole surfaces of the armature 4 and the iron core 1 are configured as flat surfaces. This is what is shown.

仮に第6図のように鉄芯1と接極子4の両磁極部とも平
面の場合、部品の寸法誤差や組立誤差のためギャップt
とギャップt′が同一でなく、どちらかが狭いとより接
極子4の横ぶれしようとする力が増え、継鉄3の月形エ
ツジと接極子4の■溝の摩耗が変則的に片寄り、接極子
4と継鉄3のかみ合せ部がはずれてしまう不都合がある
If both the magnetic pole parts of the iron core 1 and the armature 4 are flat as shown in Fig. 6, the gap t will be reduced due to dimensional errors and assembly errors of the parts.
and the gap t' are not the same, and if either is narrower, the force that tends to cause the armature 4 to wobble laterally will increase, and the wear of the moon-shaped edge of the yoke 3 and the ■ groove of the armature 4 will be irregularly uneven. , there is an inconvenience that the engagement portion between the armature 4 and the yoke 3 may come off.

第4図は第1図に示した従来の開閉電磁弁の静吸引力特
性、第5図は本発明一実施例の静吸引力特性である。
FIG. 4 shows static attraction force characteristics of the conventional open/close solenoid valve shown in FIG. 1, and FIG. 5 shows static attraction force characteristics of an embodiment of the present invention.

第4図の従来例の特性図において、実線■112+I3
はそれぞれの電流(II <I2 <i3)における静
吸引力特性、破線はスプリング111のストロークと力
の関係を示す。
In the characteristic diagram of the conventional example shown in Fig. 4, the solid line ■112+I3
indicates the static attraction force characteristics at each current (II < I2 < i3), and the broken line indicates the relationship between the stroke of the spring 111 and the force.

横軸の点Scは弁閉IJ=位置、点Soは弁全開位置、
縦軸の点Pcは横軸の点Scにおけるばねの力すなわち
弁閉1h力である。
Point Sc on the horizontal axis is the valve closed IJ = position, point So is the valve fully open position,
Point Pc on the vertical axis is the spring force at point Sc on the horizontal axis, that is, the valve closing 1h force.

従来の開閉電磁弁ではスプリング111の力より常に大
きな磁気的吸引力の得られる電流■3を人、切して使用
するのであるが、本発明を対応して、今仮りに電流を0
からしだいに増加する場合の動作を考えると、スプリン
グ111の弁閉重力Pcと等しい吸引力の得られる電流
■、以下では弁は静屯しているが、■1 より弁は浮上
を開始する。
In conventional open/close solenoid valves, the current (3), which always produces a magnetic attraction force greater than the force of the spring 111, is turned off.
Considering the operation when the current gradually increases from 1 to 1, the valve is static below the current (2) which provides an attractive force equal to the valve-closing gravity Pc of the spring 111, but from (1) the valve starts to float.

しかしさらに少し電流を増加し■2になるとスプリング
111との吻合点を失い■2より犬なる電流では瞬時に
弁は全開位置Soまで移動してしまう。
However, when the current is increased a little further to (2), the anastomosis point with the spring 111 is lost, and (2) the valve instantly moves to the fully open position So at a current that is even lower than (2).

第5図は本発明一実施例の特性図で、図中の記号は第4
図と同じである。
FIG. 5 is a characteristic diagram of one embodiment of the present invention, and the symbol in the figure is the fourth
Same as the figure.

図から明らかな通り第5図の吸引力特性は第4図に比べ
て極めて平坦であり、弁閉d−力Pcと同じ吸引力を得
る電流■1から弁を全開する電流12 までストローク
全域にわたって電流■1(It≦■1 ≦I2 )で
ばねの力と均合う事がわかる。
As is clear from the figure, the attraction force characteristics in Figure 5 are extremely flat compared to those in Figure 4, and over the entire stroke from current 1 which obtains the same attraction force as the valve closing d-force Pc to current 12 which fully opens the valve. It can be seen that the current is balanced with the force of the spring at ■1 (It≦■1≦I2).

この吸引力特性が平坦あるいは左下りの特性にどうして
なるのかについて、前記本発明実施例の動作の説明と合
わせて行なったが、鉄芯1と接極子4と吸引力との関係
を簡略モデル化した第11図を用いて今一度説明する。
The reason why this attractive force characteristic becomes flat or downward to the left has been explained in conjunction with the explanation of the operation of the embodiment of the present invention, but the relationship between the iron core 1, the armature 4, and the attractive force is simply modeled. This will be explained once again using FIG. 11.

動作開始位置の接極子4は実線で描いた。The armature 4 at the operation start position is drawn with a solid line.

この状態で傾斜した鉄芯磁極面りに垂直な方向の吸引力
Foを生じるコイル電流■1 を通電した時、接極子4
を支点B中心に回動しようとする分力はf。
In this state, when the coil current ■1 is energized, which generates an attractive force Fo in the direction perpendicular to the inclined iron core magnetic pole surface, the armature 4
The component of force that tries to rotate around fulcrum B is f.

となる。becomes.

つまりこのf。が第5図のグラフ縦軸の吸引力である。In other words, this f. is the attraction force on the vertical axis of the graph in FIG.

同一コイル電流■、において接極子4が2点鎖線で示し
た位置にある場合、鉄芯磁極面りと接極子4の先端部C
との空隙つまりそれぞれの吸引作用面の磁気ギャップが
短くなり、磁極面りに垂直な方向の吸引力はFl と、
前記F。
When the armature 4 is at the position shown by the two-dot chain line at the same coil current ■, the iron core magnetic pole surface and the tip C of the armature 4
The air gap between the magnetic poles, that is, the magnetic gap between each attraction surface becomes shorter, and the attraction force in the direction perpendicular to the magnetic pole surface becomes Fl.
Said F.

よりも大きくなる。becomes larger than

しかし接極子4を回動させる方向の分力f1 は、前記
f。
However, the component force f1 in the direction of rotating the armature 4 is equal to the above-mentioned f.

とほとんど同じかあるいはやや小さくなる。almost the same or slightly smaller.

これは接極子4が支点Bを中心に円弧運動をし、先端部
CがRの線上を移動して行くにしたがって、接極子4が
鉄芯磁極面りに垂直な方向に近づいていくためである。
This is because the armature 4 moves in an arc around the fulcrum B, and as the tip C moves on the line R, the armature 4 approaches the direction perpendicular to the iron core magnetic pole face. be.

理解しやすいために接極子4を破線で示した位置、すな
わち磁極面りに垂直になる回動位置を説明すると、磁極
面Aと先端部Bとの磁気的空隙は最も小さくなるため、
磁極面りに垂直方向の吸引力F2は最大となる。
To make it easier to understand, the position of the armature 4 indicated by a broken line, that is, the rotating position perpendicular to the magnetic pole surface, will be explained. Since the magnetic gap between the magnetic pole surface A and the tip B is the smallest,
The attractive force F2 in the direction perpendicular to the magnetic pole surface is maximum.

しかしこの時、接極子4を回動させる方向の分力はなく
なる。
However, at this time, the component force in the direction of rotating the armature 4 disappears.

実使用上はこの位置にいたる手前で動作範囲を規制する
ように第3図のようにストッパ14を設けている。
In actual use, a stopper 14 is provided as shown in FIG. 3 to restrict the operating range before reaching this position.

第7図、第8図、第9図、第10図は本発明の他の実施
例で特に鉄芯1と接極子4とストッパ14だけを斜視図
で示し、他の構成要素は省略しである。
7, 8, 9, and 10 show other embodiments of the present invention, in particular only the iron core 1, armature 4, and stopper 14 are shown in perspective views, and other components are omitted. be.

第7図は接極子4の磁極面形状を山形凸状に形成したも
ので、第2図で円孤形凸状にしたのと同様に接極子4の
横ぶれの防止作用があり、■溝を摩耗させることが防1
.でき長期間安定して作動する耐久信頼性の高い電磁石
装置が可能となる。
In Fig. 7, the magnetic pole surface of the armature 4 is formed into a chevron-shaped convex shape, which has the same effect as the arc-shaped convex shape shown in Fig. 2, and has the effect of preventing sideways wobbling of the armature 4. 1. Prevents wear.
.. This makes it possible to create a highly durable and reliable electromagnetic device that operates stably for a long period of time.

同様に第8図は鉄芯1の磁極面を円孤形凸状に、第9図
は同じく鉄芯1の磁極面を山形凸状にそれぞれ形成した
もので、第7図と同様の作用効果が得られる。
Similarly, Fig. 8 shows the magnetic pole surface of the iron core 1 having a circular convex shape, and Fig. 9 shows the magnetic pole face of the iron core 1 having a chevron-shaped convex shape. is obtained.

第10図は鉄芯1の磁極面と接極子4の磁極面いずれも
円孤形凸状に形成したもので、この構成においても同様
の効果を得ることができる。
In FIG. 10, both the magnetic pole surface of the iron core 1 and the magnetic pole surface of the armature 4 are formed in a circular convex shape, and the same effect can be obtained with this configuration.

また本発明の電磁石装置は励磁コイルの電流に対して、
比較的大きいストロークの円滑で安定な比例的動作を接
極子4が行なえるものであり、その接極子4に弁5を弁
取付具6を介して遊着し、接極子4の動きに弁5を連動
させる構成であることから、例えば本発明を弁に応用し
た場合給湯用ガス瞬間湯沸器のバーナへのガス供給経路
に取付は湯温をサーミスタで検知して制御すれば、負荷
の変動に関係なく一定温度の温水が得られる。
Furthermore, the electromagnet device of the present invention has
The armature 4 is capable of smooth and stable proportional movement with a relatively large stroke, and a valve 5 is loosely attached to the armature 4 via a valve fitting 6, so that the movement of the armature 4 causes the valve 5 to move smoothly and stably. For example, if the present invention is applied to a valve, it can be installed in the gas supply path to the burner of a gas instantaneous hot water heater.If the water temperature is detected and controlled with a thermistor, load fluctuations can be prevented. Hot water at a constant temperature can be obtained regardless of the temperature.

また従来の液体膨張式比例弁では不可能であった熱源部
から遠く離れて温度を変える事も可能である。
It is also possible to change the temperature far away from the heat source, which was not possible with conventional liquid expansion type proportional valves.

あるいは従来の開閉電磁弁による温度制御で生ずる点火
音、消火音の騒音も解消できる。
Additionally, it is possible to eliminate the ignition and extinguishing noises caused by temperature control using conventional open/close solenoid valves.

以上のように、本発明によれば、励磁コイルを具備する
鉄芯と、継鉄と、この継鉄の一端に支点を介して支持さ
れ、復帰はねと鉄芯の吸引力との作用力で動作する接極
子を設け、前記鉄芯の吸弓作用面には、動作開始位置に
おける接極子先端部の回転動作円弧接線に対して傾斜し
、かつその傾斜の方向が、前記接極子が鉄芯の吸引方向
に回動するとき、前記接極子の先端部と鉄芯磁極面との
空隙がわずかずつ狭まる方向とした傾斜面を設け、前記
傾斜した鉄芯磁極面と、前記接極子の先端部との間で主
動作空隙を形成するとともに、前記鉄芯または接極子の
吸引作用面を凸状に構成したので、接極子の変位に対し
て、はぼ平坦な接極子回転力を維持する吸引力特性が得
られ、大きいストローク範囲において円滑な比例的動作
が得られるだけでなく、接極子の横ふれかなく長期間安
定した作動が可能な高い耐久信頼性が得られるものであ
る。
As described above, according to the present invention, an iron core including an excitation coil, a yoke, a yoke supported at one end of the yoke via a fulcrum, and the action of the return spring and the attraction force of the iron core. The armature is provided with an armature that operates at an angle, and the armature has a bow-sucking surface of the iron core that is inclined with respect to a tangent to the rotational arc of the tip of the armature at the operation start position, and the direction of the inclination is such that the armature is made of iron. An inclined surface is provided in such a direction that the gap between the tip of the armature and the iron core magnetic pole surface narrows little by little when the armature rotates in the attraction direction of the core, and the inclined iron core magnetic pole surface and the tip of the armature In addition to forming a main operating gap between the iron core and the armature, the suction surface of the iron core or the armature is configured to have a convex shape, so that a nearly flat armature rotational force is maintained against displacement of the armature. This not only provides attractive force characteristics and smooth proportional operation over a large stroke range, but also provides high durability and reliability that allows stable operation over a long period of time without sideways wobbling of the armature.

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

第1図は従来例の開閉式電磁弁の断面図、第2図は本発
明の実施例を示す電磁石装置の平面図、第3図は断面図
、第4図は従来例の静吸引力特性図、第5図は本発明の
静吸引力特性図、第6図は本発明の一般に考え得る鉄芯
および接極子の不都合な対面状態を説明する平面図、第
7図、第8図第9図および第10図は本発明の他の実施
例の鉄芯および接極子の斜視図、第11図は本発明の吸
引力作用説明図である。 1・・・・・・鉄芯、2・・・・・・励磁コイル、4・
・・・・・接極子、5・・・・・・弁、8・・・・・・
復帰ばね、C・・・・・・接極子の磁極面、D・・・・
・・傾斜磁極面。
Fig. 1 is a sectional view of a conventional open/close type solenoid valve, Fig. 2 is a plan view of an electromagnet device showing an embodiment of the present invention, Fig. 3 is a sectional view, and Fig. 4 is a static attraction force characteristic of the conventional example. 5 is a static attraction force characteristic diagram of the present invention, FIG. 6 is a plan view illustrating a generally conceivable inconvenient facing state of the iron core and armature of the present invention, FIGS. 7, 8, and 9. 10 and 10 are perspective views of an iron core and an armature according to another embodiment of the present invention, and FIG. 11 is a diagram illustrating the effect of the attractive force of the present invention. 1... Iron core, 2... Excitation coil, 4...
... Armature, 5 ... Valve, 8 ...
Return spring, C...Magnetic pole surface of armature, D...
...Slanted magnetic pole surface.

Claims (1)

【特許請求の範囲】[Claims] 1 励磁コイルを具備する鉄芯と、前記鉄芯を固定する
継鉄と、この継鉄の一端に支点を介して支持され復帰は
ねと鉄芯の吸引力との作用力で動作する接極子を設け、
前記鉄芯の吸引作用面には動作開始位置における接極子
先端部の回転動作円弧接線に対して傾斜し、かつその傾
斜方向が前記接極子が鉄芯の吸引方向に回動するとき、
前記接極子の先端部と鉄芯磁極面との空隙がわずかずつ
狭まる方向とした傾斜面を設け、前記傾斜した鉄芯磁極
面と、前記接極子の先端部との間で主動作空隙を形成す
るとともに、前記鉄芯または接極子の吸引力作用面を凸
状に構成した電磁石装置。
1. An iron core equipped with an excitation coil, a yoke that fixes the iron core, and an armature that is supported at one end of the yoke via a fulcrum and operates by the action of the return spring and the attractive force of the iron core. established,
The suction action surface of the iron core is inclined with respect to the circular arc tangent of the rotational movement of the tip of the armature at the operation start position, and the direction of the inclination is when the armature rotates in the suction direction of the iron core,
An inclined surface is provided in a direction in which a gap between the tip of the armature and the iron core magnetic pole surface gradually narrows, and a main operating gap is formed between the inclined iron core magnetic pole surface and the tip of the armature. In addition, an electromagnet device in which an attractive force acting surface of the iron core or armature is configured to have a convex shape.
JP51148240A 1976-12-08 1976-12-08 electromagnet device Expired JPS5843883B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP51148240A JPS5843883B2 (en) 1976-12-08 1976-12-08 electromagnet device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP51148240A JPS5843883B2 (en) 1976-12-08 1976-12-08 electromagnet device

Publications (2)

Publication Number Publication Date
JPS5372166A JPS5372166A (en) 1978-06-27
JPS5843883B2 true JPS5843883B2 (en) 1983-09-29

Family

ID=15448369

Family Applications (1)

Application Number Title Priority Date Filing Date
JP51148240A Expired JPS5843883B2 (en) 1976-12-08 1976-12-08 electromagnet device

Country Status (1)

Country Link
JP (1) JPS5843883B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63147658A (en) * 1986-12-11 1988-06-20 Seikosha Co Ltd Printing head

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5059556U (en) * 1973-09-28 1975-06-02

Also Published As

Publication number Publication date
JPS5372166A (en) 1978-06-27

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